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GENERAL INFORMATION
Welcome to CLEO®/Europe-IQEC at Laser 2013 02Conference Structure and Technical Sessions 02Short Courses at a Glance 04Conference Days at a Glance 05How to Find the Room? 10Sessions at a Glance 10How to Read the Session Codes? 16Topics 17Committees 21O!cial Congress Opening 28Prizes and Awards 28Poster Sessions 28Speakers' Information 29Technical Focus Sessions 29Short Courses 29Laboratory Tours 29Reception and Social Events 30Exhibition Information 30Application Panels 30On site Facilities for Attendees 30Conference Venue 32How to reach the ICM Centre 32Conference Registration 33
Cancellation 33Note to Exhibitors 33Registration Hours 33
Hotel Information 34Transportation in Munich 34Munich, Germany 34Conference Management 36Language 36
TECHNICAL PROGRAMME
Short Courses 37Technical Focus sessions 44Plenary sessions 45Tutorial Talks 47Keynote Talks 48Invited Talks 49
SundayOral Sessions 58Poster Sessions 86
MondayOral Sessions 94Poster Sessions 114
TuesdayOral Sessions 122Poster Sessions 138
WednesdayOral Sessions including Postdeadlines 146Poster Sessions 168
ThursdayOral Sessions 176Poster Sessions 196
Authors’ Index 204
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Welcome to the 2015 Conference on Lasers and Electro-Optics Europe & the European Quantum Electronics Conference (hereafter CLEO®/Europe-EQEC 2015) at the World of Photonics Congress 2015
Following on from the very successful previous conferences held in Amsterdam (1994), Hamburg (1996), Glasgow (1998), Nice (2000) and Munich (2003, 2005, 2007, 2009, 2011, 2013), the General and Programme Chairs warmly welcome you to CLEO®/Europe-EQEC 2015 conference, which is being held in Munich from June 21 - 25, 2015.
We extend a special welcome to postgraduate and PhD students attending, and we wish them every success, especially if this is their first participation in a major scientific conference.!e CLEO®/Europe-EQEC conference series has established a strong tradition as the largest, most comprehensive and prestigious gathering of op-tics and photonics researchers and engineers in Europe. With technical co-sponsorship provid-ed by the European Physical Society (EPS), the Institute of Electrical and Electronics Engineers (IEEE) Photonics Society and the Optical Society (OSA), CLEO®/Europe and EQEC has a strong international presence in the complementary research areas of laser science, photonics and quantum electronics. More specifically, CLEO®/Europe emphasizes applied physics, optical engi-neering and applications of photonics and laser technology, whereas EQEC addresses more ba-sic research in laser physics, nonlinear optics and quantum optics.!is combination provides a unique forum to benefit from informative overviews and discuss recent advances in a wide spectrum of topics, from fundamental light-matter interactions and new sources of coherent light to technology de-velopment, system engineering and applications in industry, science and medicine. Over five days CLEO®/Europe-EQEC 2015 will showcase over 1600 technical contributions in the form of oral presentations in parallel sessions and posters from university, research organisations and in-dustry, drawn from all countries around the world and will provide an unparalleled opportunity to bring together scientists, engineers and end-us-ers of laser and photonics technology under the same roof.Topics will cover a very wide spectrum of tech-nical areas including the latest developments in laser sources, materials, ultrafast science, fi-bre optics, nonlinear optics, terahertz sources,
high-field physics, optical telecommunications, nanophotonics and biophotonics, fundamentals of quantum optics, quantum information, atom optics, ultrafast optics, nonlinear phenomena and self-organization, plasmonics, and metamaterials. In 2015 two new topical areas will concern pho-tonics in defense and security and theoretical and computational photonics.Particular highlights of the 2015 programme will be a series of special symposia. Additionally a series of joint sessions held in cooperation with co-located conferences will be organised. See de-scriptions in the Conference Structure.Also as you certainly know, 2015 is a special year proclaimed International Year of Light and Light-Based Technologies. Special events add-ed on this occasion made us change the structure of the conference especially on Monday where half sessions are built in order to fit in the very tight schedule.As in former years, the meeting will be comple-mented by LASER 2015 World of Photonics, the world’s largest tradeshow of laser and optical technology, which will provide researchers with the opportunity to see the latest developments in a very wide range of laser sources, optical and photonics products, and components.CLEO®/Europe-EQEC is co-located with a num-ber of smaller specialist conferences and topical meetings, including:• ECBO 2015 - European Conferences on Bi-omedical Optics organised by SPIE with OSA support.
• LiM 2015 - Lasers in Manufacturing organised by WLT (German Scientific Laser Society).
• EOS Topical Meetings organized by the EOS (European Optical Society)
• Optical Metrology 2015 is organized by SPIE Europe Ltd
All the co-located conferences will share registra-tion and allow delegates to attend sessions.
Conference Structure and Technical Sessions
CLEO®/Europe-EQEC consists of a large number of technical presentations in a number of di"er-ent formats:A Plenary Talk is a broad-scope, 45 or 60-min-ute long talk given by a world-leading scientist and accessible to a general technical audience including conference attendees, exhibitors, and exhibit visitors. Plenary talks are not held in parallel with other sessions, allowing maximum possible attendance. On the occasion of the 2015 International Year of Light and Light-Based Technologies, it is our pleasure to feature five ple-nary talks including four Nobel Prize laureates. Tutorials (60 minute talk) and Keynote Pres-entations (45 minute talk) are also given by the world leaders in particular technical areas. !ey are generally directed at a more specific audience, and are thus delivered in parallel with other ses-sions. Keynotes provide a survey of exciting recent developments, and Tutorials are particularly val-uable for those unfamiliar with a particular field.An attractive feature of the CLEO®/Europe technical programme is the Tech-Focus format. Tech-Focus sessions concentrate on selected photonics applications of industrial importance. CLEO®/Europe-EQEC 2015 features two Tech-Focus sessions on Ultrafast Solid-state and Fibre Lasers and Materials Structuring Using Short Laser Pulses jointly held with LiM 2015, which showcase this exciting field through pres-entations from leading academic and industrial researchers. Both sessions take place on Tues-day a#ernoon.Additionally four other joint sessions are held with co-located conferences:• Two sessions on Bioimaging and Optical Ma-nipulation of Biomatter jointly organised with ECBO take place on Wednesday morning.
2015 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference
CLEO®/Europe - EQEC 2015Munich, ICM Congress Centre, Germany, 21 - 25 june 2015
www.cleoeurope.org
Sponsored by• European Physical Society
Quantum Electronics and Optics Division• IEEE Photonics Society• The Optical Society
CLEO
EUROPE
2015EQEC
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Welcome
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• A session on Diagnostics and Control jointly organised with LiM 2015 takes place on Tues-day morning.
• A session on Computational Photonics for Metrology Applications jointly organised with SPIE/Optical Metrology takes place on Mon-day a#ernoon.
Other very much appreciated CLEO®/Eu-rope-EQEC meetings are the special Symposia settled to anticipate and capture emerging fields in optics by giving emphasis to fast developing, well defined topics. Five such symposia have been identified for CLEO®/Europe-EQEC 2015:• JSI -$Joint Symposium on Light Management in Photovoltaics
• JSII - Joint Symposium on Photonic Lab-on-a-chip Biosensors
• JSIII - Joint Symposium on Laser-driven Acceleration
• JSIV - Joint Symposium on Optics in Graphene and Other Two-dimensional Materials
• JSV - Joint Symposium on Integrated Quantum Optics
CLEO®/Europe-EQEC 2015 will also present ten Short Courses:• Ultrashort Pulse Characterization presented by Selçuk Aktürk (Istanbul Technical Univer-sity, Istanbul, Turkey).
• Optical Parametric Oscillators presented by Majid Ebrahim-Zadeh (ICFO, Barcelona, Spain).
• Super-resolution Optical Microscopy present-ed by Christian Eggeling (Weatherall Institute of Molecular Medicine, University of Oxford, Oxford, United Kingdom).
• Laser Beam Analysis, Propagation and Spa-tial Shaping Techniques presented by James R. Leger (University of Minnesota, Minneapolis, United States).
• Practical Quantum Optics presented by Gerd Leuchs (University of Erlangen, Erlan-gen, Germany).
• Numerical Photonics on High Performance Computing Architecture presented by Jerome V. Moloney (University of Arizona, Tucson, AZ, USA)
• Frequency Combs and Applications present-ed by !omas Udem (Max-Planck-Institut für Quantenoptik, Garching, Germany).
• Silicon Photonics presented by Dries Van !ourhout (Ghent University, Ghent, Belgium).
• Terahertz Measurements and their Applica-tions presented by Daniel M. Mittleman (Rice University, Houston, TX, USA).
• High Power and High Brightness Semiconduc-tor Laser Diodes and Applications presented by Paul Crump and Katrin Paschke (Ferdinand- Braun-Institut (FBH), Berlin, Germany).
All courses will take place in parallel on Sunday, 21 June 2015 at the ICM Congress Centre.The conference will also have two postdead-line sessions scheduled for Wednesday evening, 24 June 2015 (18:45 to 20:15). !e purpose of$the postdeadline sessions is to give the audience the chance to listen to the latest breaking news in op-tics, and this is usually one of the most attractive events that certainly contributes to the great at-mosphere that makes the CLEO®/Europe-EQEC conference a unique meeting.In addition to the technical sessions involving oral presentations, all scientific areas of both CLEO®/Europe and EQEC will be covered in Poster Ses-sions, which will provide an interactive and less formal way for researchers to discuss their work, interact and exchange ideas.CLEO®/Europe-EQEC is now established as the largest and most comprehensive gathering of optics and photonics researchers and engineers in Europe, spanning classical and quantum optical science, laser technology and photonics applications. !e conference programme could not have been elaborated without the vital support and effort of 278 scientists, forming 14 CLEO®/Europe, 9 EQEC, 5 Joint Symposia, 3 Joint sessions and
1 Tech-Focus technical programme sub-commit-tees, who have assembled an excellent series of talks and posters covering a wide range of fields in optics and quantum electronics. !e technical programme consists of 5 plenary sessions, 5 tutorials, 8 key-notes, 6 technical Focus, 89 invited talks, and 924 oral presentations. CLEO®/Europe-EQEC 2015 will feature a poster programme including 574 posters to be presented among the five poster sessions. !e Conference Chairs would like to extend sin-cere thanks to the technical programme commit-tee members for all their hard and fruitful work. A conference as large as CLEO®/Europe-EQEC requires two years of planning and organisation. !erefore, we would like to thank the sta" of the European Physical Society and the local conference
chair in Munich for invaluable professional assis-tance during this period. We also thank Messe Munich GmbH and all the Sponsoring Societies for their guidance, support, and their invaluable advice, which ensures that this event not only re-mains at the core of optics and photonics research for many nations, but will also be the Major Event of the International Year of Light in Europe. Let us finally thank all the attendees. !e real suc-cess of CLEO®/Europe-EQEC 2015 indeed rests on the e"orts and commitments of researchers and students, who all contribute to the tremen-dous evolution of our research field and to the high quality of the papers that will be presented here.
We thank you all!
Member Societies of the European Physical Society
Albanian Physical SocietyArmenian Physical SocietyAustrian Physical SocietyBelarusian Physical SocietyBelgian Physical SocietyUnion of Physicists in BulgariaCroatian Physical SocietyCyprus Society of PhysicistsCzech Physical SocietyDanish Physical SocietyEstonian Physical SocietyFinnish Physical SocietyFrench Physical SocietyGeorgian Physical SocietyGerman Physical SocietyHellenic Physical SocietyEotvos Lorand Physical SocietyIcelandic Physical SocietyIsrael Physical SocietyItalian Physical SocietyLatvian Physical SocietyLiechtenstein Scientific Society (Physical Section)
Lithuanian Physical SocietyAssociation Luxembourgeoise des PhysiciensMoldovan Physical SocietyPhysical Society of MontenegroNetherlands Physical SocietyNorwegian Physical SocietyPolish Physical SocietyPortuguese Physical SocietySociety of Physicists of MacedoniaRomanian Physical SocietyUnited Physical Society
of the Russian FederationSerbian Physical SocietySlovak Physical SocietySociety of Mathematicians Physicists
and Astronomers of SloveniaSpanish Royal Physics SocietySwedish Physical SocietySwiss Physical SocietyTurkish Physical SocietyUkrainian Physical Society!e Institute of Physics (IOP)
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ROOM 12a ROOM 12b ROOM 21a ROOM 21b ROOM 22
SH-1A
Short Course 1: Ultrashort Pulse Characterization 1
SH-3A
Short-Course 3: Super-Resolution Optical Microscopy 1
SH-10A
Short-Course 10: High Power and High Brightness Semiconductor Laser Diodes and Applications 1
SH-8A
Short-Course 8: Silicon Photonics 1
SH-5A
Short-Course 5: Practical Quantum Optics 1
COFFEE BREAK
SH-1B
Short Course 1: Ultrashort Pulse Characterization 2
SH-3B
Short-Course 3: Super-Resolution Optical Microscopy 2
SH-10B
Short-Course 10: High Power and High Brightness Semiconductor Laser Diodes and Applications 2
SH-8B
Short-Course 8: Silicon Photonics 2
SH-5B
Short-Course 5: Practical Quantum Optics 2
LUNCH BREAK
SH-4A
Short-Course 4: Laser Beam Analysis, Propagation and Spatial Shaping Techniques 1
SH-9A
Short-Course 9: Terahertz Measurements and their Applications 1
SH-7A
Short-Course 7: Frequency Combs and Applications 1
SH-2A
Short-Course 2: Optical Parametric Oscillator 1
SH-6A
Short-Course 6: Numerical Photonics on High Performance Computing Architecture 1
COFFEE BREAK
SH-4B
Short-Course 4: Laser Beam Analysis, Propagation and Spatial Shaping Techniques 2
SH-9B
Short-Course 9: Terahertz Measurements and their Applications 2
SH-7B
Short-Course 7: Frequency Combs and Applications 2
SH-2B
Short-Course 2: Optical Parametric Oscillator 2
SH-6B
Short-Course 6: Numerical Photonics on High Performance Computing Architecture 2
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Sunday at a glance
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b ROOM 14c CURIE EDISON EINSTEIN HERTZ MAIMAN NEWTON 2
CK-1
Subwave Length- and Di"raction Gratings
EG-1
Nano Opto- mechanics
CM-1
Direct Laser Writing
CJ-1
Beam Combining of Fibre Lasers
CA-1
Solid State Raman Lasers
CE-1
Fibre Technology
CD-1
Applications of Optical Fibres I
EA-1
Non-Classical Light and Entanglement
EF-1
Localized States of Light
CH-1
Measurement and Analysis
CC-1
THz Quantum Cascade Laser I
EE-1
Ultrafast Spectroscopy and Extreme Light Sources
JSI-1
Novel Light Management Concepts
CI-1
Overcoming the Capacity Crunch
COFFEE BREAK
CK-2
Single- emitter and Nanovolume Photonics
EG-2
Light-matter Interaction with 2D-System
CM-2
Laser Nano-processing
CJ-2
Mode-locked Fibre Oscillators
CA-2
Ultrashort Pulse Oscil-lators and Amplifiers…
CE-2
Fabrication of Photonic Structures and Components
CD-2
Photonics and QPM
EA-2
Atoms and Photons
EF-2
Symmetry Breaking, Photon Fluids and…
CH-2
New Photonic Sensor Technologies
CC-2
THz Quantum Cascade Laser II
EE-2
Filamentation and Intense Light Matter Interaction
JSI-2
Light Management in Thin-film Solar Cells
CI-2
Ultra High Bit-rate and Short-reach Transmission
LUNCH BREAK
CA, CC, CL, CM AND EE POSTER SESSIONS ! HALL B0
CK-3
Photonic Crystal Lasers
EG-3
Quantum Nano Optics
CM-3
Beam Shaping for Laser Micro-machining
CJ-3
Novel Fibre Designs
CA-3
High-Power Pulsed Solid-state Lasers
CE-3
Metamaterials and Photon Manipulation
CD-3
Phenomena in Nonlinear Optics
EA-3
Quantum Interference
EF-3
Soliton Dynamics
CH-3
Mid Infrared Sensing and Measure-ments
CC-3
High Field THz Radiation
EE-3
Ultrafast Spectroscopy and Extreme Light Sources
JSIV-1
Optical and Ultrafast Spectrosco-py of…
CI-3
Signal Processing
COFFEE BREAK
EG-4
Probing Nanoscale Electro-magnetic
CM-4
3D Device Laser Writing
CJ-4
Characteri- zation and Passive Com- ponents…
CA-4
Nanosecond 2#m Solid-state Lasers
CE-4
Silicon Photonics
CD-4
MIR Wavelength Generation
EA-4
Opto- mechanics
CH-4
Bio-medical Sensing
CC-4
THz Coherent Control and Spectroscopy
EE-4
Attosecond and High Field Physics
JSIV-2
Graphene Plasmonics and Devices
CI-4
Advanced Optical Solutions
PL-1 ROOM 1
ECBO - CLEO®/Europe 2015 International Year of Light Event and Plenary Talks
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ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b ROOM 21 CURIE EDISON EINSTEIN NEWTON 2
ED-1a Frequency Combs I
EG-5a Interac- tion of Electrons with Optical…
CM-5a Funda- mental Aspects of Laser Matter…
CK-4a Quantum Information Processing I
CA-5a Microchip Lasers I
CE-5a Semicon- ductor Techno- logy and…
CD-5a Applications of Nonlinearities I
EF-4a Extreme Events in Optics I
JSII-1a Optofluidic Biosensors
EE-5a Material Dynamics on Ultrafast Time…
PL-2
2015 World of Photonic Congress Opening and Plenary Talk
COFFEE TO GO RÖNTGEN
CJ-5
Mid-IR Fibre Laser Sys-tems I
ED-2
Combs and Precision Measure-ment
EG-6
Cavity Assisted Interactions
CM-6
Laser Volume Micro and Nanostructu-ring
CK-5
Nonlinear Micro/Nano-photonics
CA-6
Diode-pum-ped UV, Visi- ble and NIR Solid-state…
CE-6
Nanomaterials for Photonic Applications
CD-6
Frequency Conversion and Applications
EB-1
Quantum States and Characte- rization
EF-5
Turbulence, Optical Rogue Waves and Modulation…
JSII-2
Integrated On-Chip Diagnostics
JSIII-1
Laser Driven Acceleration
CI-5
Optical Computing, Data Proces-sing, RoF
LUNCH BREAK
CB, CK, ED, EG AND JSV POSTER SESSIONS ! HALL B0
PL-3
CLEO®/Europe 2015 Plenary
CJ-6a Waveguide Lasers
ED-1b Frequency Combs II
EG-5b Interac- tion of Electrons with Optical…
CM-5b Funda- mental Aspects of Laser Matter…
CK-4b Quantum Information Processing II
CA-5b Microchip Lasers II
CE-5b Semicon- ductor Techno-logy and…
CD-5b Applica-tions of Non-linearities II
EB-2a Quantum Coherence
EF-4b Extreme Events in Optics II
EE-5b Material Dynamics on Ultrafast Time…
COFFEE BREAK
JS SPIE/ OM/EQEC Computatio-nal Photonics for Metrology Applications
ED-3
Optical Clocks
EG-7
Nanospec-troscopy
CM-7
Laser Struc-turing of Surfaces and 2D Materials
CK-6
Micro/Nanos-tructures and Metasurfaces
CA-7
Advanced Concepts in Solid-state Lasers
CE-7
Oxide Lasers, Waveguides and Compo-nents
CD-7
Nonlinear Phenomena I
EA-5
Rare Earth Ions
EF-6
Nonlinear Beam Pro-pagation
CC-5
THz Near-field Micros-copy and Spectroscopy
LASER WORLD OF PHOTONICS OPENING RECEPTION, ICM FOYER, GROUND FLOOR, CONGRESS CENTRE"END 22:00#
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Tuesday at a glance
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b ROOM 21 CURIE EINSTEIN
CD-8
Nonlinear Phenomena II
EC-1
Quantum Gases Manipulation Correlation and Entanglement
EB/EG
Polaritons and Quantum Memories
CM/LIM
Diagnostics and Control
CF-1
Ultrafast Femtosecond Amplifiers
CK-7
Photonics Integration
CA-8
Visible Solid-state Lasers
CB-1
New Frontiers in Semiconductor Lasers
EF-7
Nonlinear Beha-viour of Light in Waveguides and Photonic Lattices
CC-6
Ultrafast THz Generation and Detection
COFFEE BREAK
PL-4
EQEC 2015 Plenary Talk and Awards Ceremony
LUNCH BREAK
CD, CE, CI, CN, EC, EI, JSI, JSII AND JSIV POSTER SESSIONS ! HALL B0
CD-9
Information and Quantum Computing
EC-2
Control of Ultracold Atoms and Molecules with Light
EA-6
Single Photons and Single-photon Detectors
TF-1
Ultrafast Solid-state and Fibre Lasers
CF-2
Ultrafast Parametric Amplifiers
CK-8
Plasmonic Micro/Nanostructures
CE-8
Organic Materials for Lasers Waveguides and Nonlinear Optics
CB-2
Vertical Cavity Lasers (VCSELs) I
EF-8
Spatio-Temporal Dynamics in Nonlinear Optical Systems
CG-1
Novel Attosecond Light Sources
COFFEE BREAK
CD-10
Whispering Gallery Mode- applications
EC-3
Cavity Mediated Control of Quantum Matters
EA-7
Quantum Light Sources
TF-2
Materials Structuring Using Short Laser Pulses
CF-3
Spectral Broadening of Ultrashort Pulses
CK-9
Photonic Micro- and Nanocavities
CE-9
Fabrication and Characterization of Organic and Inorganic Nonlinear Materials
CB-3
Vertical Cavity Lasers (VCSELs) II
CH-5
Photonic Crystals and Microstruc-tured Fibres for Sensing
CG-2
High Average/Peak Power Sources and Appli-cations
CLEO®/EUROPE$EQEC CONFERENCE RECEPTION "END 23:00#
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b ROOM 21 CURIE EINSTEIN
EH-1
Chirality in Plasmonics and Metamaterials
EB-3
Sources of Quan-tum Light
CJ-7
Mid-IR Fibre Laser Systems II
CLEO/ECBO-1
Bioimaging
CK-10
Optomechanics and Mems
CE-10
Optical Devices Based on Dia-mond and Silica
CB-4
Semiconductor Micro- and Nano-Lasers
CH-6
Fibre and Waveguide Based Sensors
CG-3
Attosecond Applications of Mid-IR Sources
COFFEE BREAK
EH-2
Plasmons in Low Dimensional Materials
EB-4
Quantum Key Distribution
CJ-8
Ultrafast Fibre Laser Systems
CLEO/ECBO-2
Optical Manipula-tion of Biomatter
CK-11
Interactions and Photonic Control
CE-11
Novel Lasers and Light Emitters Based on Semi-conductors
CB-5
High-power Semiconductor Lasers
CH-7
Spectroscopy
CG-4
Attosecond Photoemission Delays
LUNCH BREAK
CF, CJ, EB, AND EH POSTER SESSIONS ! HALL B0
CN-1
Laser Sources for Defence and Security
EH-3
Dielectrics and Hyperbolic Metamaterials
EB-5
Quantum Simulation
CJ-9
Pulsed Fibre Laser Sources
CF-4
Novel Ultrafast Lasers
CK-12
Integrated Photonic Sources
CE-12
Thin Films
CB-6
Quantum Cascade Lasers
CH-8
Optical Sources for Sensing and Metrology
CG-5
Attosecond Photoionization Dynamics
COFFEE BREAK
CN-2
Optical Sensing for Defence and Security
EH-4
Active Plasmonics and Metamaterials
CL-1
Low-cost Label-free Diagnostic Devices
CJ-10
Mode Instabilities in High Power Fibre Laser
CF-5
Ultrashort Pulse Measurement and FELs
CK-13
Fundamental Interaction and Novel Devices
EA-8
Semiconductor Quantum Light Sources
CB-7
Semiconductor Laser Dynamics
CH-9
Advanced Measurement Methods and Devices
CG-8
Sub-fs Dynamics in Molecules
HAPPY HOUR SPONSORED BY EPS$QEOD, EPS$EPL, SPIE AND AAAF/SCIENCEICM FOYER, GROUND FLOOR, CONGRESS CENTRE
PD-A
Postdeadline A (end 20:15)
PD-B
Postdeadline B (end 20:15)
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Thursday at a glance
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b ROOM 21 CURIE EINSTEIN
CD-11
Optical Microscopy
EH-5
Emission Control with Nanoantennas
CL-2
Fluorescence Imaging and Optical Manipulation
CJ-11
High-Power CW Fibre Laser Systems
CF-6
Characterization of Ultrafast Lasers
CA-9
Yb3+ -doped Solid State-lasers and Amplifiers
EA-9
Controlled Light-matter Interactions I
CB-8
Optical Feed-back and Optical Injection
EF-9
Mechanical Properties of Light and Self-organisation
JSV-1
Photon Pair Sources
COFFEE BREAK
CD-12
Applications of Optical Fibres II
EH-6
Nanoantennas: From Sensing to Thermoplas-monics
CL-3
Multiphoton and Multimodal Microscopy
CJ-12
Erbium Fibre and Waveguide Lasers
CF-7
Ultrafast Spectroscopy and Imaging
CA-10
Thin Disk Lasers and Amplifiers
EA-10
Controlled Light-matter Interactions II
CB-9
Quantum-dot Lasers
EI-1
Structured Light and Structured Materials
JSV-2
Source Engineering
LUNCH BREAK
CG, CH, EA, AND EF POSTER SESSIONS ! HALL B0
CD-13
Nonlinear Phenomena III
EH-7
Coherent E"ects in Nanophotonics
CL-4
Vibrational and High Resolution Imaging and Sensing
CJ-13
Thulium-doped Fibre Laser Systems I
CF-8
High Harmonic Generation Ultra-fast Technology
CA-11
Nd3+-doped Solid-state Lasers and Amplifiers
CK-14
Fabrication and Sources in Micro/Nano Optics
CB-10
Ultrafast Semi-conductor Lasers and Frequency Combs
EI-2
Nonlinear Dynamics
JSV-3
Complex Interferences in Waveguides
COFFEE BREAK
CL-5
Fibre-based Bioimaging and Sensing
CJ-14
Thulium-doped Fibre Laser Systems II
CF-9
Novel Trends in Ultrafast Optics
CA-12
In-band Pumped Solid-state Lasers
CB-11
Advanced Fabrication of Semiconductor Lasers
EI-3a
Multi-physics Modeling
JSV-4
Manipulation of Quantum Information on Chip
CONFERENCE ENDS
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PLENARY SESSIONS
PL-1 ECBO-CLEO®/Europe 2015 International Year of Light Event and Plenary TalksSunday, 17:15 - 18:45 • Room 1
PL-2 2015 World of Photonic Congress Opening and Plenary TalkMonday, 9:00 - 11:00 • Room 1
PL-3 CLEO®/Europe 2015 Plenary TalkMonday, 14:30 - 15:30 • Room 1
PL-4 EQEC 2015 Plenary Talk and Awards CeremonyTuesday, 10:30 - 12:30 • Room 1
CLEO®/Europe 2015 SESSIONS
CA SOLID!STATE LASERS
CA-1 Solid State Raman LasersSunday, 08:30 – 10:00 • Room 13b
CA-2 Ultrashort Pulse Oscillators and Amplifiers in Disordered Solid-state Media Sunday, 10:30 – 12:00 • Room 13b
CA-P CA Poster SessionSunday, 12:30 – 13:30 • Hall B0
CA-3 High-Power Pulsed Solid-state Lasers
Sunday, 13:30 – 15:00 • Room 13b
CA-4 Nanosecond 2%m Solid-state Lasers
Sunday, 15:30 – 17:00 • Room 13b
CA-5a Microchip Lasers I Monday, 08:00 – 8:45 • Room 13b
CA-6 Diode-pumped UV, Visible and NIR Solid-state LasersMonday, 11:15 – 12:45 • Room Röntgen
CA-5b Microchip Lasers IIMonday, 15:45 – 16:30 • Room 13b
CA-7 Advanced Concepts in Solid-state LasersMonday, 17:00 – 18:30 • Room 13b
CA-8 Visible Solid-state LasersTuesday, 08:30 – 10:00 • Room 14b
CA-9 Yb3+-doped Solid State-lasers and Amplifiers!ursday, 08:30 – 10:00 • Room 14a
CA-10 Thin Disk Lasers and Amplifiers!ursday, 10:30 – 12:00 • Room 14a
CA-11 Nd3+-doped Solid-state Lasers and Amplifiers!ursday, 14:00 – 15:30 • Room 14a
CA-12 In-band Pumped Solid-state Lasers!ursday, 16:00 – 17:30 • Room 14a
CB ! SEMICONDUCTOR LASERS
CB-P CB Poster SessionMonday, 13:30 – 14:30 • Hall B0
CB-1 New Frontiers in Semiconductor LasersTuesday, 08:30 – 10:00 • Room 21
CB-2 Vertical Cavity Lasers (VCSELs) ITuesday, 14:00 – 15:30 • Room 21
How to find the room?
A map locating the rooms can be found in the inner cover of the advance programme.
Talks: All talks take place in the congress centre (called ICM) or over the exhibition halls. !ese rooms are named as Curie, Edison, Einstein, Hertz, Maiman, Newton 2 and Röntgen.
To save space in the layout of the parallel ses-sions, all locations were abbreviated to the strict minimum such as "Room 1" instead of "Room 1, Ground Floor / 1st Floor, Congress Centre".
Below you will find the detailed locations of all the rooms used for the WoP Congress:
Room 1, Ground Floor / 1st Floor, Congress Centre
Room 2, Ground Floor, Congress CentreRoom 3, Ground Floor, Congress CentreRoom 4a, Ground Floor, Congress CentreRoom 4b, Ground Floor, Congress CentreRoom 5, Ground Floor, Congress Centre
Room 11, 1st Floor, Congress CentreRoom 12a, 1st Floor, Congress CentreRoom 12b, 1st Floor, Congress CentreRoom 13a, 1st Floor, Congress CentreRoom 13b, 1st Floor, Congress CentreRoom 13b, 1st Floor, Congress CentreRoom 14a, 1st Floor, Congress CentreRoom 14b, 1st Floor, Congress CentreRoom 14c, 1st Floor, Congress Centre$Room 21, 2nd Floor, Congress CentreRoom 21a, 2nd Floor, Congress CentreRoom 21b, 2nd Floor, Congress CentreRoom 22, 2nd Floor, Congress CentreRoom 22a, 2nd Floor, Congress CentreRoom 22b, 2nd Floor, Congress Centre
$Room Curie, 1st Floor, Exhibition Hall A1 (A11/A12)
Room Curie 1, 1st Floor, Exhibition Hall A1 (A11)
Room Curie 2, 1st Floor, Exhibition Hall A1 (A12)
Room Edison, 1st Floor, Exhibition Hall A2 (A21/A22)
Room Edison 1, 1st Floor, Exhibition Hall A2 (A21)
Room Edison 2, 1st Floor, Exhibition Hall A2 (A22)
Room Newton, 1st Floor, Exhibition Hall A3 (A31/A32)
Room Newton 1, 1st Floor, Exhibition Hall A3 (A31)
Room Newton 2, 1st Floor, Exhibition Hall A3 (A32)
Room Röntgen, 1st Floor, Exhibition Hall A4 (A41/42) (*)
Room Einstein, 1st Floor, Exhibition Hall B1 (B11)Room Hertz, 1st Floor, Exhibition Hall B2 (B21)Room Maiman, 1st Floor, Exhibition Hall B3 (B32)Room Zeppelin, NovotelRoom Weißkopf, Novotel
WARNING:(*) Only the CA-6 session (Diode-pumped UV, Visible and NIR Solid-state Lasers) takes place in the Röntgen room on Monday (11:15-12:45). !e room is not located on the map in the inner cover of the advance programme but guidance signs to the room will be installed.
Posters: All Posters take place in the Hall B0, Ground Floor, Congress Centre.
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CB-3 Vertical Cavity Lasers (VECSELs) IITuesday, 16:00 – 17:30 • Room 21
CB-4 Semiconductor Micro- and Nano-LasersWednesday, 08:30 – 10:00 • Room 21
CB-5 High-power Semiconductor Lasers
Wednesday, 10:30 – 12:00 • Room 21
CB-6 Quantum Cascade LasersWednesday, 14:00 – 15:30 • Room 21
CB-7 Semiconductor Laser Dynamics
Wednesday, 16:00 – 17:30 • Room 21
CB-8 Optical Feedback and Optical Injection!ursday, 08:30 – 10:00 • Room 21
CB-9 Quantum-dot Lasers!ursday, 10:30 – 12:00 • Room 21
CB-10 Ultrafast Semiconductor Lasers and Frequency Combs!ursday, 14:00 – 15:30 • Room 21
CB-11 Advanced Fabrication of Semiconductor Lasers!ursday, 16:00 – 17:30 • Room 21
CC ! TERAHERTZ SOURCES AND APPLICATIONS
CC-1 THz Quantum Cascade Laser ISunday, 08:30 – 10:00 • Room Einstein
CC-2 THz Quantum Cascade Laser IISunday, 10:30 – 12:00 • Room Einstein
CC-P CC Poster SessionSunday, 12:30 – 13:30 • Hall B0
CC-3 High Field THz Radiation Sunday, 13:30 – 15:00 • Room Einstein
CC-4 THz Coherent Control and SpectroscopySunday, 15:30 – 17:00 • Room Einstein
CC-5 THz Near-field Microscopy and SpectroscopyMonday, 17:00 – 18:30 • Room Einstein
CC-6 Ultrafast THz Generation and DetectionTuesday, 08:30 – 10:00 • Room Einstein
CD ! APPLICATIONS OF NONLINEAR OPTICS
CD-1 Applications of Optical Fibres ISunday, 08:30 – 10:00 • Room 14b
CD-2 Photonics and QPMSunday, 10:30 – 12:00 • Room 14b
CD-3 Phenomena in Nonlinear OpticsSunday, 13:30 – 15:00 • Room 14b
CD-4 MIR Wavelength GenerationSunday, 15:30 – 17:00 • Room 14b
CD-5a Applications of Nonlinearities IMonday, 08:00 – 8:45 • Room 14b
CD-6 Frequency Conversion and Applications Monday, 11:15 – 12:45 • Room 14b
CD-5b Applications of Nonlinearities IIMonday, 15:45 – 16:30 • Room 14b
CD-7 Nonlinear Phenomena IMonday, 17:00 – 18:30 • Room 14b
CD-8 Nonlinear Phenomena IITuesday, 08:30 – 10:00 • Room 1
CD-P CD Poster SessionTuesday, 13:00 – 14:00 • Hall B0
CD-9 Information and Quantum ComputingTuesday, 14:00 – 15:30 • Room 1
CD-10 Whispering Gallery Mode-applicationsTuesday, 16:00 – 17:30 • Room 1
CD-11 Optical Microscopy!ursday, 08:30 – 10:00 • Room 1
CD-12 Applications of Optical Fibres II
!ursday, 10:30 – 12:00 • Room 1
CD-13 Nonlinear Phenomena III!ursday, 14:00 – 15:30 • Room 1
CE ! OPTICAL MATERIALS, FABRICATION AND CHARACTERISATION
CE-1 Fibre TechnologySunday, 08:30 – 10:00 • Room 14a
CE-2 Fabrication of Photonic Structures and ComponentsSunday, 10:30 – 12:00 • Room 14a
CE-3 Metamaterials and Photon ManipulationSunday, 13:30 – 15:00 • Room 14a
CE-4 Silicon PhotonicsSunday, 15:30 – 17:00 • Room 14a
CE-5a Semiconductor Technology and Semiconductor Characterization I Monday, 08:00 – 8:45 • Room 14a
CE-6 Nanomaterials for Photonic Applications Monday, 11:15 – 12:45 • Room 14a
CE-5b Semiconductor Technology and Semiconductor Characterization II Monday, 15:45 – 16:30 • Room 14a
CE-7 Oxide Lasers, Waveguides and ComponentsMonday, 17:00 – 18:30 • Room 14a
CE-P CE Poster SessionTuesday, 13:00 – 14:00 • Hall B0
CE-8 Organic Materials for Lasers Waveguides and Nonlinear Optics Tuesday, 14:00 – 15:30 • Room 14b
CE-9 Fabrication and Characterization of Organic and Inorganic Nonlinear Materials Tuesday, 16:00 – 17:30 • Room 14b
CE-10 Optical Devices Based on Diamond and SilicaWednesday, 08:30 – 10:00 • Room 14b
CE-11 Novel Lasers and Light Emitters Based on SemiconductorsWednesday, 10:30 – 12:00 • Room 14b
CE-12 Thin Films Wednesday, 14:00 – 15:30 • Room 14b
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CF ! ULTRAFAST OPTICAL TECHNOLOGIES
CF-1 Ultrafast Femtosecond AmplifiersTuesday, 08:30 – 10:00 • Room 13b
CF-2 Ultrafast Parametric AmplifiersTuesday, 14:00 – 15:30 • Room 13b
CF-3 Spectral Broadening of Ultrashort PulsesTuesday, 16:00 – 17:30 • Room 13b
CF-P CF Poster SessionWednesday, 13:00 – 14:00 • Hall B0
CF-4 Novel Ultrafast LasersWednesday, 14:00 – 15:30 • Room 13b
CF-5 Ultrashort Pulse Measurement and FELsWednesday, 16:00 – 17:30 • Room 13b
CF-6 Characterization of Ultrafast Lasers!ursday, 08:30 – 10:00 • Room 13b
CF-7 Ultrafast Spectroscopy and Imaging!ursday, 10:30 – 12:00 • Room 13b
CF-8 High Harmonic Generation Ultrafast Technology!ursday, 14:00 – 15:30 • Room 13b
CF-9 Novel Trends in Ultrafast Optics!ursday, 16:00 – 17:30 • Room 13b
CG ! HIGH!FIELD LASER PHYSICS AND ATTOSECOND TECHNOLOGIES
CG-1 Novel Attosecond Light SourcesTuesday, 14:00 – 15:30 • Room Einstein
CG-2 High Average/Peak Power Sources and ApplicationsTuesday, 16:00 – 17:30 • Room Einstein
CG-3 Attosecond Applications of Mid-IR SourcesWednesday, 08:30 – 10:00 • Room Einstein
CG-4 Attosecond Photoemission DelaysWednesday, 10:30 – 12:00 • Room Einstein
CG-5 Attosecond Photoionization DynamicsWednesday, 14:00 – 15:30 • Room Einstein
CG-6 Sub-fs Dynamics in MoleculesWednesday, 16:00 – 17:30 • Room Einstein
CG-P CG Poster Session!ursday, 13:00 – 14:00 • Hall B0
CH ! OPTICAL SENSING AND METROLOGY
CH-1 Measurement and AnalysisSunday, 08:30 – 10:00 • Room Edison
CH-2 New Photonic Sensor TechnologiesSunday, 10:30 – 12:00 • Room Edison
CH-3 Mid Infrared Sensing and MeasurementsSunday, 13:30 – 15:00 • Room Edison
CH-4 Bio-medical SensingSunday, 15:30 – 17:00 • Room Edison
CH-5 Photonic Crystals and Microstructured Fibres for SensingTuesday, 16:00 – 17:30 • Room Curie
CH-6 Fibre and Waveguide Based Sensors
Wednesday, 08:30 – 10:00 • Room Curie
CH-7 SpectroscopyWednesday, 10:30 – 12:00 • Room Curie
CH-8 Optical Sources for Sensing and MetrologyWednesday, 14:00 – 15:30 • Room Curie
CH-9 Advanced Measurement Methods and DevicesWednesday, 16:00 – 17:30 • Room Curie
CH-P CH Poster Session!ursday, 13:00 – 14:00 • Hall B0
CI ! OPTICAL TECHNOLOGIES FOR COMMUNICATIONS AND DATA STORAGE
CI-1 Overcoming the Capacity Crunch Sunday, 08:30 – 10:00 • Room Newton 2
CI-2 Ultra High Bit-rate and Short-reach TransmissionSunday, 10:30 – 12:00 • Room Newton 2
CI-3 Signal ProcessingSunday, 13:30 – 15:00 • Room Newton 2
CI-4 Advanced Optical SolutionsSunday, 15:30 – 17:00 • Room Newton 2
CI-5 Optical Computing, Data Processing, RoFMonday, 11:15 – 12:45 • Room Newton 2
CI-P CI Poster SessionTuesday, 13:00 – 14:00 • Hall B0
CJ ! FIBRE AND GUIDED WAVE LASERS AND AMPLIFIERS
CJ-1 Beam Combining of Fibre Lasers Sunday, 08:30 – 10:00 • Room 13a
CJ-2 Mode-locked Fibre OscillatorsSunday, 10:30 – 12:00 • Room 13a
CJ-3 Novel Fibre DesignsSunday, 13:30 – 15:00 • Room 13a
CJ-4 Characterization and Passive Components for Fibre Laser SystemsSunday, 15:30 – 17:00 • Room 13a
CJ-5 Mid-IR Fibre Laser Systems IMonday, 11:15 – 12:45 • Room 1
CJ-6a Waveguide LasersMonday, 15:45 – 16:30 • Room 1
CJ-7 Mid-IR Fibre Laser Systems IIWednesday, 08:30 – 10:00 • Room 13a
CJ-8 Ultrafast Fibre Laser SystemsWednesday, 10:30 – 12:00 • Room 13a
CJ-P CJ Poster SessionWednesday, 13:00 – 14:00 • Hall B0
CJ-9 Pulsed Fibre Laser SourcesWednesday, 14:00 – 15:30 • Room 13a
CJ-10 Mode Instabilities in High Power Fibre Laser SystemsWednesday, 16:00 – 17:30 • Room 13a
CJ-11 High-Power CW Fibre Laser Systems!ursday, 08:30 – 10:00 • Room 13a
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CJ-12 Erbium Fibre and Waveguide Lasers
!ursday, 10:30 – 12:00 • Room 13a
CJ-13 Thulium-doped Fibre Laser Systems I!ursday, 14:00 – 15:30 • Room 13a
CJ-14 Thulium-doped Fibre Laser Systems II!ursday, 16:00 – 17:30 • Room 13a
CK ! MICRO! AND NANO!PHOTONICS
CK-1 Subwave Length- and Di&raction GratingsSunday, 08:30 – 10:00 • Room 1
CK-2 Single-emitter and Nanovolume PhotonicsSunday, 10:30 – 12:00 • Room 1
CK-3 Photonic Crystal LasersSunday, 13:30 – 15:00 • Room 1
CK-4a Quantum Information Processing IMonday, 08:00 – 08:45 • Room 13a
CK-5 Nonlinear Micro/NanophotonicsMonday, 11:15 – 12:45 • Room 13a
CK-P CK Poster SessionMonday, 13:30 – 14:30 • Hall B0
CK-4b Quantum Information Processing IIMonday, 15:45 – 16:30 • Room 13a
CK-6 Micro/Nanostructures and MetasurfacesMonday, 17:00 – 18:30 • Room 13a
CK-7 Photonics IntegrationTuesday, 08:30 – 10:00 • Room 14a
CK-8 Plasmonic Micro/ Nanostructures
Tuesday, 14:00 – 15:30 • Room 14a
CK-9 Photonic Micro- and Nanocavities
Tuesday, 16:00 – 17:30 • Room 14a
CK-10 Optomechanics and MemsWednesday, 08:30 – 10:00 • Room 14a
CK-11 Interactions and Photonic ControlWednesday, 10:30 – 12:00 • Room 14a
CK-12 Integrated Photonic SourcesWednesday, 14:00 – 15:30 • Room 14a
CK-13 Fundamental Interaction and Novel DevicesWednesday, 16:00 – 17:30 • Room 14a
CK-14 Fabrication and Sources in Micro/Nano Optics!ursday, 14:00 – 15:30 • Room 14b
CL ! BIOPHOTONICS AND APPLICATIONS
CL-P CL Poster SessionSunday, 12:30 – 13:30 • Hall B0
CLEO/ECBO-1 BioimagingWednesday, 08:30 – 10:00 • Room 13b
CLEO/ECBO-2 Optical Manipulation of Biomatter
Wednesday, 10:30 – 12:00 • Room 13b
CL-1 Low-cost Labelfree Diagnostic DevicesWednesday, 16:00 – 17:30 • Room 4b
CL-2 Fluorescence Imaging and Optical Manipulation!ursday, 08:30 – 10:00 • Room 4b
CL-3 Multiphoton and Multimodal Microscopy!ursday, 10:30 – 12:00 • Room 4b
CL-4 Vibrational and High Resolution Imaging and Sensing!ursday, 14:00 – 15:30 • Room 4b
CL-5 Fibre-based Bioimaging and Sensing!ursday, 16:00 – 17:30 • Room 4b
CM ! MATERIALS PROCESSING WITH LASERS
CM-1 Direct Laser Writing Sunday, 08:30 – 10:00 • Room 4b
CM-2 Laser NanoprocessingSunday, 10:30 – 12:00 • Room 4b
CM-P CM Poster SessionSunday, 12:30 – 13:30 • Hall B0
CM-3 Beam Shaping for Laser MicromachiningSunday, 13:30 – 15:00 • Room 4b
CM-4 3D Device Laser WritingSunday, 15:30 – 17:00 • Room 4b
CM-5a Fundamental Aspects of Laser Matter Interaction IMonday, 08:00 – 08:45 • Room 4b
CM-6 Laser Volume Micro and NanostructuringMonday, 11:15 – 12:45 • Room 4b
CM-5b Fundamental Aspects of Laser Matter Interaction IIMonday, 15:45 – 16:30 • Room 4b
CM-7 Laser Structuring of Surfaces and 2D MaterialsMonday, 17:00 – 18:30 • Room 4b
CM/LIM Diagnostics and ControlTuesday, 08:30 – 10:00 • Room 13a
CN ! PHOTONICS IN DEFENSE AND SECURITY
CN-P CN Poster sessionTuesday, 13:00 – 14:00 • Hall B0
CN-1 Laser Sources for Defence and SecurityWednesday, 14:00 – 15:30 • Room 1
CN-2 Optical Sensing for Defence and SecurityWednesday, 16:00 – 17:30 • Room 1
NOTES
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EQEC 2015 Sessions
EA ! QUANTUM OPTICS
EA-1 Non-Classical Light and EntanglementSunday, 08:30 – 10:00 • Room 14c
EA-2 Atoms and Photons Sunday, 10:30 – 12:00 • Room 14c
EA-3 Quantum InterferenceSunday, 13:30 – 15:00 • Room 14c
EA-4 OptomechanicsSunday, 15:30 – 17:00 • Room 14c
EA-5 Rare Earth IonsMonday, 17:00 – 18:30 • Room 21
EA-6 Single Photons and Single-photon DetectorsTuesday, 14:00 – 15:30 • Room 4b
EA-7 Quantum Light SourcesTuesday, 16:00 – 17:30 • Room 4b
EA-8 Semiconductor Quantum Light SourcesWednesday, 16:00 – 17:30 • Room 14b
EA-9 Controlled Light-matter Interactions I
!ursday, 08:30 – 10:00 • Room 14b
EA-10 Controlled Light-matter Interactions II!ursday, 10:30 – 12:00 • Room 14b
EA-P EA Poster Session!ursday, 13:00 – 14:00 • Hall B0
EB ! QUANTUM INFORMATION, COMMUNICATION, AND SIMULATION
EB-1 Quantum States and CharacterizationMonday, 11:15 – 12:45 • Room 21
EB-2a Quantum CoherenceMonday, 15:45 – 16:30 • Room 21
EB/EG Polaritons and Quantum MemoriesTuesday, 08:30 – 10:00 • Room 4b
EB-3 Sources of Quantum LightWednesday, 08:30 – 10:00 • Room 4b
EB-4 Quantum Key DistributionWednesday, 10:30 – 12:00 • Room 4b
EB-P EB Poster SessionWednesday, 13:00 – 14:00 • Hall B0
EB-5 Quantum SimulationWednesday, 14:00 – 15:30 • Room 4b
EC ! ATOM OPTICS AND QUANTUM MATTER
EC-1 Quantum Gases Manipulation Correlation and EntanglementTuesday, 8:30 – 10:00 • Room 4a
EC-P EC Poster SessionTuesday, 13:00 – 14:00 • Hall B0
EC-2 Control of Ultracold Atoms and Molecules with LightTuesday, 14:00 – 15:30 • Room 4a
EC-3 Cavity Mediated Control of Quantum MattersTuesday, 16:00 – 17:30 • Room 4a
ED" # PRECISION METROLOGY AND FREQUENCY COMBS
ED-1a Frequency Combs I Monday, 08:00 – 08:45 • Room 3
ED-2 Combs and Precision MeasurementMonday, 11:15 – 12:45 • Room 3
ED-P ED Poster SessionMonday, 13:30 – 14:30 • Hall B0
ED-1b Frequency Combs IIMonday, 15:45 – 16:30 • Room 3
ED-3 Optical ClocksMonday, 17:00 – 18:30 • Room 3
EE ! ULTRAFAST OPTICAL SCIENCE
EE-1 Ultrafast Spectroscopy and Extreme Light SourcesSunday, 08:30 – 10:00 • Room Hertz
EE-2 Filamentation and Intense Light Matter InteractionSunday, 10:30 – 12:00 • Room Hertz
EE-P EE Poster SessionSunday, 12:30 – 13:30 • Hall B0
EE-3 Ultrafast Temporal Dynamics and Extreme EventsSunday, 13:30 – 15:00 • Room Hertz
EE-4 Attosecond and High Field PhysicsSunday, 15:30 – 17:00 • Room Hertz
EE-5a Material Dynamics on Ultrafast Time Scale IMonday, 08:00 – 08:45 • Room Einstein
EE-5b Material Dynamics on Ultrafast Time Scale IIMonday, 15:45 – 16:30 • Room Einstein
EF ! NONLINEAR PHENOMENA, SOLITONS AND SELF!ORGANIZATION
EF-1 Localized States of LightSunday, 08:30 – 10:00 • Room Curie
EF-2 Symmetry Breaking, Photon Fluids and Structured MaterialsSunday, 10:30 – 12:00 • Room Curie
EF-3 Soliton DynamicsSunday, 13:30 – 15:00 • Room Curie
EF-4a Extreme Events in Optics I Monday, 08:00 – 08:45 • Room Curie
EF-5 Turbulence, Optical Rogue Waves and Modulation Instabilities in Optical Fibres Monday, 11:15 – 12:45 • Room Curie
EF-4b Extreme Events in Optics IIMonday, 15:45 – 16:30 • Room Curie
EF-6 Nonlinear Beam PropagationMonday, 17:00 – 18:30 • Room Curie
EF-7 Nonlinear Behaviour of Light in Waveguides and Photonic LatticesTuesday, 08:30 – 10:00 • Room Curie
EF-8 Spatio-Temporal Dynamics in Nonlinear Optical Systems Tuesday, 14:00 – 15:30 • Room Curie
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EF-9 Mechanical Properties of Light and Self-organisation!ursday, 08:30 – 10:00 • Room Curie
EF-P EF Poster Session!ursday, 13:00 – 14:00
EG # LIGHT!MATTER INTERACTIONS AT THE NANO!SCALE
EG-1 Nano OptomechanicsSunday, 08:30 – 10:00 • Room 4a
EG-2 Light-matter Interaction with 2D-System Sunday, 10:30 – 12:00 • Room 4a
EG-3 Quantum Nano OpticsSunday, 13:30 – 15:00 • Room 4a
EG-4 Probing Nanoscale Electromagnetic FieldsSunday, 15:30 – 17:00 • Room 4a
EG-5a Interaction of Electrons with Optical Near-fields IMonday, 08:00 – 08:45 • Room 4a
EG-6 Cavity Assisted InteractionsMonday, 11:15 – 12:45 • Room 4a
EG-P EG Poster SessionMonday, 13:30 – 14:30 • Hall B0
EG-5b Interaction of Electrons with Optical Near-fields II Monday, 15:45 – 16:30 • Room 4a
EG-7 NanospectroscopyMonday, 17:00 – 18:30 • Room 4a
EH # PLASMONICS AND METAMATERIALS
EH-1 Chirality in Plasmonics and MetamaterialsWednesday, 08:30 – 10:00 • Room 4a
EH-2 Plasmons in Low Dimensional Materials Wednesday, 10:30 – 12:00 • Room 4a
EH-P EH Poster SessionWednesday, 13:00 – 14:00 • Hall B0
EH-3 Dielectrics and Hyperbolic MetamaterialsWednesday, 14:00 – 15:30 • Room 4a
EH-4 Active Plasmonics and MetamaterialsWednesday, 16:00 – 17:30 • Room 4a
EH-5 Emission Control with Nanoantennas!ursday, 08:30 – 10:00 • Room 4a
EH-6 Nanoantennas: From Sensing to Thermoplasmonics !ursday, 10:30 – 12:00 • Room 4a
EH-7 Coherent E&ects in Nanophotonics!ursday, 14:00 – 15:30 • Room 4a
EI # THEORETICAL AND COMPUTATIONAL PHOTONICS
EI-P EI Poster SessionTuesday, 13:00 – 14:00 • Hall B0
EI-1 Structured Light and Structured Materials!ursday, 10:30 – 12:00 • Room Curie
EI-2 Nonlinear Dynamics!ursday, 14:00 – 15:30 • Room Curie
EI-3a Multi-physics Modeling!ursday, 16:00 – 16:45 • Room Curie
CLEO®/Europe-EQEC Joint Symposia Sessions
"JSI !"JOINT SYMPOSIUM ON LIGHT MANAGEMENT IN PHOTOVOLTAICS
JSI-1 Novel Light Management ConceptsSunday, 08:30 – 10:00 • Room Maiman
JSI-2 Light Management in Thin-film Solar CellsSunday, 10:30 – 12:00 • Room Maiman
JSI-P JSI Poster SessionTuesday, 13:00 – 14:00 • Hall B0
JSII ! JOINT SYMPOSIUM ON PHOTONIC LAB!ON!A!CHIP BIOSENSORS
JSII-1a Optofluidic BiosensorsMonday, 08:00 – 08:45 • Room Edison
JSII-2 Integrated On-Chip DiagnosticsMonday, 11:15 – 12:45 • Room Edison
JSII-P JSII Poster SessionTuesday, 13:00 – 14:00 • Hall B0
JSIII ! JOINT SYMPOSIUM ON LASER!DRIVEN ACCELERATION
JSIII-1 Laser Driven AccelerationMonday, 11:15 – 12:45 • Room Einstein
JSIV ! JOINT SYMPOSIUM ON OPTICS IN GRAPHENE AND OTHER TWO!DIMENSIONAL MATERIALS
JSIV-1 Optical and Ultrafast Spectroscopy of Two-dimensional MaterialsSunday, 13:30 – 15:00 • Room Maiman
JSIV-2 Graphene Plasmonics and DevicesSunday, 15:30 – 17:00 • Room Maiman
JSIV-P JSIV Poster SessionTuesday, 13:00 – 14:00 • Hall B0
JSV ! JOINT SYMPOSIUM ON INTEGRATED QUANTUM OPTICS
JSV-P JSV Poster Session Monday, 13:30 – 14:30 • Hall B0
JSV-1 Photon Pair Sources!ursday, 08:30 – 10:00 • Room Einstein
JSV-2 Source Engineering !ursday, 10:30 – 12:00 • Room Einstein
JSV-3 Complex Interferences in Waveguides!ursday, 14:00 – 15:30 • Room Einstein
JSV-4 Manipulation of Quantum Information on Chip!ursday, 16:00 – 17:30 • Room Einstein
SPIE-Optical Metrology-EQEC 2015 Joint Session
JS SPIE/OM/EQEC Computational Photonics for Metrology Applications
Monday, 17:00 – 18:30 • Room 1
LIM!CLEO®/EUROPE 2015 JOINT TECHNICAL FOCUS SESSIONS
TF-1 Ultrafast Solid-state and Fibre LasersTuesday, 14:00 – 15:30 • Room 13a
TF-2 Materials Structuring Using Short Laser PulsesTuesday, 16:00 • 17:30 • Room 13a
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NOTES
How to read the Session Codes?
!e following pages contain the abstracts of the papers presented at the conference CLEO®/Europe-EQEC 2015.
All CLEO®/Europe sessions are on a white background and have a code beginning with a C.All EQEC sessions are on a shaded background and have a code that begins with an E.
E$%&'()*+, -&+()*+&. /&0*1 23& *+ 2 .234 /2%453*6+.:• Short courses referenced with a SH• Plenary talks referenced with a PL• CLEO®/Europe-EQEC joint symposia referenced with a JS. • Technical focus sessions jointly held with the LIM conferences (Ultrafast
Solid-State and Fibre Lasers / Materials Structuring Using Short Laser Pulses) referenced with a TF.
• !e CLEO®/Europe-ECBO joint sessions referenced with CLEO/ECBO-1 and CLEO/ECBO-2 in the CL topic.
• SPIE-Optical Metrology/EQEC joint session on Computational Pho-tonics for Metrology Applications referenced with JS SPIE-OM/EQEC.
O320 P3&,&+(2()*+,Oral presentations have a code made up of three parts, e.g.
CD-1.1 TUE (Invited) 9:00
!e first part indicates the Conference, the topic title, the session title and the placement of the presentation within the session, e.g. CD1.1 = CLEO®/EuropeCD1.1 = Applications of Nonlinear OpticsCD1.1 = Applications of Optical Fibres ICD1.1 = First paper presented in the "Applications of Optical Fibres I"
session of the CD topic !e second part indicates the day when the presentation takes place.SUN = Sunday TUE = Tuesday THU = !ursday MON = Monday WED = Wednesday
!e figures on the right specify at what time the talk begins (09:00 am).Plenary, Tutorial, Keynote and Invited Talks are marked between brackets.
WARNING - EXCEPTIONS:2015 is a special year proclaimed International Year of Light (IYL) and Light-Based Technologies. !e CLEO®/Europe-EQEC conference is the major event organized in Europe related to IYL. Special events added on this occasion led us to change the structure of the conference in order to welcome more sessions than in the past editions of the meeting. Especially on Monday, half sessions (45 minutes long) have been organised to fit in the tight schedule. 7ese half sessions are labelled with the letters a or b in the session codes.
Example: ED-1a.1 MON 08:00
7e following topics have two full half sessions taking place on Monday morning, from 08:00 to 08:45, and Monday a8ernoon, from 15:45 to 16:30, namely,
CA, CD, CE, CK, CM, ED, EE, EF, and EG.
7e following topics only have one half session taking place on Monday a8ernoon, from 15:45 to 16:30 or 7ursday a8ernoon, from 16:00 to 16:45, namely,
CJ, EB, and EI.
P*,(&3,Poster presentations have a code made up of two parts, e.g.
ID-P.1 MON 13:30
!e first part indicates the Conference, the topic title, the poster destination, and the order of presentation within the topic, e.g. ED-P.1 = EQECED-P.1 = Precision Metrology and Frequency CombsED-P.1 = PosterED-P.1 = First poster in the "Precision Metrology and Frequency Combs"
topic of the EQEC conference.
!e second part indicates the day when the poster presentation takes place with the same abbreviations as for the oral presentations. All posters are displayed per topic according to their reference numbers over the conference days (see “days at a glance”).
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CLEO®/Europe 2015 Topics
CA - SOLID-STATE LASERS
Advances in solid-state lasers: novel solid-state lasers and amplifiers; high-power and high-en-ergy lasers; power-scalable laser architectures, solid-state micro-chip and nanolasers; random lasers; pulse generation; short wavelength lasers; mid-infrared lasers; tunable lasers; intracavity wavelength conversion; upconversion lasers; thermal e"ects and their mitigation, beam qual-ity characterisation; linewidth reduction and wavelength tuning techniques; amplitude and frequency stability; novel pump sources and pumping configurations; laser resonator design; spectroscopic characterisation of solid-state gain media; advanced laser crystals and glasses; laser characterisation and modelling, novel solid-state lasers for system applications.CHAIR: Mauro Tonelli, Universita' di Pisa, Pisa, Italy
CB - SEMICONDUCTOR LASERS
New technology, devices and applications; semi-conductor optical amplifiers; novel characteriza-tion techniques; vertical (extended) cavity surface emitting lasers; optically-pumped semiconductor lasers, photonic crystal semiconductor lasers, mi-cro-cavity lasers; quantum dot/dash lasers; sem-iconductor ring lasers; short wavelength lasers: blue and green; near-infrared long wavelength lasers; mid-infrared and far-infrared semicon-ductor lasers; high power and high brightness lasers; short-pulse generation, mode locking; functional applications: switching, clock recov-ery, signal processing; semiconductor lasers in integrated photonic circuits; synchronization, multimode dynamics, chaos.CHAIR: Maria Ana Cataluna, University of Dundee, Nethergate, Dundee, United Kingdom
CC - TERAHERTZ SOURCES AND APPLICATIONS
Sources for generating terahertz (far-infra-red) radiation in the range from 200 GHz to 100 THz, based on various physical princi-ples including ultrafast time-domain systems, direct generation using terahertz lasers, and sources based on nonlinear optical mixing and laser-created plasmas; applications using tera-hertz radiation for sensing, spectroscopy and imaging; advances in terahertz communica-tions; new terahertz measurement techniques and instrumentation, including advances in imaging configurations, detector technologies, terahertz optical components and terahertz im-aging and modeling of plumes, turbulent air, or gaseous flows.CHAIR: Thomas Dekorsy, University of Konstanz, Konstanz, Germany
CD - APPLICATIONS OF NONLINEAR OPTICS
Novel applications of nonlinear optical phe-nomena and new devices; nonlinear frequency conversion for the UV, visible and IR; telecom-munications applications and all-optical switch-ing; all-optical delay lines and slow light; optical parametric devices such as optical parametric amplifiers and oscillators; nonlinear optics in waveguides and fibres, including photonic crys-tal structures and microstructured optical fibres; quasi-phasematched materials and devices; novel nonlinear materials and structures; stim-ulated scattering processes and devices; appli-cations of optical solitons and photorefractives; electro-optic and Kerr devices in crystals and semiconductors; Raman based devices includ-ing amplifiers and lasers; nonlinear probing of surfaces; multi-photon imaging and coherent Raman microscopy.CHAIR: Concita Sibilia, Università di Roma “La Sapienza”, Roma, Italy
CE - OPTICAL MATERIALS, FABRICATION AND CHARACTERISATION
Fabrication of optical materials; new crystal-line and glass laser materials in bulk, fiber and waveguide geometry; micro- and nano-fab-rication and -engineering techniques; opti-cal characterisation of laser and nonlinear materials, micro-structured fiber and pho-tonic crystal waveguides, micro- and nano- crystalline materials, single defect centres, quantum wells, quantum wires and quantum dots, nano-tubes and nano-needles, innovative organic materials.CHAIR: Stefan Kück, Physikalisch- Technische Bundesanstalt, Braunschweig, Germany
CF - ULTRAFAST OPTICAL TECHNOLOGIES
Femtosecond and picosecond pulse gener-ation from solid state, fiber and waveguide sources; mode-locked lasers; few-cycle opti-cal pulses; pulse compression, carrier-envelope phase stabilization and pulse characteriza-tion; light waveform synthesis metrology; ul-trashort-pulse semiconductor lasers and devices; ultrafast parametric and nonlinear optical conversion; ultrashort-pulse mid-IR radiation; supercontinuum generation; dis-persion compensation; ultrafast electro-op-tics; pulse-shaping; carrier-envelope e"ects; ultrafast characterization methods and meas-urement techniques, ultrafast optoelectronic systems and devices; applications of ultrafast technology, applications of femtosecond pulse filamentation; technological aspects of ultrafast spectroscopy; coherent control using femtosec-ond pulses; ultrafast microscopic techniques; electro-optic sampling; ultrafast x-ray experi-ments and attosecond phenomena.CHAIR: Thomas Südmeyer, University of Neuchâtel, Neuchâtel, Switzerland
CG - HIGH-FIELD LASER PHYSICS AND ATTOSECOND TECHNOLOGIES
Strong field ionization and attosecond XUV/x-ray pulse generation; generation of high bright-ness attosecond pulses; probing of nonlinear and ultrafast dynamics by intense free-electron laser pulses; optimal control of ultrafast non-linear processes; time-resolved Auger or XUV/soft x-ray spectroscopy, interferometry and microscopy; time-resolved Coulomb explosion imaging; strongly coupled electron-nuclear dy-namics; attosecond and femtosecond electron di"raction imaging; dynamics in fixed-in-space molecules; ultrafast electron dynamics in bulk media, nanostructures and quantum-confined structures; probing of surface electron dynamics and physiochemical processes via time-resolved UPS/so# XPS; time-resolved XAS, XANES & EXAFS; femtosecond-laser-produced plasmas and particle acceleration.CHAIR: Matthias Kling, Ludwig-Maximilians-Universität München, Garching, Germany
CH - OPTICAL SENSING AND METROLOGY
Inspection of a wide range of objects, from the macroscopic to the nanometric scale; recent progress in all aspects of optical sensing and metrology, particularly in new photonic sen-sor technologies and applications ; new trends in optical remote sensing; fiber sensors using conventional and photonic crystal fibers; active multispectral and hyperspectral imaging; sensor multiplexing; novel spectroscopic techniques, applications and systems; optical precision metrology; novel measurement methods and devices based on interferometry; holography; di"ractometry or scatterometry; critical dimen-sion metrology; virtual metrology; multiscale surface metrology; UV and DUV microscopy; resolution enhancement technologies in
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microscopy; inverse problems; adaptive optics; phase retrieval.CHAIR: Trevor Benson, University of Nottingham, Nottingham, United Kingdom
CI - OPTICAL TECHNOLOGIES FOR COMMUNICATIONS AND DATA STORAGE
Fibre devices including dispersion compensating and nonlinear fibres, fibre propagation and po-larization e"ects, fibre gratings; semiconductor devices for generation, processing and detection of optical signals including laser sources, detec-tors and modulators, performance monitoring devices, switches, optical components for ena-bling WDM and OTDM systems including fil-tering and switching; digital signal processing and coding techniques; transmission techniques for submarine, core and metropolitan transport networks, communication and access networks; optical sub-systems including clock recovery techniques, packet/burst switching subsystems, advanced modulation formats, subcarrier-mul-tiplexing, receivers for coherent detection, radio-over-fiber and microwave photonic tech-nologies, optical regeneration, optics in storage area networks, optical delays and bu"ering, ho-lographic and 3D optical data storage, near-field recording and super-resolution.CHAIR: Erwan Pincemin, Orange Labs Networks, Lannion, France
CJ - FIBRE AND GUIDED WAVE LASERS AND AMPLIFIERS
Waveguide and fibre laser oscillator and ampli-fiers including novel waveguide and fibre ge-ometries; power scaling of waveguide and fibre lasers - including beam combination techniques (for both pump and signal beams) and new waveguide coupling approaches; upconversion
lasers; nonlinear frequency conversion and pulse generation and compression; advances in fibre waveguide materials; fabrication techniques for doped waveguide and fibre devices; active mi-crostructured fibre and waveguide laser devices; novel waveguide and fibre sources for industri-al applications.CHAIR: Thomas Vestergaard Andersen, NKT Photonics A/S, Birkerod, Denmark
CK - MICRO- AND NANO-PHOTONICS
Nanostructured materials for photonic applica-tions; novel phenomena occurring when light is created, transported and detected in environ-ments where either dimensionality or size are reduced and, in particular, when light-matter in-teraction occurs in regions smaller than or similar to the wavelength of light (nanophotonics). Peri-odic or quasi-periodic nanostructures (photonic crystals); integrated optics; optical MEMS; mate-rials aspects and fabrication techniques, including inorganic/organic nano-layers/wires, nanocrys-tals in periodic structures and single molecules; issues related to order/disorder in nanostructured materials; and applications tending to the integra-tion into photonic devices for biology, lighting, communication, sensing and energy e%ciency.CHAIR: Tapio Niemi, Tampere University of Technology, Tampere, Finland
CL - BIOPHOTONICS AND APPLICATIONS
Emerging concepts in biophotonics: single particle/molecule detection and tracking; spa-tio-temporal manipulation of light fields for biomedicine; enhanced linear and nonlinear ex-citation and detection; micro-fluidics, optofluid-ics and micro-optics; new optical probes for local measurements including organic and inorganic nanoparticles, electric fields and temperature
measurements; New routes and modalities for optical detection in biophotonics: spectroscopy; holography, adaptive optics, phase conjugation time reversal; optics in biological media: scatter-ing; coherence; polarization; symmetry and invar-iance. Advanced light sources and geometries for microscopy, phototherapy, surgery, biomedicine.CHAIR: Thomas Huser, University of Bielefeld, Bielefeld, Germany
CM - MATERIALS PROCESSING WITH LASERS
Fundamentals of laser-materials interactions: phase transformation, chemical reactions, di"u-sion processes, ablation; high-power laser-ma-terials processing: welding, cutting, surface treatment; laser ablation; thin-film growth: PLD, LCVD; direct write techniques: MAPLE, LIFT, near-field techniques; 2D and 3D micro/nano structuring; plasma related processes; laser assist-ed nanosynthesis; femtosecond micromachining; ultrafast laser processing: volume modification, index engineering; laser-assisted manufacturing.CHAIR: Marc Sentis, Aix-Marseille University, Marseille, France
CN - PHOTONICS IN DEFENSE AND SECURITY
Optics for new military and non-military threats, peace keeping missions in urban theaters, border security. Novel imaging sys-tems with increased discrimination capabilities and spectroscopic techniques to characterize suspicious materials; three-dimensional im-aging, directed infrared countermeasures, and other new defense concepts; multispectral and polarimetric imaging.$ Automated target de-tection and identification. Enabling laser and focal plane arrays technologies. Light detection and ranging, incoherent and coherent LIDAR, laser velocimetry, vibrometry and profilometry;
LIDAR-RADAR concepts. Spectroscopic tech-niques for sensing biological and chemical species, including time resolved fluorescence, absorption, Raman, and LIBS spectroscopy. Detection and imaging of illegal substances (vapor phase, liquids and solid traces). Stand-o" detection of explosives and antipersonnel mines. Detector technologies from the UV to the THz range. Directed energy applications (e.g., laser weapon concepts). Propagation and turbulences e"ects mitigation. Beam directors and adaptive optics. Femtosecond lasers and as-sociated e"ects, e.g., filamentation and remote plasma generation.CHAIR: Joachim Wagner, Fraunhofer Institut für Angewandte Festkörperphysik, Freiburg, Germany
EQEC 2015 Topics
EA - QUANTUM OPTICS
Quantum light sources and applications; nonlo-cality and quantum interference; squeezing and entanglement; quantum correlations, coherence, and measurement; multimode and mesoscopic quantum optics; single photon emission and ab-sorption; quantum optics in cavities; slow light and quantum memories; quantum imaging and quantum lithography; quantum coherent e"ects in biology.CHAIR: Stephan Götzinger, Max Planck Institute for the Science of Light, Erlangen, Germany
EB - QUANTUM INFORMATION, COMMUNICATION, AND SIMULATION
Quantum computers and quantum communi-cation systems; quantum algorithms and com-munication protocols, quantum simulations, quantum key distribution, quantum logic gates,
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entanglement distribution and distillation, inter-faces between static and flying qubits, quantum memories;$integrated quantum devices, quantum nano-mechanics, ion-trap arrays, superconduct-ing structures, quantum dots, cavity QED systems.CHAIR: Gregor Weihs, University of Innsbruck, Innsbruck, Austria
EC - ATOM OPTICS AND QUANTUM MATTER
Developments in few- and many-body phe-nomena with ultracold quantum gases of atoms and molecules; quantum simulation of strongly correlated systems with artificial gauge fields, frustration, disorder and impuri-ties; out-of-equilibrium many-body phenome-na; superfluidity and thermodynamics in Bose and Fermi systems; dipolar physics with atoms and molecules; Efimov physics; quantum atom interferometry; controllable multiparticle en-tanglement; hybrid systems.CHAIR: Herwig Ott, University of Kaiserslautern, Kaiserslautern, Germany
ED – PRECISION METROLOGY AND FREQUENCY COMBS
Precision interferometry and spectroscopy in-cluding frequency combs; quantum metrology; ultimate limitations of measurement precision as imposed by the nature of quanta; tests of fundamental symmetries; definition of basic units; measurement of fundamental constants; applications in di"erent spectral ranges, includ-ing mid-infrared.CHAIR: Thomas Udem, Max Planck Institute of Quantum Optics, Garching, Germany
EE - ULTRAFAST OPTICAL SCIENCE
Fundamental aspects of ultrafast science in
all spectral regimes: attosecond science; carri-er-envelope e"ect; propagation and instabili-ties of ultrashort pulses in linear and nonlinear media, supercontinuum generation, ultrafast filamentation, extreme events and rogue waves; ultrafast spectroscopy in physics, chemistry and biology; propagation media: gas, liquid, and solid materials; free-space and waveguid-ed geometries.CHAIR: Goëry Genty, Tampere University of Technology, Tampere, Finland
EF - NONLINEAR PHENOMENA, SOLITONS AND SELF-ORGANIZATION
Nonlinear optical phenomena including dynam-ics and self-organization; frequency conversion, wave mixing, parametric processes, conservative and dissipative solitons, pattern formation, in-teraction between disorder and nonlinearities, complex behaviours and statistically heavy-tailed phenomena. Applications of nonlinear phenom-ena; nonlinear imaging and manipulation, novel optical materials, devices and systems. Funda-mental aspects of nonlinear dynamics in single or coupled photonic devices, polariton condensates, micro and nano lasers, photonic crystals, optom-echanical systems. CHAIR: Massimo Giudici, Institut Non Linéaire de Nice, Valbonne, France
EG – LIGHT-MATTER INTERACTIONS AT THE NANO-SCALE
Fundamental aspects of light-matter interactions at the nanoscale: single-photon sources, switches and detectors; nanoantennas and nanophotonic architectures; nano-optical detection, imaging and spectroscopy; coherent, quantum and non-linear optical e"ects; nanoscale electron sources, photovoltaics and catalysis; optical forces and
tweezers; radiative transfer.CHAIR: Mario Agio, National Institute of Optics (CNR - INO), Firenze, Italy
EH – PLASMONICS AND METAMATERIALS
Metal nanophotonics from fundamentals towards applications and including all spectral regimes: plasmonic nanostructures, antennas, cavities and waveguides; metamaterials; hybrid materials; nonlinear structures and e"ects; active systems, systems with gain.CHAIR: Jérôme Wenger, Institut Fresnel, Aix-Marseille University, Marseille, France
EI – THEORETICAL AND COMPUTATIONAL PHOTONICS
Predictive theoretical and computational ap-proaches for all fields of optics and photonics: full and semi-analytical treatments; applied math-ematics and numerical analysis of partial di"er-ential equations; high-performance computing, massively parallel codes, including utilization of hardware accelerators; singular nonlinear pro-cesses, shocks, wave collapse; material processing; first principle calculations of optical properties in dielectrics, plasmas, semiconductors and plas-monic structures; artificial optical materials.CHAIR: Stefan Skupin, CELIA, Université Bordeaux 1, Talence, France
CLEO®/Europe-EQEC 2015 Joint Symposia Topics
JSI - JOINT SYMPOSIUM ON LIGHT MANAGEMENT IN PHOTOVOLTAICS
In one hour, the sun delivers enough energy to the earth to meet global needs for an entire year. However, currently available semicon-ductor-based solar technologies are generally
unable to harvest a large portion of such lu-minous energy, in particular photons whose energy lies below the device band-gap. More than fi#y years ago, Shockley–Queisser (SQ) developed a detailed balance analysis which can be used to establish the limit e%ciency for single-junction solar cells at approximately 33.5% under the standard AM1.5G flat-plate solar spectrum. Nonetheless, record single junction cells have not yet achieved the full theoretical SQ e%ciency. For a solar cell device to approach the SQ limit, radiative recombina-tion must become the dominant loss mecha-nism and eventually be the only one to survive. When this occurs photonic considerations play a dominant role overtaking the electronic ones. !is symposium will provide an overview of novel photovoltaic (PV) concepts based on innovative approaches to light management and solar spectrum matching. Contributions are expected to address approaches to bring PV cell e%ciencies close to or beyond Shock-ley-Queisser theoretical limits.Topics will include, but are not limited to: pho-tonic and plasmonic materials to improve the performance of photovoltaic devices; surface tex-turing for light recycling in solar cell devices; use of random and periodic structured surfaces to in-crease the optical path length in photovoltaic ma-terials; light coupling into light trapping modes; substrate texturing to couple into whispering gallery modes; luminescent solar concentrators; down-shi#ing materials to convert UV or blue light into the visible or IR region; up-conversion of sub-bandgap photons; and novel non-Hermi-tian concepts.CO!CHAIRS: Jennifer Dionne, Stanford University, Stanford, CA, USAJordi Martorell, ICFO - The Institute of Photonic Sciences, Castelldefels, Barcelona, Spain
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JSII - JOINT SYMPOSIUM ON PHOTONIC LAB-ON-A-CHIP BIOSENSORS
!is symposium aims to provide the latest in-novations in photonic nanobiosensors and lab-on-a-chip optical systems having cutting-edge device performance as well as innovative in-tegration concepts and key emerging trends in a highly multi-disciplinary approach. !is symposium will cover topics including na-no-optics, plasmonics, silicon nanophotonics, quantum dots or graphene enabling novel op-tical transducing mechanisms such as label-free detection, single molecule detection, enhanced fluorescence, surface enhanced vibrational spec-troscopy ranging from mid-infrared, Raman to terahertz. It will also cover recent advances for lab-on-chip integration, low-cost and hand-held point-of-care imaging and detection devices, miniaturization, automation, and highly mul-tiplexed detection technologies.$ Applications are wide spread and cover highly impactful ap-plication areas such as genomics, proteomics, medical diagnostics, pharmacology, health care, environmental monitoring, food analysis, global health, agriculture, defense and security. !is symposium is a unique opportunity, of interest to both academic and industrial researchers, to discuss and exchange the latest developments in this extremely active field. Authors are invited to submit original develop-ments in nanobiosensors and lab-on-a-chip bi-ophotonic systems as well as recent up-coming applications of miniaturized and/or parallelized systems combined with advanced signal handling and telecommunication.CO!CHAIRS: Hatice Altug, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, SwitzerlandLaura M. Lechuga, Catalan Institute in Nanoscience and Nanotechnology (ICN2), CSIC & CIBER-BBN, Bellaterra (Barcelona), Spain
JSIII - JOINT SYMPOSIUM ON LASER-DRIVEN ACCELERATION
Particle accelerators play an essential role as tools for enabling scientific exploration.$ La-ser-based accelerator technology has evolved dramatically in the last decade, demonstrating orders of magnitude increase in the accelerating gradient, compared to conventional accelerators, and making the dream of compact accelerators feasible.$ Laser-plasma-driven wakefield acceler-ators deliver today high-quality electron beams in the few GeV range, with excellent stability, accelerated with gradients that exceed a few hundred GV/m using PW class laser systems at a repetition rate of 1 Hz.$ Laser-dielectric accelerators produce accelerating structures with a few hundred MV/m using more com-pact laser systems that operate at kHz repetition rates.$ !ese two complementary approaches have made significant progress and may provide the basis for future accelerators for high-ener-gy physics applications. !is new generation of laser-driven electron accelerators are already used to produce ultra-bright radiation beams in the keV to MeV range that are suitable for applications such as ultra-fast spectroscopy or contrast imaging.$ !ey have been also con-sidered for medical applications, radiotherapy, ultra-fast chemistry, radiobiology, and material science (for example, for non destructive mate-rial inspection).$ Significant progresses have also been made in research related to development of a compact FEL (Free-Electron Laser) that can benefit from the properties of the laser-acceler-ated electron beams. In addition to laser-driv-en acceleration of electrons, intense laser-solid interactions have demonstrated high gradient acceleration of ions.$ With the rapid develop-ment of laser technology, new, highly e%cient, regimes of ion acceleration using laser-solid interactions become possible.$ Such compact
sources of energetic ions can be used for ra-diography of dense matter and have attracted great interest for hadron therapy applications. !is joint symposium will focus on these three novel laser-driven acceleration techniques and their societal applications. Topics include: la-ser-plasma acceleration, relativistic laser-plas-ma interactions, ultra-bright radiation sources, compact FEL development, X-ray imaging, la-ser-dielectric acceleration, injection in laser-die-lectric accelerators, control of beam parameters in laser plasma accelerators, and laser acceler-ation of ions.CO!CHAIRS: Victor Malka, Laboratoire d'Optique Appliquée, Palaiseau, FranceCarl Schroeder, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
JSIV - JOINT SYMPOSIUM ON OPTICS IN GRAPHENE AND OTHER TWO-DIMENSIONAL MATERIALS
Graphene, a single-atomic sheet of carbon, has already led to many breakthroughs in diverse ar-eas of science and engineering. Due to its unique combination of electronic and optical proper-ties, it has also been recognized as a promising material in optoelectronics and optics in gen-eral. For example, the absence of a bandgap in graphene enables devices operating at ultra-high speeds and over an ultra-wide wavelength range, and the electrical tunability of the Dirac fermi-ons allows for a new class of plasmonic devices. More recently, other two-dimensional materi-als – most notably atomically thin transition metal dichalcogenides – have received much attention. These materials can complement graphene by overcoming its lack of a bandgap while still sharing many of graphene’s excellent properties. Significant progress has already been made in this exciting new field. !is symposium
will focus on fundamental aspects and applica-tions of graphene and other two-dimensional materials in optics and optoelectronics. It aims at bringing together scientists and engineers from academia and industry to exchange ideas and discuss recent results, potential applications and challenges.Topics include: Fundamental aspects of light-mat-ter interactions in 2D materials; ultrafast dynam-ics, nonlinear phenomena, and mode-locked lasers; light sources, modulators, detectors, and other optoelectronic devices; photovoltaics; smart windows and flexible displays; terahertz devices; tunable plasmonics and metamaterials; integra-tion with cavities and waveguides; multi-layered 2D heterostructures.CO!CHAIRS: Frank Koppens, ICFO - The Institute of Photonic Sciences, Castelldefels (Barcelona), SpainThomas Mueller, Vienna University of Technology, Vienna, Austria
JSV - JOINT SYMPOSIUM ON INTEGRATED QUANTUM OPTICS
!e possibility of generating, manipulating and measuring quantum state of light in miniatur-ized integrated optical structure is one of the most promising approaches for the realisation of practical quantum devices. At present there is a strong technological e"ort for increasing the complexity of the available devices towards the production of multi-photon quantum states that propagate over large integrated optical network and their detection on chip. Di"erent approach-es for the generation of nonclassical state of light include parametric down conversion in nonlin-ear waveguides and single emitters like quantum dots and single-defect centres. !ese sources can be integrated with cavity-type structure in order to control the spectral property and
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directionality of the emitted photons. Reconfig-urable quantum circuits are used for the manip-ulation of photons. Devices where multi-mode waveguides interference can be controlled us-ing tunable phase-shi#ers have been recently demonstrated. Typical implementations of reconfigurable circuits are realized by thermal heating or electro-optics e"ect. Recently high e%ciency superconducting single-photon de-tectors have also been integrated in waveguides providing one of the essential building block for the implementation of a fully integrated opti-cal platform. !e increased process complexity with the high coherence properties of integrat-ed quantum photonics o"ers a new avenue for quantum simulation and computation. Appli-cations of large-scale quantum walks can have application in e%cient simulation of physical, bi-ological and chemical systems, such as quantum e"ect in photosynthetic complexes and quan-tum transport. Moreover research on quantum sensing will certainly benefit from advances in quantum integrated photonics. !e integration of quantum sensors may lead to sensing devices having unprecedented resolution, such as accel-erometers, temperature sensors, stretch sensors. !is joint Symposium will deal with several as-pects of this new research area highlighting its recent development and its current challenges. Topics include: Generation of nonclassical state of light on integrated structure; manipulation of photons in waveguides; integrated single photon detectors; implementation of quantum informa-tion protocols on a chip; quantum simulation and quantum walk; Boson sampling; integrated quantum sensing and quantum interferometry.CO!CHAIRS: Mirko Lobino, Gri!th University, Brisbane, AustraliaFabio Sciarrino, Sapienza Università di Roma, Rome, Italy
LiM-CLEO®/Europe 2015 Joint Technical Focus Sessions
Two Technical Focus Sessions on Ultrafast Sol-id-State and Fibre Lasers (TF-1) and Materials Structuring Using Short Laser Pulses (TF-2) to take place on Tuesday a#ernoon are jointly held by CLEO®/Europe and LiM and will comprise three invited speakers each.CO!CHAIRS: Anatoly Grudinin, Fianium Ltd, Southampton, Hampshire, United KingdomLudger Overmeyer, Institut für Transport- und Automatisierungstechnik, Garbsen, Germany
LiM-CLEO®/Europe 2015 Joint Session
One session on Diagnostics and Control (CM/LiM) to take place on Tuesday morning is jointly held by CLEO®/Europe and LiM and will com-prise three invited talks.CO!CHAIRS: Anatoly Grudinin, Fianium Ltd, Southampton, Hampshire, United KingdomMarc Sentis, Aix-Marseille University, Marseille, France
ECBO-CLEO®/Europe 2015 Joint Sessions on Biophotonics:
Systems and Applications
Two sessions on Bioimaging (CLEO/ECBO-1) and Optical Manipulation of Biomatter (CLEO/ECBO-2) to be presented on Wednesday morning are jointly organised by CLEO®/Europe (CL com-mittee) and ECBO and will comprise a tutorial talk, two invited talks and contributed talks.CO!CHAIRS: Giulio Cerullo, Politecnico di Milano, Milan, Italy
Rainer Leitgeb, Medical University Vienna, Vienna, Austria
SPIE-Optical Metrology-EQEC 2015 Joint Session
One session on Computational Photonics for Metrology Applications (JS SPIE/OM/EQEC) to be presented on Monday a#ernoon is jointly organised by SPIE-Optical Metrology-EQEC and will comprise three invited speakers.CO!CHAIRS: Stefan Skupin, CELIA, Université Bordeaux 1, Talence, FranceBernd Bodermann, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany
CLEO®/Europe 2015 Committees
Steering Committee
EUROPEAN PHYSICAL SOCIETY (EPS): CHAIR: W. Andrew Clarkson, University of Southampton, Southampton, United Kingdom
Thorsten Ackemann, University of Strathclyde, Glasgow, United Kingdom
Luc Bergé, CEA - DAM, Arpajon, France
Giulio Cerullo, Politecnico di Milano, Milan, Italy
John Dudley, Université de Franche-Comté, Besançon, France
Jürgen Eschner, Universität des Saarlandes, Saarbrücken, Germany
Patrick Georges, Institut d'Optique Graduate School, Palaiseau, France
Patricia Helfenstein, European Physical Society, Mulhouse, France
Martti Kauranen, Tampere University of Technology, Finland
Reinhard Kienberger, Max Planck Institute for Quantum Optics, Garching, Germany
David Lee, European Physical Society, Mulhouse, France
Markus Pollnau, KTH - Royal Institute of Technology, Stockholm, Sweden
Valerio Pruneri, ICFO - The Institute of Photonic Sciences and ICREA, Castelldefels, Spain
Christine Silberhorn, University of Paderborn, Paderborn, Germany
IEEE PHOTONICS SOCIETY:Christine Bluhm,IEEE Photonics Society, Piscataway, NJ, USA
Martin Dawson, University of Strathclyde, Glasgow, United Kingdom
Anders Larsson, Chalmers University, Göteborg, Sweden
John Gerard McInerney, National University of Ireland, Cork, Ireland
THE OPTICAL SOCIETY (OSA):Peter E. Andersen, DTU Fotonik - Technical University of Denmark, Roskilde, Denmark
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Kari Apter, The Optical Society, Los Altos, CA, USA
Stefan Maier, Imperial College London, London, United Kingdom
Elizabeth Rogan, The Optical Society, Washington DC, USA
Alphan Sennaro"lu, Koç University, Istanbul, Turkey
Organising Committees
GENERAL CHAIRS:Luc Bergé, CEA-DAM, Arpajon, France
Patrick Georges, Institut d'Optique Graduate School, Palaiseau, France
PROGRAMME CHAIRS:Giulio Cerullo, Politecnico di Milano, Milano, Italy
Valerio Pruneri, The Institute of Photonic Sciences & ICREA, Castelldefels, Spain
LOCAL CHAIR:Reinhard Kienberger, Max Planck Institute of Quantum Optics, Garching, Germany
Programme Committee:
CA - SOLID-STATE LASERS
CHAIR: Mauro Tonelli, Universita' di Pisa, Pisa, Italy
David Coutts, Macquarie University, Sydney, Australia
Frédéric Druon, Laboratoire Charles Fabry de l’Institut d’Optique, Palaiseau, France
Christian Kraenkel, University of Hamburg, Hamburg, Germany
Nikolay Kuleshov, Belarusian State Polytechnic Academy, Minsk, Belarus
Jacob Mackenzie, University of Southampton, Southampton, Hampshire, United Kingdom
Yasutake Ohishi, Toyota Technological Institute, Nagoya, Japan
Valdas Pasiskevicius, KTH - Royal Institute of Technology, Stockholm, Sweden
Valentin Petrov, Max-Born Institute, Berlin, Germany
Martin Schellhorn, French-German Research Institute (ISL), Saint-Louis, France
Evgeny Sorokin, Technical University of Vienna, Vienna, Austria
CB - SEMICONDUCTOR LASERS
CHAIR: Maria Ana Cataluna, University of Dundee, Nethergate, Dundee, United Kingdom
Erwin Bente, Technische Universiteit Eindhoven, COBRA Research Institute, Eindhoven, The Netherlands
Dan Botez, University of Wisconsin-Madison, Madison, USA
Stefan Breuer, Technical University of Darmstadt, Darmstadt, Germany
Mariangela Gioannini, Politecnico di Torino, Torino, Italy Guido Giuliani,
Università di Pavia, Pavia, Italy Mircea Guina, Tampere University of Technology, Tampere, Finland
Michel Krakowski, Thales Research & Technology France, Palaiseau, France
Marc Sorel, University of Glasgow, Glasgow, United Kingdom
Gottfried Strasser, Technical University of Vienna, Vienna, Austria
Dimitris Syvridis, National and Kapodestrian University of Athens, Athens, Greece
CC - TERAHERTZ SOURCES AND APPLICATIONS
CHAIR: Thomas Dekorsy, University of Konstanz, Konstanz, Germany
Jorge Bravo-Abad, Universidad Autónoma de Madrid, Madrid, Spain
Jérôme Faist, ETH - Institute for Quantum Electronics, Zürich, Switzerland
Kazuhiko Hirakawa, University of Tokyo, Tokyo, Japan
Petr Ku#el, Academy of Sciences of the Czech Republic, Prague, Czech Republic
Edmund Linfield, University of Leeds, Leeds, United Kingdom
James Lloyd-Hughes, University of Oxford, Oxford, United Kingdom
Paul Planken, Advanced Research Center for Nanolithography (ARRCNL), Amsterdam, The Netherlands
Jérôme Tignon, Ecole Normale Supérieure, Paris, France
Alessandro Tredicucci, Scuola Normale di Pisa, Pisa, Italy
Stelios Tzortzakis, FORTH, Crete, Greece
CD - APPLICATIONS OF NONLINEAR OPTICS
CHAIR: Concita Sibilia, Università di Roma “La Sapienza”, Roma, Italy
Ady Arie, Tel Aviv University, Tel Aviv, Israel
Gaetano Assanto, University degli Studi di Roma Tre, Roma, Italy
Oleg Egorov, Friedrich-Schiller-Universität Jena, Jena, Germany
Joe. W. Haus, University of Dayton, Dayton, USA
Miroslaw Karpierz, Warsaw University of Technology, Warsaw, Poland
Gregor Knopp, Paul Scherrer Institute, Villigen, Switzerland
Guy Millot, CNRS, Université de Bourgogne, Dijon, France
Roberto Morandotti, Université Laval, Varennes (Québec), Canada
Fabrice Raineri, LPN-CNRS, Marcoussis, France
Ventsislav Valev, University of Cambridge, Cambridge, United Kingdom
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CE - OPTICAL MATERIALS, FABRICATION AND CHARACTERISATION
CHAIR: Stefan Kück, Physikalisch- Technische Bundesanstalt, Braunschweig, Germany
Patrice Camy, University of Caen, Caen, France
Martin Dawson, University of Strathclyde, Glasgow, United Kingdom
Volkmar Dierolf, Lehigh University, Bethlehem, USA
Kenichi Goushi, Kyushi University, Fukuoka City, Japan
Michael Jetter, University of Stuttgart, Stuttgart, Germany
Pascal Loiseau, Laboratoire de Chimie de la Matière Condensée de Paris, Paris, France
Mikhail A. Noginov, Norfolk State University, Norfolk, VA, USA
Witold Ryba-Romanowski, Polish Academy of Science, Wroclaw, Poland
Pier Sazio, University of Southampton, Southampton, UK
Val Zwiller, Delft University of Technology, Delft, The Netherlands
CF - ULTRAFAST OPTICAL TECHNOLOGIES
CHAIR: Thomas Südmeyer, University of Neuchâtel, Neuchâtel, Switzerland
Daniele Brida, Konstanz University, Konstanz, Germany
Kjeld Eikema, Vrije Universiteit, Amsterdam, The Netherlands
Alan Fry, Stanford University, SLAC National Accelerator Laboratory, Menlo Park, CA, USA
Takao Fuji, Institute for Molecular Science, Okazaki, Japan
Rupert Huber, University of Regensburg, Regensburg, Germany
Rodrigo Lopez-Martens, LOA, ENSTA-ParisTech, CNRS, Ecole Polytechnique, Palaiseau, France
Fabian Rotermund, Ajou University, Suwon, Korea
Jan Rothhardt, Jena University, Jena, Germany
Taro Sekikawa, Hokkaido University, Sapporo, Japan
Hans-Jakob Woerner, ETH Zürich, Zürich, Switzerland
CG - HIGH-FIELD LASER PHYSICS AND ATTOSECOND TECHNOLOGIES
CHAIR: Matthias Kling, Ludwig-Maximilians-Universität München, Garching, Germany
Peter Dombi, Wigner Research Centre for Physics, Budapest, Hungary
Lukas Gallmann, ETH Zürich, Zürich, Switzerland
Franck Lepine, LASIM-CNRS, Lyon, France
Fernando Martin, University of Madrid, Madrid, Spain
Johan Mauritsson, Lund University, Lund, Sweden
Karoly Osvay, University of Szeged, Szeged, Hungary
Gerhard Paulus, Jena University, Jena, Germany
Giuseppe Sansone, Politecnico di Milano, Milano, Italy
Paris Tzallas, University of Crete – FORTH, Heraklion, Crete, Greece
Amelle Zaïr, Imperial College London, London, United Kingdom
CH - OPTICAL SENSING AND METROLOGY
CHAIR: Trevor Benson, University of Nottingham, Nottingham, United Kingdom
Francisco J. Arregui, Universidad Publica de Navarra, Pamplona, Spain
Francis Berghmans, Vrije Universiteit Brussel, Brussels, Belgium
Wojtek Bock, Université du Québec en Outaouais, Gatineau, Quebec, Canada
Paolo De Natale, Istituto Nazionale di Ottica-CNR, Firenze, Italy
Sonia Garcia Blanco, University of Twente, Enschede, The Netherlands
Stephen James, Cranfield University, Cranfield, United Kingdom
Henrik Krisch, Krohne Messtechnik GmbH, Duisburg, Germany
Walter Lubeigt, M Squared Lasers LTD, Glasgow, United Kingdom
Marian Marciniak, National Institute of Telecommunications, Warsaw, Poland
Walter Margulis, ACREO, Kista, Sweden
CI - OPTICAL TECHNOLOGIES FOR COMMUNICATIONS AND DATA STORAGE
CHAIR: Erwan Pincemin, Orange Labs Networks, Lannion, France
Juan-Diego Ania-Castanon, Instituto de Optica, Consejo Superior de Investigaciones Cientificas (CSIC), Madrid, Spain
Sander Jansen, ADVA Optical Networking, Martinsried/Munich, Germany
Yves Jaouen, Telecom ParisTech, Paris, France
Dimitrios Klonidis, Athens Information Technology Centre, Peania-Attika, Greece
Franko Küppers, University of Darmstadt, Darmstadt, Germany
Bob Manning, University College Cork, Tyndall National Institute, Cork, Ireland
Dan Marom, Hebrew University of Jerusalem, Jerusalem, Israel
Marco Romagnoli, Advanced Technologies for Photonic Integration at CNIT and Scuola Superiore S. Anna, Pisa, Italy
Alessandro Tonello, Université de Limoges, Limoges, France
CJ - FIBRE AND GUIDED WAVE LASERS AND AMPLIFIERS
CHAIR: Thomas Vestergaard Andersen, NKT Photonics A/S, Birkerod, Denmark
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Claude Aguergaray, Auckland University, Auckland, New Zealand
Alexander Argyros, University of Sydney, Sydney, Australia
Géraud Bouwmans, University of Lille, Lille, France
Ryszard Buczynski, University of Warsaw, Warsaw, Poland
Annamaria Cucinotta, University of Parma, Parma, Italy
Ammar Hideur, Université de Rouen, UMR 6614 CORIA, Saint-Etienne du Rouvray, France
Matthias Jäger, Institute of Photonic Technologies (IPHT), Jena, Germany
Kent Erik Mattsson, LightWork, Virum, Denmark
César Jauregui Misas, Institute of Applied Physics, Jena, Germany
Yoann Zaouter, Amplitude Systèmes, Bordeaux, France
CK - MICRO- AND NANO-PHOTONICS
CHAIR: Tapio Niemi, Tampere University of Technology, Tampere, Finland
Alexandra Boltasseva, Purdue University, West Lafayette, IN, USA
Olivier Gauthier-Lafaye, LAAS-CNRS, Toulouse, France
Uli Lemmer, Karlsruhe Institute of Technology, Karlsruhe, Germany
Heidi Ottevaere, Vrije Universiteit Brussel, Brussels, Belgium
Stefano Pelli, CNR-IFAC, Sesto Fiorentino (FI), Italy
Frank Peters, Tyndall National Institute, Cork, Ireland
Alex Rozhin,Aston University, Birmingham, United Kingdom
Peter G.R. Smith, University of Southampton, Southampton, United Kingdom
Jos van der Tol, Technische Universiteit Eindhoven, Eindhoven, The Netherlands
Kresten Yvind, Technical University of Denmark, Lyngby, Denmark
CL - BIOPHOTONICS AND APPLICATIONS
CHAIR: Thomas Huser, University of Bielefeld, Bielefeld, Germany
Laurent Cognet, CNRS & Université Bordeaux, Talence, France
Christian Eggeling, University of Oxford, Oxford, United Kingdom
Annika Enejder, Chalmers University of Technology, Göteborg, Sweden
Paul M. W. French,Imperial College London, London, United Kingdom
Robert Huber, Universität zu Lübeck, Lübeck & Ludwig-Maximilians-Universität, München, München, Germany
Varpu Marjomäki, University of Jyväskylä, Jyväskylä, Finland
Hermann L. O$erhaus, University of Twente, Enschede, The Netherlands
Francesco Pavone, University of Florence, Sesto-Fiorentino (Firenze), Italy
Halina Rubinsztein-Dunlop, University of Queensland, Kenmore, Brisbane, Australia
CM - MATERIALS PROCESSING WITH LASERS
CHAIR: Marc Sentis, Aix-Marseille University, Marseille, France
Yves Bellouard, Ecole Polytechnique Fédérale de Lausanne (EPFL), Neuchâtel, Switzerland
Marta Castillejo, Instituto de Quimica Fisica Rocasolano, Spanish National Research Council (CSIC), Madrid, Spain
Lan Jiang, Beijing Institute of Technology, Beijing, China
Peter Kazansky,University of Southampton, Highfield, Southampton, United Kingdom
Vitaly Konov, Natural Sciences Center, Moscow, Russia
Stefan Nolte, Friedrich-Schiller-University Jena, Jena, Germany
Gerard O'Connor, National University of Ireland, Galway, Ireland
Takashige Omatsu, Chiba University, Tokyo, Japan
Roberto Osellame, Politecnico di Milano, Milano, Italy
Emmanuel Stratakis, IESL, Foundation for Research and Technology - Hellas (FORTH), Heraklion, Greece
CN - Photonics in Defense and SecurityCHAIR: Joachim Wagner, Fraunhofer Institut für Angewandte Festkörperphysik, Freiburg, Germany
Mark Eichhorn, French-German Research Institute of Saint-Louis (ISL), Saint-Louis, France
Peter Geiser, Norsk Elektro Optikk AS, Skedsmokorset, Norway
Markus Haiml, AIM Infrarot-Module GmbH, Heilbronn, Germany
Chris Howle, Defence Science and Technology Laboratory, Salisbury, United Kingdom
Eric Lallier, Thales Research and Technology, Palaiseau, France
Jerry Meyer, Naval Research Laboratory, Washington, DC, USA
Antoni Rogalski, Military University of Technology, Warsaw, Poland
Peter Schunemann, BAE Systems, Nashua, USA
David Stothard, Fraunhofer Centre for Applied Photonics, Glasgow, United Kingdom
Hans Tholl, Diehl BGT Defence GmbH & Co. KG, Ueberlingen, Germany
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EQEC 2015 Committee
Organising Committee
GENERAL CHAIRS:Jürgen Eschner, Universität des Saarlandes, Saarbrücken, Germany
Martti Kauranen, Tampere University of Technology, Tampere, Finland
EQEC PROGRAMME CHAIRS:Thorsten Ackemann, Strathclyde University, Glasgow, United Kingdom
Christine Silberhorn, Universität Paderborn, Paderborn, Germany
CLEO®/EUROPE-EQEC LOCAL CHAIR:Reinhard Kienberger, Max Planck Institute of Quantum Optics, Garching, Germany
Programme Committees EA - QUANTUM OPTICS
CHAIR: Stephan Götzinger, Max Planck Institute for the Science of Light, Erlangen, Germany
Charles S. Adams, Durham University, Durham, United Kingdom
Mete Atature, University of Cambridge, Cambridge, United Kingdom
Mikael Afzelius, University of Geneva, Geneva, Switzerland
Michael Chapman, Georgia Institute of Technology, Atlanta, Georgia, USA
Markus Hennrich, University of Innsbruck, Innsbruck, Austria
David Hunger, Max Planck Institute of Quantum Optics, Munich, Germany
Ping Koy Lam, The Australian National University, Canberra, Australia
Julien Laurat, Laboratoire Kastler Brossel, Université P. et M. Curie, ENS, CNRS, Paris, France
Juan Pérez Torres, The Institute of Photonic Sciences - ICFO, Castelldefels, Spain
Nikolay Vitanov, Sofia University, Sofia, Bulgaria
EB - QUANTUM INFORMATION, COMMUNICATION, AND SIMULATION
CHAIR: Gregor Weihs, University of Innsbruck, Innsbruck, Austria
Miloslav Dusek, Palacky University, Olomouc, Czech Republic
Jens Eisert, Freie Universität Berlin, Berlin, Germany
Alessandro Fedrizzi, The University of Queensland, Brisbane St Lucia, Australia
Hartmut Hae$ner, University of California at Berkeley, Berkeley, CA, USA
Alan Migdall, NIST, Gaithersburg, MD, USA
Yasser Omar, Technical University of Lisbon, Lisbon, Portugal
Andreas Poppe, AIT Austrian Institute of Technology GmbH, Vienna, Austria
Andrew Shields, Toshiba Research Europe Ltd., Cambridge, United Kingdom
Nicolas Treps, Université Pierre et Marie Curie, Laboratoire Kastler Brossel, Paris, France
Harald Weinfurter, Ludwig-Maximilians-Universität München, München, Germany
EC - ATOM OPTICS AND QUANTUM MATTER
CHAIR: Herwig Ott, University of Kaiserslautern, Kaiserslautern, Germany
Aidan Arnold, Strathclyde University, Glasgow, United Kingdom
Philippe Bouyer, Université Bordeaux 1, Talence, France
Olivier Dulieu, Laboratoire Aimé Cotton, Orsay, France
Zoran Hadzibabic, University of Cambridge, Cambridge, United Kingdom
Corinna Kollath, University of Geneva, Geneva, Switzerland
Michele Modugno, Universidad del Pais Vasco, Bilbao, Spain
Hanns-Christoph Nägerl, University of Innsbruck, Innsbruck, Austria
Gupta Subhadeep, University of Washington, Seattle, WA, USA
Philipp Treutlein, University of Basel, Basel, Switzerland
Chris Vale, Swinburne University of Technology, Hawthorn, Victoria, Australia
ED – PRECISION METROLOGY AND FREQUENCY COMBS
CHAIR: Thomas Udem, Max Planck Institute of Quantum Optics, Garching, Germany
Livio Gianfrani, University of Napoli, Caserta, Italy
Hidetoshi Katori, The University of Tokyo, Saitama, Japan
Nikolai N. Kolachevsky, Russian Academy of Sciences, P.N. Lebedev Physical Institute, Moscow, Russia
Yann Le Coq, LNE SYRTE, Observatoire de Paris, Paris, France
Helen Margolis, National Physical Laboratory, Teddington, United Kingdom
François Nez, Université Pierre et Marie Curie, Laboratoire Kastler Brossel, Paris, France
Chris W. Oates, NIST, Boulder, CO, USA
Vitaly D. Ovsiannikov, Voronezh State University, Voronezh, Russia
Stephan Schiller, Heinrich-Heine-Universität Düsseldorf, Düsseldorf, Germany
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EE - ULTRAFAST OPTICAL SCIENCE
CHAIR: Goëry Genty, Tampere University of Technology, Tampere, Finland
Stéphane Coen, University of Auckland, Auckland, New Zealand
Daniele Faccio, Heriot-Watt University, Edinburgh, United Kingdom
Mark Foster, John Hopkins University, Baltimore, MD, USA
Stefan Haacke, University of Strasbourg, CNRS IPCMS, Strasbourg, France
Peter Hommelho$, University of Erlangen-Nuremberg, Erlangen, Germany
Daniil Kartashov, Friedrich-Schiller University, Jena, Germany
Christoph Lienau, University of Oldenburg, Oldenburg, Germany
Luca Perfetti, Ecole Polytechnique, Palaiseau, France
Tenio Popmintchev, University of Colorado, Boulder, Co, USA
John Travers, Max Planck Institute for the Science of Light, Erlangen, Germany
EF - NONLINEAR PHENOMENA, SOLITONS AND SELF-ORGANIZATION
CHAIR: Massimo Giudici, Institut Non Linéaire de Nice, Valbonne, France
Salvador Balle, Universitat de les Illes Balears, Palma de Mallorca, Spain
Randy Bartels, Colorado State University, Fort Collins, USA
Carlota Canalias, KTH - Royal Institute of Technology, Stockholm, Sweden
Iacopo Carusotto, Università di Trento, Trento, Italy
Rachel Grange, ETH-Zürich, Zürich, Switzerland
Philippe Grelu, Université de Bourgogne, Dijon, France
Ariel Levenson, CNRS, Laboratoire de Photonique et de Nanostructures, Marcoussis, France
Lino Misoguti, Universidade de São Paulo, São Paulo, Brazil
Noel Smyth, University of Edinburgh, Edinburgh, United Kingdom
Andrei Vladimirov, Weierstrass Institute for Applied Analysis and Stochastics, Berlin, Germany
EG – LIGHT-MATTER INTERACTIONS AT THE NANO-SCALE
CHAIR: Mario Agio, National Institute of Optics (CNR - INO), Firenze, Italy
Fedor Jelezko, University of Ulm, Ulm, Germany
Astrid Lambrecht, Université Paris 6, Laboratoire Kastler Brossel, Paris, France
Brahim Lounis, Institut d'Optique Graduate School, CNRS & Université Bordeaux, Talence France
David Norris, ETH Zürich, Zürich, Switzerland
Romain Quidant, ICFO - The Institute of Photonic Sciences, Castelldefels, Spain
Markus Raschke, University of Colorado & JILA, Boulder, CO, USA
Païvi Törmä, Aalto University, Aalto, Finland
Ewold Verhagen, FOM Institute AMOLF, Amsterdam, The Netherlands
Thomas Volz, Macquarie University, Sydney, Australia
Rashid Zia, Brown University, Providence, USA
EH – PLASMONICS AND METAMATERIALS
CHAIR: Jérôme Wenger, Institut Fresnel, Aix-Marseille University, Marseille, France
Javier Aizpurua, Center for Material Physics (CSIC - UPV/EHU and DIPC), Donostia - San Sebastian, Spain
Andrea Alù, University of Texas at Austin, Austin, USA
Alexandre Bouhelier, CNRS, Laboratoire Interdisciplinaire Carnot de Bourgogne, Dijon, France
Sol Carretero Palacios, Instituto de Cienca de Materiales de Sevilla, Sevilla, Spain
Luca Dal Negro, Boston University, Boston, USA
Vassili Fedotov, University of Southampton, Southampton, United Kingdom
Femius Koenderink, FOM Institute AMOLF, Amsterdam, The Netherlands
Kristjan Leosson, Innovation Center Iceland, Reykjavik, Iceland
Din Ping Tsai, National Taiwan University, Taipei, Taiwan
Ralf Vogelgesang, University of Oldenburg, Oldenburg, Germany
EI – THEORETICAL AND COMPUTATIONAL PHOTONICS
CHAIR: Stefan Skupin, CELIA, Université Bordeaux 1, Talence, France
Uwe Bandelow, WIAS, Berlin, Germany
Eduardo Cabrera Granado, Universidad Complutense de Madrid, Madrid, Spain
Claudio Conti, Sapienza Università di Roma, Rome, Italy
Anton S. Desyatnikov, The Australian National Laboratory, Canberra, Australia
Miroslav Kolesik, University of Arizona, Tucson, AZ, USA
David Lannes, Ecole Normale Supérieure, DMA, Paris, France
Emmanuel Lorin de la Grandmaison, Carleton University, Ottawa, Canada
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Gian-Luca Oppo, University of Strathclyde, Strathclyde, United Kingdom
Dmitry Pelinovsky, McMaster University, Hamilton, Canada
Carsten Rockstuhl, TFP KIT, Karlsruhe, Germany
CLEO®/Europe-EQEC 2015 JOINT SYMPOSIA COMMITTEES
JSI - JOINT SYMPOSIUM ON LIGHT MANAGEMENT IN PHOTOVOLTAICS
CO-CHAIRS:Jennifer Dionne, Stanford University, Stanford, CA, USAJordi Martorell, ICFO - The Institute of Photonic Sciences, Castelldefels, Barcelona, Spain
JSII - JOINT SYMPOSIUM ON PHOTONICS LAB-ON-A-CHIP BIOSENSORS
CO-CHAIRS:Hatice Altug, Ecole Polytechnique Fédérale de Lausanne (EPFL), Lausanne, SwitzerlandLaura M. Lechuga, Catalan Institute in Nanoscience and Nanotechnology (ICN2), CSIC & CIBER-BBN, Bellaterra (Barcelona), Spain
JSIII - JOINT SYMPOSIUM ON LASER-DRIVEN ACCELERATION
CO-CHAIRS:Victor Malka, Laboratoire d'Optique Appliquée, Palaiseau, FranceCarl Schroeder,Lawrence Berkeley National Laboratory, Berkeley, CA, USA
JSIV - JOINT SYMPOSIUM ON OPTICS IN GRAPHENE AND OTHER TWO-DIMENSIONAL MATERIALS
CO-CHAIRS:Frank Koppens, ICFO - The Institute of Photonic Sciences, Castelldefels (Barcelona), SpainThomas Mueller, Vienna University of Technology, Vienna, Austria
JSV - JOINT SYMPOSIUM ON INTEGRATED QUANTUM OPTICS
CO-CHAIRS:Mirko Lobino, Gri!th University, Brisbane, AustraliaFabio Sciarrino, Sapienza Università di Roma, Rome, Italy
LiM-CLEO®/Europe 2015 Joint Technical Focus Sessions
TF-1 ULTRAFAST SOLID-STATE AND FIBRE LASERS
TF-2 MATERIALS STRUCTURING USING SHORT LASER PULSES
CO-CHAIRS: Anatoly Grudinin, Fianium Ltd, Southampton, Hampshire, United KingdomLudger Overmeyer, Institut für Transport- und Automatisierungtechnik, Garbsen, Germany
Joint Session LiM-CLEO®/Europe 2015
CM/LIM - DIAGNOSTICS AND CONTROL
CO-CHAIRS:Anatoly Grudinin, Fianium Ltd, Southampton, Hampshire, United KingdomMarc Sentis, Aix-Marseille University, Marseille, France
Joint Sessions ECBO-CLEO®/Europe 2015 on Biophotonics:
Systems and Applications
CLEO/ECBO-1 BIOIMAGING
CLEO/ECBO-2 OPTICAL MANIPULATION OF BIOMATTER
CO-CHAIRS:Giulio Cerullo, Politecnico di Milano, Milan, ItalyRainer Leitgeb, Medical University Vienna, Vienna, Austria
SPIE-Optical Metrology-EQEC 2015 Joint Session
JS SPIE/OM/EQEC - COMPUTATIONAL PHOTONICS FOR METROLOGY APPLICATIONS
CO-CHAIRS:Stefan Skupin, CELIA, Université Bordeaux 1, Talence, FranceBernd Bodermann, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany
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GENERAL INFORMATION
Abstracts of the papers to be presented at CLEO®/Europe-EQEC 2015 appear in this advance pro-gramme. !e presentation of the large number of contributed papers requires that up to 14 parallel sessions will take place daily during the conference. !e programme includes 10 short courses, 14 CLEO®/Europe topics, 9 EQEC top-ics, 5 joint CLEO®/Europe-EQEC symposia, 2 LiM-CLEO®/Europe technical focus sessions, 1 CLEO®/Europe-LiM joint session, 1 SPIE-Opti-cal Metrology-EQEC joint session and 2 CLEO®/Europe-ECBO joint sessions. !e short courses and all sessions will be held at the International Congress Centre in Munich (so called ICM) and over the exhibition halls of the trade fair grounds LASER World of PHOTONICS 2015. These rooms are named according to famous physicists: Curie, Edison, Einstein, Hertz, Maiman, Newton 2 and Röntgen.!e CLEO®/Europe-EQEC 2015 technical pro-gramme features 1611 presentations. !ese in-clude 5 Plenary talks, 5 Tutorial talks, 8 Keynote talks, 82 Invited talks, 7 upgraded talks to invited, 6 Technical Focus talks, and a total of 924 oral contributions. 2 Postdeadline sessions (18 oral talks) are also added. !e conference also features 574 posters. As you know, 2015 is a special year for the photon-ics community proclaimed International Year of Light and Light-Based Technologies by the United Nations. !e World of Photonics Congress being a major event in the global IYL calendar, it features a number of activities that celebrate the e"ects that light-based technologies have on the quality of life and as a key force that drives the economy.
Please note that special events added to cele-brate the 2015 International Year of Light and
Light-Based Technologies made us change the structure of the conference especially on Monday where half sessions are built in order to fit in the very tight schedule.
Conference Dates
CLEO®/Europe-EQEC 2015 will be running from Sunday 21 June, 8:30 to !ursday 25 June, 17:30.
2015 World of Photonics Congress Opening and Plenary Talk
!e o%cial World of Photonics Congress opening will take place on Monday 22 June, from 9:00 to 11:00, Room 1.In the honour of the UN proclaimed 2015 In-ternational Year of Light and Light-Based Technologies, the ceremony dedicated to “Light solutions for the Society Challenges of our World” will start with a couple of welcome ad-dresses, short invited talks and will be followed by a Plenary Talk.
T"#$ %&'$()*$:09:30 – 10:00
! Words of Welcome by Reinhard Pfei+er, Deputy CEO, Messe München International.
! Welcome Address by Flavia Schlegel, As-sistant Director-General for Natural Scienc-es, UNESCO.
! International Year of Light – !e Europe-an Perspective
by Günther Oettinger, Commissioner Dig-ital Economy & Society.
! International Year of Light – !e Ameri-can Perspective
by Lawrence S. Goldberg, Senior Engineer-ing Advisor, Division of Electrical, Communi-cations and Cyber Systems (ECCS) National Science Foundation.
! International Year of Light – !e African Perspective
by Yanne K. Chembo, ERC Starting Grand Laureate, Centre National de la Recherche Scientifique (CNRS) Paris, African Physi-cal Society.
Moderation: John Dudley, Université de Franche-Comté, Besançon, France, Chair-man of the International Year of Light Steer-ing Committee
10:00 – 10:45! Opening Plenary Lecture of World of Pho-
tonics Congress High Performance Quantum Cascade La-
sers from the Mid-IR to the Far-IR and their impact on Science and Technology
by Federico Capasso, Professor of Applied Physics, University of Harvard, Cambridge, MA, USA.
Session Chair: Patrick Georges, Institut d'Optique Graduate School, Laboratoire Charles Fabry, Palaiseau, France
Prizes and Awards
A series of Prize and Award ceremonies will take place during the Plenary session scheduled Tues-day 23 June from 10:30 to 12:30, Room 1.During this session Serge Haroche, Collège de France, Laboratoire!Kastler!Brossel & École Normale Supérieure, Paris, France, will present a plenary talk on “Real and Artificial Atoms Interacting with Photons: From Fundamental Physics to Quantum Information”.
!e following Prizes and Awards will be presented:! EPS-QEOD and EPS Young Minds 2015 Trav-
el Grant Student Awards ! 2015 Awards of the European Physical Society
– Quantum Electronics and Optics Division:
! (2) Quantum Electronics Prizes. ! (2) Fresnel Prizes. ! (4) PhD !esis Prizes. See EPS-QEOD Prize Ceremony brochure.! OSA Robert E. Hopkins Leadership Award! OSA Fellow Member Recognition! OSA/DPG Herbert Walther Award! IUPAP Commission 17 - Laser Physics and
Photonics biennial Young Scientists Prizes 2015! Announcement of the LIGHT2015 Awards
!e European Optical Society and the LIGHT2015 project will announce the winners for the LIGHT2015 Young Photonics Entrepreneur Award and the LIGHT2015 Young Women in Photonics Awards. !e Award Ceremony will take place on Wednesday 24 June, 16:00 - 16:20, Room 2.
See programme in the parallel sessions.
Poster Sessions
Posters are a major attraction and provide an intimate interaction between the presenter and the viewer. To allow participants to see as many posters as possible, all CLEO®/Europe-EQEC 2015 posters will be displayed in Hall B0 (ground floor) next to the ICM centre. !e conference will feature 5 poster sessions taking place from Sunday to !ursday a#er lunchtime. !ere will be no oral presentations during this time.
P,%-$. -"#$ %&'$()*$%:! Sunday: 12:30 - 13:30 (CA, CC, CL, CM and EE topics)! Monday: 13:30 - 14:30 (CB, CK, ED, EG and JSV topics)! Tuesday: 13:00 - 14:00 (CD, CE, CI, CN, EC, EI, JSI, JSII and JSIV topics)! Wednesday: 13:00 - 14:00 (CF, CJ, EB, and EH topics)! !ursday: 13:00 - 14:00 (CG, CH, EA, and EF topics)
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Authors are requested to display their poster on their allocated board in the morning of the day of their presentation. !e poster presentations can remain on the boards until 5:00pm.In order to present their work and answer ques-tions, authors are requested to be present in the vicinity of their poster on the day of their pres-entation time. !ere will be no oral presentations during this time.Each author is provided with one board on which to display a summary of the paper. !e size of the poster should not exceed 100-105 cm wide & 150 cm high. Fixing material (adhesive tape) will be provided.!e boards will be grouped by topics and marked with the poster reference numbers. !e schedule of the poster sessions is presented on the respective pages of the advance programme.All poster presenters need to be physically pres-ent during their assigned poster session on the assigned day. In case of no show, the poster pres-entation will be discarded from the publications.
Speakers’ Information
D)./-",0 ,1 -'$ -/*2%:! Contributed presentations are 15 minutes in-
cluding discussion.! Invited presentations are 30 minutes includ-
ing discussion.! Tutorial presentations are 60 minutes includ-
ing discussion.! Keynote presentations are 45 minutes includ-
ing discussion.! Plenary presentations are 45 minutes including
discussion and may extend up to 60 minutes with the Chair presentation.
Speakers are asked to check-in with the session chair in the room of their relevant session ten minutes before the beginning of the session.
During the World of Photonics Congress a net-work-based presentation system will be used along with a congress specific interface to ensure a high quality of all presentations.Speakers were requested to upload their presenta-tions prior the conference began, to a protected server of M Events Cross Media GmbH (http://www.m-events.com). !ose who did not do it are kindly requested to upload their presenta-tion on-site in the Speakers’ Check-In (Hall B0, ground floor, congress centre). Speakers may check and/or alter their slides up to three hours prior their presentation.
I#3,.-/0-: In any case all speakers need to check their pres-entations at the Speakers’ Check-In when they arrive to the ICM!
Please be assured that the presentations are se-curely protected against any external access. !is applies for both the online upload as well as the upload on-site. A#er the conference all submitted files will be deleted from all storage media.
U3*,/( ,0-%"-$ /- -'$ S3$/2$.%’ C'$&2-I0:!e final and complete presentations must be submitted to the Speakers’ Check-In at least three hours prior to the scheduled session.!is regulation does not apply for sessions that start before 10 a.m. - in this case we recommend upload-ing the final presentation one day prior to the lecture.!e Speakers’ Check-In is located in the hall B0, ground floor, congress centre and will be open during the following hours, with technicians available to assist:! Sunday 21 June 2015: 07:00 - 18:30! Monday 22 June 2015: 07:00 - 18:30! Tuesday 23 June 2015: 07:00 - 18:30! Wednesday 24 June 2015: 07:00 - 18:30! !ursday 25 June 2015: 07:00 - 12:00
N,-$: Even though there are more than 20 up-loading stations available at the Speakers’ Check-IN, there might be waiting periods at peak times.
G)"($*"0$% 1,. 3.$%$0-/-",0 1,.#/-%:Only presentation material in the form of MS-PowerPoint 2010 or earlier versions (*.ppt and *.pptx) with a screen ratio of 4:3 and a min-imum resolution of 1024x768 will be accepted. If you are using PowerPoint 2007 or older please do not forget to submit any videos as separate files as PowerPoint will not include them into the presentation. Only MS O%ce standard fonts are supported. Custom fonts cannot be embedded. No provisions are being made for overhead or traditional slide presentations.
P.$%$0-/-",0 T$&'0,*,45:Each meeting room is equipped with a laptop, a data-projector and podium microphone and/or wireless lavalieres. A network-based presenta-tion system will be used along with a conference specific interface to ensure the perfect quality of all presentations. !erefore, own laptops cannot be connected in the lecture room. All presenta-tions must be uploaded in advance to the server.
Laser pointers are not provided.
Technical Focus Sessions
A feature of CLEO®/Europe-EQEC 2015 will be the Technical Focus sessions which will con-centrate on a selected Fibre and Solid-State Lasers topic. It will consist of a combination of extended tutorial introductory material and authoritative technical reviews. CLEO®/Europe-EQEC 2015 will feature two Technical Focus sessions on Ultrafast Solid-state and Fibre Lasers and Materials Structuring Us-ing Short Laser Pulses, jointly held with the
LiM conference and taking place on Tuesday a6ernoon, Room 13a.All paid registrants are invited to attend the Technical Focus sessions at no additional charge. !ose wishing to attend the Tech-Focus who are NOT FULL FEE registrants must pay the one-day fee.
Short Courses
Ten short courses at an extra cost will be pre-sented in parallel on Sunday 21 June 2015 (half days each). Each course is scheduled in two parts: Course Part I (1 hour '), co"ee break (30 min-utes), Course Part II (1 hour '). !e courses are open to attendees of the World of Photonics Con-gress and Laser World of Photonics Exhibition subject to payment of the course fee.Advance registration is required in order to obtain the short course material. !is material will not be available for purchase during the conference.
Laboratory Tours
Guided laboratory tours through selected Munich (Garching) Laser Laboratories will take place on Friday morning, 26 June 2015 from 10:00 to 12:00.!e programme will be on line at http://www.cleoeurope.org/laboratory-tours.CLEO®/Europe-EQEC participants can sign up for the laboratory visits during the conference: !ey will be invited to sign up on lists hanging on the message board located in the corridor be-tween Entrance West and ICM.If possible, laboratory tour attendants should book their return flights in the evening, to be sure, that there is enough time. I#3,.-/0-: T./0%3,.-7Transportation will need to be arranged by the visitor.
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To find connections from the hotel to the cho-sen laboratory, please go to the Munich Public Transport Internet site (MVV) with a screen for English speakers:http://efa.mvv-muenchen.de/mvv/XSLT_TRIP_ REQUEST2?language=en
You can enter either the street or subway sta-tion near the hotel as a starting point and, respectively, the same choice, for your in-tended destination. Please type in the field “arrival”: 9:35. You head for Garching? Please specify by typing: “Garching b München”. For additional information on the Munich public transportation see http://www.mvv-muenchen.de/en/homepage/index.html
Reception and Social Events
LASER W,.*( ,1 PHOTONICS O3$0-"04 R$&$3-",0Monday 22 June 2015, from 18:00 to 21:00, ICM Foyer, Ground Floor, Congress CentreAll exhibitors and attendees of the World of Pho-tonics Congress are cordially invited to attend the opening reception dedicated to the declared 2015 International Year of Light. Enjoy music, food and cold drinks and use the atmosphere to network.
CLEO®/E).,3$-EQEC C,01$.$0&$ D"00$.Tuesday 23 June 2015, beginning from 19:00, Löwenbräukeller, Munich!e delegates registered with the CLEO®/Eu-rope-EQEC 2015 are invited to the conference reception at a special cost of ( 10,- per participant and ( 35,- per additional guest. !e dinner will take place at the famous Löwenbräukeller (http://www.loewenbraeukeller.com/en/) in downtown Munich. A rich selection of fine Bavarian food will be provided.
I0-$.0/-",0/* Y$/. ,1 L"4'- H/335 H,).Wednesday 24 June 2015, from 17:45 to 18:45, ICM Foyer, Ground Floor, Congress Centre!e event is sponsored by the Quantum Elec-tronics and Optics Division and the EPL (for-merly Europhysics Letters) of the European Physical Society together with SPIE and AAAS/Science. Beer and pretzels will be served. !e postdeadline sessions will take place just a#er the Happy Hour.
Exhibition Information
From 22 to 25 June, a major exhibition of laser and electro-optic equipment and services, LA-SER World of PHOTONICS 2015 will be held in conjunction with the congress. !e latest technology first hand will be exhibited. !e range of products exhibited will cover inno-vative optical technologies:• Laser and Optoelectronics;• Optics;• Manufacturing Technology for Optics;• Sensors, Test and Measurement;• Laser and Laser Systems for Production Engineering;• Optical Information and Communication;• Biophotonics and Medical Engineering;• Imaging;• Illumination and Energy;• Security.
NEW: • Special show “Photonics Applications in the Au-tomotive Sector“ (Hall B3)
• Special show “3D Printing—Additive Manufac-turing“ (Hall B3)
• Special show Photons in Production “Next Gen-eration“ (Hall A2)
All conference registrants will have free entrance to the technical exhibition. Longer lunch breaks
are organised to allow visits to the exhibition.This combination of theory and practice, an extensive program of conferences and related events and the presence of all market leaders, de-cision-makers and users, make LASER World of PHOTONICS unique and, at the same time, the most important international information and networking platform for the industrial, research and development sectors.LASER World of PHOTONICS features more than 1,200 exhibitors in 5 halls and gives a complete overview of all the latest trends and applications. Further information on the exhibition is available at http://world-of-photonics.net/en/laser/visitors
O3$0"04 ',).% ,1 -'$ $8'"9"-",0The exhibition will be opened from Monday through Wednesday 09:00 - 17:00 and on !urs-day 09:00 - 16:00.
Application Panels
The application panels organised by Messe München International are now a permanent part of the World of Photonics Congress. !e series of lectures that are held in the forums of the LASER World of PHOTONICS 2015 exhi-bition halls bridge the gap between science and practical application.Well-known speakers from industry and research institutes report on the latest industrial and med-ical application findings in the sector for opti-cal technologies and discuss current challenges with you.A series of 16 panels will be held from 22 to 25 June 2015. Broken down into four main cate-gories – i.e. Biophotonics and Medical Appli-cations (4 topics - Hall B3), Industrial Laser Applications (6 topics - Hall A3), Lasers and Optics (3 topics, Hall B3) and Optical Metrol-ogy and Imaging (3 topics, Hall A2) – they will
give attendees a comprehensive look at the latest trends and developments.!e admission is free for all trade-fair visitors, exhibitors and congress participants. All are held in English.For further information see the brochure (http://fs-media.nmm.de/ftp/LCO/files/pdf/Appli-cation-panels-program.pdf) or http://www.world-of-photonics.com/trade-fair/events/forums/application-panls/)
On-Site Facilities for Attendees
O0*"0$ *$&-).$ (/-/9/%$!e entire programme of events at the World of Photonics Congress is available online at http://www.photonics-congress.com/congress-pro-gram.html. With this online database you can get information about every conference, sub confer-ence, session, oral lecture or poster presentation. For every lecture at least the information about the room and time data, the speaker and the as-signment to the structure is available. O#en there are also the co-authors and the abstracts of the lecture displayed.
NEW: W,.*( ,1 P',-,0"&% C,04.$%% A33World of Photonics Congress o"ers an innovative tool which can be used to prepare your stay in an easy and professional way. !is tool will allow to find the complete congress programme, save sessions/lectures in your personal calendar, easily create and access favourite lists, access detailed conference room plans, give general information about the congress.Links to the App stores:! Android: http://play.google.com/store/apps/
details?id=de.eyeled.android.eyeguidecf.wopc15! iOs: https://itunes.apple.com/us/app/world-
photonics-congress-2015/id987488500?mt=8 &at=&ct=&ign-mpt=uo%3D6
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$I0-$.0$- /0( W-LAN L,)04$All congress participants using their own laptops/notebooks/pads have free access to two W-LAN Lounges located at the Congress Centre (ICM):! ICM foyer Süd! ICM main foyer of the ICM main entrance.Internet is with high-speed access and unlimit-ed download.In the rooms, only the wifi-version with limit-ed bandwidth and limited download volume is available.
C/.$$. C$0-$. (H/** B:)Are you looking for a position or a new chal-lenge in the photonics industry? The LASER World of PHOTONICS Career Center gives you a number of specific options for your profession-al development.
Valuable contacts directly at the fair:Messe Munich works with Wirth + Partner, a re-nowned consulting group, to organise the Career Center. Located in Hall B1.561, it will give a com-plete overview of the exhibitors’ job vacancies and available trainee and apprenticeship positions. You can get to know potential employers directly at the fair and make valuable contacts.
Online Career Center:Already now you can find the exhibitor’s job va-cancies in the Online Career Center.See http://www.world-of-photonics.com/ trade-fair/events/career-center/#online_ career_center
Free career counselling from personnel professionals:Both college graduates and experienced engineers and physicists can receive free career counselling from experienced personnel consultants. Set up your consulting appointment at the stand in Hall
B1 or by sending an e-mail to [email protected]
Further information at http://www.world-of-pho-tonics.com/trade-fair/events/career-center/
C/-$."04All conference attendees are invited to attend the free co"ee breaks as marked in the tables of the days at a glance (first pages of the advance programme). Lunches are not included in the conference fee.A number of gastronomy facilities are available on site.Depending on the weather the beer garden out-side will be open.• Besides two permanent food service operations in the foyer – the ICM Bistro and the ICM Café – you can also visit the restaurant “Am See”, which can be reached directly via the 1st floor.
• Snack bars with large assortments of snacks and beverages are located on the ground floor in each hall. !e snack bars in the ICM are located on the ground floor and the first floor.
• Full-service restaurants are located on the first floors of the East and West Entrances and above the halls. Other self-service restaurants locat-ed on the first floor can also be found in the exhibition halls o"ering international cuisine. Many snack bars located in the exhibition halls o"er Alpine, American, Asian, and Ital-ian cuisine.
• Other catering places can be found at the “Riem Arcaden” shopping centre located at the exit of the “Messestadt West” subway station.
B)%"0$%% C$0-.$!e ICM centre o"ers a first-class International Business-Centre (open from Monday to !urs-day from 08:00 to 17:00 hour, closed Saturday and Sunday).
O;ce services are currently proposed at cost:• PC workstation with printers (applications from all MS O%ce packages)
• Internet access• Laptop connections• Prepaid wireless-LAN connect card including support (requested in case you are not in the W-LAN Lounge at the congress centre)
• E-mail (receive/send)• Colour/black-and-white copies• Fax (receive/send)• Stamps It also o+ers additional services:• Information about cultural attractions in Munich• Hotel information• Flight/train information• Information about Munich International Trade Fairs
• Taxi service (directly in front of ICM main entrance)
B/02%No bank-counter but ATM-machines to with-draw money.Two of them are operated by ReiseBank in the West Entrance, ground floor, and on the 1st floor along the Expressway between Halls B3 and B4.Stadtsparkasse München has three cash ma-chines, located on the ground floor of the East Entrance (near the corridor to Hall B6), the North Entrance (under the stairs) and the Northwest En-trance (in the passageway to the parking garage). At the “Riem Arcaden” (three-minute walk from West Entrance) you will find:• An ATM self-service machine (Münchner Bank).• A branch o%ce of the Sparda-Bank for custom-ers to make deposits and withdraw funds. No currency exchange.
Other banks are also to be found in the centre of Munich or at the main railway station.
T/8" %$.<"&$!e taxi service is located in front of the ICM main entrance.
A".3,.- %')--*$An airport shuttle is organised in connection with the trade fair from 21 to 25 June 2015. Cost ( 8 one-way, ( 13,50 round trip.Shuttle buses directly stop in front of the West, East and North Entrances and in front of the en-trance of the ICM Congress Centre.Shuttle buses provide service between the Munich Airport and the trade-fair centre during the fol-lowing schedule (every 30 minutes, on the hour and half-hour):• Airport -Trade-fair centre: 8 am - 6 pm • Trade-fair centre - Airport: 9:30 am - 7 pm!e trip takes approximately 45 minutes. Infor-mation regarding departure locations and special fares is available at all information counters at the trade-fair centre.
F".%--/"(First-aid stations are located in the East and West Entrances.As a service partner of Munich International Trade Fairs, Aicher Ambulanz Union is respon-sible for the medical needs of guests and visitors at the trade-fair center and the ICM. Phone: +49 89 742200, +49 89 949-28103 (for first-aid emergency call), mobile: +49 171 5663514.
L,%- /0( 1,)0( ,11"&$Items found are deposited with the security o%ce located in the Administration Building by Gate 1. It is open around-the-clock and accessible both from the inside (via the Administration Building) and from the outside.
P'/.#/&5!e nearest pharmacy is “SaniPlus” in the Riem
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Arcaden shopping centre. It is located on the ground floor in the right portion of the building.Opening hours: Monday through Saturday 09:00 - 20:00.
O3-"&"/0!e Optician “Fielmann” has a retail outlet in the Riem Arcaden shopping centre.
G.,&$."$% ="-' 9/2$.5, &*,/2.,,#, /0( I01,.#/-",0/-./<$* %$.<"&$ … are located in the Main Hall of the Entrance West leading to Halls A1 and B1.
P,%- ,11"&$Deutsche Post has a small branch o%ce in the Riem Arcaden shopping centre (lower level next to the “Edeka” supermarket).
D.5 &*$/0"04“Pan-o-tex” dry cleaning is located in the Riem Arcaden shopping centre.
M$%%/4$ B,/.(A message board will be installed. Participants should consult it daily for internal messages. It will be placed in the corridor between Entrance West and ICM.
P.$%% S$.<"&$%All members of the Press are requested to register by Messe Munich. !ey will receive the conference material and badges that will admit them to all technical sessions and the exhibition.
C*,/2.,,#A Cloakroom is located on the lower level of the West Entrance. As a rule, it starts one hour before the exhibition begins and ends one hour a#er the exhibition closes.
N,-$ 1,. %#,2$.%Smoking in the ICM is forbidden. Smoking on the grounds of the exhibition center is only permitted in designated smoking areas outside the halls. We thank you for your understanding!
Conference Venue
CLEO®/Europe-EQEC 2015 will take place at the New Munich Trade Fair Centre at the ICM - International Congress Centre, Am Messesee 6, 81829 Munich, Germany. Please visit http://www.messe-muenchen.de/ or http://www.icm-muenchen.de .
How to reach the ICM Centre
B5 &/.: simply follow the trade fair signs from the out-skirts and throughout the city to the ICM. !ere you will find parking space.
B5 -./"0: !e ICM is about 20 minutes from Munich cen-tral station (Hauptbahnhof) by underground U2, exit ‘’Messestadt West’’. !e U2 subway runs from 4:12 in the morning to about 1:00 a#er midnight. Further information on the underground is avail-able at http://www.mvv-muenchen.de/ or at the information counters on the trade fair grounds.
F.,# -'$ /".3,.-: At Munich airport, the station for urban railway lines S1 and S8 is directly below the central area. Trains in the direction of the city centre run at 10-minute intervals. !ere are two routes from the airport to the ICM:• Route S1 / U2: S1 from the airport to Feldmoch-ing station or Munich Central Station (Haupt-bahnhof). Change to underground U2 that takes you directly to the ICM - Messestadt West.
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• Route S8 / U2: S8 from the airport to Munich central station (Hauptbahnhof). Change to un-derground U2 that takes you directly to the ICM - Messestadt West.
B5 -/8" 1.,# -'$ /".3,.-:Taxis are available in front of the terminals. !e journey takes about 35 minutes, depending on the volume of tra%c (cost around 60 EUR).
B5 '".$ &/. 1.,# -'$ /".3,.-:All the major car rental firms are represented at Munich airport. !e car rental centre with its own parking facilities is in front of module A, to the north of car park P6.Please take the following route: From Munich Airport follow the signs “Messe/ICM” on the A92 in the direction of Munich to the motorway intersection Eching/Neufahrn. !en take the A9 in the direction of Munich to the motorway in-tersection München-Nord. Continue on the mo-torway ring road A99 in the direction of Salzburg to the motorway intersection München-Ost. !en take the A94 in the direction of Munich to the exit Feldkirchen-West or München-Riem. !e journey takes about 35 minutes, depending on the volume of tra%c.
H,= -, -/2$ / -/8" 1.,# -'$ ICM C$0-.$ -, -'$ /".3,.-You will find taxi ranks at all trade fair entranc-es and in front of the ICM going to the airport (Central Building).
A".3,.- %')--*$An airport shuttle is organised in connection with the trade fair from 12 to 16 May 2013. Cost ( 8 one-way, ( 13,50 round trip.Shuttle buses directly stop in front of the West, East and North Entrances and in front of the en-trance of the ICM Congress Centre.
Shuttle buses provide service between the Munich Airport and the trade-fair centre during the fol-lowing schedule (every 30 minutes, on the hour and half-hour):Airport -Trade-fair centre: 8 am - 6 pm Trade-fair centre - Airport: 9:30 am - 7 pm!e trip takes approximately 45 minutes. Infor-mation regarding departure locations and special fares is available at all information counters at the trade-fair centre.
Conference Registration
CONFERENCE REGISTRATION FEESEPS/OSA/IEEE Memberwith the online digest ( 590Non-Memberwith the on line digest ( 710EPS/OSA/IEEE Student Member (*)with the online digest ( 195Student Non-Member (*)with the online digest ( 230One Day without the online digest ( 290Student (*) extra fee for Short Course ( 220Regular extra fee for Short Course ( 350Reception ticket per participant ( 10Additional reception ticket per guest ( 35(All registration fees are exempt from Value Added Tax).(*) Applications for the student rates must in-clude a copy of an o%cial student identity card, which must also be presented on-site when col-lecting registration materials.
The full week registration fee for the meeting includes admission to all CLEO®/Europe-EQEC 2015 technical sessions, as well as to those of all conferences collocated with the congress. It in-cludes admission to the technical exhibition. Digest will be online. A login and password will be given.
Co"ee Breaks are included (two per days except on Monday only one in the a#ernoon). Tickets for public transportation are not included in the fees.One-day registration fees are available for those wishing to attend one particular session rather than the whole conference. Please note that the online digest will not be included. Co"ee Breaks are included. Tickets for public transportation are not included in the fees.N,-$: One-day registration tickets are activat-ed on the day the participant goes through the gates of the congress or the fair and will only be valid for that day.Registration forms are available on site.
Cancellation Policy
An administration charge of euro 50 will be made for processing refunds. A request for cancellation must be made in writing. In the case of cancella-tion, requests received on or before Wednesday, 10 June 2015 will be refunded (less the administra-tion charge). No refunds will be available if notice of cancellation is received a#er 10 June 2015.
Note to Exhibitors
Each exhibitor at LASER World of PHOTONICS 2015 is entitled to one free ticket to the World of Photonics Congress 2015. Each exhibitor may also purchase up to five congress tickets for a spe-cial price.All tickets are personalized, i.e. they are valid only for the person whose name appears on the ticket, and they are not transferrable.Special tickets to the World of Photonics Con-gress may only be ordered and used by exhibit-ing companies.!e o%cial Congress Proceedings are not in-cluded in the discount price for special tickets for exhibitors.
Tickets will be pre-produced and will be available for pick-up at the World of Photonics Registra-tion Desk in the West Entrance. Messe Munich manages the order of these tickets.Beyond that, exhibitors must purchase any addi-tional tickets to the World of Photonics Congress from one of the organizing scientific associations at the regular price.
P*$/%$ 0,-$: Neither the free special tickets nor the discount special tickets are available to speakers or poster presenters appearing at the World of Photonics Congress 2015. Speakers and poster presenters must register with the respective organizing association.
Registration Hours and Location
Registration for technical sessions will take place at the ICM centre. To enter the ICM centre please take the main Entrance West (named “Hauptein-gang WEST”). CLEO®/Europe-EQEC 2015 reg-istration counters are located on the le# side at the end of the main corridor just prior you enter the exhibition halls.
R$4"%-./-",0 H,).%Saturday 20 June 16:00-18:00Sunday 21 June 07:30-17:15Monday 22 June 07:30-17:15Tuesday 23 June 08:00-17:00Wednesday 24 June 08:00-17:00!ursday 25 June 08:00-15:00
C,01$.$0&$ H,).%Sunday 21 June 08:30-12:00/12:30-18:45Monday 22 June 08:00-12:45/13:30-18:30Tuesday 23 June 08:30-12:30/13:00-17:30Wednesday 24 June 08:30-12:00/13:00-20:15!ursday 25 June 08:30-12:00/13:00-17:30
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S',.- C,).%$ H,).%Sunday 21 June 08:30-12:00/13:30-17:00
S)33,.-%All supports were distributed. No additional re-quests can be received.
Hotel Information
!e International Congress Centre (ICM) is lo-cated about 20 minutes from the Munich Central Station (Hauptbahnhof) by underground U2, exit “Messestadt West”. Whether you are looking for a hotel, a guesthouse, a private accommodation, or a boarding house you should be able to find your accommodation downtown or in the surrounding area of Munich.Messe Munich has arranged for an on-line ho-tel reservation which can also be used for the CLEO®/Europe-EQEC 2015 participants at:http://www.tradefairs.com/index.html!e Hotel Guide of the Munich Trade Fairs of-fers you a large variety of accommodation pos-sibilities for a pleasant stay. Whether near the ICM or centrally located and in the middle of the nightlife of Munich’s trendy neighbourhoods or close to the mountains with a high recreation value - here you will find a comprehensive of-fer of accommodation in and around Munich as well as in the alpine upland - meeting your personal criteria.Hotels can be directly searched and booked via the Hotel Directory.A larger variety of rooms can be found using the links:• http://www.muenchen.de/int/en• http://www.muenchen.de/int/en/accomoda-tion-hotels.html
• http://www.hotel.de/ or go directly to Mu-nich (München) via http://www.hotel.info/en/munich/hotels-38344/
Rooms, apartments and holidays homes can be found using the following link:• http://www.checkin-muenchen.de/index.php?mms=1
Hotels, pensions, apartments or youth hostels in Munich can also be found at:• ht tp : / / w w w. mu n i c h - i n f o. d e / h ot e l s /welcome_en.html
• http://www.hostelworld.com/hostels Transportation in Munich
Munich o"ers very good transportation means (hire cars, trams, metro and buses).Participants of the World of PHOTONICS con-gress who use local public transportation to get to Neue Messe Munich must buy a travel ticket, at their own expense.Tickets can be purchased from all bus drivers, tram drivers, automatic ticket-dispensing ma-chines at stations (S and U-Bahn stops) and from kiosks displaying the MVV logo. Some ticket ma-chines accept 10 ( and 20 ( banknotes and most will give change. Please have some small coins ready! You can select your respective language on the ticket machines.Buy your ticket depending on the zones you will cross and the time length you will need to travel:• Stripe ticket (Streifenkarte): Stamp two stripes per zone. You are allowed to change and inter-rupt your journey. Return and round trips are not permitted.
• Single trip ticket: Valid for one person for one trip. You are allowed to change and interrupt your journey. Return and round trips are not permitted. !e fare depends on the number of zones passed through.
• Single day ticket (Tageskarte): !e most pop-ular day tickets are also available as excellent value-for-money 3-day tickets. If you want to
stay for 2 days, 4 days or even longer, simply combine the 1-day ticket and 3-day tickets.
• Partner day ticket: Available for as many trips as you like for up to five adults together.
F/.$% 1,. %"04*$ (/5 -"&2$-%1. Inner District (Innenraum) white zone ( 6,202. Munich XXL (München XXL) white and green zones ( 8,303. Outer District (Außenraum) green, yellow, red zones ( 6,204. Entire Network (Gesamtnetz) all zones ( 12,00
Fare for 3-day Inner District white zone ( 15,50
For your trip Munich city / Munich airport you will need a stripe ticket (8 stamps) or an entire network ticket. Inner District includes the city centre (Marienplatz, Hauptbahnhof, ...) and Neue Messe Munich.Once you have purchased your ticket, be sure to validate it by stamping it in the blue boxes you will see. !is should be done prior to entering the station or immediately a#er boarding a bus or tram. To validate a stripe ticket (Streifenkarte) you must fold back the sections not required and insert the ticket into the validating machine (see below for number of required sections). Once you have validated your ticket, you can travel with any form of transport as long as you continue to travel in the same direction.
More information on the MVV, see http://www.mvv-muenchen.de/en/homepage/index.htmlA subway map can be downloaded from http://www.travelsthroughgermany.com/website2/mu-nichsubway.htm
Munich, Germany
!e celebrated capital of Bavaria, located in the foothills of the Alps, is one of the major cities in Europe. !e 1,3 million inhabitants city is famous for its science and industry environ-ment. Munich o"ers fantastic opportunities for shopping, museums, theatres, art galleries and sightseeing. Its October beer festival is world fa-mous. Tourist attractions include the Bavarian beer and South German cuisine tradition, and many half-day or one-day excursion opportuni-ties to the nearby Bavarian Alps or places such as the fairy-tale castle of Neuschwanstein or the beautiful Tegernsee.In June the weather is likely to be warm and the sun is likely to shine, although rain is not impossible.Munich enjoys an outstanding public transpor-tation system, and the modern Münchner Messe complex where CLEO®/Europe-EQEC 2015 and all Laser 2015 events will be held is easy to reach from the airport, from the city centre and from most parts of the city by U-Bahn and S-Bahn lines. Shuttle bus service to the Munich airport will be available as well during most of the Laser 2013 week.
M)0"&'’% C').&'$%:Munich is well-known for its many churches, among them:! Frauenkirche (Church Of Our Lady),
1 Frauenplatz,Munich
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Opening hours: 07:00-19:00,Thu 07:00-20:30, Fri 07:00-18:00 (no visits during the church services).Getting there: all S-Bahn train, U-Bahn lines 3/6 to Marienplatz
! Alter Peter (Church Of St. Peter),1 Rindermarkt,MunichOpening hours: daily 07:30-19:00, Wed afternoon closed (no visits during the church services).Opening hours of the tower: Mon-Sat 09:00-19:00, Sun and holidays 10:00-19:00Getting there: all S-Bahn trains,U-bahn lines 3/6, Bus 52 to Marienplatz
! Heiliggeistkirche,Tal 77, 80331 Munich, Tel. 089/22 44 02Opening hours: 7.00-18.00 (Midday from 12.00-15.00 and no visits during the church services)Getting there: U-Bahn lines 3/6 to Marienplatz
M)0"&'’% M)%$)#%:! Glyptothek
Königsplatz 3, 80333 München, Tel. 089/28 61 00Opening hours: Tue, Wed, Fr-Su 10:00-17:00, !u 10.00-20.00, Mo closedCost: Adult 3,50 (, Reduced 2,50 (, Sun 1,00 (Getting there: U-Bahn line 2 to KönigsplatzThe Glyptothek was commissioned by the Crown Prince (later King) Ludwig I of Bavaria alongside other projects as a monument to an-cient Greece. It contains sculptures dating from the archaic age (around 650 BC) to the Roman era (around 550 AD).
! Deutsches MuseumMuseumsinsel 1, 80538 München, Tel: 089 / 2179-0 oder 2179 433 (recorded information)
Opening hours: daily 9:00-17:00 Getting there: all S-Bahn trains, to Isartor; Tram 18, to Museumsinsel!e Deutsches Museum is the world’s largest Museum of science and technology.!e laws of nature, instruments and technolog-ical methods are presented on a scientifically high level using an entertaining way.Also part of the Deutsches Museum: the Ver-kehrszentrum (featuring all kinds of vehicles - from formula 1 car to bicycle) and the Flugwer# (focussing on airplanes)
! Deutsches Museum Verkehrszentrum!eresienhöhe 14a, 80339 München, Tel. 89/21 79 529Opening hours: daily 9:00-17:00, !u 9.00-20.00
! Deutsches Museum Flugwer6 Schleißheim E"nerstr. 18, 85764 Oberschleißheim, Tel. 089/315 71 40Opening hours: daily 9:00-17:00Getting there: S-Bahn line 1 to Ober-schleißheim, Bus 292
! Neue PinakothekBarer Str. 29, Entrance at Theresienstraße, 80799 München,Tel. 089/238 05-195
Opening hours: daily (except Mo) 10:00-17:00, Tue and !u 10:00-20:00Getting there: Tram 27 to Pinakothek!e museum contains outstanding works of European art and sculpture from the late 18th to the beginning of the 20th century.
! Kunsthalle der Hypo-Kultursti6ung!eatinerstr. 15, 80333 München, Tel. 089/22 44 12Opening hours: daily 10:00-18:00, Thu till 21:00Getting there: U-Bahn lines 3/4/5/6 to Ode-onsplatz or Tram 19http://www.hypo-kunsthalle.de
! Villa Stuck Prinzregentenstr. 60, 81675 München, Tel. 089/45 55 51 25 Opening hours: Tue-Su 10:00-17:00, Tue till 21:00, Mo closedGetting there: U-Bahn line 4 to Prinzregenten-platz or U-Bahn line 5 to Max-Weber-Platz or Bus 53 or Tram 18 to Friedensengelhttp://www.villastuck.de/
! Bayerisches NationalmuseumPrinzregentenstr. 3, 80538 München, Tel. 089/211 24-1
Opening hours: Tue-Su 10:00-17:00, Mo closed, !u 10:00-20:00 Getting there: Bus 53, Tram 17 to Haus der Kunst/Nationalmuseum, U-Bahn lines 4/5 to Lehelhttp://www.bayerisches-nationalmuseum.de/Engl/b.htm
! BMW Museum!is museum, with its distinctive architecture in the shape of a futuristic silver bowl, is among the most attractive museums in Munich. !e "time horizons" exhibition takes you on an exciting journey through technical feats of pioneering - from the historic BMW sports car through leg-endary prototypes, right up to futuristic study of automobiles and motorcycles. !e path also takes the visitor past topical subjects like alter-native propulsion methods, recycling and coop-erative tra%c management. !e neighbouring BMW World opened for the public in 2007
! Münchner Stadtmuseum Sankt-Jakobs-Platz 1, 80331 München, Tel. 089/233-223 70 and 233-255 86 Opening hours: Tue- Su 10:00-18:00 (Mon-days closed)Getting there: all S-Bahn trains to Marienplatz, U-Bahn line 3/6 to Marienplatz, U-Bahn lines 1/2 to Sendlinger Tor, Bus 52 to Viktualien-markt, Bus 56 to Blumenstraßehttp://www.muenchner-stadtmuseum.de/en.html
M)0"&'’% 1/#,)% 3*/&$% -, 9$ <"%"-$(:! Marienplatz
!e Marienplatz is named according to the column of the Virgin Mary at its centre. !e statue, erected in 1638 to celebrate the end of the Swedish invasion, is topped by a gilded statue of Virgin Mary which was sculpted earlier, in
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1590 by Hubert Gerhard. At each corner of the column's pedestal is a statue of a putti, created by Ferdinand Murmann. !e four putti's sym-bolize the city's overcoming of war, pestilence, hunger and heresy.The place is famous for its carillon in the New Town Hall Tower (Glockenspiel im Rathausturm). !is is the largest carillon in Germany, with near-lifesize figures perform-ing the traditional Coopers' Dance and a joust-ing match. !ree times a day at 11:00, 12:00 and 17:00.!e Marienplatz is a central place for the city’s Founding Festival as well as for Fasching (car-nival) celebrations and the popular Christmas market. The major restaurants, coffees and shops are located in this area. Shops are com-pletely closed on Sunday.
! KönigsplatzCommissioned by Ludwig I, this neo-Classical square boasts the Propyläen gateway and the Glyptothek, a small but enchanting collection of Greek and Roman sculpture. Also the sight of an annual summer outdoor concert series.
! Isartor (Isar Gate)Most easterly of Munich's three remaining town gates, dating from the 14th century. Careful res-toration has recreated the dimensions and ap-pearance of the original structure. !e Isar Gate accommodates the Valentin Museum.
! Karlstor (Charles' Gate)Westerly town gate from 14th century. Incor-porated at the end of the 18th century into the square known as "Stachus" (officially Karl-splatz). Today it marks one end of Munich's primary pedestrian zone.
! Sendlinger Tor (Sendlinger Gate) Remaining towers of southerly fortifications from the 14th century.
B$$. G/.($0%Nothing defines Munich more than its beer. You cannot talk about one without the other and you could never fully discover Munich without at least sampling its brews. Today the Munich breweries dispense 123 million gallons of beer annually. !at is why many beer gardens are located in Munich:
! Augustiner-GroßgaststättePedestrian Zone, Neuhauser Straße 16, 80331 Munich, Tel. 089/2 60 41 06.!e Augustiner Großgaststätte is one of the more traditional Munich establishments, with a history that reaches back to 1328. !e Augustin Brothers began brewing something heavenly in Augustiner's back rooms up until 1855 when the actual brewing plant was moved to Lands-berger Straße. Today Augustiner Großgaststätte
is a traditional beer hall with a small courtyard beer garden, smack dab in the middle of Mu-nich's Marienplatz pedestrian zone. !e food is great and the beer is the best.
! Altes HackerhausSendlinger Str. 14, Munich, Tel. 089/2605026, http://www.hackerhaus.deOpening hours: 9 am to midnight daily.Located in Munich's newspaper publishing dis-trict and near Sendlinger Tor, Altes Hackerhaus has a long history involving two of the City's most renowned beer producing families, the Hackers and the Pschorrs. An entire wall in the restaurant is dedicated to the family tree, dating back to 1738 when the first Hackerhaus was founded. Highlights include a small but com-fortable interior courtyard beer garden, and an outstanding restaurant serving excellent Ba-varian fare. Although average by Munich high standards, Altes Hackerhaus benefits from its proximity to the Marienplatz (just a few blocks away) and easy access from the nearby U-Bahn stop at Sendlinger Tor.
! Chinesischer Turm (Chinese Tower) One of Munich's largest beer gardens, and per-haps its most famous. With more than 7,000 seats around the famous erzat Chinese pagoda
in the middle of Englischer Garten (900-acre park with shaded paths, brooks, ponds and swans), this place could hardly be overlooked. Location: Englischer Garten 3, open from 11:00 to midnight.!e park stretches from the centre of the city (near Odeonsplatz) to the northern city border. Access: !e best way to reach it is the bus No. 54 from "Muenchner Freiheit" underground station (exit at stop "Chinesischer Turm")
Munich is very famous for its theatres but also for its Olympic Park (see http://www.olympiapark.de/index.html) located Spiridon-Louis-Ring 21, 80809 Munich, Tel.: 089/30 67 - 0, Fax: 089/30 67 - 22 22Getting there: U-Bahn line 3 to Olympiazentrum
Further information on Munich is available at http://www.muenchen.de/ (8 languages available).
Conference Management
European Physical Society6 rue des Frères Lumière68200 Mulhouse, France!is programme is edited by P. Helfenstein and A. Wobst.
Language
English is the o%cial language of the conferences.
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SHORT COURSES
CLEO®/Europe EQEC 2015 will present ten Short Courses held in parallel. These courses will take place on Sunday 21 June 2015 at the ICM (Rooms 12a, 12b, 21a, 21b and 22). !e courses are at extra cost.Advance registration is recommended in order to obtain the short course material. !is ma-terial will not be available for purchase during the conference.!e courses are intended for engineers, scien-tists and graduate students with some general knowledge of optics and photonics, who wish to improve their detailed understanding of the par-ticular technical domains covered. Each course is scheduled in two parts: Course Part I (90 min-utes), co"ee break (30 minutes), Course Part II (90 minutes).
Detailed Programme:
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Short Course 1 SH-1
Ultrashort Pulse Characterization
Selçuk Aktürk, Istanbul Technical University, Istanbul, Turkey
Course Description:Response times of electronic detectors are still orders of magnitude behind the time scales achieved in ultrafast optics, spanning picosec-ond femtosecond and attosecond ranges [1]. As a
result, special characterization methods are need-ed for measuring such extreme short durations [2]. Most characterization methods stem from the idea of autocorrelation; using an event to measure itself. However, today we have gone much further than the limited estimates from simple autocore-lations. We can extract the complete temporal or spectral evolution of ultrashort pulses, including both the intensity and phase information in time and frequency domains. Even further, spatial and complete spatio-temporal evolutions can also be measured with high sensitivity, resolution and re-liability. In this course, we will review principles of ultrashort pulse characterization and then detail on particular commonly used methods such as FROG, SPIDER and their relatives. We will also discuss additional considerations required for extremely short (near single cycle regime), long/narrowband, and extremely complicated pulses.
Benefits and Learning Objectives:• Understand the basic principles of Ultrafast Op-tics and Nonlinear Optics
• Understand the basics of ultrashort pulse characterization
• Learn the basics of autocorrelation and Inter-ferometric autocorrelation
• Learn the basics of intensity and phase measure-ments with more advanced techniques
• Obtain a detailed understanding, applicability and limitations of commonly used methods
• Identify the critical issues, relevant to measure-ments of pulses in the single-cycle regime
• Obtain an understanding of spatio-temporal dynamics of femtosecond pulses
• Learn the necessary techniques for spatio-tem-poral pulse measurements
• Obtain the relevant practical skills for building of pulse characterization devices
• Obtain an appreciation for recent trends and advances in the area of pulse characterization
Intended Audience:!is course is intended for researchers working with fundamental or applied aspects of Ultrafast Optics, in both academic or industrial institu-tions. Basic background and familiarity in Ul-trafast Optics will be su%cient. Ultrashort pulse characterization methods will be covered from basic concepts to advanced techniques.
Biography:Selcuk Aktürk received his BS degree in Physics from Bilkent University in Ankara, Turkey (2001), and PhD degree in Physics from Georgia Institute of Technology in Atlanta, Ga, USA (2005). He worked as a post-doc researcher at GaTech and Research Scientist at Swamp Optics LLC until 2006. He continued his post-doctoral research at Laboratoire d'Optique Appliquée, Ecole Pol-ytechnique – ENSTA in Palaiseau, France from 2006 to 2009. Since April 2009, he is at the Istan-bul Technical University, Department of Physics, currently at Associate Professor level.Selcuk Akturk’s research activities involve ultra-short pulse characterization in time and space, interactions of high intensity laser pulses with matter, and laser material processing. He co-au-thored about 40 peer-reviewed journal articles and numerous conference proceedings. His achievements were recognized by several awards from institutions including Georgia Institute of Technology, Turkish Academy of Sciences, !e Abdus-Salam International Centre for !eoret-ical Physics and International Commission for Optics. He is a member of Optical Society of America and SPIE.
References[1] J. C. Diels and W. Rudolph, Ultrashort Laser Pulse
Phenomena (Academic Press, 1996).[2] R. Trebino, Frequency-Resolved Optical Gating (Klu-
wer Academic Publishers, 2002).
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Short Course 10 SH-10
High Power and High Brightness Semiconductor Laser Diodes and Applications
Paul Crump, Ferdinand-Braun-Institut (FBH), Berlin, Germany
Katrin Paschke, Ferdinand-Braun-Institut (FBH), Berlin, Germany
Course Description:GaAs-based diode lasers are the most e%cient technology for converting electrical input power into useful optical output. As devices and tech-nology continue to improve, an ever wider range of applications is enabled, from ultra-high power pump lasers (kilowatts) for large laser facilities, through highly brilliant sources (10’s to 100’s of watts, into a defined beam) for direct material processing to high power sources for use in dis-play and sensing (at the watt level in a single mode at a target wavelength).!e short course reviews current status of this rapidly developing field, starting with an overview of the device technology used to construct state of the art high power and high brightness diode
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lasers, including epitaxial growth, wafer process-ing, facet treatment and packaging technology. !e second part of the course will review pro-gress in the diode laser applications, illustrating how rapid performance improvement in indus-try-standard configurations has been achieved, together with an overview of the new applications that have been enabled by these improvements. In each case, the capability of the technology is illus-trated using recent published results, with open challenges reviewed, illustrating the importance of continually improved understanding of device physics and materials science for improved per-formance in high power applications.
Intended audience and learning benefits:!e course is intended to give a detailed summary of current status and challenges in the field of high power lasers. !e content is designed to provide a good basis of understanding of the high-power, high-brightness semiconductor field to non-spe-cialist engineers and scientists. In addition, the performance summary and overview of techno-logical challenges will be su%ciently rigorous to form a useful update for the specialist. Finally, the course will illustrate for laser users and optical system designers the potential and flexibility of diode lasers for use in many applications.
Biographies:Paul Crump received the BA in natural science (physics) from Oxford University, UK, in 1992, and the Ph.D. degree in physics from Nottingham University, UK, in 1996. From 1995 to 2001, he was with Agilent Technologies Inc., Ipswich, UK, where he helped develop high-power and high-speed single-mode InP semiconductor lasers. From 2001 to 2007, he worked for nLight Pho-tonics Corp, Vancouver, WA, USA, where he was involved in developing high-power, high-e%cien-cy GaAs and InP-based broad area diode lasers. In
2007, he joined the optoelectronics group of the FBH. He is currently group leader responsible for the development of high-power broad area diode lasers and bars at the institute. In the 18 years since completing his PhD studies, Dr Crump has published more than 100 scientific articles and conference papers and is a co-inventor of 7 patents. He also regularly presents invited talks at international conferences and has co-chaired two laser workshops on high power and e%ciency diode lasers (IEEE Semiconductor Laser Con-ference, Mallorca, Spain 2014 and IEEE Summer Topical Conference, Seattle USA 2012).Katrin Paschke received her diploma in physics in 1996 from the University of Potsdam, Germa-ny. In 1997 she joined Ferdinand-Braun-Institut, Leibniz-Institut für Höchstfrequenztechnik in Berlin, working on noise and reliability of opto-electronic devices. She obtained her Ph.D. in elec-trical engineering from the Technical University of Berlin for the realization of a high brilliance a-DFB laser in 2006. Since 2007 she has been the group leader at FBH responsible for research on hybrid diode laser systems. She subsequent-ly spent time working on sabbatical at the De-partment of Electrical Engineering at Princeton University, USA and National Taiwan University.Her current research activities include the devel-opment of high brightness diode lasers based on GaAs in the wavelength range from 632 to 1180 nm and new powerful hybrid diode laser modules in the infrared spectral range and with frequency conversion for applications ranging from sensors to entertainment. !e matchbox-size light sources are not only maintenance free at comparatively low manufacturing costs, but also distinguished by precise wavelengths, direct modulation, output stability, small dimensions, low energy consump-tion, and high reliability.Katrin Paschke has authored or co-authored over 120 journal publications, over 80 conference
contributions and 4 patents. She is a frequent review-er for Optics letters, Optics Communications and Applied Optics. In 2013 she attained a scholarship from the Alexander von Humboldt foundation.
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Short Course 3 SH-3
Super-resolution Optical Microscopy
Christian Eggeling, Weatherall Institute of Molecular Medicine, University of Oxford, Oxford, United Kingdom
Course Description:!is course provides an overview of super-reso-lution optical microscopy, introducing the basics but showing also limitations and applications. !e course will begin with a description of the fun-damentals of optical microscopy and its limited spatial resolution, and a thorough discussion on the basic idea of the concept behind super-reso-lution optical microscopy (i.e. the breaking of the aforementioned limitation). !is will be followed by a comparison of the di"erent approaches for achieving this, introducing each method’s advan-tages and limitations with a specific focus on pho-to toxicity and photo bleaching in fluorescence microscopy. Finally, a few biological applications will be given, such as the investigation of the or-ganization of molecules in the plasma membrane of living cells.Specifically, the course participants will gain knowledge of the basic principles of optical and fluorescence microscopy, including di"erent as-pects of introducing labels and of biasing e"ects
by the illumination light (such as lasers); the basic principle of breaking the limit in spatial resolu-tion of an optical microscope (as given by di"rac-tion of light); di"erences in STED, RESOLFT, (f)PALM, (d)STORM, GSDIM, SIM etc. super-res-olution microscopy; principles of fluorescence and photobleaching; biological applications rang-ing from multi-colour protein co-localization, 3D-imaging to enclosure of protein dynamics; plasma membrane organization and lipid “ra#s”.
Intended Audience and Learning Objectives:!is course is intended for researchers with little or no background in fluorescence microscopy, as well as those more familiar with the subject area, who wish to enhance their understanding and update their knowledge of the latest devel-opments in advanced optical microscopy. Also those researchers are addressed with interest in investigating the living cell using optical micros-copy (with a light focus on biophysical studies of plasma membrane organization / lipid ra#s). !e course will benefit graduate students and other industrial and academic researchers already in-volved or in early stages of using fluorescence microscopy for their studies.
Biography:Christian Eggeling is a trained physicist, with long-standing experience in the field of fluores-cence microscopy and super-resolution optical microscopy. After working over 2 years in in-dustry at the biotechnology company Evotec in Hamburg, Germany (developing advanced fluores-cence microscopy tools for high-throughput drug screening), and performing pioneering research on super-resolution optical (STED) microscopy (or nanoscopy) in the group of Prof. Stefan Hell (one of the inventors of optical nanoscopy) at the Max-Planck-Institute of Biophysical Chemistry, Göttingen, Germany, he in October 2012 joint the
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MRC Human Immunology Unit at the Weatherall Institute of Molecular Medicine (WIMM) at the University of Oxford. He is a Professor of Molec-ular Immunology, group leader of the Nano-Im-munology group as well as the scientific director of the WIMM imaging facility (Wolfson Imaging Centre Oxford). He is establishing cutting-edge (live-cell) optical (super-resolution) microscopy for investigating molecular distributions and dy-namics in the plasma membrane, especially during cellular immune responses. He has published over 90 papers in peer-reviewed journals, edited 2 books and editorials, (co-)chaired several international conferences, and has given more than 80 invited talks in seminars and on conferences and work-shops. !roughout his career, he was rewarded the Otto-Hahn Medal of the German Max-Planck So-ciety in 2000, the Cozarelli Award of the Proceed-ings of the National Academy of Sciences (2006), the Nernst-Haber-Bodenstein Prize of the German Bunsen/Physical-Chemistry Society (2011), and the Recognition of a Professor of Molecular Im-munology from the University of Oxford (2014).
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Short Course 5 SH-5
Practical Quantum Optics
Gerd Leuchs, University of Erlangen-Nürnberg and MPI for the Science of Light, Erlangen, Germany
Course Description:What does it mean if optics is quantum? Is hard-core quantum optics solely con cerned with the
study of fundamental physics questions or is it also useful for prac tical applications? !e course will give answers to these questions. An introduc-tion to quantum aspects in optics will be given and experimental demonstra tions will under line some of the counter-intuitive quantum phenom-ena. !e generation, propagation and detection of quantum light are central topics. Practical quantum optics is all about noise, noise reduc-tion and over coming established sensitivity limits in inter ferometry, imaging, communication and sensing. Such applications of modern quantum optical technologies will be addressed in detail. Mathematical descriptions of the light field and its interaction with matter will be given whenever necessary but emphasis is put on practical consid-erations. Possible limits that quantum e"ects may impose on or opportunities that they may o"er for applications in industry in the foreseeable future will be discussed.
Experimental demonstrations at the course:• Demonstration of the di"erent properties of classical and quantum noise
• Demonstration of the strong correlations of photon pairs generated in parametric down conversion.
Benefits and Learning Objectives:• Understanding the quantum limitations in optics – such as in sensing, amplification and phase conjugation – and appreciating the opportunities
• Learn the basic tools for describing quan-tum noise
• Acquire the practical skills for experimenting with non classical light – generation, character-ization and control
• Learn to assess the potential benefit when at-tempting to exploit quantum aspects in standard optical scenarios including telecom applications.
Intended Audience:!e course is designed to appeal to an audience without prior experience in quantum optics as well as to researchers who want to refresh and be updated with current trends. !is course is intended to be beneficial for graduate students and industrial and academic researchers alike having a general interest in quantum optics and its practical application.
Biography:Gerd Leuchs studied Physics and Mathematics at the University of Cologne until 1975 and finished with the diploma degree. In 1975 he moved to the University of Munich as research associate in the group of Prof. Dr. H. Walther. His PhD-thesis in 1978 deals with the fine structure splitting of sodi-um Rydberg atoms. From 1979 to 1980 he was visit-ing fellow at the University of Colorado in Boulder, USA. In 1982 he received the Habilitation degree at the University of Munich on multiphoton processes in atoms. In 1980 he obtained a Feodor-Lynen Sti-pend of the Alexander-von-Humboldt Foundation and, from 1983 to 1985, a Heisenberg-Fellowship of the Deutsche Forschungsgemeinscha#, which he used to work at JILA and NIST in Boulder. From 1985 to 1989 he led the gravitational wave detec-tion group of the Max-Planck-Society in Garching. !ere one focus of his research was the generation of quantum noise reduced light beams and their application towards the improvement of the sen-sitivity of laser interferometers. From 1990 to 1994 he served as Technical Director of Nanomach AG at Buchs in Switzerland. A#er having spent 5 years in industry he took over the chair of optics at the University of Erlangen-Nuremberg and continued to do research on quantum noise reduced light, this time focussing on soliton pulses in optical fibers including world first demonstrations. !is led to the generation of entangled intense beams with applications in quantum information and quantum
key distribution. He discovered, that quantum cryptography with intense coherent beams has no in principle distance limitation, which came as a surprise. Since 1994 he is Professor of Physics at the University Erlangen-Nuremberg. In 2000 he started the Center of Modern Optics at Erlangen. In 2004 he was appointed Fellow of the Optical Society of America and Fellow of the Institute of Physics, UK. In 2005 he won the Quantum Elec-tronics Prize of the European Physical Society and was appointed member of the German Academy of Science Leopoldina. From 2004 to 2008 he served as director of the 'Max Planck Research Group of Optics, Information and Photonics'. A#er two successful scientific evaluations the Max Planck Society decided to establish the new Max Planck Institute for the Science of Light at Erlangen and since January 2009 Gerd Leuchs is one of the di-rectors of the Max-Planck Institute for the Science of Light (MPL).Gerd Leuchs published more than 250 publi-cations in peer reviewed scientific journals and numerous invited papers, he is editor of 3 books and inventor of 10 patents. In 2012 he received the Cross of Merit of the Federal Republic of Ger-many. Since 2012 he is Adjunct Professor at the University of Ottawa in Canada.
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Short Course 8 SH-8
Silicon Photonics
Dries Van !ourhout, Center for Nano and Biophotonics (NB Photonics), Ghent University & Department of Information Technology, Ghent University - IMEC, Ghent, Belgium
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Course Description:!is short course discusses both fundamentals and applications of silicon photonics. Silicon photon-ics is rapidly emerging as an attractive platform for realizing cheaper photonic integrated circuits. Active optical cables based on silicon photonics are now already being employed in some of the highest performance supercomputers and several major semiconductor companies have announced activities in this domain. !e course explains the reasons for this sudden interest and the possible advantages of the platform. Next the fundamentals of the waveguide platform and its performance are discussed (straight and bend waveguides, filters, fiber-chip coupling ...). Subsequently also more advanced devices such as detectors, high speed modulators and lasers are discussed. In each case we also touch upon the problems that still need to be resolved and give a comprehensive overview of the current state-of-the-art. In a second part we discuss the integration in a standard CMOS processing environment and di"erent approaches to integrate silicon photonics circuits with optical circuits. Finally we give a review of current and future applications, in optical communications, op-tical interconnect and optical sensing. !e course targets members from academia and industry who want to get a comprehensive review of current state of the art in silicon photonics and get insight in its advantages and challenges. It is intended for re-searchers with little or no background in silicon photonics as well as those with a more specialist view who want to get a broader understanding of the emerging developments in the field.!e course in particular could benefit those want-ing to get insight in the question “is silicon pho-tonics the solution for my problem?”. !e tutorial contains extensive references for further study. Benefits and Learning Objectives:• Understand why silicon photonics forms a
promising platform for realizing densely inte-grated photonic integrated circuits.
• Understand the operation of basic (splitters, fil-ters, couplers) and more advanced (detectors, modulators, lasers) silicon photonics devices
• Understand the main challenges still to be resolved
• Get insight in the di"erent approaches to com-bine silicon photonics with electronics
• Get insight in the fabrication technology and in possibilities for getting processed devices in a cost-e"ective way, e.g., though the epixfab mul-tiproject wafer service
• Understand for what type of applications sili-con photonics may form a suitable technolo-gy platform
Intended Audience:!e course targets members from academia and industry who want to get a comprehensive review of current state of the art in silicon photonics and get insight in its advantages and challenges. It is intended for researchers with little or no back-ground in silicon photonics as well as those with a more specialist view who want to get a broader understanding of the emerging developments in the field. !e course in particular could benefit those wanting to get insight in the question “is silicon photonics the solution for my problem?”
Biography:Dries Van !ourhout got his PhD in applied physics from Ghent University in 2000 and subsequently spent 2 years at Bell Laboratories, Crawford Hill, NJ US.$ Currently he is a pro-fessor at Ghent University and associated with imec, Europe’s largest nano-electronics research centre. He has extensive experience in integrat-ed optics, silicon photonics and heterogene-ous integration on silicon photonics.$ He has worked on fundamental research topics (such
as optomechanics in the ITN-network cQOM and nanocrystals) but has also been involved in more application oriented projects such as the EU projects WADIMOS (optical intercon-nect) and SMARTFIBER (silicon photonics read out chip for fibre bragg sensing), which he was coordinating and in the EU funded integrated project HELIOS, which covers the whole value chain of silicon photonics.$ He has authored or co-authored over 150 journal publications, over 300 conference contributions and over 10 patents.$ He has given tutorials on silicon pho-tonics at major conferences such as OFC, ACP and CLEO.$ He was associated reviewer for IEEE PTL and holds an ERC starting grant. In 2012 he was awarded with the “Laureate of the Academy” prize of the Belgian Academy of Sciences.
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Short Course 2 SH-2
Optical Parametric Oscillator
Majid Ebrahim-Zadeh, ICFO - "e Institute of Photonic Sciences, Castelldefels (Barcelona), Spain
Course Description:!is course provides an overview of optical par-ametric oscillators (OPOs), from basic opera-tion principles to advanced devices. !e course will begin with a description of the fundamen-tal concepts in nonlinear optics and frequency conversion, followed by a discussion of OPO de-vices, an overview of the latest advances in OPO
technology, and applications. !e discussion will cover OPOs operating in all temporal regimes, from the continuous-wave (cw) to the ultrafast femtosecond time-scales. Specifically, the course participants will gain knowledge of the basic principles of nonlinear frequency conversion and optical parametric generation; phase-matching, amplification and tuning; OPO design issues, including nonlinear material and pump laser selection criteria; OPO operation in di"erent time-scales, generic device architectures, pumping and resonance config-urations; cw OPOs: singly-resonant, pump-en-hanced, doubly- and triply-resonant oscillators, pump power threshold and frequency behaviour, frequency tuning and control, solid-state, fibre, and semiconductor disk laser pumping, visible to mid-IR generation, novel device architectures; pulsed OPOs: operating principle, threshold condition, compact all-solid-state oscillators, high- and low-energy devices, single-mode op-eration, UV to mid-IR and THz generation; syn-chronously-pumped OPOs: picosecond OPOs: high-repetition-rate cw and pulsed oscillators, solid-state, Ti:sapphire and fiber laser pumping, birefringent and quasi-phase-matched devices, UV to mid-IR generation; femtosecond OPOs: Ti:sapphire, solid-state, and fiber-pumped de-vices, collinear and noncollinear pumping, bi-refringent and quasi-phase-matched oscillators,
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spectral and temporal control, UV to mid-IR generation; applications of OPO devices in spec-troscopy, trace gas sensing, imaging, frequency synthesis and comb generation; commercial developments in OPO technology.
Benefits and Learning Objectives:• Understand the basic principles of optical par-ametric generation and amplification of light.
• Learn the operating principles of optical para-metric devices, in particular optical parametric oscillators (OPOs).
• Obtain an understanding of nonlinear gain, phase-matching, operation threshold, device architectures, resonator configurations, tuning, spectral and temporal behaviour.
• Identify the critical issues in the design of opti-cal parametric devices, including material and pump laser selection.
• Acquire the required skills and apply the neces-sary procedures in the practical implementation of OPO devices in cw, pulsed, picosecond and femtosecond operation.
• Learn the necessary techniques for spatial, spec-tral, and temporal control of OPO devices in di"erent operating regimes.
• Gain a perspective of current OPO technology, the important recent developments in the field, as well as novel and emerging applications of OPO sources.
Intended Audience:!is course is intended for researchers with lit-tle or no background in OPOs, as well as those more familiar with the subject area, who wish to enhance their understanding and update their knowledge of the latest developments in OPO device technology. !e course will benefit grad-uate students and other industrial and academic researchers already involved or in early stages in OPO development.
Biography:Majid Ebrahim-Zadeh is an ICREA (Institucio Catalana de Recerca i Estudis Avancats) Professor at ICFO-!e Institute of Photonic Sciences, Barce-lona, Spain. He has been active in the advancement of nonlinear frequency conversion technology and parametric sources for over 20 years. His contri-butions to the field have led the realization of new generations of innovative light sources from the UV to mid-IR and in all time-scales, from continu-ous-wave to ultrafast picosecond and femtosecond regime. He has published over 450 journal papers and peer-reviewed communications, including 70 invited papers and 11 post-deadline papers at major international conferences. He has edited 2 books and has authored 11 major invited book chapters and reviews in volumes such as Science, OSA Handbook of Optics, Springer, Handbook of Laser Technology and Applications, Laser and Photonics Review, and Phil. Tans. Roy. Soc. A (2003). He has been a regular instructor of the short course on OPOs at CLEO/USA since 1997 and at CLEO/Europe since 2007.Majid Ebrahim-Zadeh has served more than 40 times on the technical, organizing, advisory, and steering committees of major internation-al conferences and has chaired 3 international conferences. He has served as advisory editor of Optics Letters, guest editor of J. Opt. Soc. Am. B, topical editor of Optics Letters, associate editor of Advances in Nonlinear Optics, and associate editor of IEEE Photonics Journal, and serves as the current Chair of Nonlinear Optics Techni-cal Group at OSA. Majid Ebrahim-Zadeh is the co-founder, president and chief scientist of Ra-diant Light (www.radiantis.com), a company he created from his research laboratory in Barcelona in 2005. He is a recipient of Innova Prize for tech-nology innovation and enterprise (Spain: 2004), Berthold Leibinger Innovationspreis (Germany: 2010), and a fellow of OSA and SPIE.
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Short Course 4 SH-4
Laser Beam Analysis, Propagation and Spatial Shaping Techniques
James R. Leger, Department of Electrical and Computer Engineering, University of Minnesota, Minneapolis, Minnesota, USA
Course Description:!e propagation and focusing properties of real laser beams are greatly influenced by beam shape, phase distortions, degree of coherence, and aper-ture truncation e"ects. !e ability to understand, predict, and correct these real-world e"ects is es-sential in optical engineering. !is short course develops the analytical tools for measuring and quantifying the important characteristics of a real laser beam, allowing the optical engineer to calculate the performance of the beam in a given optical system. In addition, the intensity, phase, and polarization of laser beams can o#en be engineered to enhance system performance. !e course explores a wide variety of engineering approaches to beam optimization using intuitive design methods coupled with a rigorous mathe-matical treatment of fundamental limits.!e course starts with a basic and highly descrip-tive discussion of the propagation characteris-tics of coherent light from an ideal laser. Simple analytical formulae are developed to calculate the properties of this ideal Gaussian beam in a complex optical system. !ese concepts are ex-tended to higher-order coherent fields, including Hermite-Gaussian beams, beams with top-hat
intensity shapes and “non-di"racting” beams. Fi-nally, the propagation characteristics of coherent light arrays are described mathematically. A set of simple analytical equations is derived to predict the focusing ability of complex coherent light dis-tributions, where the e"ects of beam intensity and phase distribution can immediately be discerned.Laser beam characterization methods such as M2, Strehl ratio, and TDL are reviewed. Incoherent and partially coherent light distributions are investi-gated, and the focusing limits dictated by the ra-diance theorem are developed. Simple expressions for estimating the e"ects of laser aberrations and coherence on beam focusing and propagation are reviewed. Coupling of light into single and mul-ti-mode fibres, as well as far-field light concentra-tion limits are explored as real-world examples. !e concept of “étendue” is introduced as an engi-neering tool to optimize optical design, and simple analytical approaches are presented to estimate the e"ects of spatial beam shape and phase aberrations on beam concentration of incoherent light.!e course ends with a description of various beam-shaping techniques. Intensity beam shaping methods are described for applications where the phase at the target is unimportant. Next, methods for shaping the complex light amplitude in the near- and far-field are developed. Polarization methods including cylindrical vector beams are reviewed. Finally, several intra-cavity beam-shap-ing methods are shown that engineer the intensity and phase of the light inside a laser resonator and improve laser performance.
Benefits and Learning Objectives!is course will enable participants to:• Measure the quality of a laser beam using sev-eral methods.
• Interpret the meaning of various laser specifications.• Understand Gaussian laser beam properties from an intuitive standpoint.
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• Predict the propagation and focusing properties of non-ideal and aberrated laser beams.
• Determine the concentration limits of a light field.
• Design optimal beam concentration optics.• Compare di"erent beam profiles for specific applications and calculate ideal performance.
• Design beam-shaping optics using polarization and phase manipulation.
Intended Audience:!is course is designed to provide laser engineers, optical system designers, and technical manage-ment professionals with a working knowledge of laser beam characterization, analysis, and mod-ification. Physical and intuitive explanations of most topics are designed to make the concepts accessible to a wide range of participants.
Biography:James Leger received his BS degree in Applied Physics from the California Institute of Technol-ogy (1974) and Ph.D. degree in Electrical Engi-neering from the University of California, San Diego (1980). He has held previous positions at the 3M Company, and MIT Lincoln Laboratory. He is currently professor of Electrical Engineer-ing at the University of Minnesota, where he holds both the Cymer Professorship of Electrical Engi-neering and the Mr. and Mrs. George W. Taylor distinguished professorship. His research group is studying a wide variety of optical techniques, including laser mode control and beam shaping techniques, spectral and coherent laser beam combining, optical metrology, solar energy op-tics, design of nonclassical imaging systems, and micro optical engineering. Prof. Leger is currently serving as deputy editor of Optics Express, and has recently served as a member of the CLEO (US) steering committee and the Board of Directors of the Optical Society of America.
James Leger has been awarded the 1998 Joseph Fraunhofer Award/Robert M. Burley Prize by the Optical Society of America, the 1998 Eta Kap-pa Nu outstanding teaching professor award, the 2000 George Taylor Award for Outstand-ing Research at the University of Minnesota, the 2006 Eta Kappa Nu Outstanding teaching Professor award, the ITSB professor of the year award (2006), the Morse Award for Outstand-ing Undergraduate Teaching (2006), the George Taylor Distinguished Teaching Award (2007), and the George Taylor Service Award (2008). He has recently been inducted into the acad-emy of distinguished teachers at the Universi-ty of Minnesota. He is a Fellow of the Optical Society of America, Fellow of the Institute of Electrical and Electronic Engineers (IEEE), and Fellow of the International Society of Optical Engineers (SPIE).
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Short Course 9 SH-9
Terahertz Measurements and their Applications
Daniel M. Mittleman, Rice University, Department of Electrical and Computer Engineering, Houston, TX, USA
Course Description:!is short course discusses several of the most commonly used techniques for performing meas-urements in the terahertz (THz) region of the electromagnetic spectrum. !is spectral range has received heightened attention in recent years,
due to the many promising applications ranging from fundamental spectroscopic measurements of materials to imaging and sensing for security, quality control, and process monitoring. Many di"erent systems have been developed for ac-cessing the THz range based on a wide range of di"erent technology platforms, each with its own capabilities and challenges.In this course, we will review the fundamen-tals of common source, detector, and system technologies. !is will include both electron-ics-based approaches such as mixers and fre-quency multipliers, as well as photonics-based approaches such as time-domain spectroscopy, photo mixing, and THz quantum cascade la-sers. We will consider various figures of mer-it for each technology, which will provide a framework for selecting a particular THz sys-tem for any given application. Although it is not possible to cover all THz technologies at an exhaustive level of detail, we will discuss the most commonly used systems as well as a few of the more exciting new research devel-opments. Application examples will be provid-ed throughout, to illustrate the strengths and weaknesses of existing systems.
Benefits and Learning Objectives:Upon completion of this course, the student should have an understanding of:• A short history of the field of terahertz science and technology.
• !e general concept of how terahertz radiation interacts with various materials.
• !e capabilities and limitations of various tera-hertz measurement systems.
• Which terahertz systems are commercially available, and which ones are still in the basic research stage.
• Some of the more promising science and en-gineering applications of terahertz techniques.
Intended Audience:!is course is intended for scientists and engineers from academia and industry with an interest in the growing field of THz science and technology. It is intended for researchers with an understanding of photonics but with little or no background in the field, as well as for those specialists who wish to get a broader view of emerging developments.
Biography:Daniel Mittleman received his B.S. in physics from the Massachusetts Institute of Technology in 1988, and his M.S. in 1990 and Ph.D. in 1994, both in physics from the University of California, Berkeley, under the direction of Dr. Charles Shank. His thesis work involved the spectroscopy of semiconductor nanocrystals using laser pulses with durations of less than 20 femtoseconds, at wavelengths from 480 nm to 670 nm. He then joined AT&T Bell Labora-tories as a post-doctoral member of the technical sta", working first for Dr. Richard Freeman on a terawatt laser system, and then for Dr. Martin Nuss on terahertz spectroscopy and imaging. Daniel Mittleman joined the ECE Department at Rice University in 1996. At Rice, his research interests involve various aspects of spectroscopy, sensing, and imaging using terahertz radiation. His group reported the first THz measurements on nanom-eter-sized water pools, and developed new types of plasmonic waveguides for broadband THz pulses. He pioneered the use of coherent THz radiation in the study of multiply scattered photons, and the use of apertureless scattering-type imaging for near-field THz spectroscopy. In 2015, his research group has moved from Rice University to Brown Uni-versity, where they continue to work in the field of THz science and technology. Daniel Mittleman edited one of the first books on THz techniques, and is the author of over 150 papers on the top-ic. He founded the conference series on Optical Terahertz Science and Technology (OTST), and
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is currently serving as the Vice-Chairman of the IRMMW-THz Society. He is a Fellow of the Optical Society of America, the American Physical Society, and the IEEE.
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Short Course 6 SH-6
Numerical Photonics on High Performance Computing Architecture
Jerome V. Moloney, University of Arizona, Tucson, AZ, USA
Course Description:!e main objective of the course is to introduce the novice to high performance computing for pho-tonics applications. !e course will cover key steps involved in transitioning serial photonics codes onto commercial parallel computing platforms. !ree key requirements necessary to transition se-rial code to a highly optimized, parallel and scalable form include: (1) Choice of algorithm, (2) Suitabil-ity for distributed/shared or mixed memory par-allelization and (3) suitable computing hardware.I will use two important examples to highlight each of these requirements: (1) Vector Maxwell solvers for computational plasmonics/nanophotonics and, (2) large scale optical carrier wave resolved pulse propagators relevant to filamentation and higher harmonic generation in solid and gaseous (hollow waveguide, photonic crystal and bulk) media.As an example of a scalable parallel Vector Max-well solver we employ the Finite Difference
Time Domain (FDTD) method. We also exam-ine modern FDTD variants that exploit the scale invariance of Maxwell’s equations under gener-alized coordinate transformations to motivate the implementation of both perfectly matched layer (PML) absorbing boundaries and a novel Transformation Optics (TO) based scheme for resolving localized nanostructures. !e numerical and computational aspects of dealing with gener-al shaped boundaries on a Cartesian mesh will be discussed in the context of adaptive mesh refine-ment schemes and the new TO-FDTD method.!e second topic will discuss the essential ele-ments of coding the Unidirectional Pulse Prop-agation equation (UPPE) developed in my group some years ago. Particular examples will be based on the public domain g-UPPE so#ware module, which will be made available to attendees. We will illustrate extreme NLO propagation in photonic crystal fibres with nanometer scale thin strands of dielectric material and in bulk media where ex-treme self-focusing and carrier shock waves place a tremendous stress on the numerical algorithms.
Benefits and Learning Objectives:Essentially all computationally intensive photon-ics so#ware is now designed to run on multi-core CPU processors in high performance workstations or on large-scale massively parallel supercomputers. !e overall e%ciency and scaling potential of these codes, on a given hardware architecture, will depend strongly on choices made during algorithm design and subsequent so#ware implementation. Moreo-ver, special applications can benefit from partition-ing certain code elements to run on GPU processors. At one end of the spectrum the course could benefit senior researchers or research directors who seek an overview of the state-of-the-art in computational photonics on HPC platforms. For those who are invested in developing computer codes in their research, they will get a fast track introduction to
techniques for parallel coding and should avoid the many pitfalls faced by the unitiated.
Intended Audience:Graduate students and senior researchers with a basic knowledge of the physics underlying both topics and with some experience in writing computer codes.
Biography:Jerome V Moloney is a Professor of Mathematics and Optical Sciences at the University of Arizona and is Director of the Arizona Center for Math-ematical Sciences, an internationally recognized research center in applied mathematics. He is a fellow of the Optical Society of America and a recent recipient of the Alexander von Humboldt Prize in physics. Research interests span a wide range of photonics and nonlinear optics fields including ultrashort, high power femtosecond pulse propagation; computational nanophoton-ics, fibre laser modelling, many-body physics of semiconductor optical properties and modelling semiconductor passive and active devices. He has published more than 400 papers in peer-reviewed journals and has given over two hundred invited papers at national and international conferences.
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Short Course 7 SH-7
Frequency Combs and Applications
!omas Udem, Max-Planck-Institut für Quantenoptik, Garching, Germany
Course Description:A laser frequency comb allows the conversion of the very rapid oscillations of visible light of some 100s of THz down to frequencies that can be han-dled with conventional electronics. !is capability has enabled the most precise laser spectroscopy experiments yet, that allowed testing quantum electrodynamics, to determine fundamental con-stants and to search for possible slow changes of these constants.Using an optical frequency reference in com-bination with a laser frequency comb has made it possible to construct all optical atomic clocks that are now outperforming even the best cesium atomic clocks. Direct frequency comb spectroscopy by employing individual modes of the comb may be used for recording broadband molecular absorption. While this has practical relevance for sensitive trace gas analysis, frequency combs may be converted to the extreme ultra violet where no single mode laser exists.!erefore this method might allow high-res-olution laser spectroscopy in this unexplored region for the first time. Frequency combs are also used to calibrate astronomical spectrographs and might reach an accuracy that is su%cient to observe the change of the expansion rate of the universe in real time and to find Earth-like extra solar planets. I will discuss the frequency comb principles in detail and present the vari-ous applications.
Benefits and Learning Objectives:• A short history of the frequency comb.• Basic properties both, in the time domain and frequency domain.
• Frequency metrology.• Time domain applications.• Practical issues for setting up and running a frequency comb.
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• Various methods of direct frequency comb spectroscopy.
• XUV frequency combs.• Applications such as all optical clocks and in astronomy.
Intended Audience:This course is intended to be beneficial for graduate students and industrial and academ-ic researchers who plan to work with frequen-cy combs.
Biography:!omas Udem studied physics at the Universi-ty of Giessen/Germany and at the University of Washington in Seattle/USA. In 1993 he received his diploma from the University of Giessen. A#er that he was working towards the PhD at the Max-Planck Institute of Quantum Optics in Garching/Germany, which he received from the Ludwigs Maximilians Universität Munich/Ger-many in 1997. Since then he has been working at the Max-Planck Institut of Quantum Optics and at the National Institute for Standards and Tech-nology in Boulder/USA. In 2004 he received his habilitation from the Ludwigs Maximilians Uni-versität Munich/Germany and became a fellow of the Max-Planck Institute of Quantum Optics. His scientific work includes precision optical me-trology that involves simple atomic systems such as hydrogen, opto-mechanics and precision spec-troscopy with ion traps and precision astronomy. In addition he is conducting research that aims at making XUV radiation from high harmonic generation useful for high-resolution spectros-copy. !omas Udem received the 2006 Röntgen Award of the University of Giessen and the 2014 EPS Prize for Research in Laser Science and Ap-plications. He is a fellow of the Optical Society of America and the American Physical Society as well as a member of the German Physical Society.
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TECHNICAL FOCUS SESSIONS
An attractive feature of the CLEO®/Europe tech-nical programme has been the Tech Focus format. Technical Focus sessions concentrate on selected photonics applications of industrial importance. !e 2015 programme features two joint technical focus sessions entitled “Ultrafast Solid-State and Fibre Lasers” and “Materials Structuring Using Short Laser Pulses”$jointly held with the LiM 2015 conference, which showcase these exciting fields through presentations from leading academic and industrial researchers. Both sessions consisting of a total of 6 invited presentations take place on Tuesday a#ernoon.
CLEO®/Europe-EQEC 2015 paid registrants are invited to attend these sessions at no additional charge. !ose wishing to attend the technical focus sessions, but who are NOT FULL FEE registrant of the conferences, must pay the one-day fee.
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TF-1: Ultrafast Solid-state and Fibre Lasers
TF-1.1 Tue 14:00
Micromachining and Materials Processing with High Energy Ultrafast Fiber Lasers
Tim Gerke, Fianium, Southampton, Unit-ed KingdomThe short pulsewidth and high peak power provided with ultrafast lasers allow for new processing regimes and materials. For example, processing transparent materials and inside the bulk of materials is newly enabled.
TF-1.2 Tue 14:30Mid IR Fiber Frequency Combs and Applications
Martin Fermann, Kevin Lee, Christian Mohr, Jie Jiang, Naoya Kuse, IMRA America Inc, Ann Arbor, United StatesWe review recent developments in fiber based mid IR combs based on supercontinuum gen-eration, DFG, OPOs and OPAs and discuss their applications in spectroscopy.
TF-1.3 Tue 15:00
Industrial Ultrafast Lasers for Advanced Manu-facturing Applications
Eric Mottay, Amplitude Systèmes, Pessac, FranceUltrafast lasers play a key role in many industrial processes. We review the current status of high pow-er ultrafast laser technology, and present selected manufacturing applications in the pharmaceutical, mobile display and medical device industries.
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TF-2: Materials Structuring Using Short Laser Pulses
TF-2.1 Tue 16:00
Functional Surfaces Generated with Femtosecond Lasers
Rainer Kling, Marc Faucon, Girolamo Mincuzzi, ALPhANOV, Talence, FranceIn this presentation the creation mechanisms of LIPSS are introduced with the feedback on laser specifications and handling systems. Applications of the laser induced surface functions covering dec-oration, tribology and antireflection are discussed.
TF-2.2 Tue 16:30Ultrafast Burst-Mode Fiber Lasers: Source Development and Material Processing
F. Oemer Ilday, Department of Electrical and Electronics Engineering, Department of Physics, Bilkent University, Ankara, TurkeyUltrafast burst-mode micromachining allows enhanced control against thermal e"ects and increases processing speed. Developments in burst-mode fiber lasers and their applications to processing of metals, dielectrics, so# and hard tissue will be presented.
TF-2.3 Tue 17:00
Additive and Subtractive 3D-Microfabrication of Micro/Nanostructures
Yongfeng Lu, University of Nebraska, Lincoln, United StatesIn this study, we developed a complementary 3D micro/nanofabrication process by integrating both additive two-photon polymerization (TPP) and subtractive multi-photon ablation (MPA) into a single platform of femtosecond-laser di-rect writing process.
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PLENARY SESSIONS
PL-1: ECBO-CLEO®/Europe 2015 International Year of Light Event and Plenary Talks
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In the honour of the 2015 International Year of Light, Professors Eric Betzig and Stefan Hell, two of the 2014 Nobel Prize in Chemistry laureates for the development of super-resolved fluorescence microscopy, will present two plenary talks:
PL-1.1 Sun 17:15
Far-field Optical Nanoscopy: Principles and Recent Advancements
Stefan W. Hell, Max Planck Institute for Biophysical Chemistry, Göttingen, Germany
BiographyStefan W. Hell is a director at the Max Planck In-stitute for Biophysical Chemistry in Göttingen. Since 2003 he also leads the Optical Nanoscopy division at the German Cancer Research Center (DKFZ) in Heidelberg, Germany.Stefan W. Hell received his doctorate (1990) in physics from the University of Heidelberg. From 1991 to 1993 he worked at the European Molec-ular Biology Laboratory and from 1993 to 1996 at the University of Turku, Finland.He has received several awards for breaking the
di"raction resolution barrier in light-focusing microscopy: most recently he shared the 2014 Kavli Prize in Nanoscience and the 2014 Nobel Prize in Chemistry.
Abstract!roughout the 20th century it has been widely ac-cepted that, at the end of the day, a light microscope relying on conventional lenses (far-field optics) can-not discern details that are finer than about half the wavelength of light (> 200 nm). However, in the 1990s, it was discovered that overcoming the di"raction barrier is realistic and that fluorescent samples can be resolved virtually down to molecular dimensions. Here we discuss the simple yet pow-erful principles that allow neutralizing the resolu-tion-limiting role of far-field optical di"raction[1,2]. In a nutshell, features residing closer than the dif-fraction barrier are prepared in di"erent molecular (quantum) states so that they are distinguishable for a brief detection period. As a result, the resolu-tion-limiting role of di"raction is overcome, and the interior of transparent samples, such as living cells and tissues can now be imaged non-invasively at the nanoscale using focused light in 3D.Besides discussing basic principles, we will show most recent advancements. In particular, we demonstrate massive parallelization of RESOLFT and STED recording using simple patterns of light, by more than 100,000 fold[3]. Likewise, we demonstrate the relevance of emerging ‘far-field optical nanoscopy’ to various areas, especially to the life and the material sciences.
References[1] Hell, S.W. Far-Field Optical Nanoscopy. Science 316,
1153-1158 (2007).[2] Hell, S.W. Microscopy and its focal switch. Nature
Methods 6, 24-32 (2009).[3] Chmyrov, A. et al. Nanoscopy with more than
100,000 'doughnuts'. Nature Methods (2013).
PL-1.2 Sun 18:00
Imaging Life at High Spatiotemporal Resolution
Eric Betzig, Janelia Research Campus, HHMI, Ashburn, VA, United States
BiographyA#er obtaining a BS in Physics from Caltech, Eric Betzig moved to Cornell, where his thesis involved the development of near-field optics -- the first method to break the di"raction barrier in light microscopy.$He then became a PI at AT&T Bell Labs in Murray Hill, NJ, where he further refined the technology and explored many ap-plications, including high-density data storage, semiconductor spectroscopy, and super resolu-tion fluorescence imaging of cells.$In 1993, he was the first to image single fluorescent molecules under ambient conditions, and determine their positions to better than 1/40 of the wavelength of light.$Tiring of academia, he then served as VP of R&D in his father's machine tool company, de-veloping a high speed motion control technology based on an electro hydraulic hybrid drive with adaptive control algorithms. Looking for new directions, his researches eventually culminated in the invention and demonstration of the super resolution technique PALM by himself and his fellow colleague, Harald Hess. Since 2005, he has been a Group Leader at Janelia, developing new optical imaging technologies for biology. In 2014 he was the co-recipient of the 2014 Nobel Prize in Chemistry.
AbstractAs our understanding of biological systems has increased, so has the complexity of our ques-tions and the need for more advanced optical tools to answer them. For example, there is a hundred-fold gap between the resolution of con-ventional optical microscopy and the scale at which molecules self-assemble to form sub-cel-lular structures. Furthermore, as we attempt to peer more closely at the dynamic complexity of living systems, the actinic glare of our micro-scopes can adversely influence the specimens we hope to study. Finally, the heterogeneity of living tissue can seriously impede our ability to image at high resolution, due to the resulting warping and scattering of light rays. I will describe three areas focused on addressing these challenges: super-resolution microscopy for imaging spe-cific proteins within cells down to near-molec-ular resolution; plane illumination microscopy using non-di"racting beams for non-invasive imaging of three-dimensional dynamics within live cells and embryos; and adaptive optics to recover optimal images from within optically heterogeneous specimens.
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PL-2: 2015 World of Photonic Congress Opening and Plenary Talk
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World of Photonics 2015 Opening Remarks and Speeches
PL-2.1 Mon 10:00
High Performance Quantum Cascade Lasers from the Mid-IR to the Far-IR and their impact on Science and Technology
Federico Capasso,Harvard University, Cambridge, MA, United States
BiographyFederico Capasso is the Robert Wallace Professor of Applied Physics at Harvard University, which he joined in 2003 a#er 27 years at Bell Labs where he was Member of Technical Sta", Department Head and Vice President for Physical Research. He is a co inventor of the Quantum Cascade Laser and pioneered the technique known as band-structure engineering. He performed the first measurement of the repulsive Casimir force. His most recent contributions are on metasurfac-es including the discovery of the generalized laws of refraction and reflection and flat lenses without spherical and chromatic aberrations. He is a member of the National Academy of Sciences, the National Academy of Engineering, the American Academy of Arts and Sciences.
His awards include the King Faisal Prize, the IEEE Edison Medal, the SPIE Gold Medal, the APS Arthur Schawlow Prize, the European Physical Society Quantum Electronics Prize, the Jan Czochralski Award for lifetime achieve-ments in Materials Science, the IEEE Sarno" Award, the Materials Research Society Medal, the Wetherill Medal of the Franklin Institute, the Rank Prize in Optoelectronics, the Opti-cal Society Wood Prize, the Berthold Leibinger Future Prize and the Julius Springer Prize in Applied Physics. He holds honorary doctorates from Lund University, Paris Diderot University and University of Bologna.
Abstract!e mid-infrared and far-infrared regions of the spectrum (3-300 )m) for a long time did not real-ize its full potential, scientifically and technologi-cally, notwithstanding its paramount importance for chemistry, spectroscopy and a myriad of po-tential applications, mainly because of the lack of a compact, room temperature, widely tunable and eye-safe laser. !is situation drastically changed with the advent of the Quantum Cascade Laser (QCL) in 1994 and its subsequent momentous development in the following two decades [1-4]. I will highlight the fundamentally di"erent design principles and underlying physics of QCLs, which showcase a rich variety of optical and transport phenomena. I will illustrate the impact of QCLs in spectroscopy, chemical physics and atmospher-ic chemistry and technology, present and future, ranging from IR countermeasures to a wide range of sensor applications including health care, the environment, security and, ultimately, the “inter-net of everything”.
References[1] J. Faist, F. Capasso, D. L. Sivco, A. L. Hutchinson, and
A. Y. Cho, Science 264, 553 (1994)
[2] F. Capasso, Journal of Optical Engineering 49, 111102 (2010)
[3] R. F. Curl, F. Capasso, C. Gmachl, A. A. Kosterev, B. McManus, R., Lewicki, M. Pusharsky, G. Wysocki, and F. K. Tittel, Chem. Phys. Lett. 487, 1 (2010)
[4] N. Horiuchi Nature Photonics 8, 577 (2014); Nature Photonics 8, 819 (2014)
PL-3: CLEO/Europe 2015 Plenary Talk
! M,0(/5, :C:?@ – :D:?@Location: Room 1
PL-3.1 Mon 14:30
New Horizons for Combs of Light
!eodor W. Hänsch,Ludwig-Maximilians-University, Munich & Max-Planck-Institute of Quantum Optics, Garching, Germany
BiographyCarl-Friedrich-von-Siemens Professor for Exper-imental Physics at the Ludwig-Maximilians-Uni-versity, Munich, Germany, and Director at the Max-Planck-Institute of Quantum Optics in Garching, Germany. Professor Hänsch is widely known for his seminal contributions in the field of laser spectroscopy. His early work includes the first narrowband tun-able dye laser, the invention of commonly used techniques of Doppler-free laser spectroscopy, and the first proposal for laser cooling of atomic gases. Since the early 1970's, Hänsch has pursued precision spectroscopy of the simple hydrogen
atom, which permits unique confrontations be-tween experiment and fundamental theory. !is work has yielded accurate values of the Rydberg constant, the Lamb shi# of the hydrogen ground state, and the charge radii of proton and deuteron. More recently, he has pioneered the revolution-ary frequency comb technique for measuring the frequency of light with ultrashort pulses. Explor-ing the quantum physics of cold neutral atoms, Hänsch and his co-workers have realized the first two- and three-dimensional atomic lattices bound by light, they have demonstrated the first atom la-ser that emits a continuous beam of coherent mat-ter waves, and they have shown how to integrate a quantum laboratory for ultracold atoms on a microfabricated "atom chip". With a Bose-Einstein condensate in an optical lattice potential, they have been the first to observe a quantum phase tran-sition between a wave-like superfluid state and a particle-like Mott insulator crystal. In 2005, !e-odor W. Hänsch has been awarded the Physics Nobel Prize jointly with Roy Glauber and John L. Hall “for his contributions to the development of laser-based precision spectroscopy, including the optical frequency comb technique".
AbstractMode-locked femtosecond lasers and related emerging miniaturized devices can produce optical frequency combs, which consist of a large number of precisely evenly spaced spectral lines. Almost two decades ago, such combs were introduced as tools for optical frequency metrology, motivated by the challenges of precision laser spectrosco-py of atomic hydrogen as tests for fundamental physics laws. Laser frequency combs provide the long-missing clockwork for optical atomic clocks, which are now approaching relative frequen-cy uncertainties of 10-18. Distant clocks can be compared via optical fiber links at the 10-19 level, opening new opportunities for relativistic geodesy
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and astronomical interferometry. As calibration tools for astronomical spectrographs, frequency combs are facilitating the search for exoplanets, and they may lead to direct evidence for the accel-erating expansion of space in our universe. Laser combs are also becoming powerful instruments for broadband molecular spectroscopy. !ey can dramatically improve the resolution and recording speed of Fourier spectrometers, and they are creat-ing intriguing new opportunities for highly mul-tiplexed nonlinear spectroscopy and microscopy.
PL-4: EQEC 2015 Plenary Talk and Awards Ceremony
! T)$%(/5, :@:?@ – :A:?@Location: Room 1
A series of Prizes and Award Ceremonies will be presented together with the Plenary talk. See General Information.
PL-4.1 Tue 11:30
Real and Artificial Atoms Interacting with Photons: From Fundamental Physics to Quantum Information
Serge Haroche,Collège de France, Laboratoire Kastler Brossel, Paris, France
BiographySerge Haroche was born in 1944 in Casablanca. He graduated from École Normale Supérieure
(ENS), receiving his doctorate from Paris VI University in 1971 (thesis advisor: Claude Co-hen-Tannoudji). A#er a post-doctoral visit to Stanford University in the laboratory of Arthur Schawlow (1972-73), he became full professor at Paris VI University in 1975, a position he held until 2001, when he was appointed Professor at Collège de France (Holder of the chair in quan-tum physics and Director since 2012). He has been Maître de Conférence at École Polytech-nique (1974-1984), visiting professor at Harvard (1981), part time professor at Yale University (1984-1993), member of Institut Universitaire de France (1991-2000) and chairman of the ENS Department of Physics (1994-2000). His research has mostly taken place in Laboratoire Kastler Brossel at ENS, where he now works with a team of senior co-workers, postdocs and grad-uate students. Serge Haroche has received many prizes and awards, including the Grand Prix Jean Ricard of the French Physical Society (1983), the Einstein Prize for Laser science (1988), the Humboldt Award (1992), the Michelson Medal from the Franklin Institute (1993), the Tomas-soni Award from La Sapienza University (Rome, 2001), the Quantum Electronics prize of the Eu-ropean Physical Society (2002), the Quantum Communication Award of the International Or-ganization for Quantum Communication, Meas-urement and Computing (2002), the Townes Award of the Optical Society of America (2007), the CNRS Gold Medal (2009) and the Herbert Walter Prize of the German Physical Society and the Optical Society of America (2010). In 2012 he was awarded the Nobel Prize in Physics to-gether with David Wineland. He is a member of the French Academy of Sciences and a Foreign Member of the National Academy of Sciences of the United States. He has received in 2009 a five year advanced research grant from the European Research Council (ERC).
AbstractCavity Quantum Electrodynamics (CQED) studies the interaction of atoms with photons stored in cavities. In the microwave domain, it consists in coupling large electric dipole carrying Rydberg atoms to a very high Q superconduct-ing cavity. With this system, fundamental tests of quantum physics have been realized, including the generation and reconstruction of Schröding-er cat states of light and the observation of their decoherence. Basic quantum information pro-cedures have also been demonstrated. During the last decade, microwave CQED has been ex-tended into a new domain of mesoscopic physics called "Circuit QED", where artificial two level atoms made of superconducting Josephson junctions interact with high Q radiofrequency resonators. !ese systems, based on well-de-veloped solid-state technology are very prom-ising for quantum information science. Atomic CQED and Circuit QED bear strong similarities and also present some marked di"erences which will be illustrated by recent experiments per-formed in both fields.
TUTORIAL TALKS
EE-4: Attosecond and High Field Physics
! S)0(/5, :D:?@ - :B:@@Location: Room Hertz
EE-4.1 Sun 15:30
Population Trapping, Filamentation and Applications
See Leang Chin, Laval University, Center for Optics, Photonics and Laser (COPL), Quebec City, CanadaIonizing femtosecond laser fields can trap electrons into Rydberg states and promote
super-excited states in molecules. Fluorescing fragments exhibit lasing inside air filaments.!ese can be exploited for remote sensing of pol-lutants and snow/rain formation.
EB/EG: Polaritons and Quantum Memories
! T)$%(/5, >:?@ - :@:@@Location: Room 4b
EB/EG.1 Tue 08:30
Cavity Polaritons: from Fundamental Physics to Non-linear and Quantum Devices
Jacqueline Bloch, LPN/CNRS, Marcoussis, FranceSemiconductor microcavities operating in the exciton photon strong coupling regime pro-vide a new platform to manipulate quantum fluid of lights in non-linear devices, and em-ulate complex Hamiltonians using lithography and etching.
CLEO/ECBO-1: Bioimaging
! W$(0$%(/5, >:?@ - :@:@@Location: Room 13b
CLEO/ECBO-1.1 Wed 8:30
Optical Coherence Tomography - A Novel Diagnostic Standard?
Wolfgang Drexler, Center for Medical Physics and Biomedical Engineering, Medical University, Vienna, AustriaIn the last 25 years optical coherence tomography has advanced to be one of the most innovative and most successful translational optical imag-ing techniques, achieving substantial economic impact as well as clinical acceptance.
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CK-12: Integrated Photonic Sources
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 14a
CCK-12.1 Wed 14:00
Rare-earth-doped Lasers on a Silicon Chip
Markus Pollnau, KTH-Royal Institute of Tech-nology, Stockholm, SwedenRare-earth-doped lasers integrated on a sili-con wafer are reviewed. !e theory of contin-uous-wave lasers is extended by considering spontaneous emission in the laser rate equation, thereby deriving the laser eigenvalue, coherence time, Q-factor, and linewidth.
CD-12: Applications of Optical Fibres II
! T').%(/5, :@:?@ - :A:@@Location: Room 1
CD-12.1 Thu 10:30
Scientifc Applications of Photonic Crystal and Microstructured Fibres
Philip Russell, Max Planck Institute for the Science of Light, Erlangen, GermanyMicrostructured and photonic crystal fibres are making possible a whole range of novel experiments on light-matter interactions, including supercon-tinuum generation, ultrafast nonlinear dynamics in gases, enhanced optomechanical e"ects, and manipulation of orbital angular momentum states.
KEYNOTE TALKS
CK-2: Single-emitter and Nanovolume Photonics
! S)0(/5, :@:?@ - :A:@@Location: Room 1
CK-2.1 Sun 10:30
Single-Molecule Ultrafast Photonics
Niek F. van Hulst, ICFO - "e Institute of Photonic Sciences, Castelldefels & ICREA -In-stitucito Catalana de Recerca i Estudis Avancats, Barcelona, SpainResonant optical nanoantennas and phase shaped fs pulses are used to control individual quantum emitters on the nanoscale. !is way e%cient ul-trafast coherent energy transfer is revealed in individual bacterial antenna complexes at phys-iological conditions.
EG-2: Light-matter Interaction with 2D-System
! S)0(/5, :@:?@ - :A:@@Location: Room 4a
EG-2.4 Sun 11:15
Spinoptical Metasurfaces: Spin-Controlled Photonics
Erez Hasman, Technion - Israel Institute of Technology, Haifa, IsraelWe report on a generic concept to control multiple wavefronts by spinoptical gra-dient metasurfaces with a customtailored geometric phase. Spinoptical metasurfaces offer all-optical manipulation by multitask wavefront shaping via a single ultrathin pho-tonic nanodevice.
EA-3: Quantum Interference
! S)0(/5 :?:?@ - :D:@@Location: Room 14c
EA-3.1 Sun 13:30
Interferometry with Atoms and Macromolecules: From Mind-bogglers of Quantum Optics to Elements of Biology
Markus Arndt, University of Vienna, Faculty of Physics, VCQ, QuNaBioS, Vienna, AustriaThis talk reviews some key elements of mat-ter-wave optics, in particular beam splitter tech-niques and interferometers for atoms and large molecules with applications in precision meas-urements and biology.
CE-4: Silicon Photonics
! S)0(/5 :D:?@ - :B:@@Location: Room 14a
CE-4.1 Sun 15:30
Silicon Photonics: an Enabler for Fundamental Science, for the Internet and for the Life Sciences
Roel Baets, Ghent University - imec, Ghent, BelgiumIn this keynote talk the rapid development of the field of silicon photonics is reviewed and an outlook is given on its potential to enable a broad range of applications as well as fundamen-tal science.
EC-3: Cavity Mediated Control of Quantum Matters
! T)$%(/5 :E:@@ - :B:?@Location: Room 4a
EC-3.1 Tue 16:00
Microcavity polaritons: from quantum optics to quantum fluids
Elisabeth Giacobino, Laboratoire Kastler Bros-sel, UPMC, CNRS, ENS, Paris, FranceWe show how photons in an optical microcavity containing a nonlinear medium can both exhibit quantum squeezing and super fluid properties similar to those of low temperature Helium, to-gether with solitons and quantized vortices.
CL-1: Low-cost Labelfree Diagnostic Devices
! W$(0$%(/5 :E:@@ - :B:?@Location: Room 4b
CL-1.1 Wed 16:00
Lens-free On-chip Microscopy for Biomedical Imaging, Sensing and Diagnostics
Aydogan Ozcan, UCLA, Los Angeles, CA, United StatesWe review the recent progress on lens-free com-putational microscopy tools for biomedical imag-ing, sensing and diagnostics applications.
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CF-5: Ultrashort Pulse Measurement and FELs
! W$(0$%(/5 :E:@@ - :B:?@Location: Room 13b
CF-5.4 Wed 16:45
Ultrafast Optics for X-ray Free-electron lasers
Franz Kärtner, Center for Free-Electron Laser Science, DESY and University of Hamburg, Hamburg, GermanyUltrafast optics in X-ray free-electron lasers is reviewed. Progress and needs in photo-injector, pump-probe and seedlasers, timing distribution, THz-pulse generation and its use for X-ray pulse characterization and potentially driving attosec-ond free-electron lasers is discussed.
EF-9: Mechanical Properties of Light and Self-organisation
! T').%(/5 >:?@ - :@:@@Location: Room Curie
EF-9.1 Thu 8:30
Push and Twist: the Mechanical Properties of Light
• Stephen Barnett1, Robert Cameron1, Alison Yao2, Rodney Loudon3
1University of Glasgow, Glasgow, United Kingdom, 2University of Strathclyde, Glasgow, United Kingdom, 3University of Essex, Colchester, United KingdomWe shall describe the two distinct momenta that light carries in a medium, including magnetic and meta materials. !e combination of electric and magnetic e"ects is crucial, also, in exploiting the properties of chiral molecules.
INVITED TALKS
CM-1: Direct Laser Writing
! S)0(/5, @>:?@ - :@:@@Location: Room 4b
CM-1.1 Sun 08:30
Femtosecond Laser Direct Writing for Rapid Fabrication of Functional Devices
Hong-Bo Sun, Jilin University, Changchun, China
CJ-1: Beam Combining of Fibre Lasers
! S)0(/5, @>:?@ - :@:@@Location: Room 13a
CJ-1.1 Sun 8:30
Coherent Combining Techniques to Scale the Performances of Ultrafast Fiber Amplifiers
Marc Hanna1, Florent Guichard1,2, Yoann Zaouter2, Frédéric Druon1, Patrick Georges1
1Laboratoire Charles Fabry, Institut d'Optique, CNRS, Palaiseau, France, 2Amplitude Systèmes, Pessac, France
CC-1: THz Quantum Cascade Laser I
! S)0(/5, @>:?@ - :@:@@Location: Room Einstein
CC-1.1 Sun 08:30
Widely tunable room temperature THz quantum cascade laser sources
Yifan Jiang1, Seungyong Jung1, Aiting Jiang1, Karun Vijayraghavan1, Frederic Demmerle2, Gerhard Boehm2, Xiaojun Wang3,
Mariano Troccoli3, Markus-Christian Amann2, Mikhail A Belkin1
1"e University of Texas at Austin, Austin, TX, United States, 2Technical University of Munich, Garching, Germany, 3Adtech Optics, City of Industry, CA, United States
JSI-1: Novel Light Management Concepts
! S)0(/5, @>:?@ - :@:@@Location: Room Maiman
JSI-1.1 Sun 08:30
Engineering Photonic Structures For Solar Cells: Current, Voltage and Heat
Shanhui Fan, Stanford University, Stanford, United States
EG-1: Nano Optomechanics
! S)0(/5, @>:?@ - :@:@@Location: Room 4a
EG-1.3 Sun 09:00
Nano-Optomechanics in a Focused Laser Beam
Olivier Arcizet, Institut Néel, Grenoble, France
EE-1: Ultrafast Spectroscopy and Extreme Light Sources
! S)0(/5, @>:?@ - :@:@@Location: Room Hertz
EE-1.3 Sun 09:00
Two-Dimensional Mid-Infrared Spectroscopy in Vibrational Ladder
Vincent Kemlin, Louis Daniault, !ibault Vieille,
Adeline Bonvalet, Manuel Jo+re, Laboratoire d'Optique et Biosciences - École Polytechnique - CNRS, Palaiseau, France and INSERM U1182, Palaiseau, France
CH-1: Measurement and Analysis
! S)0(/5, @>:?@ - :@:@@Location: Room Edison
CH-1.5 Sun 09:30
New Directions in Optomechanics: Microfluidc Optomechancis and Levitating Optomechancis
Tal Carmon, Technion - Israel Institute of Technology, Haifa, Israel
CI-1: Overcoming the Capacity Crunch
! S)0(/5, @>:?@ - :@:@@Location: Room Newton2
CI-1.3 Sun 09:00
Potential solutions to overcome the capacity crunch
Andrew Ellis, Mary McCarthy, Mariia Sorokina, Naoise Mac Suibhne, Sergei Turitsyn, Stelianos Sygletos, Aston University, Birmingham, United Kingdom
CM-2: Laser Nanoprocessing
! S)0(/5, :@:?@ - :A:@@Location: Room 4b
CM-2.1 Sun 10:30
Laser Printing of Nanoparticles
Boris Chichkov, Laser Zentrum Hannover e.V., Hannover, Germany
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CA-2: Ultrashort Pulse Oscillators and Amplifiers in Disordered Solid-state Media
! S)0(/5, :@:?@ - :A:@@Location: Room 13b
CA-2.1 Sun 10:30
Ultrafast Solid-State Oscillators and High-Power Amplifiers Based on Broadband, Multisite Yb-doped Crystals
Federico Pirzio1, Etienne Caracciolo1,2, Samuele Davide Di Dio Cafiso1,2, Matthias Kemnitzer2, Annalisa Guandalini2, Florian Kienle2, Stefano Veronesi3, Mauro Tonelli3, Juerg Aus der Au2, Antonio Agnesi1
1Università di Pavia, Dipartimento di Ingegneria Industriale e dell'Informazione, Pavia, Italy, 2Spectra Physics, Rankweil, Austria, 3NEST Istituto Nanoscienze-CNR and Dipartimento di Fisica, Università di Pisa, Pisa, Italy
CD-2: Photonics and QPM
! S)0(/5, :@:?@ - :A:@@Location: Room 14b
CD-2.1 Sun 10:30
From Optical Sunflowers to Optical Tornados Light Propagation in Complex Nonlinear Photonic Lattices
Cornelia Denz, F. Diebel, M. Boguslawski, P. Rose, Institute of Applied Physics and Center for Nonlinear Science (CeNoS), Münster, Germany
EE-2: Filamentation and Intense Light Matter Interaction
! S)0(/5, :@:?@ - :A:@@Location: Room Hertz
EE-2.1 Sun 10:30
Air Waveguides from Femtosecond Filaments
Eric Rosenthal, Nihal Jhajj, John Palastro, Sina Zahedpour, Jared Wahlstrand, Howard Milchberg, Institute for Research in Electronics and Applied Physics, University of Maryland, College Park, United States
JSI-2: Light Management in Thin-film Solar Cells
! S)0(/5, :@:?@ - :A:@@Location: Room Maiman
JSI-2.1 Sun 10:30
Light management and light manipulation technologies for thin film photovoltaics applications
Christoph J. Brabec1,2, Mirowslaw Batentschuk1, Karen Forberich1
1Friedrich-Alexander University Erlangen-Nurnberg, i-MEET, Erlangen, Germany, 2ZAE Bayern e.V, Erlangen, Germany
EF-2: Symmetry Breaking, Photon Fluids and Structured Materials
! S)0(/5, :@:?@ - :A:@@Location: Room Curie
EF-2.3 Sun 11:00
Photonic Mesh Lattices: From PT Solitons to Optical Superfluidity
Martin Wimmer1,2, Alois Regensburger1,2, Mohammad-Ali Miri3, Christoph Bersch1, Demetrios Christodoulides3, Ulf Peschel4
1Institute of Optics, Information and Photonics,
Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany, 2Erlangen Graduate School in Advanced Optical Technologies (SAOT), Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany, 3CREOL, College of Optics and Photonics, University of Central Florida, Orlando, United States, 4Institute of Solid State "eory and Optics, Friedrich Schiller University Jena, Jena, Germany
CH-2: New Photonic Sensor Technologies
! L,&/-",0: R,,# E("%,0Sunday, 10:30 - 12:00
CH-2.3 Sun 11:00
Breaking the mirror symmetry of spontaneous emission via spin-orbit interaction of light
Arno Rauschenbeutel, Vienna Center for Quantum Science and Technology, Institute of Atomic and Subatomic Physics, Vienna University of Technology, Wien, Austria
CE-3: Metamaterials and Photon Manipulation
! S)0(/5, :?:?@ - :D:@@Location: Room 14a
CE-3.1 Sun 13:30
Supersymmetric scattering and transformation optics
Matthias Heinrich1,2, Mohammad-Ali Miri2, Simon Stützer1, Stefan Nolte1, Demetrios N. Christodoulides2, Alexander Szameit1
1Institute of Applied Physics, Abbe Center of Photonics, Friedrich-Schiller-University, Jena, Germany, 2CREOL "e College of Optics and Photonics, University of Central Florida, Orlando, United States
CH-3: Mid Infrared Sensing and Measurements
! S)0(/5, :?:?@ - :D:@@Location: Room Edison
CH-3.1 Sun 13:30
Recent Advances in Quartz Enhanced Photoacoustic Spectroscopy for Trace Gas Sensing
Vincenzo Spagnolo1, Pietro Patimisco1, Angelo Sampaolo1,2, Gaetano Scamarcio1, Frank K. Tittel2
1Dipartimento Interateneo di Fisica, Università e Politecnico di Bari, Bari, Italy, 2Department of Electrical and Computer Engineering, Rice University, Houston, United States
JSIV-1: Optical and Ultrafast Spectroscopy of Two-dimensional Materials
! S)0(/5, :?:?@ - :D:@@Location: Room Maiman
JSIV-1.1 Sun 13:30
2D Materials Beyond Graphene: Optical Properties of Atomically Thin Transition Metal Dichalcogenide Crystals
Tony F. Heinz, Stanford University and SLAC National Accelerator Laboratory, Stanford, CA, United States
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CK-3: Photonic Crystal Lasers
! S)0(/5, :?:?@ - :D:@@Location: Room 1
CK-3.3 Sun 14:00
Photonic Crystal Lasers on Si
Shinji Matsuo1,2, Koji Takeda1,2, Takuro Fujii1,2, Tomonari Sato1
1Nanophotonics Center, NTT Corporation, Atsugi, Japan, 2NTT Device Technology Laboratories, Atsugi, Japan
EG-3: Quantum Nano Optics
! S)0(/5, :?:?@ - :D:@@Location: Room 4a
EG-3.3 Sun 14:00
Single organic molecules as sources of high-flux and narrow-band single photons
Mohammed Rezai1, Kim Kafenda1, Jörg Wrachtrup1,2, Ilja Gerhardt1,2
1Physikalisches Institut, Universität Stuttgart, Stuttgart Research Center of Photonic Engineering (SCoPE), and the Center for Integrated Quantum Science and Technology (IQST), Stuttgart, Germany, 2Max Planck Institute for Solid State Research, Stuttgart, Germany
CM-3: Beam Shaping for Laser Micromachining
! L,&/-",0: R,,# C9Sunday, 13:30 - 15:00
CM-3.3 Sun 14:00
Spatial temporal focusing with
application to micromachining with femtosecond laser pulses
Je+ Squier1, Erica Block1, Michael Young1, Charles Durfee1, Jens !omas2, David Winters3, Randy Bartels3
1Colorado School of Mines, Golden, United States, 2Friedrich-Schiller University, Jena, United States, 3Colorado State University, Fort Colllins, United States
CD-3: Phenomena in Nonlinear Optics
! S)0(/5, :?:?@ - :D:@@Location: Room 14b
CD-3.4 Sun 14:15
PT symmetry in optics and nonlinear optics
Matthias Heinrich, Mohammad-Ali Miri, Mercedeh Khajavikhan, Demetrios Christodoulides, CREOL, "e College of Optics and Photonics, University of Central Florida, Orlando, United States
EA-4: Optomechanics
! S)0(/5, :D:?@ - :B:@@Location: Room 14c
EA-4.1 Sun 15:30
New Frontiers in Quantum Optomechanics: from levitation to gravitational quantum physics
Markus Aspelmeyer, University of Vienna, Faculty of Physics, VCQ, Vienna, Austria
CH-4: Bio-medical Sensing
! S)0(/5, :D:?@ - :B:@@Location: Room Edison
CH-4.1 Sun 15:30
A novel label-free biosensing platform using interference e&ect in an exposed core optical fibre
Linh Nguyen1,2, Kelly Hill1,3, Stephen Warren-Smith2, Tanya Monro2,4,5
1Plant Biosecurity Cooperative Research Centre, Bruce, Australia, 2Institute for Photonics and Advanced Sensing, School of Chemistry and Physics, "e University of Adelaide, Adelaide, Australia, 3South Australian Research and Development Institute, Urrbrae, Australia, 4University of South Australia, Adelaide, Australia, 5ARC Centre of Excellence for NanoBio Photonics, "e University of Adelaide, Adelaide, Australia
JSIV-2: Graphene Plasmonics and Devices
! S)0(/5, :D:?@ - :B:@@Location: Room Maiman
JSIV-2.1 Sun 15:30
Two-Dimensional Optics with Graphene Plasmons
Rainer Hillenbrand, CIC nanoGUNE and UPV/EHU, San Sebastián and IKERBASQUE, Basque Foundation for Science, Bilbao, Spain
CI-4: Advanced Optical Solutions
! S)0(/5, :D:?@ - :B:@@Location: Room Newton2
CI-4.1 Sun 15:30
Passive amplification and real-time averaging of repetitive waveforms by Talbot e&ect
Jose Azana1, Reza Maram1, James Van Howe1,2, Ming Li1,3
1Institut National de la Recherche Scientifique (INRS) * Energie, Matériaux et Télécommunications, Montreal, Canada, 2Department of Physics and Astronomy, Augustana College, Rock Island, United States, 3State Key Laboratory on Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing, China
CA-4: Nanosecond 2%m Solid-state Lasers
! S)0(/5, :D:?@ - :B:@@Location: Room 13b
CA-4.3 Sun 16:00
2 %m Wavelength, 39 mJ Energy, Picosecond Ho:YLF Cryogenic Chirped Pulse Amplifier for Mid-Infrared OPCPA
Michaël Hemmer1, Daniel Sánchez1, Michal Jelínek2, Vadim Smirnov3, Helena Jelinkova2, Václav Kubecek2, Jens Biegert1,4
1ICFO-Institut de Ciencies Fotoniques, Mediterranean Technology Park, Castelldefels, Barcelona, Spain, 2Czech Technical University in Prague, Faculty of Nucl. Sciences and Phys. Eng., Prague, Czech Republic, 3OptiGrate Corp., Oviedo, Florida, United States, 4ICREA - Institució Catalana de Recerca i Estudis Avançats, Barcelona, Spain
CC-4: THz Coherent Control and Spectroscopy
! S)0(/5, :D:?@ - :B:@@Location: Room Einstein
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CC-4.3 Sun 16:00
Local THz Resonances in Semiconductors: Active Control of Near-Fields, THz Extinction and Beaming
Jaime Gomez Rivas1,2, Giorgos Georgiou1, Arkabrata Bhattacharya1
1Center for Nanophotonics, FOM Institute AMOLF, Amsterdam, "e Netherlands, 2COBRA Research Institute, Eindhoven University of Technology, Eindhoven, "e Netherlands
CA-5a: Microchip Lasers I
! M,0(/5, @>:@@ - @>:CDLocation: Room 13b
CA-5a.1 Mon 08:00
Monoclinic Double Tungstate Microchip Lasers at 1 and 2 %m
Xavier Mateos1, Josep Maria Serres1, Pavel Loiko1,2, Konstantin Yumashev2, Nikolai Kuleshov2, Valentin Petrov3, Uwe Griebner3, Magdalena Aguiló1, Francesc Díaz1, 1Universitat Rovira i Virgili, Tarragona, Spain, 2Center for Optical Materials and Technologies, Belarusian National Technical University, Minsk, Belarus, 3Max Born Institute for Nonlinear Optics and Short Pulse Spectroscopy, Berlin, Germany
CK-5: Nonlinear Micro/Nanophotonics
! M,0(/5, ::::D - :A:CDLocation: Room 13a
CK-5.1 Mon 11:15
Photonic Crystal Nonlinear Waveguides: Compressing Nonlinear Fiber Optics on a Chip
Alfredo De Rossi, Sylvain Combrié, "ales Research and Technology, Palaiseau, France
EF-5: Turbulence, Optical Rogue Waves and Modulation Instabilities in Optical Fibres
! M,0(/5, ::::D - :A:CDLocation: Room Curie
EF-5.1 Mon 11:15
Optical Wave Turbulence in Fibre Lasers
Sergei Turitsyn, Aston Institute of Photonic Technologies, Birmingham, United Kingdom
JSII-2: Integrated On-Chip Diagnostics
! M,0(/5, ::::D - :A:CDLocation: Room Edison
JSII-2.1 Mon 11:15
Chip-based Raman spectroscopy for biomedical diagnosis
Juergen Popp, Leibniz Institute of Photonic Technology e.V., Jena, and Institute of Physical Chemistry & Abbe Center of Photonics, Friedrich Schiller University, Jena, Germany
JSIII-1: Laser Driven Acceleration
! M,0(/5, ::::D - :A:CDLocation: Room Einstein
JSIII-1.1 Mon 11:15
Laser wakefield acceleration of multi-GeV electron beams with PW laser pulses
Hyung Taek Kim1,2, Ki Hong Pae1, Vishwa Bandhu Pathak1, Kazuhisa Nakjima1, I Jong Kim1,2, Seong Ku Lee1,2, Jae Hee Sung1,2, Tae Moon Jeong1,2, François Sylla3, Agustin Lifschitz4, Victor Malka4, Chang Hee Nam1,5
1Center for Relativistic Laser Science, IBS, Gwangju, Korea, South, 2Advanced Photonics Research Institute, GIST, Gwangju, Korea, South, 3SourceLAB-Laser Plasma Technologies, LOA, Palaiseau, France, 4Laboratoire d'Optique Appliquée, ENSTA ParisTech, CNRS UMR7639, École Polytechnique, Palaiseau, France, 5Department of Physics and Photon Science, GIST, Gwangju, Korea, South
CJ-5: Mid-IR Fibre Laser Systems I
! M,0(/5, ::::D - :A:CDLocation: Room 1
CJ-5.3 Mon 11:45
Fiber lasers at 3 microns and beyond
Real Vallee, Martin Bernier, Vincent Fortin, Adil Haboucha, Simon Duval, Jean-Christophe Gauthier, Frederic Jobin, Center for Optics Photonics and Lasers, Quebec, Canada
JSIII-1: Laser Driven Acceleration
! M,0(/5, ::::D - :A:CDLocation: Room Einstein
JSIII-1.2 Mon 11:45
Laser-plasma acceleration of electrons to 2 GeV and beyond
Michael Downer, University of Texas at Austin, Austin, United States
CE-6: Nanomaterials for Photonic Applications
! M,0(/5, ::::D - :A:CDLocation: Room 14a
CE-6.5 Mon 12:15
Materials for Medical Imaging and Bio-Imaging
Bruno Viana, IRCP Chimie Paristech, Paris, France
EB-1: Quantum States and Characterization
! M,0(/5, ::::D - :A:CDLocation: Room 21
EB-1.5 Mon 12:15
Testing quantum correlations of three entangled photons generated in cascaded parametric down-conversion
!omas Jennewein1, Deny R. Hamel1,2, Lynden K. Shalm1,3, Hannes Hübel4, Aaron J. Miller3,5, Francesco Marsili3, Varun B. Verma3, Richard P. Mirin3, Sae Woo Nam3, Kevin J. Resch1
1Institute for Quantum Computing, University of Waterloo, Waterloo, Canada, 2Département de physique et d’astronomie, Université de Moncton, Moncton, Canada, 3National Institute of Standards and Technology, Boulder, United States, 4Department of Physics, Stockholm University, Stockholm, Sweden, 5Albion College, Albion, United States
JSII-2: Integrated On-Chip Diagnostics
! M,0(/5, ::::D - :A:CDLocation: Room Edison
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JSII-2.4 Mon 12:15
Opto Acoustic Toolbox for Disease Diagnostics
Jonathan M. Cooper, Julien Reboud, Rab Wilson, Steven N. Neale, Christian Witte, University of Glasgow, Glasgow, United Kingdom
CK-4b: Quantum Information Processing II
! M,0(/5, :D:CD - :E:?@Location: Room 13a
CK-4b.1 Mon 15:45
Quantum Information Processing Using Active Silicon Photonic Integrated Circuits
Dirk Englund1, Jacob Mower1, Nicholas Harris1, Gregory Steinbrecher1, Faraz Najafi1, Yoav Lahini2, Tom Baehr-Jones3, Michael Hochberg3, Karl Berggren1
1Research Laboratory of Electronics, Massachusetts Institute of Technology, Cambridge, United States, 2Department of Physics, Massachusetts Institute of Technology, Cambridge, United States, 3Coriant Advanced Technology Group, Naperville, United States
CE-5b: Semiconductor Technology and Semiconductor Characterization II
! M,0(/5, :D:CD - :E:?@Location: Room 14a
CE-5b.1 Mon 15:45
Integration of cubic III/V semiconductors on silicon (001)
Kerstin Volz, Faculty of Physics and Materials Science Center, Philipps Universität, Marburg, Germany
CD-5b: Applications of Nonlinearities II
! M,0(/5, :D:CD - :E:?@Location: Room 14b
CD-5b.1 Mon 15:45
Chirp determination of ultrashort pulses via transverse second-harmonic generation random nonlinear crystals
Bingxia Wang1, Crina Cojocaru1, Inigo Sola2, Albert Parra1, Wieslaw Krolikowski3,4, Yan Sheng3, Ramon Vilaseca1, Jose Trull1
1Universitat Politècnica de Catalunya, Barcelona, Spain, 2Universidad de Salamanca, Salamanca, Spain, 3Australian National University, Canberra, Australia, 4Texas A&M University at Qatar, Doha, Qatar
JS SPIE/OM/EQEC: Computational Photonics for Metrology Applications
! M,0(/5, :B:@@ - :>:?@Location: Room 1
JS SPIE/OM/EQEC.1 Mon 17:00
Analysis of Bi-Periodic Composite Materials made of Stacks of Tilted One-Dimensional Arrays of Rods
Gérard Granet, Clermont Universités, Université Blaise Pascal, Institut Pascal, Clermont-Ferrand, France and CNRS UMR 6602, IP, Aubière, France
ED-3: Optical Clocks
! M,0(/5, :B:@@ - :>:?@Location: Room 3
ED-3.1 Mon 17:00
Making the Best Atomic Clock
Jun Ye, JILA, NIST and University of Colorado, Boulder, United States
CD-7: Nonlinear Phenomena I
! M,0(/5, :B:@@ - :>:?@Location: Room 14b
CD-7.1 Mon 17:00
Expanding the Scope of Optical Nonlinearity
David Andrews, University of East Anglia, Norwich, United Kingdom
EA-5: Rare Earth Ions
! M,0(/5, :B:@@ - :>:?@Location: Room 21
EA-5.1 Mon 17:00
Storing light up to one minute by EIT in a doped solid
!omas Halfmann, Technical University of Darmstadt, Darmstadt, Germany
JS SPIE/OM/EQEC: Computational Photonics for Metrology Applications
! M,0(/5, :B:@@ - :>:?@Location: Room 1
JS SPIE/OM/EQEC.2 Mon 17:30
Nonlocal Light-Matter Interactions in Noble-Metal and Graphene Nanostructures
N. Asger Mortensen, Department of Photonics Engineering, Technical University of Denmark, Kongens Lyngby, Denmark
JS SPIE/OM/EQEC: Computational Photonics for Metrology Applications
! M,0(/5, :B:@@ - :>:?@Location: Room 1
JS SPIE/OM/EQEC.3 Mon 18:00
Motion Contrast 3D Scanning
Oliver Cossairt1, Nathan Matsuda1, Mohit Gupta2
1Northwestern University, Evanston, United States, 2Columbia University, New York, United States
EC-1: Quantum Gases Manipulation Correlation and Entanglement
! T)$%(/5, @>:?@ - :@:@@Location: Room 4a
EC-1.1 Tue 08:30
Ultracold Fermions in Periodic Potentials: a Bottom-Up Approach
Selim Jochim, Universität Heidelberg, Heidelberg, Germany
CM/LIM: Diagnostics and Control
! T)$%(/5, @>:?@ - :@:@@Location: Room 13a
CM/LIM.1 Tue 08:30
Laser Process Monitoring and Control of Real Process Features
Stefan Kaierle, Laser Zentrum Hannover e.V., Hannve, Germany
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CK-7: Photonics Integration
! T)$%(/5, @>:?@ - :@:@@Location: Room 14a
CK-7.1 Tue 08:30
InP-Based Generic Photonic Integration - Capabilities and Limitations
Francisco Soares1, Moritz Baier1, Tom Gaertner1, Wolfgang Passenberg1, Jean Decobert2, Jean-Louis Gentner2, Mohand Achouche2, Martin Möhrle1, Norbert Grote1
1Fraunhofer Heinrich-Hertz Institute, Berlin, Germany, 2III-V Lab, Marcoussis, France
CB-1: New Frontiers in Semiconductor Lasers
! T)$%(/5, @>:?@ - :@:@@Location: Room 21
CB-1.1 Tue 08:30
Electrically Driven Exciton-polariton Lasers
Sven Höfling1,2, Christian Schneider1, Arash Rahimi-Iman1, Na Young Kim3,4, Julian Fischer1, Ivan Savenko5,6, Matthias Amthor1, Matthias Lermer1, Adriana Wolf1, Lukas Worschech1, Vladimir Kulakovskii7, Ivan Shelykh5,6, Martin Kamp1, Stephan Reitzenstein1,8, Yoshihisa Yamamoto3,9, Alfred Forchel1
1Universität Würzburg, Würzburg, Germany, 2University of St Andrews, St Andrews, United Kingdom, 3Stanford University, Stanford, United States, 4University of Tokyo, Tokyo, Japan, 5University of Iceland, Reykjavik, Iceland, 6Nanyang Technological University, Singapore, Singapore, 7Russian Academy of Science, Chenrnogolovka, Russia, 8Technische Universität Berlin, Berlin, Germany, 9National Institute of Informatics, Tokyo, Japan
EF-7: Nonlinear Behaviour of Light in Waveguides and Photonic Lattices
! T)$%(/5, @>:?@ - :@:@@Location: Room Curie
EF-7.1 Tue 08:30
Nonlinear Interactions in Highly Dispersive Nanostructured Lithium Niobate
!omas Pertsch, Institute of Applied Physics, Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, Germany
CM/LIM: Diagnostics and Control
! T)$%(/5, @>:?@ - :@:@@Location: Room 13a
CM/LIM.2 Tue 09:00
Control of Femtosecond Pulsed Laser Deposition by Temporal Pulse Shaping
Florence Garrelie, Florent Bourquard Anne-Sophie Loir Christophe Donnet, Université de Lyon, Lyon, France and Université de Saint-Étienne, Laboratoire Hubert Curien, Saint-Etienne, France
CA-8: Visible Solid-state Lasers
! T)$%(/5, @>:?@ - :@:@@Location: Room 14b
CA-8.3 Tue 09:00
Wavelength Tuning of Diode-Pumped Pr3+-Lasers
Philip Werner Metz1, Daniel-Timo Marzahl1, Christian Kränkel1,2, Günter Huber1,2
1Institut für Laser-Physik, Universität Hamburg, Hamburg, Germany, 2"e Hamburg Centre for Ultrafast Imaging, Universität Hamburg, Hamburg, Germany
CM/LIM: Diagnostics and Control
! T)$%(/5, @>:?@ - :@:@@Location: Room 13a
CM/LIM.3 Tue 09:30
Ship-in-a-bottle Fabrication of Functional Biochips by Hybrid Femtosecond Laser Processing
Koji Sugioka, Jian Xu, Felix Sima, Dong Wu, Katsumi Midorikawa, RIKEN Center for Advanced Photonics, Wako, Japan
CB-1: New Frontiers in Semiconductor Lasers
! T)$%(/5, @>:?@ - :@:@@Location: Room 21
CB-1.4 Tue 09:30
GeSn as gain material for infrared group IV laser devices
Stephan Wirths1, Richard Geiger2,3, Nils von den Driesch1, Gregor Mussler1, Zoran Ikonic4, Jean-Michel Hartmann5, Jérome Faist3, Siegfried Mantl1, Detlev Grützmacher1, Hans Sigg2, Dan Buca1
1Peter Grünberg Institute 9 and JARA-Fundamentals of Future Information Technology, Forschungszentrum Jülich, Jülich, Germany, 2Laboratory for Micro- and Nanotechnology, Paul Scherrer Institute, Villigen, Switzerland, 3Institute for Quantum Electronics, ETH Zürich, Zürich, Switzerland, 4Institute of Microwaves
and Photonics, School of Electronic and Electrical Engineering, University of Leeds, Leeds, United Kingdom, 5University of Grenoble Alpes & CEA, Leti, MINATEC Campus, Grenoble, France
EC-2: Control of Ultracold Atoms and Molecules with Light
! T)$%(/5, :C:@@ - :D:?@Location: Room 4a
EC-2 1 Tue 14:00
Why Do Single Cold Atoms Matter?
Peter E. Toschek, Universität Hamburg, Institut für Laser-Physik, Hamburg, Germany
CF-2: Ultrafast Parametric Amplifiers
! T)$%(/5, :C:@@ - :D:?@Location: Room 13b
CF-2 1 Tue 14:00
Scaling Mid-IR Driver Sources to Terawatt Peak Powers
Andrius Baltuska1,2, Audrius Pugzlys1,2, Skirmantas Alisauskas1, Valentina Shumakova1, Giedrius Andriuskaitis1, Tadas Balciunas1, Guangyu Fan1, Tobias Floery1, Pavel Malevich1, Tsuneto Kanai1
1Photonics Institute Vienna University of Technology, Vienna, Austria, 2Center for Physical Sciences & Technology, Vilnius, Lithuania
CE-8: Organic Materials for Lasers Waveguides and Nonlinear Optics
! T)$%(/5, :C:@@ - :D:?@Location: Room 14b
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CE-8.1 Tue 14:00
Overcoming Losses in Organic Lasers
!omas Riedl, University of Wuppertal, Wuppertal, Germany
CG-1: Novel Attosecond Light Sources
! T)$%(/5, :C:@@ - :D:?@Location: Room Einstein
CG-1.1 Tue 14:00
Laser-Induced Electron Wave Packets as a Sub-nanometer and Sub-femtosecond Probe
Louis Di Mauro, "e Ohio State University, Columbus, OH, United States
CD-9: Information and Quantum Computing
! T)$%(/5, :C:@@ - :D:?@Location: Room 1
CD-9.3 Tue 14:30
E'cient Photonic Quantum Computing
Fabio Antonio Bovino, Quantum Technologies Lab Finmeccanica-Selex, Genova and Dip. Scienze di Base Applicate all'Ingegneria, La Sapienza, Roma, Italy
EH-1: Chirality in Plasmonics and Metamaterials
! W$(0$%(/5, @>:?@ - :@:@@Location: Room 4a
EH-1.1 Wed 08:30
Spinning and orbiting surface plasmons: twisted light and near-field chiral forces
Cyriaque Genet, University of Strasbourg & CNRS, Strasbourg, France
CE-10: Optical Devices Based on Diamond and Silica
! W$(0$%(/5, @>:?@ - :@:@@Location: Room 14b
CE-10 1 Wed 08:30
Diamond - an Engineer's Best Friend
Andrew Bennett, Daniel Twitchen, Element Six, US Corp., Santa Clara, United States
CB-4: Semiconductor Micro- and Nano-Lasers
! W$(0$%(/5, @>:?@ - :@:@@Location: Room 21
CB-4.1 Wed 08:30
Semiconductor Alloy Nanowires and Nanobelts with Widely Tunable Bandgaps for Full-Spectrum Emission and Multi-Color Lasing
Fan Fan1, Sunay Turkdogan1, Zhicheng Liu1, Cun-Zheng Ning1,2
1Arizona State University, Tempe, AZ, United States, 2Tsinghua University, Beijing, China
CJ-7: Mid-IR Fibre Laser Systems II
! W$(0$%(/5, @>:?@ - :@:@@Location: Room 13a
CJ-7 3 Wed 09:00
Improving the prospects for fluoride-glass-based mid-infrared fibre lasers
Stuart Jackson1, Darren Hudson2, Tomonori Hu2, Stephanie Crawford2
1MQ Photonics, Department of Engineering, Macquarie University, North Ryde, Sydney, Australia, 2Centre for Ultrahigh bandwidth Devices for Optical Systems (CUDOS), Institute of Photonics and Optical Science, School of Physics, "e University of Sydney, Sydney, Australia
EB-3: Sources of Quantum Light
! W$(0$%(/5, @>:?@ - :@:@@Location: Room 4b
EB-3.5 Wed 09:30
Quantum-dot-based Quantum-optical Circuits
Maurice Skolnick, University of She#eld, She#eld, United Kingdom
CG-3: Attosecond Applications of Mid-IR Sources
! W$(0$%(/5, @>:?@ - :@:@@Location: Room Einstein
CG-3.5 Wed 09:30
New Opportunities in Ultrafast Science with the European Light Infrastructure (ELI)
Giuseppe Sansone, Dipartimento di Fisica, Politecnico di Milano, Milano, Italy and ELI-Attosecond Light Pulse Source, ELI-Hu K$, Szeged, Hungary
CLEO/ECBO-2: Optical Manipulation of Biomatter
! W$(0$%(/5, :@:?@ - :A:@@Location: Room 13b
CLEO/ECBO-2.1 Wed 10:30
Twice around is more: The benefits of spatial phase modulation larger than 2 pi for imaging and trapping
Monika Ritsch-Marte, Biomedical Physics, Innsbruck, Austria
CJ-8: Ultrafast Fibre Laser Systems
! W$(0$%(/5, :@:?@ - :A:@@Location: Room 13a
CJ-8.3 Wed 11:00
Coherent Addition of Ultrafast Fiber Laser Pulses
Jens Limpert, Friedrich-Schiller-Universität Jena, Institute of Applied Physics, Jena and Helmholtz-Institute Jena and Fraunhofer IOF Jena, Jena, Germany
CLEO/ECBO-2: Optical Manipulation of Biomatter
! W$(0$%(/5, :@:?@ - :A:@@Location: Room 13b
CLEO/ECBO-2.4 Wed 11:30
Accelerating Progress in Biomedical Imaging
Kishan Dholakia, University of St. Andrews, SUPA, North Haugh, Fife, United Kingdom
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EH-3: Dielectrics and Hyperbolic Metamaterials
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 4a
EH-3.1 Wed 14:00
All-dielectric Nanophotonics: Magnetic Response, Fano Resonances, Functional Metasurfaces, and Nonlinear E&ects
Isabelle Staude, Yuri Kivshar, Nonlinear Physics Centre, Research School of Physics and Engineering, "e Australian National University, Canberra, Australia
CF-4: Novel Ultrafast Lasers
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 13b
CF-4.1 Wed 14:00
High-Power Sub-300-fs Semiconductor Disk Lasers
Mario Mangold1, Dominik Waldburger1, Sandro M. Link1, Matthias Golling1, Emilio Gini2, Bauke W. Tilma1, Ursula Keller1
1Department of Physics, Institute for Quantum Electronics, ETH Zurich, Zurich, Switzerland, 2FIRST Center for Micro- and Nanosicence, ETH Zurich, Zurich, Switzerland
CB-6: Quantum Cascade Lasers
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 21
CB-6.1 Wed 14:00
Widely Tunable Interband Cascade Lasers for the Mid-Infrared
Michael von Edlinger1, Robert Weih2, Julian Scheuermann1, Lars Nähle1, Marc Fischer1, Sven Höfling2,3, Johannes Koeth1, Martin Kamp2
1Nanoplus GmbH, Gerbrunn, Germany, 2Technische Physik, Universität Würzburg, Würzburg, Germany, 3School of Physics and Astronomy, St. Andrews, United Kingdom
CN-1: Laser Sources for Defence and Security
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 1
CN-1.3 Wed 14:30
High Sensitive CMOS Image Sensor for Low Light Level Imaging
Ofer Nesher, Elad Gross, Ran Ginat, Aerospace Division, Elbit Systems Ltd., Haifa, Israel
CG-5: Attosecond Photoionization Dynamics
! W$(0$%(/5, :C:@@ - :D:?@Location: Room Einstein
CG-5.1 Wed 14:00
Attosecond Insight into Electron Correlation
Mathieu Gisselbrecht1, Diégo Guénot1, Erik Månsson1, David Kroon1, Marija Kotur1, Esben Larsen1, Susane Kasper1, Marcus Dahlström2, Eva Lindroth2, Anatoli Kheifets3, Cord Arnold1, Johan Mauritsson1, Stacey Sorensen1, Anne L'Huillier1
1Department of Physics, Lund University, Lund, Sweden, 2Department of Physics, Stockholm University, Stockholm, Sweden, 3Research School of Physical Sciences, "e Australian National University, Canberra, Australia
EB-5: Quantum Simulation
! W$(0$%(/5, :C:@@ - :D:?@Location: Room 4b
EB-5.3 Wed 14:30
Quantum simulation with optical lattices
Ulrich Schneider, Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom; Fakultät für Physik, Ludwig-Maximilians-Universität München, München, Germany and Max-Planck-Institut für Quantenoptik, Garching, Germany
CN-2: Optical Sensing for Defence and Security
! W$(0$%(/5, :E:@@ - :B:?@Location: Room 1
CN-2.1 Wed 16:00
Active Stand-O& Detection in the Mid-Infrared Using Broadband Femtosecond Optical Parametric Oscillators
Zhaowei Zhang1, Luke Maidment1, Stephen Lee3, Rhea Clewes2, Christopher Howle2, Derryck Reid1
1Heriot-Watt University, Edinburgh, United Kingdom, 2Defence Science and Technology Laboratory, Salisbury, United Kingdom, 3"ales Optronics, Glasgow, United Kingdom
EA-8: Semiconductor Quantum Light Sources
! W$(0$%(/5, :E:@@ - :B:?@Location: Room 14b
EA-8.1 Wed 16:00
Quantum Nanophotonics
Jelena Vuckovic, Ginzton Laboratory, Stanford University, Stanford, CA, United States
JSV-1: Photon Pair Sources
! T').%(/5, @>:?@ - :@:@@Location: Room Einstein
JSV-1.1 Thu 08:30
Silicon Quantum Photonics
Damien Bonneau, Josh W. Silverstone, Ra"aele Santagati, Jeremy L. O'Brien, Mark G. !ompson, Centre for Quantum Photonics, H.H. Wills Physics Laboratory and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
CL-2: Fluorescence Imaging and Optical Manipulation
! T').%(/5, @>:?@ - :@:@@Location: Room 4b
CL-2.3 Thu 09:00
Fluorescence lifetime imaging of cellular-level metabolic heterogeneity in cancer
Melissa Skala, Vanderbilt University, Nashville, United States
CD-11: Optical Microscopy
! T').%(/5, @>:?@ - :@:@@Location: Room 1
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CD-11.5 Thu 09:30
Quantum Microscopy with NOON States
Yonatan Israel, Shamir Rosen, Yaron Silberberg, Weizmann Institute of Science, Rehovot, Israel
CJ-12: Erbium Fibre and Waveguide Lasers
! T').%(/5, :@:?@ - :A:@@Location: Room 13a
CJ-12.1 Thu 10:30
Emerging Fiber Lasers and Amplifiers for Telecoms
David Richardson, Yongmin Jung, Qionque Kang, Jayanta Sahu, Saurabh Jain, Zhihong Li, Shaiful Alam, Optoelectronics Research Centre, Southampton, United Kingdom
CB-9: Quantum-dot Lasers
! T').%(/5, :@:?@ - :A:@@Location: Room 21
CB-9.1 Thu 10:30
InGaN/GaN Quantum Dot Lasers: The Next Frontier
Pallab Bhattacharya, !omas Frost, Arnab Hazari, University of Michigan, Ann Arbor, United States
EI-1: Structured Light and Structured Materials
! T').%(/5, :@:?@ - :A:@@Location: Room Curie
EI-1.1 Thu 10:30
Graphene Nanophotonics
Javier De Abajo, ICFO Institut de Ciències Fotòniques, Castelldefels (Barcelona), Spain
CF-7: Ultrafast Spectroscopy and Imaging
! T').%(/5, :@:?@ - :A:@@Location: Room 13b
CF-7.3 Thu 11:00
Mapping Atomic Motions with Ultrabright Electrons
R.J. Dwayne Miller, Max Planck Institute for the Structure and Dynamics of Matter, Hamburg, Germany and University of Toronto, Toronto, Canada
CL-3: Multiphoton and Multimodal Microscopy
! T').%(/5, :@:?@ - :A:@@Location: Room 4b
CL-3.5 Thu 11:30
High-Throughput Second Harmonic Imaging
Sylvie Roke, Carlos Macias-Romero, Marie Didier, Laboratory for fundamental BioPhotonics, Ecole Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
CA-10: Thin Disk Lasers and Amplifiers
! T').%(/5, :@:?@ - :A:@@Location: Room 14a
CA-10.5 Thu 11:30
High-power femtosecond thin-disk oscillators
Oleg Pronin1, Jonathan Brons1, Marcus Seidel1, Jinwei Zhang1, Michael Trubetskov2, Dominik Bauer3, Dirk Sutter3, Vladimir Kalashnikov4, Alexander Apolonski1,2, Vladimir Pervak2, Ferenc Krausz1,2
1Max-Planck-Institute of Quantum Optics, Garching, Germany, 2Ludwig-Maximilians-University Munich, Garching, Germany, 3TRUMPF-Laser GmbH and Co. KG, Schramberg, Germany, 4Aston University, Institute of Photonic Technologies, Birmingham, United Kingdom
JSV-3: Complex Interferences in Waveguides
! T').%(/5, :C:@@ - :D:?@Location: Room Einstein
JSV-3.1 Thu 14:00
Multiphoton quantum interference in multiport integrated optical circuits: from teleportation to Boson Sampling
Ian Walmsley1, Ben Metcalf1, Justin Spring1, Peter Humphreys1, Marco Barbieri3, Steven Kolthammer1, James Gates2, Peter Smith2
1University of Oxford, Oxford, United Kingdom, 2University of Southampton, Southampton, United Kingdom, 3Universita degli Studi Roma Tre, Roma, Italy
CF-8: High Harmonic Generation Ultrafast Technology
! T').%(/5, :C:@@ - :D:?@Location: Room 13b
CF-8.5 Thu 15:00
Multidimensional harmonic phase spectroscopy
A. Camper, N. Lin, B. Manschwetus, R. Géneaux, E. Skantzakis, V. Gruson, B. Carré, T. Auguste, P. Salières, T. Ruchon, CEA, IRAMIS, Lasers, Interactions and Dynamics Laboratory - LIDyL, CEA-SACLAY, Gif-sur-Yvette, France
NOTES
CLEO®/Europe-EQEC 2015 ⋅ Sunday 21 June 2015
ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b8:30 – 10:00CK-1: Subwave Length-and Di�raction GratingsChair: Olivier Gauthier-Lafaye, LAAS-CNRS,Toulouse, France
8:30 – 10:00EG-1: NanoOptomechanicsChair: Stephan Götzinger,Max Planck Institute for theScience of Light, Erlangen,Germany
8:30 – 10:00CM-1: Direct LaserWritingChair: Marc Sentis, Univer-sity of Aix Marseille, Marseille,France
8:30 – 10:00CJ-1: Beam Combiningof Fibre LasersChair: �omas Schreiber,Fraunhofer-Institut fürAngewandte Optik undFeinmechanik, Jena, Germany
8:30 – 10:00CA-1: Solid StateRaman LasersChair: Valdas Pasiskevicius,KTH, Stockholm, Sweden
8:30 – 10:00CE-1: Fibre TechnologyChair: Pier Sazio, Universityof Southampton, Southamp-ton, United Kingdom
8:30 – 10:00CD-1: Applications ofOptical Fibres IChair: Valentin Vlad, Uni-versity of Bucharest-Academia,Bucharest, Romania
CK-1.1 SUN 8:30Silicon NitrideSub-Wavelength Gratingsfor the Generation ofRadially PolarisedCylindrical Vector Beams atVisible Wavelengths�D. Stellinga, Y. Wang, andT.F. Krauss; University of York,York, United KingdomMiniaturising super reso-lution microscopy requirescompact beam shapingtechniques in the visiblespectrum. We show that sub-wavelength gratings in siliconnitride can generate radiallypolarised cylindrical vectorbeams thereby providing thisfunctionality.
EG-1.1 SUN 8:30Position-Squared Couplingin a Photonic CrystalCavity-OptomechanicalSystem�T. Paraiso1,2, L. Zang1, H.Pfeifer1, M. Kalaee2, andO. Painter2; 1Max PlanckInstitute for the Science ofLight, Erlangen, Germany;2California Institute of Tehc-nology, Pasadena, CA, UnitedStatesA multi-moded photoniccrystal optomechanicalresonator is introduced,in which the optical cavitymode interact quadraticallywith the mechanical modes.Electrostatic actuation isused to control the structureand demonstrate very largequadradic coupling strengths.
CM-1.1 SUN (Invited) 8:30Femtosecond Laser DirectWriting for RapidFabrication of FunctionalDevices�H.-B. Sun; Jilin University,Changchun, China, People’sRepublic of (PRC)�e recent progress in fem-tosecond laser direct writingwill be reported. Particularemphasis will be placed onmovable devices or parts suchas photo-reduced graphenewalking robots, and dynamiclaser prototyping enabled�ower blooming.
CJ-1.1 SUN (Invited) 8:30Coherent CombiningTechniques to Scale thePerformances of UltrafastFiber Ampli�ers�M. Hanna1, F. Guichard1,2,Y. Zaouter2, F. Druon1, andP. Georges1; 1LaboratoireCharles Fabry, Institutd’Optique, CNRS, Palaiseau,France; 2Amplitude Systemes,Pessac, FranceVarious coherent combiningtechniques in the space andtime domains have been usedto scale the performances ofultrafast �ber ampli�ers. Wediscuss these concepts andpresent several experimentsperformed in this �eld.
CA-1.1 SUN 8:30Femtosecond-pumpeddiamond Raman laser withtuneable second-Stokesoutput�M. Murtagh1,2, J. Lin1, D. J.Spence1, and G. McConnell2;1Macquarie University, Syd-ney, Australia; 2University ofStrathclyde, Glasgow, UnitedKingdomWe report a tuneablefemtosecond-pumped dia-mond Raman laser operatingwith a second-Stokes outputbetween 1082 -1200 nm.�rough this Raman conver-sion process we can access awavelength range beyond thereach of standard Ti:Sapphirelasers.
CE-1.1 SUN 8:30Evidence of Yb-to-Er energytransfer in AlPO4 :Yb3+/Er3+nanoparticle-doped silicaoptical �ber preform�L. Bigot1, I. Savelii1, H. ElHamzaoui1, G. Bouwmans1,S. Plus1, B. Capoen1, A.-M.Blanchenet2, A. Pastouret3,C. Chanéac4, and M.Bouazaoui1; 1PhLAM, CNRSUniversité Lille 1, IRCICA,59658 Villeneuve D’ascq,France; 2UMET, UniversitéLille 1, 59655 VilleneuveD’ascq, France; 3PrysmianGroup, Parc des IndustriesArtois Flandres, 62138Billy-Berclau, 62092 Haisnes,France; 4Sorbonne Universités,UPMC CNRS, Collège deFrance, LCMCP, 75005 Paris,France�is paper reports on thesynthesis and characterizationof silica optical �ber pre-form and PCF �ber dopedwith AlPO4:Yb/Er nanoparti-cles. Yb-Er energy transferand presence of nanoparticlesin the core preform are put inevidence.
CD-1.1 SUN 8:30E�cient TunableFrequency-Shi�ing of anOptical Signal via RamanCoherence Waves inHydrogen-Filled HC-PCF�S. Bauerschmidt, D. Novoa, A.Abdolvand, B. Trabold, and P.Russell; Max Planck Institutefor the Science of Light, Erlan-gen, GermanyA pre-excited vibrationalRaman coherence wave isused for pressure-tunable,70% e�cient, phase-matchedfrequency up-conversion ofan arbitrary signal betweenLP01 modes in hydrogen-�lled kagomé-PCF. �etechnique is tunable for theUV to the NIR.
CK-1.2 SUN 8:45High Order modes in CavityResonator IntegratedGuided mode resonanceFilters (CRIGFs)�R. Laberdesque1,2, O.Gauthier-lafaye1,2, H.Camon1,2, A. Monmayrant1,2,M. Petit3, O. Demichel3, andB. Cluzel3; 1CNRS-LAAS,Toulouse, France; 2Universitéde Toulouse, Toulouse, France;3Laboratoire InterdisciplinaireCarnot de Bourgogne, Univer-sité de Bourgogne, Grenoble,FranceWe report experimental ob-servation and modeling ofnew multimodal high-Q re-�ector. Combining coupled-wave modeling with moiréanalysis, unusual mode pro-
EG-1.2 SUN 8:45Graphene HybridOptomechanics�K. Schädler; ICFO, Barcelona,SpainWe present a novel hybridoptomechanical systemcomprising a graphene drumresonator coupled to thenear �eld of an NV centre.We demonstrate indirect,time-resolved readout ofthe resonator’s nano-motionthrough NV centre emission.
CA-1.2 SUN 8:45Diode-side-pumped,continuous-wave Nd:YVO4self-Raman laser at 1176nmbased on DBMC technologyC. Kores1, D. Geskus2, H.Pask3, and �N. Wetter1;1Centro de Lasers e Aplicações,IPEN-CNEN/SP, São Paulo,Brazil; 2Dep. of Materialsand Nano Physics, KTH,Stockholm, Sweden; 3MQ Pho-tonics, Department of Physicsand Astronomy, MacquarieUniversity, Sydney, AustraliaIn this work we demonstratefor the �rst time, to ourknowledge, cw operation ofa side-pumped Nd:YVO4 self-Raman laser at 1176 nm, withsingle mode TEM00 laser op-eration.
CE-1.2 SUN 8:45Rare-earth dopedchalcogenide �bers forall-optical gas sensing in themid-infrared spectral range�A.-L. Pelé1, A. Braud1, J.-L.Doualan1, R. Chahal2, V.Nazabal2, R. Moncorgé1,and P. Camy1; 1Centre deRecherche sur les ions, lesmatériaux et la photonique(CIMAP), Caen, France;
CD-1.2 SUN 8:45Extreme Nonlinear SignalAmpli�cation�M. Närhi1, L. Orsila2, J.Sand1, G. Steinmeyer2,3, andG. Genty1; 1Physics Depart-ment, Tampere University ofTechnology, Tampere, Finland;2Optoelectronics ResearchCenter, Tampere Universityof Technology, Tampere,Finland; 3Max Born Institutefor Nonlinear Optics and ShortPulse Spectroscopy, Berlin,GermanyUsing the extreme sensitivityof supercontinuumgenerationto input pulse power �uctua-tions, we demonstrate experi-mentally the regeneration andampli�cation of a weak signalby up to 46 dB.
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ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON28:30 – 10:00EA-1: Non-ClassicalLight and EntanglementChair: David Hunger, LMUMunich, Faculty of Physics,Munich, Germany
8:30 – 10:00EF-1: Localized States ofLightChair: Philippe Grelu, Uni-versity of Bourgogne, Dijon,France
8:30 – 10:00CH-1: Measurement andAnalysisChair: Trevor Benson, Univer-sity of Nottingham, Notting-ham, United Kingdom
8:30 – 10:00CC-1: THz QuantumCascade Laser IChair: Jérôme Faist, ETH,Zürich, Switzerland
8:30 – 10:00EE-1: UltrafastSpectroscopy andExtreme Light SourcesChair: Goëry Genty, TampereUniversity of Technology, Tam-pere, Finland
8:30 – 10:00JSI-1: Novel LightManagement ConceptsChair: Jennifer Dionne, Stan-ford University, Stanford, USA
8:30 – 10:00CI-1: Overcoming theCapacity CrunchChair: Matteo Conforti,PhLAM, CNRS-UniversitéLille 1, Lille, France
EA-1.1 SUN 8:30Hybrid Entanglement ofLight for HeterogeneousQuantum Networks�O. MORIN1, H. LEJEANNIC1, K. HUANG1,2,J. LIU1, C. FABRE1, J.RUAUDEL1, Y.-C. JEONG1,and J. LAURAT1; 1LaboratoireKastler Brossel, Paris, France;2State Key Laboratory of Pre-cision Spectroscopy, Shanghai,China, People’s Republic of(PRC)�e wave-particle duality oflight has led to two di�erentencodings for optical quan-tum information processing.We report here the remotegeneration of entanglementbetween particle-like discrete-variable qubits and wave-likecontinuous-variable qubits.
EF-1.1 SUN 8:30Merging and Annihilationof Temporal Cavity SolitonsJ.K. Jang1, M. Erkintalo1,K. Luo1, G.-L. Oppo2, S.G.Murdoch1, and �S. Coen1;1�e University of Auckland,Auckland, New Zealand;2University of Strathclyde,Glasgow, United KingdomWe studymerging and annihi-lation of temporal cavity soli-tons in a �ber ring. �e dy-namics of the energy balanceis �nely resolved. Our experi-ment illuminates the behaviorof localized dissipative struc-tures in more general settings.
CH-1.1 SUN 8:30Nano-OptomechanicalSensing of nanometer-scaleresonator�A. Tavernarakis1, I.Tsioutsios1, P. Verlot1,2, andA. Bachtold1; 1ICFO, Institutde Ciencies Fotoniques,Barcelona, Spain; 2ILM,Institut Lumière Matière,Lyon, FranceWe have optically probed aSiC nanoresonator with asignal-to-noise ratio of 40dB and we have performedtime-resolved measurementsof the thermally-actuatedmotion of a suspendedsingle-wall carbon nanotubeusing an electron beam.
CC-1.1 SUN (Invited) 8:30Widely tunable roomtemperature THz quantumcascade laser sourcesY. Jiang1, S. Jung1, A.Jiang1, K. Vijayraghavan1, F.Demmerle2, G. Boehm2, X.Wang3, M. Troccoli3, M.-C.Amann2, and �M.A. Belkin1;1�e University of Texas atAustin, Austin, TX, UnitedStates; 2Technical University ofMunich, Garching, Germany;3Adtech Optics, City ofIndustry, CA, United StatesWe present broadly-tunableterahertz quantum cascadeslaser sources based on intra-cavity di�erence-frequencygeneration. Devices achievecontinuous tuning in 1.2-5.7THz range with up to 100microWatt of peak poweroutput in pulsed mode atroom-temperature.
EE-1.1 SUN 8:30Vacuum UltravioletSupercontinuumGenerationin Gas-Filled Hollow-CorePhotonic Crystal Fibres�A. Ermolov, K.F. Mak, J.C.Travers, and P.S.J. Russell;MaxPlanck Institute for the Scienceof Light, Erlangen, GermanyA supercontinuum 113-1000nm is generated from 35 fs,805 nm, 5.2 uJ pump pulsesin kagomé-PCF �lled with 28bar helium. �e mechanisminvolves the interplay betweendispersive-wave emission andan ionisation-driven solitonblue-shi�.
JSI-1.1 SUN (Invited) 8:30Engineering PhotonicStructures For Solar Cells:Current, Voltage and Heat�S. Fan; Stanford University,Stanford, United StatesWe present a combined three-dimensional optical and elec-tronic simulation to calculatethe intrinsic limits on energyconversion e�ciency in ultra-thin nanotextured crystallinesilicon solar cells. We alsodemonstrate radiative coolingof silicon solar absorbers.
CI-1.1 SUN 8:30Dynamic ModeMultiplexing withPlasmonic Metasurfaces�M. Papaioannou1, E.Plum1, J. Valente1, E.T.F.Rogers1, and N.I. Zheludev1,2;1University of Southamp-ton, Southampton, UnitedKingdom; 2Nanyang Techno-logical University, Singapore,SingaporeWe demonstrate logical oper-ations with two images usingcoherent interaction of opti-cal beams on thin �lms andmetasurfaces. �e new coher-ent image processing is illus-trated by mode selection anddeletion for spatial modemul-tiplexing.
EA-1.2 SUN 8:45GHz kinematic sensing withclassically entangled beamsof light�S. Berg-Johansen1,2, F.Töppel1,2, B. Stiller1,2, P.Banzer1,2,3, M. Ornigotti4, E.Giacobino5, G. Leuchs1,2,3, A.Aiello1,2, and C. Marquardt1,2;1MPI for the Science ofLight, Erlangen, Germany;2Inst. of Optics, Informationand Photonics, Universityof Erlangen-Nuremberg,Erlangen, Germany; 3Dep. ofPhysics, University of Ottawa,Ottawa, Canada; 4Instituteof Applied Physics, Friedrich-Schiller University Jena,Jena, Germany; 5LaboratoireKastler Brossel, Paris, FranceWe introduce a novel sens-
EF-1.2 SUN 8:45Temporal LocalizedStructures in Mode-LockedLasersM. Marconi1, J. Javaloyes2,S. Balle3, and �M. Giudici1;1Institut Non Linéaire deNice, Valbonne, France;2Universitat de les IllesBaleares, Palma de Mallorca,Spain; 3Institut Mediterranid’Estudis Avançats, Esporles,SpainWe show how temporal lo-calized structures can be im-plemented in a passive modelocked semiconductor laser,allowing for individual ad-dressing of the pulses and ar-bitrary low repetition rates.
CH-1.2 SUN 8:45A Scanning CavityMicroscope�M. Mader1,2, J. Reichel3, T.W.Hänsch1,2, and D. Hunger1,2;1Max-Planck-Institut fürQuantenoptik, Garching, Ger-many; 2Ludwig-Maximilians-Universität, München,Germany; 3LaboratoireKastler-Brosel, Paris, FranceWe present a versatile tech-nique for ultra-sensitive andspatially resolved optical char-acterization of single nanopar-ticles. Using signal enhance-ment in a high-�nesse scan-ning optical microcavity wemeasure the extinction andthe polarizability of individualnanoparticles.
EE-1.2 SUN 8:45Impulsive Excitation ofRaman Modes inHydrogen-FilledHollow-Core PCF by aSequence of TwoSelf-Compressed Pulses�A. Abdolvand, F. Belli, J.Travers, and P. Russell;MPI forthe Science of Light, Erlangen,Germany�e spectral broadening inhydrogen-�lled hollow corePCF is observed to varyperiodically with the timedelay between two identical30 fs pump pulses. Pulseself-compression results instrong impulsive excitationof ro-vibrational Ramantransitions.
CI-1.2 SUN 8:45Supersymmetric modeconverters�M. Heinrich1,2, M.-A.Miri2, S. Stützer1, S. Nolte1,A. Szameit1, and D.N.Christodoulides2; 1Instituteof Applied Physics, AbbeCenter of Photonics, Friedrich-Schiller-University, Jena,Germany; 2CREOL, Uni-versity of Central Florida,Orlando, United StatesWe experimentally demonstr-tate the global phase matchingproperties a�orded by super-symmetric optical structures,and show for the �rst timehow hierarchical sequences ofSUSY partner structures canbe utilized as compact and ef-�cient mode converters.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b
�les and frequencies are ac-curately predicted and con-trolled.
2Institut Sciences Chimiquesde Rennes, Rennes, FranceWe present results on rare-earth doped chalcogenide�bers �rst used as IR sourceand also as IR to visibleconverter for the developmentof an all-optical infrared gassensor.
CK-1.3 SUN 9:00First ExperimentalDemonstration of OriginalOptical Filter Based onMultiply CoupledWaveguidesL. O’Faolain1 and �A.Tsarev2,3; 1Scottish Universi-tiesPhysics Alliance (SUPA),School of Physics and As-tronomy, St Andrews, UnitedKingdom; 2Rzhanov Instituteof SemiconductorPhysics SBRAS, Novosibirsk, Russia;3Novosibirsk State University,Novosibirsk, RussiaPaper presents the �rst exper-imental demonstration of anoptical �lter based on multi-ply coupled waveguides. �eexperimental results �ts thenumerical modeling by 2DFDTD which utilizes a mod-i�ed e�ective index method(MEIM) approximation.
EG-1.3 SUN (Invited) 9:00Nano-Optomechanics in aFocused Laser Beam�O. Arcizet; Institut Néel,Grenoble, FranceWe investigate optome-chanical coupling of asub-wavelength sizednanoresonator in a stronglyfocused laser beam. We es-tablish the cartography of theoptomechanical interactionand investigate dynamicalbackaction of this bidimen-sional, non-conservative force�eld.
CM-1.2 SUN 9:00Femtosecond Pulsed LightPolarization InducedPeculiarities in Direct LaserWriting 3DNanolithography�M. Malinauskas1, S.Rekstyte1, T. Jonavicius1,V. Mizeikis2, E. Gamaly3,and S. Juodkazis4,5; 1VilniusUniversity, Vilnius, Lithuania;2Shizuoka University, Hama-matsu, Japan; 3AustralianNational University, Ac-ton, Australia; 4SwinburneUniversity of Technology, Mel-bourne, Australia; 5MelbourneCentre for Nanofabrication,Melbourne, AustraliaEmploying femtosecondpulses we investigate impactof light polarization to the3D polymer nanostruc-turing’s spatial resolutionand morphology. Physicalmechanisms are modeledand presented. Practicalissues regarding optimizationof reproducibility in DLWlithography are discussed.
CJ-1.2 SUN 9:00Large-pitch Multicore Fiberfor Coherent Combinationof Ultrashort Pulses�A. Klenke1,2, M. Wojdyr1,M. Müller1, M. Kienel1,2,T. Eidam1,2, H.-J. Otto1,F. Stutzki1, F. Jansen1,J. Limpert1,2,3, and A.Tünnermann1,2,3; 1Instituteof Applied Physics, AbbeCenter of Photonics, Friedrich-Schiller University Jena,Jena, Germany; 2Helmholtz-Institute Jena, Jena, Germany;3Fraunhofer Institute ofApplied Optics and PrecisionEngineering, Jena, GermanyWe report on a laser ampli-�er delivering 170 W averagepower based on coherent ad-dition of the four cores of amulticore �ber in combina-tion with a simple and com-pact beam splitter and com-biner.
CA-1.3 SUN 9:00Monolithic DiamondRaman Laser Operating at573nm Utilizing MicrolensStructures to Form a StableResonator�S. Reilly, V. Savitski, H. Liu, E.Gu, M. Dawson, and A. Kemp;Institute of Photonics, Depart-ment of Physics, University ofStrathclyde, Glasgow, UnitedKingdomA monolithic microlensed di-amond Raman laser with aconversion e�ciency of 84%from pump to combined Ra-man output is reported. �isis a simple, compact and e�-cient means to colour convertcommon ns green lasers.
CE-1.3 SUN 9:00Enabling silica for highdensity rare earth doping forintegrated opto-electronicsystems�J. Chandrappan1, G. Jose1,M. Murray1, and P. Petrik2;1University of Leeds, Leeds,United Kingdom; 2Institutefor Technical Physics andMaterials Science, Hungar-ian Academy of Sciences,Budapest, Hungary�e physical and chemicaldoping limitations in silicaare overcome through ultra-fast laser assisted hybrid inte-gration of rare earth enrichedtellurite and silica is achieved,exhibiting the highest ever re-ported lifetime-density prod-uct 1.51x10^20 s. cm-3.
CD-1.3 SUN 9:00Observation of acousticavoided crossing in anoptical �ber taper�J.C. Beugnot1, A. Raja2, M.Rochette2, J.c. Tchahame1, V.Laude1, H. Maillotte1, andT. Sylvestre1; 1FEMTO-STinstitute, Besancon, France;2Department of Electrical andComputer Engineering, McGillUniversity, Montreal, CanadaWe experimentally demon-strate the �rst phonon avoidedcrossing in chalcogenide mi-crowire by means of theBrillouin scattering nonlin-earity. Numerical calculationsbased on electrostrictionmodelling explain the result.
CK-1.4 SUN 9:15Control of spatial �ltering inlight propagation throughwoodpile photonic crystals�lled with liquid crystal�C.-H. Ho1, Y.C. Cheng2, L.Maigyte2, H. Zeng1, J. Trull2,C. Cojocaru2, D. Wiersma1,and K. Staliunas2,3; 1EuropeanLaboratory for Non LinearSpectroscopy (LENS), Univer-sity of Florence, Florence, Italy;2Dep. de Física i EnginyeriaNuclear, Universitat Politèc-nica de Catalunya, Terrassa,Spain; 3Institucio Catalanade Reserca i Estudis Avançats(ICREA), Barcelona, Spain
CM-1.3 SUN 9:15Bulk and surfacefunctionalization of DirectLaser Writing fabricatedstructures�A. Selimis1, A.N. Giakou-maki1,2, N. Chamakou1,3, K.Alexaki1,4, E. Stratakis1,3,and M. Farsari1; 1Institute ofElectronic Structure and Laser(I.E.S.L.), Foundation forResearch & Technology-Hellas(FO.R.T.H.), Heraklion,Greece; 2Dep. of Chemistry,University of Crete, Heraklion,Greece; 3Dep. of MaterialsScience and Technology,University of Crete, Heraklion,
CJ-1.3 SUN 9:15Ultrafast multicoreYb-doped �ber ampli�erL.P. Ramirez1, �M. Hanna1,G. Bouwmans2, H. El Ham-zaoui2, M. Bouazaoui2, D.Labat2, K. Delplace2, J. Pouy-segur1,3, F. Guichard1,3, P.Rigaud4, V. Kermène4, A.Desfarges-Berthelemot4, A.Barthélémy4, F. Prévost5, L.Lombard5, Y. Zaouter3, F.Druon1, and P. Georges1;1Lab. Charles Fabry, Institutd’Optique, CNRS, Palaiseau,France; 2Lab. PhLAM, Univer-sité Lille 1, CNRS, Villeneuved’Ascq, France; 3Amplitude
CA-1.4 SUN 9:15E�cient Picosecond RamanConverter Based on aSrWO4 Crystal Pumped by aMulti-Watt MOPA Laser at1064 nmP. Farinello1, �F. Pirzio1,X.-Y. Zhang2, V. Petrov3,and A. Agnesi1; 1Universitàdi Pavia, Dipartimento diIngegneria Industriale edell’Informazione, Pavia,Italy; 2School of InformationScience and Engineering,Shandong University, Jinan,China, People’s Republic of(PRC); 3Max-Born-Institute,Berlin, Germany
CE-1.4 SUN 9:15Experimental Comparisonof Di�ering DesignApproaches ForMultichannel Fibre BraggGratings�A. Gbadebo, E. Turitsyna,and J. Williams; Aston Uni-versity, Birmingham, UnitedKingdomWe demonstrate experimen-tally how a coupling coef-�cient spreading design ap-proach for multichannel �breBragg gratings gives rise tomore easily realisable devicesthat alsomore accurately meetthe design target spectrum.
CD-1.4 SUN 9:15Watt-level,Duration-tunablePicosecond Source at 560nm by Second-harmonicGeneration of a RamanFiber Laser�T. Runcorn, R. Murray, E.Kelleher, S. Popov, and J.Taylor; Femtosecond OpticsGroup, Deparment of Physics,Imperial College London,London, United KingdomWe present a novel Raman�ber laser architecture toproduce a narrow-linewidthduration-tunable picosecondsource at 1120 nm. SHG of
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CLEO®/Europe-EQEC 2015 ⋅ Sunday 21 June 2015
ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2
ing scheme based on theclassically entangled modestructure of radially polarizedbeams of light. By accessingspatial information viapolarization measurements,we experimentally achieveparticle tracking with GHztemporal resolution.EA-1.3 SUN 9:00High-order W-states forrandom number generation�M. Gräfe1, R. Heilmann1,A. Perez-Leija1, R. Keil1,2, F.Dresiow1, M. Heinrich1,3, S.Nolte1, D. Christodoulides3,and A. Szameit1; 1Instituteof Applied Physics, AbbeCenter of Photonics, Friedrich-Schiller-Universität, Jena,Germany; 2Institut für Ex-perimentalphysik, UniversitätInnsbruck, Innsbruck, Austria;3CREOL, University of CentralFlorida, Orlando, UnitedStatesWe experimentally realize thegeneration of high-order pho-ton encoded W-states involv-ing up to 16 optical modes.Morover, we utilize the inher-ent probabilistic properties ofthese multipartite entangledW-states to generate genuinerandom numbers.
EF-1.3 SUN 9:00Controlable Domain Wallsand Antiperiodic Regimes inInjected Lasers with DelayedFeedback�A. Hurtado1, T. Ackemann2,and J. Javaloyes3; 1Instituteof Photonics, University ofStrathclyde, Glasgow, UnitedKingdom; 2Departmentof Physics, University ofStrathclyde, Glasgow, UnitedKingdom; 3Departament deFisica, Universitat de les IllesBaleares, Palma de Mallorca,SpainWe study the stabilization ofdomain walls in time delayedsystems for information pro-cessing. We demonstrate arobust mechanism preventingcoarsening and report the ob-servation of stable domains inan driven semiconductor laserwith feedback.
CH-1.3 SUN 9:00Investigation of thegeometrical depth of focusof focal spots obtained byscattering lenses operatingin the transversal and lateraldirection�S.-M. Reijn1, D. Geskus1,2,and N. Wetter1; 1Instituto dePesquisas Energéticas e Nucle-ares, São Paulo, Brazil; 2RoyalInstitute of Technology, Kista,SwedenWe demonstrate, for the �rsttime, lateral focusing througha Te�on scattering lens. Wealso demonstrate that scatter-ing lenses have a very shortdepth of focus, in addition totheir sub-di�raction focusingcapability.
CC-1.2 SUN 9:00Monte-Carlo Analysis of theNonlinear Susceptibility inQuantum Cascade LaserStructures for THzDi�erence FrequencyGeneration�C. Jirauschek, H. Okeil, andP. Lugli; Technische UniversitätMünchen, Munich, GermanyBased on carrier transportMonte-Carlo simulations, weinvestigate the temperatureand frequency dependence ofthe giant nonlinear suscep-tibility in quantum cascadelaser structures for terahertzdi�erence frequency genera-tion. �e obtained results areconsistent with experiment.
EE-1.3 SUN (Invited) 9:00Two-DimensionalMid-Infrared Spectroscopyin Vibrational LadderV. Kemlin1,2, L. Daniault1,2,T. Vieille1,2, A. Bonvalet1,2,and �M. Jo�re1,2; 1Laboratoired’Optique et Biosciences -Ecole Polytechnique - CNRS,Palaiseau, France; 2INSERMU1182, Palaiseau, FranceWe report on two-dimensional infraredFourier spectroscopy per-formed on a highly-excitednon-equilibrium stateresulting from coherentvibrational ladder climbingin carboxyhemoglobin. �isapproach provides invaluableinformation on populationdistribution and vibrationalrelaxation.
JSI-1.2 SUN 9:00All-SiliconSpherical-Mie-ResonatorPhotodiode With SpectralResponse In�e InfraredRegionM. Garín1, �R. Fenollosa2,3,L. Shi2,3, R. Alcubilla1, and L.Marsal4; 1Dept. d’EnginyeriaElectrònica, UniversitatPolitècnica de Catalunya,Barcelona, Spain; 2UnidadAsociada ICMM/CSIC-UPV,Universidad Politécnica deValencia, Valencia, Spain;3Instituto de Ciencia deMateriales de Madrid (CSIC),Madrid, Spain; 4Dept.d’Enginyeria Electrònica, Elèc-trica i Automàtica, UnviersitatRovira i Virgili, Tarragona,SpainPhotovoltaic cells composedby single silicon microsphereshave been developed. �eirphotocurrent spectra showpeaks corresponding to Mieresonances, that extend theabsorption of light to the nearinfrared, up to 1600 nm ofwavelength.
CI-1.3 SUN (Invited) 9:00Potential solutions toovercome the capacitycrunch�A. Ellis, M. McCarthy, M.Sorokina, N. Mac Suibhne, S.Turitsyn, and S. Sygletos; As-ton University, Birmingham,United KingdomWe will discuss a number ofpotential solutions to enablecontinued growth of commu-nications tra�c, including theuse of conjugation to mitigatenonlinearity in single mode �-bres, optical regeneration, andthe use of spatial multiplexing.
EA-1.4 SUN 9:15Probing Quantum-ClassicalBoundary WithCompression So�wareH.S. Poh1, �P. Kurzynski1, D.Kaszlikowski1,2, S. KoduruJoshi1, A. Cere1, and C.Kurtsiefer1,2; 1Centre forQuantum Technologies,National University of Singa-pore, Singapore, Singapore;2Department of Physics, Na-tional University of Singapore,Singapore, SingaporeBy considering a model con-sisting of data generated bytwo local deterministic uni-versal Turing machines with
EF-1.4 SUN 9:15Topological solitons asaddressable phase bits in adriven laser�B. Garbin1, J. Javaloyes2, G.Tissoni1, and S. Barland1;1Institut Non-linéaire deNice - CNRS, Valbonne,France; 2Universitat de les IllesBaleares, Valldemossa, SpainWe demonstrate the existenceof topological solitons in adriven semiconductor laser inthe excitable regime within afeedback loop. We are able tostore and manipulate them asoptical phase bits for coherentcommunications.
CH-1.4 SUN 9:15Ultrastable XUVInterferometry forBroadband LenslessImaging.�G.M. Jansen1, S. Witte1,2,and K.S. Eikema1,2; 1VUUniversity Amsterdam, Am-sterdam, �e Netherlands;2Advanced Research Center forNanolithography, Amsterdam,�e NetherlandsWe present a table-top setupfor extreme ultraviolet andso�-X-ray broadband lenslessimaging. It employs high-harmonic generation of twocoherent time-delayed ultra-
CC-1.3 SUN 9:15Optical sideband generationwith mid-infrared quantumcascade lasers up to roomtemperature�A. Lebreton1, S. Houver1,M. Renaudat Saint-Jean2,M. Amanti2, C. Sirtori2, L.Li3, E. Lin�eld3, G. Davies3,J. Tignon1, and S. Dhillon1;1Laboratoire Pierre Aigrain,Paris, France; 2LaboratoireMatériaux et PhenomènesQuantiques, Paris, France;3School of Electronic andElectrical Engineering Univer-sity of Leeds, Leeds, UnitedKingdom
JSI-1.3 SUN 9:15Dissipative, chaoticwhispering galleries for lightharvesting�G. Kozyre�1, M. Mariano2,J. Bravo-Abad3, and J.Martorell2,4; 1Universitélibre de Bruxelles (U.L.B.),Brussels, Belgium; 2ICFO-Institut de Ciencies Fo-toniques, Barcelona, Spain;3Universidad Autonomade Madrid, Madrid, Spain;4Universitat Politecnica deCatalunya, Terassa, SpainAn array of silica �bres thatare fused together and cov-ered on one side by an or-
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Switching between di�erentpatterns of light beamstransmitted through theLC embedded woodpilephotonic crystals has beenstudied experimentally andnumerically. ControllingLC phase and incident lightpolarization leads to variationof spatial transmitted pattern.
Greece; 4Dep. of Physics,University of Crete, Heraklion,Greece�e potential of the bulkand surface functionaliza-tion of structures madeby nonlinear lithographyis presented. Speci�cally,it is reported the fabrica-tion of three-dimensionalstructures exhibiting eithermagnetic, conductive orsemi-conductive properties.
Systemes, Pessac, France;4XLIM Institut de Recherche,Université de Limoges, CNRS,Limoges, France; 5ONERA,Palaiseau, FranceAn ultrafast �ber ampli�erbased on an independent-7-core, cladding-pumpedytterbium-doped multicore�ber is demonstrated. Tiledaperture coherent combiningof the cores is carried outusing a spatial light modulatorand SPGD algorithm.
We present a travelling-wave,single-pass SrWO4 Ramanconverter pumped by a3.75-W, 250-kHz repetitionrate, mode-locked hybrid�ber/solid-state laser. 1.4-W,15-ps-long pulses at 1180 nmwere obtained with high slopee�ciency and good beamquality.
this source yields Watt-levelaverage power at 560 nmwith conversion e�cienciesexceeding 45%.
CK-1.5 SUN 9:30Flat Focusing Mirror�Y.C. Cheng1, S. Kicas2,J. Trull1, M. Peckus2,3, C.Cojocaru1, R. Vilaseca1, R.Drazdys2, and K. Staliunas1,4;1Departament de Física i En-ginyeria Nuclear, UniversitatPolitècnica de Catalunya,Terrassa, Spain; 2State Re-search Institute for PhysicalSciences and Technology,Vilnius, Lithuania; 3LaserResearch Center, Departmentof Quantum Electronics,Vilnius University, Vilnius,Lithuania; 4Institucio Cata-lana de Reserca i EstudisAvançats (ICREA), Barcelona,Spain�e �at focusing mirror with-out an optical axis has beendemonstrated experimentallyby a one-dimensionally mul-tilayer structure such as achirped mirror or an opti-mized mirror achieving a longfocal length up to 150 mi-crometers.
EG-1.4 SUN 9:30Molecular Optomechanicswith Plasmons: backactionat the nanoscale�P. Roelli, C. Galland, N. Piro,and T. Kippenberg; Ecole Poly-technique Fédérale de Lau-sanne, Lausanne, SwitzerlandDescribing molecular-plasmonic systems studiedin SERS as optomechanicalcavities, we unravel a hithertooverlooked mechanism: back-action force of the plasmon onthe vibration. Under preciseconditions it could lead tocoherent ampli�cation ofmolecular vibration.
CM-1.4 SUN 9:30Fabrication of Per�uoro-polyether Atomic ForceMicroscopy Tips byTwo-Photon Polymerization�T. Zandrini1, C. De Marco2,R. Suriano2, R. Osellame1,3,S. Turri2, and F. Bragheri3;1Dipartimento di Fisica,Politecnico di Milano, Milano,Italy; 2Dipartimento diChimica, Materiali e Ingeg-neria Chimica Giulio Natta,Politecnico di Milano, Milano,Italy; 3Istituto di Fotonicae Nanotecnologie del CNR,Milano, ItalyWe fabricated Atomic ForceMicroscopy hydrophobictips by Two-Photon Poly-merization on a commercialcantilever using a recentlydeveloped per�uoropolyetherbased photoresist. �ey havebeen tested with indentationmeasurements on PDMSshowing very low adhesionforces.
CJ-1.4 SUN 9:30Phase modulators andsplitting network on Si PICfor coherent �ber beamcombiningM. Antier1,2, J.Bourderionnet1, C. Larat1,E. Lallier1, C. Scarcella3,J. Su Lee3, P. O’Brien3, T.Spuesens4, G. Lepage5, P.Verheyen5, P. Absil5, and �A.Brignon1; 1�ales Research &Technology, Palaiseau, France;2�ales Optronique SA,Elancourt, France; 3TyndallNational Institute, Cork,Republic of Ireland; 4GhentUniversity-IMEC, Ghent,Belgium; 5IMEC, Leuven,BelgiumA Silicon on insulator chipwith 1-to-16 splitting networkand phase modulators array isused as a key component forcoherent �ber beam combin-ing architecture. A 2π phaseshi� is achieved for 22mWelectrical power.
CA-1.5 SUN 9:30Beam Combining Strategiesfor Raman Power Ampli�ersutilizing Low BirefringenceDiamond�A. McKay, D. Coutts, D.Spence, and R. Mildren;Macquarie University, Sydney,AustraliaWe report a non-collinearbeam combiner based onstimulated Raman scatteringin single-crystal diamond,which at kilowatt peak powersdemonstrates more than 70%power conversion of three1064-nm beams into a single1240-nm Stokes beam.
CE-1.5 SUN 9:30Dual-wavelengthhollow-core NegativeCurvature Fibre for thedelivery of high energy shortand ultrashort pulsed laserlight�P. Jaworski1, F. Yu2, R.M.Carter1, J.C. Knight2, J.D.Shephard1, and D.P. Hand1;1Applied Optics and PhotonicsGroup, Institute of Photonicsand Quantum Sciences,Heriot-Watt University,Edinburgh, United Kingdom;2Centre for Photonics andPhotonic Materials, Depart-ment of Physics, University ofBath, Bath, United KingdomA low loss dual band NegativeCurvature Fibre capable of de-livering short pulse, high en-ergy, and high average powerlaser pulses is demonstrated.Results are presented for de-livered NIR and green laserpulses.
CD-1.5 SUN 9:30Multi-octave Mid-infraredSupercontinuumGenerationin a Small-core Step-indexChalcogenide Fiber�Y. Yu1, B. Zhang2, X. Gai1,C. Zhai2, S. Qi2, W. Guo2,Z. Yang1,2, R. Wang1, D.-y. Choi1, S. Madden1, andB. Luther-Davies1; 1CUDOS,Laser Physics Centre, ResearchSchool of Physics and Engineer-ing, Australian National Uni-versity, Canberra, Australia;2Jiangsu key Lab. of Ad-vanced Laser Materials andDevices, School of Physics andElectronic Engineering, JiangsuNormal University, Xuzhou,China, People’s Republic of(PRC)By pumping a chalcogenidestep-index �ber at 4 microme-ter, supercontinuum spanningfrom 1.5 to 10 micrometerwas generated, which to ourknowledge, is the furthest intothe mid-infrared generated inchalcogenides with low powerthreshold.
CK-1.6 SUN 9:45Harnessing guided moderesonances in aone-dimensional grating forgraphene-based absorbersM. Grande1, �M.A. Vincenti2,T. Stomeo3, G.V. Bianco4, D.de Ceglia2, N. Akozbek5, V.Petruzzelli1, G. Bruno4, M. De
EG-1.5 SUN 9:45Generalized bidimensionalbackaction innano-optomechanics�A. Gloppe, E. Dupont-Ferrier,L. Mercier De Lépinay, B.Pigeau, and O. Arcizet; In-stitut Néel, Université Greno-ble Alpes - CNRS:UPR2940,
CM-1.5 SUN 9:45Advances of Additive LaserBased Micro-ManufacturingTechnologies for CartilageTissue Engineering: aPre-Clinical StudyS. Rekstyte1, S. Butkus1, E.Skliutas1, S. Juodkazis2,3, and�M. Malinauskas1; 1Vilnius
CJ-1.5 SUN 9:45Combining E�ciencyLimitation in PassivelyPhase-locked Laser Arrays�D. Kabeya1,2, V. Kermène1,A. Desfarges-Berthelemot1, A.Tonello1, and A. Barthélémy1;1Xlim Institut de RechercheUMR 7252, Université de
CA-1.6 SUN 9:45Polarization Conversion inDiamond Raman Lasers�A. McKay and R. Mildren;Macquarie University, Sydney,AustraliaA diamond Raman laser thato�ers wavelength, beam-quality and polarization
CE-1.6 SUN 9:45Supermode interferenceanalysis as an e�ectivemethod of crosstalkexamination in multicore�bers�L. Szostkiewicz2, A.Ziolowicz2, M. Szymanski1, T.Tenderenda1, M. Napierala1,3,
CD-1.6 SUN 9:452 Microns All-FiberPicosecond Pulse Sourcewith Gigahertz RepetitionRate�A. Billat, S. Cordette, and C.-S. Brès; Ecole PolytechniqueFederale de Lausanne (EPFL),Lausanne, Switzerland
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correlated inputs, we deriveand experimentally violate aninequality based on the con-cept of Normalised Compres-sion Distance.
fast laser pulses with attosec-ond time resolution, by usingbirefringent wedges.
We demonstrate di�erencefrequency generation betweena Near Infrared beam anda Mid-Infrared QuantumCascade Laser up to roomtemperature. Second ordernonlinear susceptibility isexalted thanks to resonantexcitation of the NIR pump.
ganic solar cell is studied the-oretically and experimentally.Light harvesting approachesand sometimes surpasses theperformance of random inter-faces.
EA-1.5 SUN 9:30Synchronization of SinglePhotons and OpticalHomodyne Tomography�K. Makino1, Y. Hashimoto1,J.-i. Yoshikawa1, H. Ohdan1,P. van Loock2, and A.Furusawa1; 1Department ofApplied Physics, School ofEngineering, �e University ofTokyo, Tokyo, Japan; 2Instituteof Physics, Staudingerweg7, Johannes Gutenberg-Universität Mainz, Mainz,GermanyWe experimentally demon-strate Hong-Ou-Mandelinterference of highly puresingle photons synchronizedby two individual all-opticalquantum memories forvarious maximum waitingtimes. We also show four-leaf-clover-shaped correlation ofthe state revealed with opticalhomodyne tomography.
EF-1.5 SUN 9:30Spontaneous generation andsplitting of laser cavitysolitons pinned by defectsJ. Jimenez, T. Ackemann, W.Firth, and �G.-L. Oppo; Uni-versity of Strathclyde, Glasgow,United KingdomExperimental and theoreticalevidence of spontaneousappearance of laser cavitysolitons in VCSELs withfrequency selective feedbackwhen increasing the injectioncurrent is provided. �esingle peak of the solitonssometimes splits into two.
CH-1.5 SUN (Invited) 9:30New Directions inOptomechanics: Micro�uidcOptomechancis andLevitating Optomechancis�T. Carmon; Technion - IsraelInstitute of Technology, Haifa,IsraelWe let light propagate tens ofmeters while circulating in amicro�uidic device. Mechan-ical vibrations are excited bythe pressure of light. Soundfrequencies above 10 GHz arepossible which might impacton bio-sensing.
CC-1.4 SUN 9:30Novel Photonic Concepts forTHz QCLs: Random Lasers�S. Schoenhuber1,2, C.Deutsch1,2, M. Brandstetter1,2,M. Krall1,2, H. Detz2,3, A.M.Andrews2,3, W. Schrenk2,3,G. Strasser2,3, and K.Unterrainer1,2; 1PhotonicsInstitute, Vienna Univer-sity of Technology, Vienna,Austria; 2Center for Micro-and Nanostructures, ViennaUniversity of Technology,Vienna, Austria; 3Institute ofSolid-State Electronics, ViennaUniversity of Technology,Vienna, AustriaTHz emission from electri-cally pumped random quan-tum cascade laser cavities isreported. �e devices are fab-ricated by etching a randomhole pattern into planar dou-ble metal waveguides. �e de-vices show a broadband sur-face emission with a narrowfar �eld pattern.
EE-1.4 SUN 9:30Tracing molecular dynamicsat the 1-femtosecond scalethrough XUV pump-probespectroscopyP. Carpeggiani1,2, A.Palacios3, F. Martin3, D.Charalambidis1,2, and �P.Tzallas1; 1Institute of Elec-tronic Structure and Laser(IESL), Heraklion, Greece;2Dep. of Physics, Univer-sity of Crete, Heraklion,Greece; 3Instituto Madrileñode Estudios Avanzados enNanociencia (IMDEA-Nano-ciencia), Madrid, SpainWe demonstrate the feasibilityof performing XUV-pump-XUV-probe studies ofmolecules in 1-fs time scale.�e intrinsic dynamics ofH2 has been measured usingintense XUV radiation whichcan support isolated pulses of600 asec duration.
JSI-1.4 SUN 9:30Random scatterers by designfor record e�ciency inplastic dye-sensitized solarcells�S. Carretero-Palacios1, Y.Li1, K. Yoo2, H. Míguez1, andM.J. Ko2; 1MultifunctionalOptical Materials Group,Instituto de Ciencia de Ma-teriales de Sevilla, ConsejoSuperior de InvestigacionesCientí�cas-Universidad deSevilla, Américo Vespucio49, 41092, Seville, Spain;2Photo-Electronic HybridsResearch Center, NationalAgenda Research Division,Korea Institute of Science andTechnoloy (KIST), 136-791,Seoul, Korea, SouthWe report on record e�ciencyin plastic dye-sensitized solarcells of 8.6% obtained experi-mentally, supported by a the-oretical model in which lightscatterers are randomly dis-persed in the active layer.
CI-1.4 SUN 9:30Bend InsensitiveHole-assisted MulticoreFibre For Next GenerationTransmission Systems�A. Ziolowicz1,3, M. Szy-manski2, L. Ostrowski2, M.Napierala1,4, K. Poturaj5,M. Makara1, P. Mergo5, andT. Nasilowski1; 1InPhoTech,Ltd, Warsaw, Poland; 2PolishCentre For Photonics and FibreOptics, Rogoznica, Poland;3Faculty of Physics, WarsawUniversity of Technology,Warsaw, Poland; 4Institute ofApplied Physics, Military Uni-versity of Technology, Warsaw,Poland; 5Faculty of Chemistry,Maria Curie-SklodowskaUniversity, Lublin, PolandWe present a novel 7-corehole-assisted �bre, character-ized by negligible crosstalkand bend insensitiveness. �e�bre is fully compliant withsingle mode �bre standards,hence can be e�ectively uti-lized in space division multi-plexed transmission systems.
EA-1.6 SUN 9:45Manipulating the temporalcorrelations of two-photonstates through the spatialdegree of freedom�A. Büse1,2, N. Tischler1,2,L.G. Helt1,3, M.L. Juan1,2,M.J. Steel1,3, and G. Molina-Terriza1,2; 1Department
EF-1.6 SUN 9:45Activation of localizedstructures in broad areaVCSELs using electro-opticfunnel waveguides�R. Martínez-Lorente1, J.Parrivicini2, M. Brambilla3,4,L. Columbo3,4, F. Pratti5,6,C. Rizza5,7, G. Tissoni8,
CC-1.5 SUN 9:45Terahertz Quantum CascadeLasers: from Conventionalto Novel Designs�T. Grange; Institut Néel,Grenoble, FranceCalculations of transport andgain in terahertz quantumcascade lasers using the
EE-1.5 SUN 9:45Table-top NEXFASspectroscopy at the carbonK-edge using so� X-rayharmonics generated fromsub-2-cycle, 1.85-�m 1-kHzlaser pulses�S. Cousin1, F. Silva1, S.Teichmann1, M. Hemmer1,
JSI-1.5 SUN 9:45Absorption enhancement inmonocrystalline Si thin�lms using pseudodis-ordered structures�L. Lalouat1, H. Ding1,B. Gonzalez-Acevedo1, A.Harouri1, R. Orobtchouk1, V.Depauw2, C. Seassal1, and
CI-1.5 SUN 9:45Femtosecond laser writtenintegrated passivemode-multiplexers�S. Gross1, N. Riesen2, J.D.Love3, and M.J. Withford1;1Centre for Ultrahigh band-width Devices for OpticalSystems (CUDOS), MQ
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Vittorio3,6, M. Scalora7, andA. D’Orazio1; 1Dipartimentodi Ingegneria Elettrica edell’Informazione, Politecnicodi Bari, Bari, Italy; 2NationalResearch Council, CharlesM. Bowden Research Center,RDECOM, Redstone Arsenal,United States; 3Center for Bio-Molecular Nanotechnologies,Istituto Italiano di Tecnologia(IIT), Lecce, Italy; 4Institute ofInorganic Methodologies andof Plasmas, IMIP-CNR, Bari,Italy; 5AEgis TechnologiesInc, Huntsville, United States;6National NanotechnologyLaboratory (NNL), CNR-Istituto Nanoscienze, Dip.Ingegneria dell’Innovazione,Università Del Salento, Lecce,Italy; 7Charles M. BowdenResearch Center, RDECOM,Redstone Arsenal, UnitedStatesWe theoretically and exper-imentally demonstrate thatguided-mode resonances,excited in one-dimensionalgratings, are able to stronglyenhance the graphene absorp-tion. We also investigate theiroptical behaviour in termsof polarization and angulardependence.
Grenoble, FranceWe generalize the bidimen-sional backaction experiencedby a nanowire in a stronglyfocused beam of light to thecases where the vectorial force�eld is partially delayed, al-lowing a selective cooling ofits mechanical modes.
University, Vilnius, Lithuania;2Swinburne University ofTechnology, Melbourne, Aus-tralia; 3Melbourne Centre forNanofabrication, Melbourne,AustraliaWe present advances inultrashort pulse laser basedmicro-manufacturing of syn-thetic polymer 3D sca�oldsserving as custom-shapedtemplates and their biocom-patibility studies in vitro forcell behavior and as long termbiomedical implants in vivo.
Limoges-CNRS, Limoges,France; 2CILAS, Orléans,FrancePassive phase-locking of laserarray is less e�cient far abovelaser threshold. A simple ana-lytical model and experimentson a dual-arm laser highlightthat some combining lossesoriginate from spectral �lter-ing occurring in coupled cavi-ties.
conversion in a simple com-pact device is investigated.Polarization extinction ratioof 24 dB with near quantumlimited conversion from anunpolarized beam is shown.
P. Mergo4, and T. Nasilowski1;1InPhoTech, Ltd, Warsaw,Poland; 2Polish Centre ForPhotonics and Fibre Optics,Rogoznica, Poland; 3Instituteof Applied Physics, MilitaryUniversity of Technology,Warsaw, Poland; 4Laboratoryof Optical Fibre Technology,Faculty of Chemistry, MariaCurie-Sklodowska University,Lublin, PolandWepropose a new approach tointerpret crosstalk phenom-ena in multicore �bers basedon supermode interference.�e method is suitable forcomplex �ber designs such asphotonic crystal �bers withlarge number of cores.
We report an all-�bre picosec-ond pulsed source tunableover 50nm around 1950nmand featuring a repetition-rate selectable in the GHzrange. It relies on a pulsed-pump parametric converterand subsequent ampli�cationin a thulium-doped �bre.
10:30 – 12:00CK-2: Single-emitterand NanovolumePhotonicsChair: Tapio Niemi, TampereUniversity of Technology, Tam-pere, Finland
10:30 – 12:00EG-2: Light-matterInteraction with2D-SystemChair: Valentina Parigi, ES-PCI, Paris, France
10:30 – 12:00CM-2: Laser Nanopro-cessingChair: Peter Kazansky, Uni-versity of Southampton, UnitedKingdom
10:30 – 12:00CJ-2: Mode-locked FibreOscillatorsChair: Claude Aguergaray, In-stitut d’Optique d’Aquitaine,Talence, France
10:30 – 12:00CA-2: Ultrashort PulseOscillators and Ampli-�ers in DisorderedSolid-state MediaChair: Valentin Petrov, MaxBorn Institute, Berlin, Ger-many
10:30 – 12:00CE-2: Fabrication ofPhotonic Structures andComponentsChair: Patrice Camy, Univer-sity of Caen, Caen, France
10:30 – 12:00CD-2: Photonics andQPMChair: Ventsislav Valev, Uni-versity of Bath, Bath, UnitedKingdom
CK-2.1 SUN (Keynote) 10:30Single-Molecule UltrafastPhotonics�N.F. van Hulst; ICFO - theInstitute of Photonic Sciences,Castelldefels - Barcelona,Spain; ICREA -InstitucióCatalana de Recerca i EstudisAvançats, Barcelona, Spain
EG-2.1 SUN 10:30Plasmono-atomic 2DMeta-material�E.A. Chan1, S.A. Aljunid1,G. Adamo1, M. Ducloy1,2,D. Wilkowski1,3,4, and N.Zheludev1,5; 1Centre for Dis-ruptive Photonic Technologies,Nanyang Technological Univ.,
CM-2.1 SUN (Invited) 10:30Laser printing of nanopar-ticles�B. Chichkov; Laser ZentrumHannover e.V., Hannover, Ger-manyOur recent progress in laserprinting of nanoparticles willbe reported.
CJ-2.1 SUN 10:30Fiber laser mode lockedthrough an evolutionaryalgorithm�U. Andral, R. Si Fodil, F.Amrani, F. Billard, E. Hertz,and P. Grelu; Lab. ICBUMR 6303 CNRS, Universitéde Bourgogne, Dijon, France
CA-2.1 SUN (Invited) 10:30Ultrafast Solid-StateOscillators and High-PowerAmpli�ers Based onBroadband, MultisiteYb-doped CrystalsF. Pirzio1, E. Caracciolo1,2,S.D. Di Dio Ca�so1,2, M.Kemnitzer2, A. Guandalini2,
CE-2.1 SUN 10:30High-Q Printable PolymerMicrodisk without Etching�S. Ryu1, H. Yoshioka1, C.Chen1, K. Yasui2, and Y. Oki1;1Department of Electronics,Kyushu University, Fukuoka,Japan; 2NISSAN CHEMICALINDUSTRIES, LTD, Chiba,
CD-2.1 SUN (Invited) 10:30From Optical Sun�owers toOptical Tornados LightPropagation in ComplexNonlinear Photonic Lattices�C. Denz, F. Diebel, M. Bogus-lawski, and P. Rose; Instituteof Applied Physics and Centerfor Nonlinear Science (CeNoS),
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of Physics & Astronomy,Macquarie University, Sydney,Australia; 2ARC Centre ofExcellence for EngineeredQuantum Systems, MacquarieUniversity, Sydney, Australia;3ARC Centre of Excellence forUltrahigh bandwidth Devicesfor Optical Systems, Sydney,AustraliaWe present a novel andsimple scheme to reconstructthe complex spectral wave-function of collinear typeII spontaneuos parametricdown-conversion. �eapproach is based on Hong-Ou-Mandel interference inthe spectral and temporaldomain.
A.J. Agranat9, and E. DelRe2; 1Departamento deOptica, Universitat de Va-lencia, Valencia, Spain;2Dipartimento di Fisica andIPCF-CNR, ”Sapienza” Uni-versitá di Roma, Rome, Italy;3Dipartimento Interateneo diFisica, Universitá e Politecnicodi Bari, Bari, Italy; 4CNR-IFN,Bari, Italy; 5Dipartimento diScienza & Alta Tecnologia,Universitá dell’Insubria,Como, Italy; 6CNISM, Re-search Unit of Como, Como,Italy; 7CNR-SPIN, CoppitoL’Aquila, L’Aquila, Italy;8INLN, CNRS, Universitéde Nice Sophia Antipolis,Valbonne, France; 9AppliedPhysics Department, HebrewUniversity of Jerusalem,Jerusalem, IsraelWe demonstrate experimen-tally the electro-activationof a localized optical struc-ture in a coherently drivenbroad-area VCSEL operatedbelow threshold. Control isachieved by electro-opticallysteering and changing thephase of a writing beamthrough a preprogrammablephotorefractive funnelwaveguide.
formalism of non-equilibriumGreen’s functions are re-ported. �e role of impurityscattering is fully analysed.Novel THz QCLs designsbased on nanowires areproposed.
B. Buades1, and J. Biegert1,2;1ICFO - �e Institute ofPhotonic Sciences, Castellefels(Barcelona), Spain; 2ICREA -Institucio Catalana de Recercai Estudis Avancats, Barcelona,SpainBright water-window highharmonics are generated by1.85um, sub-2-cycle, CEPstable laser pulses. �eyare used to identify X-rayabsorption �ne structure of apolyamide foil.
E. Drouard1; 1Institut desNanotechnologies de Lyon,Lyon, France; 2IMEC, Leuven,BelgiumRe�ectance measurements onpatterned 1 micron thick Silayer bonded with Al on glassshow an enhancement of theoverall absorption by usingslightly pseudodisordered lat-tices of cylindrical holes com-pared to the optimized squarelattice.
Photonics Research Centre,Department of Physics andAstronomy, Macquarie Uni-versity, Sydney, Australia;2Institute for Photonics andAdvanced Sensing (IPAS)and School of Chemistry andPhysics, �e University ofAdelaide, Adelaide, Australia;3Research School of Physicsand Engineering, �e Aus-tralian National University,Canberra, AustraliaWe present femtosecondlaser written 3D integratedmode-multiplexers formode-division multiplexedoptical communicationnetworks. �e devices arebased on tapered velocity andmode-selective directionalcouplers. �ey feature lowlosses, high coupling andmode-extinction ratios.
10:30 – 12:00EA-2: Atoms andPhotonsChair: Jürgen Eschner, Uni-versität der Saarlandes, Saar-brücken, Germany
10:30 – 12:00EF-2: Symmetry Break-ing, Photon Fluids andStructured MaterialsChair: Julien Javaloyes, Uni-versitat de les Illes Baleares,Palma, Spain
10:30 – 12:00CH-2: New PhotonicSensor TechnologiesChair: Marian Marciniak, Na-tional Institute of Telecommns,Warsaw, Poland
10:30 – 12:00CC-2: THz QuantumCascade Laser IIChair: Mikhail Belkin, Univer-sity of Texas, Austin, USA
10:30 – 12:00EE-2: Filamentation andIntense Light MatterInteractionChair: John Travers, MaxPlanck Institute for the Scienceof Light, Erlangen, Germany
10:30 – 12:00JSI-2: LightManagement in�in-�lm Solar CellsChair: Jordi Martorell, ICFO,Barcelona, Spain
10:30 – 12:00CI-2: Ultra HighBit-rate and Short-reachTransmissionChair: Atsushi Kanno, NICT,Tokyo, Japan
EA-2.1 SUN 10:30Single-Photon TransistorBased on Rydberg Blockade�D. Tiarks, S. Baur, K.Schneider, S. Dürr, and G.Rempe; Max-Planck-Institutfür Quantenoptik, Garching,GermanyWe demonstrate an all-optical
EF-2.1 SUN 10:30Experimental characterisa-tion of nonlocal photon�uids�D. Vocke1, T. Roger1, F.Marino2, E. Wright3, I.Carusotto4, and D. Faccio1;1Heriot Watt University,Edinburgh, United Kingdom;
CH-2.1 SUN 10:30Characterization of the an-gular and polarization de-pendence of a room-temper-ature predictable quantume�cient detector (RT-PQED)�K. Sal�ner, S. Nevas, and P.Schneider; Physikalisch Tech-nische Bundesanstalt, Braun-
CC-2.1 SUN 10:30Towards octave-spanningTHz frequency combs�M. Rösch, G. Scalari, M. Beck,and J. Faist; ETH Zürich, In-stitute of Quantum Electronics,Zürich, SwitzerlandWe present a possible methodto achieve octave-spanning
EE-2.1 SUN (Invited) 10:30Air Waveguides fromFemtosecond FilamentsE. Rosenthal, N. Jhajj, J.Palastro, S. Zahedpour, J.Wahlstrand, and �H. Milch-berg; Institute for Researchin Electronics and AppliedPhysics, University of Mary-
JSI-2.1 SUN (Invited) 10:30Light management and lightmanipulation technologiesfor thin �lm photovoltaicsapplications�C.J. Brabec1,2, M. Bat-entschuk1, and K. Forberich1;1Friedrich-Alexander Uni-versity Erlangen-Nurnberg,
CI-2.1 SUN 10:30Linewidth Limits for Wave-length Converting 64-QAMSignals Using FWM�S.T. Naimi, S.P.Ó. Dúill, andL.P. Barry; the Rince Institute,Department of Electronic En-gineering, Dublin City Univer-sity, Dublin, Republic of Ire-
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b
Resonant optical nanoanten-nas and phase shaped fs pulsesare used to control individ-ual quantum emitters on thenanoscale. �is way e�-cient ultrafast coherent energytransfer is revealed in indi-vidual bacterial antenna com-plexes at physiological condi-tions.
Singapore; 2Univ. Paris 13,Laboratoire de Physique desLasers, CNRS, Villetaneuse,France; 3Centre for QuantumTechnologies, National Univ.of Singapore, Singapore;4Merlion MajuLab, CNRS-UNS-NUS-NTU InternationalJoint Research Unit UMI,Singapore; 5OptoelectronicsResearch Centre & Centre forPhotonic Metamaterials, Univ.of Southampton, Southamp-ton, United KingdomWe report on a new type oftwo-dimensional materialsystem of sub-wavelengththickness, a plasmonic meta-surface in atomic gas. Suchplasmono-atomic metama-terial has unique propertiesunderpinned by interactionsin the near�eld layer of thenanostructure.
We experimentally demon-strate the ability of anevolutionary algorithm to�nd cavity parameters forself-starting mode locking ofa �ber laser. According to theobjective function used foroptimization, various pulsedregimes are obtained.
F. Kienle2, S. Veronesi3, M.Tonelli3, J. Aus der Au2,and �A. Agnesi1; 1Universitàdi Pavia, Dipartimento diIngegneria Industriale edell’Informazione, Pavia,Italy; 2Spectra Physics,Rankweil, Austria; 3NESTIstituto Nanoscienze-CNRand Dipartimento di Fisica,Università di Pisa, Pisa, ItalyWe performed a comparativestudy on several di�erentmultisite Ytterbium-dopedcrystals. Sub 50-fs pulsegeneration in e�cientand optimized low-powersingle-mode diode-pumpedoscillators and pulse energyup-scaling in regenerativepower ampli�er will bepresented.
JapanWe demonstrated a lasingbased cavity high-Q factorfrom non-etched ink-jetprinted microdisks by thecavity-ring down method.�e obtained Q-factor of 15million is acceptable as high-Q factor in the microdiskcategory.
Münster, GermanyWe introduce a paradigm shi�in optical lattice design usingnondi�racting Bessel beamsas basic entities to approxi-mate aperiodic structures. Weshow its �exibility by opticallyinducing Vogel spiral latticesmimicing spiral plants as sun-�owers.
EG-2.2 SUN 10:45Highly E�cient Wave Mani-pulation with All-DielectricHuygens’ Surfaces�M. Decker1, I. Staude1,M. Falkner2, K. Chong1, J.Dominguez3, D. Neshev1, I.Brener3, T. Pertsch2, and Y.Kivshar1; 1Nonlinear PhysicsCentre, Australian NationalUniv., Canberra, Australia;2Institute of Applied Physics,Abbe Center of Photonics,Friedrich-Schiller-Univ. Jena,Jena, Germany; 3Center forIntegrated Nanotechnologies,Sandia National Laboratories,Albuquerque, United StatesWe experimentally demon-strate all-dielectric Huygens’surfaces providing 2πtransmission-phase coveragewith record transmissione�ciencies > 55% at near-IRwavelengths. We demonstratethat e�ciencies close to 100%can be achieved and exploreapplications of our newconcept.
CJ-2.2 SUN 10:45All-�ber laser based on NPEin PM �ber with two activesections�S. Boivinet1,2, J.-B. Lecourt1,Y. Hernandez1, A. Fotiadi2,M. Wuilpart2, and P. Mégret2;1Mutitel ASBL, AppliedPhotonics Department, Mons,Belgium; 2Electromagnetismand TelecommunicationDepartment, Faculty of Engi-neering, University of Mons,Mons, BelgiumAn all-�ber mode-lockedlaser with two active sectionsis demonstrated. It is basedon non-linear polarizationrotation in PM �ber andit delivers 2.5ps pulses at arepetition rate of 3.2 MHz.
CE-2.2 SUN 10:453D nanophotonic materialsmade with a single step etchmask on inclined planes�D. Grishina1, C. Harteveld1,J. Perez-Vizcaino1,2, L.Woldering3, and W. Vos1;1Complex Photonic Systems(COPS), MESA+ Instutute forNanotechnology, University ofTwente, Enschede,�e Nether-lands; 2University Jaume I,Castellon, Spain; 3TransducersScience and Technology(TST), MESA+ Instutute forNanotechnology, Universityof Twente, Enschede, �eNetherlandsWe developed a 3D nanofabri-cation method to fabricate 3Dnanostructures on inclinedplanes with a single step etchmask with ensured alignment.We demonstrate our tech-nique by realizing functionalsilicon 3D photonic band gapcrystals.
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transistor in which a lightpulse with only one photonswitches the transmission ofa second light pulse. �edevice is based on electro-magnetically induced trans-parency with Rydberg states.
2CNR-Istituto Nazionaledi Ottica, Florence, Italy;3College of Optical Sciences,University of Arizona, Tucson,United States; 4INO-CNR BECCenter and Dipartimento diFisica, Universita di Trento,Trento, ItalyWe report two novel exper-imental techniques inspiredby a quantum �uid hydrody-namic analogy for completelycharacterising nonlocal defo-cusing nonlinear media. �etechniques measure the non-linearity, nonlocal lengths andthe e�ective phonon-like dis-persion curves.
schweig, GermanyWe report on angular andpolarization dependencemeasurements of a room-temperature predictablequantum e�cient detector,which is intended to measureoptical power with 100 ppmuncertainty and shall beused as novel-type primarystandard.
THz frequency combs usingTHz QCL by implementingdouble-chirped mirrors tocompensate for the laser’s dis-persion. Additionally, a laserwith increased bandwidth of1.94 THz is shown.
land, College Park, UnitedStatesFemtosecond pulses propa-gating as long range �lamentsin air are nonlinearly ab-sorbed to generate extremelylong-lived guiding structuresfor high peak and averagepower laser pulses. Gen-eration and use of thesestructures is reviewed.
i-MEET, Erlangen, Germany;2ZAE Bayern e.V, Erlangen,Germany�is presentation will give in-sight into recent light man-agement and light manipu-lation technologies with spe-cial relevance for thin �lm3rd generation PV technolo-gies, like organic-, hybrid- orperovskite-type solar cells.
landWe demonstrate wavelengthconversion of 64-QAMSignals using FWM in aSOA. �e required pumplaser linewidths to achievespeci�c system bit error rateperformance at the forwarderror correction threshold arecalculated.
EA-2.2 SUN 10:45Coupling, controlling, andprocessing non-transversalphotons with a single atom�J. Volz, M. Scheucher, C.Junge, E.Will, A. Hilico, andA.Rauschenbeutel; Vienna Cen-ter for Quantum Science andTechnology, TU-Wien, Atom-institut, Vienna, AustriaWe demonstrate a �ber-integrated optical Kerr-nonlinearity where a singleatom imprints the maximumnonlinear phase shi� of pibetween the one and twophoton case. We employ thisto generate entanglement be-tween previously independentphotons.
EF-2.2 SUN 10:45Universal synchronizationproperties of drivenoscillators across a Hopfinstability�M. Romanelli, M. Brunel, L.Wang, and M. Vallet; Institutde Physique de Rennes, Rennes,FranceWe measure the phase noisespectra of a self-injecteddual-frequency laser in thebounded phase regime, and�nd the same spectral purityas in the phase-lockingregime. We show that thisbehavior is universal.
CH-2.2 SUN 10:45Orbital angular momentumand topological charge inshaped optical vortex beamsA. Amaral, �E. Falcao-Filho,and C. de Araujo; Depar-tamento de Fisica, Universi-dade Federal de Pernambuco,Recife-PE, Brazil�is work describes how theorbital angular momentum(OAM) and the topologicalcharge (TC) can be measuredin beams with arbitrarilyshaped vortices cores. Var-ious scenarios are analyzedwhere OAM and TC aredistinguished quantities.
CC-2.2 SUN 10:45Coherence properties ofultra-broadband terahertzquantum cascade lasers�L. Hua1, P. La�aille1, D.Gacemi1, C. Sirtori1, S.Barbieri1, J. Leonardon2, G.Santarelli2, M. Roesch3, G.Scalari3, M. Beck3, J. Faist3, W.Hänsel4, and R. Holzwarth4;11.*Université Paris-Diderotand CNRS, Paris, France;22.*Laboratoire LP2N, CNRS,Bordeaux, France; 33.*ETHZurich, Zurich, Switzerland;44.*Menlo Systems GmbH,Munich, GermanyWe investigate the coherenceproperties of ultra-broadbandterahertz quantum cascadelasers using electro-opticsampling. �is high spectralresolution technique allowsto directly correlate thephase-noise in the roundtripspectrum with the frequencyjitter of the Fabry-Perotmodes.
CI-2.2 SUN 10:4590-GHz OFDM-16QAMSignal Transmission overIF-over-Fiber Link�A. Kanno, P. Tien Dat, and T.Kawanishi; National Instituteof Information and Commu-nications Technology, Koganei,JapanWe demonstrate 90-GHzOFDM signal transmissionover an intermediate-frequency over �ber link.Spectral e�cient signalin both optical and radiodomains will realize e�ectivesignal distribution networkto a huge number of remotesites.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14bEG-2.3 SUN 11:00Light-matter Interactions ina Polarization StandingWave�X. Fang1, K.F. MacDonald1,and N.I. Zheludev1,2;1University of Southamp-ton, Southampton, UnitedKingdom; 2Nanyang Techno-logical Universtiy, Singapore,SingaporeWe demonstrate experimen-tally that polarization, asopposed to intensity, standingwaves can be harnessed to co-herently control light-matterinteractions in photonicmetamaterials, opening upunique opportunities forall-optical data processingand polarization-dependentmolecular spectroscopy.
CM-2.2 SUN 11:00Assessment of Nanoparticlesin Femtosecond LaserAblation Plasmas of Metalsby Optical HarmonicGenerationM. Oujja1, J.G. González2,L. Bañares2, R. de Nalda1,and �M. Castillejo1; 1Institutode Química Física Ro-casolano, CSIC, Serrano119, 28006 Madrid, Spain;2Departamento de QuímicaFísica, Facultad de CienciasQuímicas (Unidad AsociadaI+D+i al CSIC), UniversidadComplutense de Madrid,28040 Madrid, SpainOptical low-order harmonicgeneration is presented as amethod for assessing fem-tosecond laser ablation plas-mas. For metallic targets,this provides information onthe plume nanoparticle popu-lation and its dependence withlaser ablation parameters.
CJ-2.3 SUN 11:00Spectral Sculpting a FiberLaser via Intracavity SpatialLight Modulator�R. Iegorov1 and O. Ilday1,2;1Department of Physics,Bilkent University, Ankara,Turkey; 2Department ofElectrical Engineering, BilkentUniversity, Ankara, TurkeyWe introduce a spatial lightmodulator inside of a mode-locked �ber laser cavity tooptimize performance viacon�gurable spectral �lteringachieving up to 50% increasein bandwidth, for the �rsttime to our knowledge.
CA-2.2 SUN 11:00Sub-100 fs mode-lockedlaser operation of newdisordered Yb :KInY(WO4)2 crystal�E. Castellano-Hernandez1, X.Han1, M. Rico2, C. Cascales1,and C. Zaldo1; 1Institutode Ciencia de Materiales deMadrid. Consejo Superior deInvestigaciones Cientí�cas,Madrid, Spain; 2Centro deLáseres Pulsados UltracortosUltraintensos, Salamanca,SpainWe present current status ofthe �rst Indium-modi�edYb:KY(WO4)2 pulsed laseroperation. We have obtainedsub-100 fs pulses directlyfrom a SESAM modelockedlaser based on this disordereddouble tungstate with 1.3 nJpulse energies.
CE-2.3 SUN 11:00Small-spot UV-writtenApodised Fibre BraggGratings at 780 nm�R.H.S. Bannerman, J.C.Gates, C. Holmes, P.L. Men-nea, C. Sima, and P.G.R.Smith; Optoelectronics Re-search Centre, University ofSouthampton, Southampton,United KingdomWe shall present a �exibletechnique for fabricating �-bre Bragg gratings for usearound 780nm. �e ap-proach uses small-spot UV-writing and a capillary guideto achieve highly apodised,chirped gratings with a widetuning range.
CD-2.2 SUN 11:00Maximizing the guidedsecond-harmonic in lithiumniobate nanowires�A. Sergeyev1, R. Geiss2, A.S.Solntsev3, A.A. Sukhorukov3,F. Schrempel2, T. Pertsch2,and R. Grange1; 1OpticalNanomaterial Group, Institutefor Quantum Electronics,Department of Physics, ETHZurich, Zurich, Switzer-land; 2Institute of AppliedPhysics, Abbe Center ofPhotonics, Friedrich SchillerUniversity, Jena, Germany;3Nonlinear Physics Center,Research School of Physicsand Engineering, AustralianNational University, Canberra,AustraliaWe demonstrate en-hancement of the guidedsecond-harmonic signal inlithium niobate nanowires.We increase the SH by a factorof 48 using phase-matchingand by a factor of 9.3 usinglength optimization.
CK-2.2 SUN 11:15Towards an Integrated LocalSpin Magnetometer:Nanomagnetometry onSingle Diamond NV-centersin Laser Written Structures�B. Sontheimer1, Q. Shi2,A.W. Schell1, M. Wegener2,and O. Benson1; 1Humboldt-Universität zu Berlin, Institutfür Physik, AG Nanooptik,Berlin, Germany; 2KarlsruherInstitut für Technologie, Insti-
EG-2.4 SUN (Keynote) 11:15Spinoptical Metasurfaces:Spin-Controlled Photonics�E. Hasman; Technion - IsraelInstitute of Technology, Haifa,IsraelWe report on a genericconcept to control multiplewavefronts by spinopticalgradient metasurfaces witha custom-tailored geometricphase. Spinoptical meta-surfaces o�er all-optical
CM-2.3 SUN 11:15Physical and Bio(Cellular)Response of Laser InducedPeriodic Surface Structureson a Pt:SS alloy using a HighRepetition RateFemtosecond Laser�C. McDaniel1, O.Gladkovskaya2, A. Flanagan3,Y. Rochev2, and G. O’Connor1;1NCLA/INSPIRE Labora-tories, School of Physics,National University of Ireland
CJ-2.4 SUN 11:15Passively mode-lockedEr-doped �ber laser for thegeneration of high-energydissipative solitonsM. Tang1, H. Wang1, R.Becheker2, J.-L. Oudar3, D.Gaponov4, T. Godin1, and �A.Hideur1; 1CORIA, NormandieUniversité, Saint Etienne duRouvray, France; 2Laboratoired’Electronique Quantique,Bab Ezzouar, Algeria; 3LPN-
CA-2.3 SUN 11:15Chirped Pulse Yb:CALGOOscillator deliveringSub-100 fs - 4 Watts pulses�P. Sévillano1, J.C. Delagnes1,F. Druon2, D. Descamps1,and E. Cormier1; 1CentreLasers Intenses et Applications,Talence, France; 2LaboratoireCharle Fabry, Palaiseau,FranceWe demonstrated a ChirpedPulse Yb:CALGO oscillator
CE-2.4 SUN 11:15Manufacturing and opticalcharacterization ofside-pumped high power�ber combiner forLMA-�bers�T. �eeg1,2, H. Sayinc1,2,L. Overmeyer1,2,3, J.Neumann1,2, and D. Kracht1,2;1Laser Zentrum Hannovere.V., Hannover, Germany;2Centre for Quantum En-gineering and Space-Time
CD-2.3 SUN 11:15Fast Tunable PicosecondOPO Based on ChirpedQuasi-Phase Matching�D. Descloux1, J.-B.Dherbecourt1, J.-M.Melkonian1, M. Raybaut1,C. Drag2, and A. Godard1;1ONERA -�e FrenchAerospace Lab, Palaiseau,France; 2Laboratoire Aimé-Cotton, CNRS-UniversitéParis Sud 11-ENS Cachan,
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ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2EA-2.3 SUN 11:00Measurement-inducedgeneration of a macroscopicspin singletN. Behbood1, F. MartinCiurana1, G. Colangelo1, M.Napolitano1, G. Toth2,3,4, �R.J.Sewell1, and M.W. Mitchell1,5;1ICFO - Institut de CienciesFotoniques, Castelldefels,Spain; 2Department of�eoretical Physics, Univer-sity of the Basque CountryUPV/EHU, Bilbao, Spain;3IKERBASQUE, Basque Foun-dation for Science, Bilbao,Spain; 4Wigner ResearchCentre for Physics, Hungar-ian Academy of Sciences,Budapest, Hungary; 5ICREA* Institucio * Catalana deRecerca i Estudis Avançats,Barcelona, SpainWe report the production ofa macroscopic spin singletvia quantum nondemolition(QND) measurement ofatomic spins, detecting 3dBof spin squeezing, indicatingthat at least half the atomsin the sample have formedsinglets.
EF-2.3 SUN (Invited) 11:00Photonic Mesh Lattices:From PT Solitons to OpticalSuper�uidity�M. Wimmer1,2, A.Regensburger1,2, M.-A.Miri3, C. Bersch1, D.Christodoulides3, and U.Peschel4; 1Institute of Optics,Information and Photonics,Friedrich-Alexander-UniversitätErlangen-Nürnberg, Erlan-gen, Germany; 2ErlangenGraduate School in AdvancedOptical Technologies (SAOT),Friedrich-Alexander-UniversitätErlangen-Nürnberg, Erlangen,Germany; 3CREOL, Collegeof Optics and Photonics,University of Central Florida,Orlando, United States;4Institute of Solid State�eory and Optics, FriedrichSchiller University Jena, Jena,GermanyBy using a time multiplexingsetup, we for the �rst time ex-perimentally observe solitonson locally and globally parity-time-symmetric mesh lattices.Furthermore, super�uid be-haviour of a pure optical �eldis demonstrated on a passivelattice.
CH-2.3 SUN (Invited) 11:00Breaking the mirrorsymmetry of spontaneousemission via spin-orbitinteraction of light�A. Rauschenbeutel; ViennaCenter for Quantum Scienceand Technology, Institute ofAtomic and Subatomic Physics,Vienna University of Technol-ogy, Wien, AustriaLight with strong intensitygradients at the wavelengthscale exhibits a signi�cant po-larization component along itsdirection of propagation. �einteraction of quantum emit-ters with such light �elds leadsto new and surprising e�ects.
CC-2.3 SUN 11:00High Gain TerahertzQuantum Cascade Ampli�er�R. Wallis, Y. Ren, Y. Shah,D. Jessop, R. Degl’Innocenti,A. Klimont, V. Kamboj, H.Beere, and D. Ritchie; Univer-sity of Cambridge, Cambridge,United KingdomA terahertz ampli�er basedon a quantum cascade gainmedium has been demon-strated using an anti-re�ectivecoating to suppress lasing.Under external seeding, amaximum gain of 30 dB andsingle mode emission wererecorded.
EE-2.2 SUN 11:00Long Range FemtosecondAtmospheric Light BulletP. Panagiotopoulos1, P.Whalen2, �J.V. Moloney1,2,and M. Kolesik1; 1College ofOptical Sciences, Universityof Arizona, Tucson, UnitedStates; 2Program in AppliedMathematics, University ofArizona, Tucson, United StatesWe predict the formation ofextremely high power mid-IRoptical bullets in the atmo-sphere utilizing a new nonlin-ear regularizing mechanismbased on the interplay of dis-persion, harmonic generationcarrier wave shock formation.
JSI-2.2 SUN 11:00Absorption enhancement inperovskite cells usingembedded goldnanoparticles�S. Carretero-Palacios and H.Míguez; Multifunctional Op-tical Materials Group, Insti-tuto de Ciencia de Materialesde Sevilla, Consejo Superiorde Investigaciones Cientí�cas-Universidad de Sevilla, Seville,SpainWe report on the theoreticalanalysis of the e�ect of goldnanoparticles embeddedin perovskite �lms. Weanalyze the e�ect of particlesize and concentration ofgold nanoparticles in theabsorption enhancement ofperovskite cells.
CI-2.3 SUN 11:00A Duplex Ultra-Dense WDM/SDM-PON with MulticoreFiber and Advanced Modu-lation Formats�B. Li1,2, Z. Feng1,2, M.Tang1,2, Z. Xu1,2, Q. Wu1,2, S.Fu1,2, R. Zhang3, L. Zhang3,S. Long3, S. Liu1, and P.P.Shum4; 1Wuhan National labfor Optoelectronics (WNLO),Huazhong Univ. of Sci&Tech(HUST), Wuhan, China,People’s Republic of (PRC);2Next Generation InternetAccess National EngineeringLab (NGIA), School of opticaland electronic information,Huazhong Univ. of Sci&Tech(HUST), Wuhan, China, Peo-ple’s Republic of (PRC); 3StateKey Laboratory of OpticalFiber and Cable ManufactureTechnology, Yangtze OpticalFibre and Cable CompanyLtd(YOFC), Wuhan, China,People’s Republic of (PRC);4School of EEE, NanyangTechnological University,SingaporeWe proposed and experimen-tally demonstrated a duplexultra-dense WDM/SDM-PON with advanced modula-tion formats transmitting on60kmmulticore (7-core) �ber.�e aggregation downstreamrate is 300Gb/s and theupstream rate is 20Gb/s perwavelength.
EA-2.4 SUN 11:15Millisecond and multimodequantum level storage in anatomic ensemble.�P. Jobez1, C. Laplane1, N.Timoney1, N. Gisin1, A.Ferrier2,3, P. Goldner2, and M.Afzelius1; 1Group of AppliedPhysics, Geneva, Switzerland;2Chimie Paristech CNRS,Paris, France; 3SorbonneUniversités, Paris, FranceWe present the �rst optical
CC-2.4 SUN 11:15Broadband quantumcascade laser based terahertzampli�er with an integratedemitterD. Bachmann1, N. Leder2, M.Rösch3, G. Scalari3, M. Beck3,H. Arthaber2, J. Faist3, K.Unterrainer1, and �J. Darmo1;1Photonics Institute, ViennaUniversity of Technology,Vienna, Austria; 2Institute ofElectrodynamics, Microwave
EE-2.3 SUN 11:15Backward 337 nm nitrogenlasing from �lament plasmainduced by circularlypolarized laser pulse�D. Pengji; Laboratoired’Optique Appliquée, EN-STA ParisTech/CNRS/EcolePolytechnique, Palaiseau,France�e backward 337 nm nitro-gen lasing emitted from �la-ment plasma generated by cir-
JSI-2.3 SUN 11:15Semi-Periodic Gratings forBroadband Absorption in�in Film Solar Cells�M. Jalali1, D. Erni1, andH. Nadgaran2; 1Generaland �eoretical ElectricalEngineering (ATE), Facultyof Engineering, University ofDuisburg-Essen, Duisburg,Germany; 2Department ofPhysics, Shiraz University,Shiraz, Iran
CI-2.4 SUN 11:15Experimental BandwidthOptimization for FlexiblePON Using Nyquist ShapedPSK�J.A. Altabas1, F. Sotelo1,J.A. Lazaro2, and I. Garces1;1Aragon Institute of Engineer-ing Research (I3A), Universityof Zaragoza, Zaragoza, Spain;2Universitat Politecnica deCatalunya, Barcelona, SpainNyquist-PSK for �exible
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tut für Angewandte Physik,Karlsruhe, GermanyWe present optically de-tected magnetic resonancemeasurements on singlenitrogen vacany centers innano diamonds embedded inlaser written photonic struc-tures. �ese structures aremanufactured coordinatelyaround a pre-characterizednano diamond by direct laserwriting.
manipulation by multitaskwavefront shaping via asingle ultrathin photonicnanodevice.
Galway, Galway, Republicof Ireland; 2National Centrefor Biomedical EngineeringScience, National Universityof Ireland Galway, Galway,Republic of Ireland; 3BostonScienti�c Galway, BallybritBusiness Park, Galway,Republic of IrelandLaser Induced Periodic Sur-face Structures are generatedat two ultra-short laser wave-lengths using high repetitionrates. In�uence on cross sec-tional grain and bio cellu-lar interactions are reportedfor Pt:SS. LIPSS are amor-phous with di�erentiated bio-responses.
CNRS, Marcoussis, France;4Novae, Limoges, FranceWe report on a passivelymode-locked Erbium-doped�ber laser featuring a largenormal dispersion and emit-ting high energy dissipativesolitons. Mode-locking isstabilized by combining ahigh nonlinearity amplitudemodulator and a narrow-bandspectral �lter.
that generates 40 nJ, 91 fs ata repetition rate of 96 MHz.In�uence of a small net pos-itive intracavity dispersion isdiscussed.
Research - QUEST, Han-nover, Germany; 3Institutfür Transport- und Automa-tisierungstechnik, LeibnizUniversität Hannover,Hannover, GermanyWe present details of manu-facturing for high power �bercombiner with LMA �bers.We will focus especially onthe temperature-controlledglass welding process.
Orsay, FranceWe report on a picosecondOPO combining an aperiod-ically poled nonlinear crystaland a rapidly tunable intracav-ity spectral �lter. Fast tuningover 80 nm around 3.84 �mis carried out in less than fewmilliseconds
CK-2.3 SUN 11:30Ultra-small mode volumecavities for the enhancementof nitrogen-vacancy center�uorescence�H. Kaupp1,2, B. Schlederer1,2,H. Fedder3, H.-C. Chang4,T.W. Hänsch1,2, and D.Hunger1,2; 1Max-PlanckInstitut für Quantenop-tik, Garching, Germany;2Ludwig-Maximilians-Universität, München,Germany; 3UniversitätStuttgart, Stuttgart, Germany;4Academia Sinica, Taipei,China, Republic of (ROC)Applying ultra-small modevolume cavities the emissionrate and collection e�ciencyof nitrogen-vacancy centersin diamond can be boosted,providing a way to builde�cient single photon sourcesor spin-photon interfaces atambient conditions.
CM-2.4 SUN 11:30In-Situ Observation ofUltrafast Laser InducedPeriodic Surface Structureson Metals by OpticalMicroscopy�C. Mauclair1,2, A. Aguilar1,3,J.-P. Colombier1, R. Stoian1,and A. Avila3; 1LaboratoireHubert Curien, Université JeanMonnet Saint-Etienne, Univer-sité de Lyon, Saint-Etienne,France; 2GIE Manutech-USD,Saint-Etienne, France; 3Centrode Investigaciones en Optica,A.C. Lomas del Bosque 115,Léon, MexicoOptical re�ective microscopywith high magni�cation isproposed to inspect nanos-tructures generated by ultra-short laser pulses on metal-lic samples. �e resolution al-lows for the characterizationof ripples pattern in situ dur-ing multipulse irradiation.
CJ-2.5 SUN 11:30Sub-100 fs pulses from anall-polarization maintainingYb-�ber oscillator withanomalous dispersionhigher-order-mode �berA. Verhoef1, L. Zhu1,2,S. Møller Israelsen3, L.Grüner-Nielsen4, K. Rottwitt3,A. Baltuska1, and �A.Fernández1,5; 1Institut fürPhotonik, TU Wien, Wien,Austria; 2Universität Wien,Institut für PhysikalischeChemie, Wien, Austria;3Technical University ofDenmark, Department ofPhotonics Engineering, Kgs.Lyngby, Denmark; 4OFSDenmark, Brøndby, Denmark;5Medical Physics and Biotech-nology, Medical University ofVienna, Wien, AustriaWe present an Yb-�beroscillator with an all-polarization-maintainingcavity with a higher-order-mode �ber for dispersioncompensation. When thecavity is operated with closeto zero net dispersion, highlystable 0.5-nJ, sub-100-fspulses are generated.
CA-2.4 SUN 11:30Sub-200 fs Mode-locked Nd3+-doped Ba(Zr,Mg,Ta)O3Ceramic Laser�Y. Higashi1, A. Shirakawa1,K.-i. Ueda1, A. A. Kaminskii2,S. Kuretake3, Y. Kintaka3,K. Murayama3, and N.Tanaka3; 1Institute for LaserScience, University of Electro-communications, Tokyo,Japan; 2Institute of Crystal-lography, Russian Academyof Science, Moscow, Russia;3Murata Manufacturing Co.,Ltd.,, Kyoto, JapanWe have demonstratedpassively mode-locked laseroperation of Nd3+-dopedBa(Zr,Mg,Ta)O3 ceramicwith a pulse duration of 196fsand a spectral bandwidthof 5.5nm. Characteristictwin peaks appeared in thespectrum due to two Nd sites.
CE-2.5 SUN 11:30Fiber-on-Planar Mechanicaland Optical Composite�C. Holmes, J.C. Gates, L.G.Carpenter, M.I.M. AbdulKudus, C.B.E. Gawith,G. Brambilla, and P.G.R.Smith; Optoelectronics Re-search Centre, University ofSouthampton, Southampton,United KingdomA composite combining bothmechanical and optical func-tionality is presented. �e re-sult provides optical interac-tion between planar and �-bre formats, enabling a routefor precision layup of �ber op-tics and lithographically pro-cessed �ber-planar hybrid de-vices.
CD-2.4 SUN 11:30Fabrication of Quasi Phase-Matching Waveguides inLithium Niobate by DirectFemtosecond Laser WritingS. Kroesen, K. Tekce, �L.Wesemann, J. Imbrock, andC. Denz; Institute of AppliedPhysics and Center for Non-linear Science, University ofMuenster, Muenster, GermanyWe demonstrate monolithicfabrication of laser-inducedquasi phase-matching waveg-uides in lithium niobate by di-rect femtosecond laser writ-ing. �e circular type-IIwaveguide with an embeddedmultiscan grating enables e�-cient second harmonic gener-ation of 1064nm radiation.
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ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2
quantum-level storage of mul-tiple modes for millisecondsusing spin-echo techniques inan ensemble-based memory.�is result paves the way forquantum storage of severalhours.
and Circuit Engineering, Vi-enna University of Technology,Vienna, Austria; 3Institute forQuantum Electronics, ETHZürich, Zürich, SwitzerlandWe demonstrate a broadbandTHz ampli�er that relies ongain switching in amulti-stackquantum cascade heterostruc-ture. An ampli�cation band-width of 500 GHz and ampli�-cation factors above 20 dB arereached.
cularly polarized laser pulse innitrogen or air was observed,which is expected to bringimprovements to the remotesensing application.
Determnistic nonperiodicback gratings were imple-mented in silicon solar cellsas light trapping techniquebecause of their controllablerandom-like features leadingto broadband excitation in thek-space of exploitable guidedand radiation modes.
PON is proposed. 1.25Gb/s(2.5Gb/s) Nyquist-PSK witha 120 homodyne coherentreceiver reduces the usedoptical bandwidth to 3.75GHz(5GHz) with receiver sen-sitivity of -48.5dBm at FEClimit.
EA-2.5 SUN 11:30Storage of light in a nano-�ber-trapped atomicensemble�B. Albrecht, C. Clausen, C.Sayrin, P. Schneeweiss, and A.Rauschenbeutel; Vienna Uni-versity of Technology, Insti-tute of Atomic and SubatomicPhysics, Vienna, AustriaHere we present the latest re-sults of our work towards a�ber-based quantummemory.We used electromagneticallyinduced transparency to suc-cessfully store a light pulse inan atomic ensemble trappedaround a tapered optical �ber.
EF-2.4 SUN 11:30Spontaneous symmetrybreaking in two coupledphotonic crystal lasersP. Hamel, S. Haddadi, F.Raineri, P. Monnier, G. Beau-doin, I. Sagnes, A. Levenson,and �A. Yacomotti; Labo-ratoire de Photonique et deNanostructures, Marcoussis,FranceWe experimentally showspontaneous breakingof mirror-symmetry intwo evanescently coupledphotonic crystal nanocavity-lasers. Coexistence of spatiallylocalized states in the cavitiesis demonstrated throughshort pulse excitation.
CH-2.4 SUN 11:30NewManifestations ofSelf-Accelerating Light:Radial & AngularSelf-Acceleration�C. Vetter1, A. Dudley2, T.Eichelkraut1, C. Schulze4, M.Ornigotti1, M. Duparré4, A.Forbes2,3, and A. Szameit1;1Institute of Applied Physics,Abbe Center of Photonics,Friedrich-Schiller-Universität,Jena, Germany; 2CSIR Na-tional Laser Centre, Pretoria,South Africa; 3School ofPhysics, University of theWitwatersrand, Johannesburg,South Africa; 4Institute ofApplied Optics, Friedrich-Schiller-Universität, Jena,GermanyWe report on new classesof self-accelerating opticalbeams that evolve on spiralingtrajectories. Important newfeatures are an acceleration inpropagation direction and thepossibility to tailor the beampro�le at will.
CC-2.5 SUN 11:30A Hybrid PlasmonicWaveguide TerahertzQuantum Cascade LaserR. Degl’Innocenti, �A. Klimont,Y. Shah, R. Wallis, Y. Ren,D. Jessop, H. Beere, and D.Ritchie; Cavendish Laboratory,University of Cambridge,Cambridge, United KingdomWe realized a terahertz quan-tum cascade laser based on ahybrid plasmonic waveguidedesign. Our approach yieldsimprovements in the far-�eldemission of standard doublemetal QCLs, while retainingtheir performance
EE-2.4 SUN 11:30Bessel Vortex Filaments forLaser Material ProcessingC. Xie1, V. Jukna2,3, C.Milian2, R. Giust1, T.Itina3, A. Couairon1, J.M.Dudley1, and �F. Courvoisier1;1Institut FEMTO-ST, UMR6174 CNRS University ofFranche-Comte, Besancon,France; 2Centre de Physique�éorique, CNRS, EcolePolytechnique, Palaiseau,France; 3Laboratoire HubertCurien, UMR CNRS 5516,Université de Lyon, UniversitéJean Monnet, Saint Etienne,FranceWe report novel nonlinearpropagation regimes of ultra-short Bessel vortex beams andproof-of principle applicationfor laser processing with tubu-lar interaction in dieletrics.3D-imaging of �lamentationin solids allows direct andquantitative comparison withsimulations.
JSI-2.4 SUN 11:303D Solar: Concepts fore�ective light trapping inthin �lm solar cells�L. Bernhard1, K. Ladislav1, U.Christoph2, and W. Matthew2;1JOANNEUM RESEARCHForschungsgesellscha� mbH,MATERIALS, Weiz, Austria;2Linz Institute for OrganicSolar Cells (LIOS), Linz,AustriaWe report a new solution forthe photon management inorganic thin �lm solar cells,with the goal to increase thesolar e�ciency. �e approachutilizes special light trappingstructures combined withluminescent down-convertingdyes.
CI-2.5 SUN 11:30Single-Section QuantumWell Mode-Locked Laser for400 Gbit/s Single-Polariza-tion IM/DD SSB-OFDMTrans- missionC. Calò1, V. Vujicic2, �R.Watts2, F. Lelarge3, C.Browning2, K. Merghem1, V.Panapakkam1, A. Martinez1,A. Ramdane1, and L.P. Barry2;1CNRS Laboratory for Photon-ics and Nanostructures, Routede Nozay, 91460 Marcoussis,France; 2School of ElectronicEngineering, Dublin CityUniversity, Glasnevin, Dublin9, Republic of Ireland; 3III-VLab, a joint Laboratory ofAlcatel Lucent Bell Labs and�ales Research & Technologyand CEA-LETI, Route deNozay, 91460 Marcoussis,FranceAn optical frequency combgenerated by a single-sectionInGaAsP/InP quantum wellmode-locked laser is used forIM/DD SSB-OFDM transmis-sion. A net aggregate capacityof 400 Gb/s in single polariza-tion is demonstrated using 16comb lines.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14bCK-2.4 SUN 11:45Nano-optomechanicalmeasurement with a singlephoton source�L. Mercier de Lepinay1, B.Pigeau1, S. Rohr1, A. Gloppe1,E. Dupont-Ferrier1, A. Kuhn1,P. Verlot2, and O. Arcizet1;1Institut Neel, UniversiteGrenoble Alpes, Grenoble,France; 2Institut LumiereMatiere, Universite ClaudeBernard, Lyon, FranceA single photon emitter (NVdefect) is granted a spatial de-gree of freedom by attach-ing it to a nanowire extrem-ity. Space-time intensity cor-relations then allow the imag-ing of trajectories in the pho-ton counting regime.
CM-2.5 SUN 11:45Laser-Patterning StainlessSteel with Nonlinear LaserLithography for EnhancedTribological Properties�I. Gnilitskyi1, I. Pavlov2, F.Rotundo3, L. Orazi1, S. Ilday2,C. Martini3, and F.O. Ilday2,4;1Department of Sciences andMethods for Engineering -University of Modena andReggio Emilia, Reggio Emilia,Italy; 2Department of Physics- Bilkent University, Ankara,Turkey; 3Industrial Engineer-ing Department - Universityof Bologna, Bologna, Italy;4Department of Electricaland Electronics Engineering- Bilkent University, Ankara,Turkey�is paper investigates anew �eld for application offemtosecond laser-inducedperiodic surface structures(LIPSS). We designed aninnovative solution to reducecoe�cient of friction ofmechanical parts by usingnonlinear laser lithographytechnique (NLL).
CJ-2.6 SUN 11:45Dissipative solitonsgenerated from a mode-locked Raman laser�U. Tegin1, P. Elahi1, C. Senel3,E. Ergecen2, and F.O. Ilday1,2;1Department of Physics,Bilkent University, Ankara,Turkey; 2Department ofElectrical and Electronics En-gineering, Bilkent University,Ankara, Turkey; 3TUBITAKNational Metrology Institute(UME), Kocaeli, TurkeyWe report on a dissipativesoliton �ber Raman laser. �elaser generates 9.7-nJ intra-cavity chirped pulses at 1120nmwith 17 nm spectral width.�e Raman pulses can be de-chirped to 135 fs.
CA-2.5 SUN 11:45Kerr-lens Mode-lockedYb3+-doped Lu3Al5O12Ceramic Laser�S. Kitajima1, H. Nakao1, A.Shirakawa1, H. Yagi2, andT. Yanagitani2; 1Institute forLaser Science, University ofElectro-Communications,1-5-1 Chofugaoka, Chofu,Tokyo, Japan; 2TakumaWorks, Konoshima ChemicalCo., 80 Kouda, Takuma,Mitoyo, Kagawa, JapanWe have achieved the �rstKerr-lensmode-locked opera-tion of Yb:LuAG ceramic witha pulse duration of 103 fs andan average output power of1.72 W. A pulse energy was20.3 nJ.
CE-2.6 SUN 11:45Planar fabrication assisted�ber nanowiremanufacturingL. Cui1, �B. Gholipour1,P. Bastock2, K. Khan2, C.Craig2, D. Hewak2, and C.Soci1; 1Center for Disrup-tive Photonic Technologies,Nanyang TechnologicalUniversity, Singapore, Sin-gapore; 2OptoelectronicsResearch Center, University ofSouthampton, Southampton,United KingdomBy combining planar fabrica-tion with �ber manufactur-ing, we demonstrate a noveltechnique for producing mul-timaterial single and 1D arraysof nanowires and nanoribbonsenclosed in glass �bers with asingle �ber draw.
CD-2.5 SUN 11:45Soliton Modelocking viaAdiabatic Excitation ofCascaded QuadraticNonlinearities in ApodizedFanout QPMDevices�C. Phillips, A.Mayer, A. Klen-ner, andU. Keller; ETHZurich,Zurich, SwitzerlandWe show soliton modelockingof a Yb:CALGO laser usingcascaded second-ordernonlinearities whereby thesecond-harmonic is adiabat-ically excited/de-excited inan apodized-fanout-PPLNcrystal. We obtain 100-fspulses at 540 MHz with 760mW average power.
13:30 – 15:00CK-3: Photonic CrystalLasersChair: Olivier Gauthier-La-faye, LAAS-CNRS, Toulouse,France
13:30 – 15:00EG-3: Quantum NanoOpticsChair: Olivier Arcizet, InstitutNéel/CNRS, Grenoble, France
13:30 – 15:00CM-3: Beam Shaping forLaser MicromachiningChair: Gerard O’Connor, Na-tional University of Ireland,Galway, Ireland
13:30 – 15:00CJ-3: Novel FibreDesignsChair: Geraud Bouwmans,Université Lille 1, Lille, France
13:30 – 15:00CA-3: High-PowerPulsed Solid-state LasersChair: Bozhidar Oreshkov,So�a University, So�a,Bulgaria
13:30 – 15:00CE-3: Metamaterialsand PhotonManipulationChair: Patrice Camy, Univer-sity of Caen, Caen, France
13:30 – 15:00CD-3: Phenomena inNonlinear OpticsChair: Marco Centini, LaSapienza Universita’ di Roma,Roma, Italia
CK-3.1 SUN 13:30Design of an e�cientphotonic crystal beam laser�D. Heiss, A. Higuera-Rodriguez, V. Pogoretskii,V. Dolores-Calzadilla, A.Fiore, and M. Smit; COBRAResearch Institute, Eindhoven,
EG-3.1 SUN 13:30Nonlinear Optics withSingle Molecules�A. Maser1,2, B. Gmeiner1,2,T. Utikal1,2, S. Götzinger2,1,and V. Sandoghdar1,2; 1MaxPlanck Institute for the Scienceof Light, Erlangen, Germany;
CM-3.1 SUN 13:30Plasma Absorption Evidencevia Chirped Pulse SpectralTransmission Measurementsof a Bessel BeamPropagating in GlassO. Jedrkiewicz1, �S. Minardi2,A. Couairon3, V. Jukna3, M.
CJ-3.1 SUN 13:30Low Bend-Sensitive All-glass Highly Yb-dopedTapered Fiber ForHigh-Peak-PowerAmpli�cation Systems�K. Bobkov1, A. Levchenko1,S. Aleshkina1, S. Semenov1,
CA-3.1 SUN 13:30Di�raction-limited,high-average powerpico-second laser formed ofa sapphire end-cappedNd:YVO4 bounce ampli�er�M. Abe1, M. Kowa1,K. Miyamoto1, and T.
CE-3.1 SUN (Invited) 13:30Supersymmetric scatteringand transformation optics�M. Heinrich1,2, M.-A. Miri2,S. Stützer1, S. Nolte1, D.N.Christodoulides2, and A.Szameit1; 1Institute of AppliedPhysics, Abbe Center of
CD-3.1 SUN 13:30Slow and Fast LightSwitching in Ruby�R. Papukutty Rajan and H.Riesen; School of Physical, En-vironmental and Mathemati-cal Sciences, �e Universityof New South Wales, UNSW
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ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2EA-2.6 SUN 11:45Observation of theNonlinear Phase Shi�Dueto Single Post-SelectedPhotons�A. Feizpour, M. Hallaji, G.Dmochowski, and A. Stein-berg; University of Toronto,Toronto, CanadaWe implement an op-tical nonlinearity usingelectromagnetically-inducedtransparency in cold atoms,and measure the resultingnonlinear phase shi� forpostselected photons. �isrepresents the �rst directmeasurement of the nonlin-ear shi� due to individualphotons.
EF-2.5 SUN 11:45Nonlinear mechanics ofphotonic crystal deformablemirrors actuated viaelectrostatic force�A. Chowdhury1, I. Yeo1, G.Beaudoin1, I. Robert-Philip1,and R. Braive1,2; 1CNRS-LPN, Marcoussis, France;2Université Paris 7, Paris,FranceSuspended nanomembranespierced by a photonic crystalact as a deformable mirroroperating at normal inci-dence. Electrostatic actuationmade by interdigitated elec-trodes integrated below themembrane induces bistabilityand high-order sub-harmonicresonances.
CH-2.5 SUN 11:45Optical phase cloning by adual-parallel Mach-ZehndermodulatorJ. Burkart1, �T. Sala2, S.Kassi1, D. Romanini1, andM. Marangoni2; 1Universityof Grenoble Alpes and CNRS,LIPhy, Grenoble, France;2Physics Department ofPolitecnico di Milano andIFN-CNR, Milan, ItalyA dual-parallel Mach-Zehnder modulator in afeed-forward con�guration isshown to provide the phasecloning of a master oscillatoronto a distributed-feedbacklaser with a 113-mrad residualphase error and multi-GHztuning and capture range
CC-2.6 SUN 11:45Terahertz emission fromtransitions betweenlight-hole states in SiGequantum cascade structures�P. Rauter1, G. Mussler2,D. Grützmacher2, and T.Fromherz1; 1Institute ofSemiconductor and SolidState Physics, Johannes KeplerUniversity Linz, Linz, Austria;2Peter-Grünberg Institut 9,Forschungszentrum Jülich,Jülich, Germany�e contribution has beenwithdrawn by the authors.
EE-2.5 SUN 11:45Increasing laser-driven THzemission with sawtoothpulse pro�les�P. Gonzalez de AlaizaMartinez1, I. Babushkin2, L.Bergé1, S. Skupin3, E. Cabrera-Granado4, C. Koehler5, U.Morgner2, A. Husakou6, and J.Herrmann6; 1CEA-DAM-DIF,Arpajon, France; 2Institute ofQuantum Optics, Leibniz Uni-versity Hannover, Hannover,Germany; 3Universite de Bor-deaux - CNRS - CEA, CentreLasers Intenses et Applications,Talence, France; 4Facultadde Optica y Optometria,Universidad Complutensede Madrid, Madrid, Spain;5Institute for Scienti�c Com-puting, TU Dresden, Dresden,Germany; 6Max-Born-Institutfuer Nichtlineare Optik undKurzzeitspektroskopie, Berlin,GermanyBroadband terahertz pulsesare routinely produced withweak conversion e�cien-cies by femtosecond laserpulses ionizing gases. Wedemonstrate that, by usingmultiple-frequency pulses ap-proaching a sawtooth pro�le,this conversion e�ciency canexceed the percent level.
JSI-2.5 SUN 11:45Highly TransparentInterconnecting Layer forOptically-optimizedTandem Organic Solar cellsAllows for 76% Fill Factor�M. Montes Bajo1, A.Martinez-Otero1, Q. Liu1,P. Mantilla-Perez1, and J.Martorell1,2; 1ICFO - �eInstitute of Photonics Sci-ences, Castelldefels, Spain;2Departament de Física i En-ginyeria Nuclear, UniversitatPolitècnica de Catalunya,Terrassa, SpainOptically-optimized tandempolymer solar cells with 76%�ll factor and both sub-cellsbased on the polymer PTB7are presented, focusingespecially on the optimiza-tion of the amount of Agwithin the MoO3/Ag/PFNinterconnecting layer.
CI-2.6 SUN 11:45Simultaneous full C-bandtuning of three integratedDS-DBR lasers in presenceof strong thermal crosstalk�W. Yao1, G. Gilardi1,M. Smit1, and M. Wale2;1Eindhoven University ofTechnology, Eindhoven, �eNetherlands; 2Oclaro Tech-nology Ltd, Caswell, UnitedKingdomWe investigate thermalcrosstalk e�ects in an arrayof three monolithicallyintegrated DS-DBR lasers anddemonstrate that simultane-ous C-band tuning accordingto ITU-grid can be achievedthrough proper adjustment ofphase tuning sections.
13:30 – 15:00EA-3: QuantumInterferenceChair: Stephan Götzinger,Max Planck Institute for theScience of Light, Erlangen,Germany
13:30 – 15:00EF-3: Soliton DynamicsChair: Alejandro Giacomotti,Laboratoire de Photonique etdes Nanostructures-CNRS,Marcoussis, France
13:30 – 15:00CH-3: Mid InfraredSensing andMeasurementsChair: Tal Carmon, Technion,Haifa, Israel
13:30 – 15:00CC-3: High Field THzRadiationChair: �omas Dekorsy, Uni-versity of Konstanz, Konstanz,Germany
13:30 – 15:00EE-3: UltrafastTemporal Dynamics andExtreme EventsChair: Stephane Coen, Uni-versity of Auckland, Auckland,New Zealand
13:30 – 15:00JSIV-1: Optical andUltrafast Spectroscopyof Two-dimensionalMaterialsChair: �omas Müller, ViennaUniversity of Technology, Vi-enna, Austria
13:30 – 15:00CI-3: Signal ProcessingChair: Stefano Wabnitz, Bres-cia University, Brescia, Italy
EA-3.1 SUN (Keynote) 13:30Interferometry with atomsand macromolecules: Frommind-bogglers of quantumoptics to elements of biology�M. Arndt; University of Vi-enna, Faculty of Physics, VCQ,QuNaBioS, Vienna, Austria
EF-3.1 SUN 13:30Soliton explosions in apassively mode-locked �berlaser�A.F.J. Runge, N.G.R. Brod-erick, and M. Erkintalo;Dodd-Walls Centre andPhysics Department, �e Uni-
CH-3.1 SUN (Invited) 13:30Recent Advances in QuartzEnhanced PhotoacousticSpectroscopy for Trace GasSensing�V. Spagnolo1, P. Patimisco1,A. Sampaolo1,2, G.Scamarcio1, and F.K.
CC-3.1 SUN 13:30THz-Induced Strong-FieldElectron Emission from aGold SurfaceC. Lombosi1, I. Márton2, Z.Ollmann1, J. Hebling1,3, G.Farkas2, P. Dombi2,4, and �J.A.Fülöp3,4; 1University of Pécs,
EE-3.1 SUN 13:30Measurement of theTemporal Coherence ofSupercontinuum Light�M. Närhi1, C. Amiot1,3,R. Dutta2, J. Turunen2, A.Friberg2, J. Dudley3, and G.Genty1; 1Physics Department,
JSIV-1.1 SUN (Invited) 13:302DMaterials BeyondGraphene: OpticalProperties of Atomically�in Transition MetalDichalcogenide Crystals�T.F. Heinz; Stanford Univer-sity and SLAC National Ac-
CI-3.1 SUN 13:30Optical Nyquist PulseGeneration in Mode-LockedFibre Laser�S. Boscolo1, C. Finot2, andS.K. Turitsyn1; 1Aston Insti-tute of Photonic Technologies,Aston University, Birm-
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�e NetherlandsWe present the design and�rst fabrication trials of anelectrically pumped micron-scale laser based on a pho-tonic crystal beam cavity. �ehigh e�ciency could enableultra-dense laser integrationfor data communication.
2Department of Physics,Friedrich-Alexander-UniversitätErlangen-Nürnberg (FAU),Erlangen, GermanyWe report on four-wavemixing by a single moleculeplaced in the focus of twolaser beams. By monitoringthe intensity of the probebeam, we observe di�erentresonance pro�les in excellentagreement with theory.
Selva4, and P. Di Trapani4;1Istituto di Fotonica eNanotec-nologie, CNR and CNISM UdrComo, Como, Italy; 2Instituteof Applied Physics, Abbe Cen-ter of Photonics, Friedrich-Schiller-University, Jena, Ger-many; 3Centre de Physique�eorique, CNRS, Ecole Poly-technique, Palaiseau, France;4Dipartimento di Scienza eAlta Tecnologia, University ofInsubria, Como, Italy�is work gives evidenceof the plasma generationdynamics and absorptionwhen a Bessel beam prop-agates in glass, thanks to anovel diagnostics based onsingle chirped pulse trans-mission measurements in theangle-wavelength domain.
A. Denisov1, M. Bubnov1, A.Laptev2, A. Guryanov2, andM. Likhachev1; 1Fiber OpticsResearch Center of the RussianAcademy of Sciences, Moscow,Russia; 2Institute of Chemistryof High-Purity Substances ofthe Russian Academy of Sci-ences, Nizhny Novgorod, Rus-siaIn this communication a noveltapered Yb-doped �ber withincreased nonlinear thresholdis demonstrated. �e energyof about 35 �J in 245 ps pulses(peak power ~ 140 kW) at1028 nm was achieved.
Omatsu1,2; 1Chiba University,Chiba, Japan; 2CREST, JST,Kawaguchi, JapanA di�raction-limited, ultra-highly e�cient (~56%) andhigh average power picosec-ond laser system formedof a sapphire end-cappedNd:YVO4 slab bounce ampli-�er is demonstrated. We alsoperform second harmonicand optical vortex generationsat high e�ciency.
Photonics, Friedrich-Schiller-University, Jena, Germany;2CREOL �e College of Opticsand Photonics, University ofCentral Florida, Orlando,United StatesWe theoretically and experi-mentally investigate the scat-tering properties of supersym-metric optical structures. Indoing so, we observe SUSYscattering for the �rst time inphotonic lattices, and intro-duce a supersymmetric exten-sion of transformation optics.
Canberra, Canberra, Australia�e contribution has beenwithdrawn by the authors.
CK-3.2 SUN 13:45Photonic Crystal MembraneLaser: Slow-light E�ects onLasing�reshold�W.Xue, Y. Yu, L. Ottaviano, Y.Chen, E. Semenova, K. Yvind,and J. Mork; DTU Fotonik,Technical University of Den-mark, Kongens Lyngby, Den-mark�e lasing threshold ofphotonic crystal cavity lasersoperating in the slow-lightregime is studied experi-mentally. We �nd that thecombined e�ects betweenslow-light propagationand disorder determine anon-monotonous lengthdependence of the threshold.
EG-3.2 SUN 13:45Quantum Optics in One-Di-mension: Single MoleculesCoupled to a DielectricNanoguide�P. Türschmann1, S. Faez1,H.R. Haakh1, T. Utikal1, N.Rotenberg1, S. Götzinger2,1,and V. Sandoghdar1,2; 1MPIfor the Science of Light, Erlan-gen, Germany; 2Departmentof Phyics, Friedrich Alexan-der University Erlangen-Nürnberg, Erlangen, GermanyWe experimentally demon-strate a highly e�cient, solid-state interface between guidedphotons and single molecules.A �lled glass capillary servesas waveguide with a stronglycon�ned mode that allows forcoupling e�ciency of up to18%.
CM-3.2 SUN 13:45Micromachining withfemtosecond laserhigher-order Bessel beams�W. Cheng and P. Polynkin;College of Optical Sciences,University of Arizona, Tucson,United StatesWe report experiments onmicromachining of frontand back surfaces of glassplates using femtosecondhigher-order Bessel beams.�e self-focusing of thebeams inside the glass resultsin the production of beadedring-shaped ablation features.
CJ-3.2 SUN 13:45Experimental demonstra-tion of single-mode largemode area multi-trench�ber for UV-VIS lighttransmission�D. Jain, Y. Jung, P. Barua,and J. Sahu; Optoelectron-ics Research Center, Universityof Southampton, Southamp-ton, United KingdomWe demonstrated all-solidand cylindrical symmetri-cal multi-trench �ber forbeam delivery with corediameters 20*m and 10*mo�ering e�ective-single-modeoperation at wavelengths632nm and 300nm respec-tively. �e �ber design issuitable for industrial-scalemanufacturing.
CA-3.2 SUN 13:45High energy pump laser forMulti-Petawatt laser�O. Casagrande, C. Derycke,A. Soujae�, P. Ramos, L. Boud-jemaa, C. Simon-Boisson, S.Laux, and F. Lureau; �alesOptronique, Elancourt, FranceATLAS 100, a compact highenergy laser delivering morethan 100 joules at the repeti-tion rate of 1 shot per minutehas been developed for thetwo 10 PetaWatt beamlines ofELI NP infrastructure.
CD-3.2 SUN 13:45Parity-Time Anti-Symmet-ric Parametric Ampli�er�D. Antonosyan, A. Solntsev,and A. Sukhorukov; Nonlin-ear Physics Centre, ResearchSchool of Physics and Engineer-ing, Australian National Uni-versity, Canberra, AustraliaWe predict that directionalcoupler of quadratically non-linear and lossy waveguidescan perform ultrafast signalswitching and parametricampli�cation, using thepump-controlled breakingof the parity-time anti-symmetry associated withnonlinear wave mixing.
CK-3.3 SUN (Invited) 14:00Photonic Crystal Lasers onSi�S. Matsuo1,2, K. Takeda1,2,T. Fujii1,2, and T. Sato1;1Nanophotonics Center, NTTCorporation, Atsugi, Japan;2NTT Device TechnologyLaboratories, Atsugi, JapanUltra-low threshold currentphotonic crystal lasers on Sihave been developed. Di-
EG-3.3 SUN (Invited) 14:00Single organic molecules assources of high-�ux andnarrow-band single photonsM. Rezai1, K. Kafenda1,J. Wrachtrup1,2, and �I.Gerhardt1,2; 13. PhysikalischesInstitut, Universität Stuttgart,Stuttgart Research Centerof Photonic Engineering(SCoPE), and the Center forIntegrated Quantum Science
CM-3.3 SUN (Invited) 14:00Spatial temporal focusingwith application to micro-machining with femto-second laser pulses�J. Squier1, E. Block1, M.Young1, C. Durfee1, J.�omas2, D. Winters3, and R.Bartels3; 1Colorado School ofMines, Golden, United States;2Friedrich-Schiller University,Jena, United States; 3Colorado
CJ-3.3 SUN 14:00Birefringent Top-HatMicrostructured Fiber�P. Gouriou1,2, F. Scol1,2,P. Calvet1,2, B. Sévigny1, C.Valentin1, Y. Quiquempois1, L.Bigot1, A. Cassez1, A. Mussot1,M. Douay1, E. Hugonnot1,and G. Bouwmans1; 1PhLAM-IRCICA, Villeneuve d’Ascq,France; 2CEA-CESTA, LeBarp, France
CA-3.3 SUN 14:00220-fs 110-mJ Yb:CaF2Multipass Booster�G. Andriukaitis1, E. Kaksis1,G. Polónyi2, J.A. Fülöp3, A.Pugžlys1,4, and A. Baltuška1,4;1Photonics Institute ViennaUniversity of Technology,Vienna, Austria; 2MTA-PTEHigh-Field Terahertz Re-search Group, Pécs, Hungary;3Institute of Physics, Univer-
CE-3.2 SUN 14:00Adiabatically tapered meta-material waveguides forextraction of high-k wavesN. Kinsey1, P. West1, �M.Ferrera1,2, A. Kildishev1, V.Shalaev1, and A. Boltasseva1;1School of Electrical & Com-puter Engineering and BirckNanotechnology Center, Pur-due University, West Lafayette,United States; 2School of Engi-
CD-3.3 SUN 14:00Adaptive and nonlinearoptics in the transverselocalization regime�M. Leonetti1, S. Karbasi2,A. Ma�3, and C. Conti4;1Center for Life Nano Sci-ence@Sapienza, IstitutoItaliano di Tecnologia,,Roma, Italy; 2Departmentof Electrical and ComputerEngineering, University of
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�is talk reviews some keyelements of matter-wave op-tics, in particular beam split-ter techniques and interfer-ometers for atoms and largemolecules with applications inprecision measurements andbiology.
versity of Auckland, Auckland,New ZealandWe report on the observationof soliton explosions in a pas-sively mode-locked �ber laser.We use single-shot, real-timemeasurements to identify ex-plosion signatures both in thespectral and in the temporaldomains.
Tittel2; 1Dipartimento Inter-ateneo di Fisica, Università ePolitecnico di Bari, Bari, Italy;2Department of Electrical andComputer Engineering, RiceUniversity, Houston, UnitedStatesWe will report on recent ad-vances of the quartz-enhancedphotoacoustic (QEPAS) tech-nique based on quantum cas-cade lasers (QCLs) in orderto realize QEPAS sensors withimproved sensitivity and se-lectivity.
Pécs, Hungary; 2Wigner Re-search Centre for Physics, Bu-dapest, Hungary; 3MTA-PTEHigh-Field Terahertz ResearchGroup, Pécs, Hungary; 4ELI-ALPS, ELI-Hu Nk�., Szeged,HungaryTHz-induced electron emis-sion is observed from a goldsurface irradiated by single-cycle THz pulses with up to300 kV/cm peak electric �eld.�e transition regime betweenmultiphoton emission and op-tical �eld emission is studied.
Tampere University of Tech-nology, Tampere, Finland;2Institute of Photonics, Uni-versity of Eastern Finland,Joensuu, Finland; 3InstitutFEMTO-ST, Université deFranche-Comté, Besançon,FranceWe experimentally measure,for the �rst time, the second-order temporal coherence ofsupercontinuum pulses fromthe time-resolved interferencefringes observed at the outputof a Michelson interferometerusing cross-correlationfrequency-resolved opticalgating.
celerator Laboratory, Stanford,CA, United StatesTransition metal dichalco-genides in the molybdenumdisul�de family can beprepared as stable single andfew-layers crystals. In thispaper, we describe their elec-tronic properties, particularlyhighlighting their distinctiveinteractions with light.
ingham, United Kingdom;2Laboratoire InterdisciplinaireCarnot de Bourgogne, Uni-versite’ de Bourgogne, Dijon,FranceWe numerically show thefeasibility of Nyquist op-tical pulse generation ina mode-locked �bre laserwith an in-cavity �at-topspectral �lter. �e proposedscheme o�ers the possibilityto generate high-qualitysinc-shaped pulses withtunable bandwidth.
EF-3.2 SUN 13:45Soliton Explosions andImplosions in Mode-LockedLasers�W. Chang and N. Akhme-diev; Australian National Uni-versity, Canberra, AustraliaExploding solitons are foundin nonlinear dissipative sys-tems such as in laser cav-ities. We study the inter-nal �ow of energy within thesoliton during explosions, andclassify them accordingly intoexploding and imploplodingsolitons.
CC-3.2 SUN 13:45THz pulses at mJ level fromorganic crystal pumped by aCr:Mg2SiO4 laser�C. Vicario1, A. Ovchinnikov2,S. Ashitkov2, M. Agranat2, andC.P. Hauri1,3; 1SwissFEL PaulScherrer Institute, Villigen-PSI, Switzerland; 2Joint In-stitute for High Temperaturesof RAS, Moscow, Russia;3Ecole Polytechnique Federalede Lausanne, Lausanne,SwitzerlandWe demonstrated 0.9 mJ ter-ahertz pulses by optical recti-�cation of a Cr:Mg2SiO4 laserin organic crystal. �e emittedspectrum covers 0.1- 5 THzand the peak �elds exceed 42MV/cm and 14 Tesla.
EE-3.2 SUN 13:45Simultaneous control of thewavelength and duration ofRaman-shi�ing solitonsusing topographic photoniccrystal �bers�F. Braud, A. Bendahmane,A. Mussot, and A. Kudlinski;Université Lille1 LaboratoirePhLAM, Villeneuve d’Ascq,FranceWe experimentally demon-strate that both the wave-length and duration ofRaman-shi�ing solitons canbe controlled simultaneouslyover a wide range of pa-rameters using meter-longtopographic photonic crystal�bers designed with aninverse algorithm.
CI-3.2 SUN 13:45Reduced Complexity Non-linear Inverse Synthesis forNonlinearity Compensationin Optical Fiber LinksS. Le1, S. Wahls2, D. Lavery3,�J. Prilepsky1, and S. Turitsyn1;1Aston Institute of PhotonicTechnologies, Birmingham,United Kingdom; 2Del�Centerfor Systems and Control, Del�,�e Netherlands; 3UniversityCollege London, London,United KingdomWe propose to apply therecently introduced fast non-linear Fourier transform toreduce the complexity of theinverse nonlinear synthesistransmission scheme fornonlinearity compensation inoptical �ber links
EF-3.3 SUN 14:00Higher-order solitonexplosion�I. Babushkin1, A. Tajalli1,A. Pape1, G. Steinmeyer2, U.Morgner1, and A. Demircan1;1Institute for Quantum Op-tics, Liebniz Universität Han-nover, 30167 Hannover, Ger-many; 2Max Born Institute,12489 Berlin, GermanyWe present a new type of
CH-3.2 SUN 14:00High-Q Mid-infraredChalcogenide RingResonatorsP. Ma, D. Choi, Y. Yu, K. Vu,X. Gai, Z. Yang, B. Luther-Davies, and �S. Madden; LaserPhysics Centre, Australian Na-tional University, Canberra,AustraliaHigh Q factor chalcogenidering resonators are fabricated
CC-3.3 SUN 14:00Self-limiting property ofterahertz generation byoptical recti�cation usingtilted-pulse-fronts�K. Ravi1, S. Carbajo2,3,4,W. Huang1, X. Wu2,3,D. Schimpf2,3, and F.Kaertner1,2,3,4; 1Massachu-setts Institute of Technology,Cambridge, United States;2Center for free electron
EE-3.3 SUN 14:00Stimulated Emission ofDispersive Waves�M. Clerici1,2, M. Petev1,N. Westerberg1, E. Rubino1,D. Moss1, A. Couairon3, F.Légaré2, R. Morandotti2,and D. Faccio1; 1School ofEngineering and Physical Sci-ences, Heriot-Watt University,Edinburgh, United Kingdom;2INRS-EMT, Varennes,
JSIV-1.2 SUN 14:00Disentangling intra andintervalley dynamics inmonolayer MoS2 byultrafast optical techniques�S. Dal Conte1,2, F. Bottegoni2,E. Pogna2, S. Ambrogio3, D.De Fazio4, A. Lombardo4,M. Bruna4, I. Bargigia5, C.D’Andrea5, A. Ferrari4, F.Ciccacci2, G. Cerullo2, and M.Finazzi2; 1IFN-CNR, Milano,
CI-3.3 SUN 14:00Preservation of Magnitudeand Chirality of OAMOrderin Continuously TwistedPCF with Six Satellite Cores�R. Beravat, G.K.L. Wong, X.Xi, M.H. Frosz, and P.S.J. Rus-sell; Max Planck Institute forthe Science of Light, Erlangen,GermanyWe show that twisted pho-tonic crystal �bre with six
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rect bonding technique is usedfor heterogeneous integratingthe photonic crystal laser onSiO2/Si substrate. Fabricateddevice exhibits threshold cur-rent of 32 uA.
and Technology (IQST),Pfa�enwaldring 57, 70569Stuttgart, Germany; 2MaxPlanck Institute for Solid StateResearch, Heisenbergstraße 1,70569 Stuttgart, GermanySingle photons from singlemolecules under cryogenicconditions are extremelynarrow-band (≈15 MHz)and simultaneously exhibita high �ux (>1 Mio de-tected counts/sec). Withatomic �lters one can �lterthese to achieve perfectindistinguishable singlephotons.
State University, Fort Colllins,United StatesAn integrated compressor sys-tem that enables the beam-aspect ratio to be varied forapplications of spatial tempo-ral focusing micromachiningis combined with an opticaldelivery system that can si-multaneously image the ma-chining process.
We design and realize a new�ber delivering a top-hat in-tensity pro�le with polariza-tion maintaining properties.�e �ber behaves as single-mode and the polarization ex-tinction ratio is higher than20dB on a 19m long �ber.
sity of Pécs, Pécs, Hungary;4Center for Physical Sciences &Technology, Vilnius, LithuaniaWe demonstrate a Yb:CaF2booster with a pass-by-passcompensated spatial gain nar-rowing. A 5-concave-mirrordesign a�ords a �exible num-ber of passes as well as 4fimage relay and progressivebeam magni�cation onto thelaser crystal.
neering and Physical Sciences,Heriot-Watt University, Edin-burgh, United KingdomBroadband outcoupling ofhigh-k waves from hyperbolicmetamaterials is approachedwith an in-plane con�gu-ration, and enhanced withadiabatic tapering. �isstrategy may allow for bettere�ciency of Purcell enhancedsources.
California, San Diego, UnitedStates; 3Department of Physicsand Astronomy and Center forHigh Technology Materials,University of New Mexico,Albuquerque, United States;4ISC-CNR and Department ofPhysics, University Sapienza,,Roma, ItalyWe report on light propa-gation in optical �bers sup-porting transverse Andersonlocalization. By exploitingthermal nonlocality we steerand control localized statesthrough action at distance.�e disorder also enhancesin the adaptive focusing e�-ciency.
CJ-3.4 SUN 14:15A �bre that guides an AirypatternI. Gris-Sánchez and �T. Birks;University of Bath, Bath,United KingdomWe present an optical �brethat guides a truncated Airypattern as one of its modes.�e index pro�le consists of4 concentric graded index re-gions. �e far �eld resemblesa top-hat distribution, as ex-pected.
CA-3.4 SUN 14:15Gain-switched diode laserseeding of ultra-high-gainNd:YVO4 bounce ampli�ersystem as a versatile pulsedlaser source�A. Teppitaksak, G. �omas,andM. Damzen; Imperial Col-lege London, London, UnitedKingdomPulsed diode seeding ofbounce geometry ampli�er(s)is investigated, demonstratingultra-high-gain ~50 dB ina preampli�er with goodspatial preservation and14.2W (from 188�W seedpower) with a second powerampli�er.
CE-3.3 SUN 14:15A three-dimensionalinfra-red metamaterial withasymmetric transmission�A. Xomalis1,2, G. Kenanakis1,A. Selimis1, M. Vamvakaki1,2,M. Farsari1, M. Kafesaki1,2,C.M. Soukoulis1,3, and E.N.Economou1; 1Institute ofElectronic Structure and Laser(I.E.S.L.), Foundation forResearch & Technology-Hellas(FO.R.T.H.), Heraklion,Greece; 2Department of Mate-rials Science and Technology,University of Crete, Heraklion,Greece; 3Ames Laboratory-USDOE and Department ofPhysics and Astronomy, Ames,Iowa, United StatesA 3D infrared metallic meta-material with asymmetrictransmission is presented.�e structure was fabricatedby nonlinear lithography andselective electroless silvercoating; a novel techniqueproducing mechanically andchemically stable photonicstructures.
CD-3.4 SUN (Invited) 14:15PT symmetry in optics andnonlinear optics�M. Heinrich, M.-A. Miri,M. Khajavikhan, and D.Christodoulides; CREOL,�e College of Optics andPhotonics, University ofCentral Florida, Orlando,United StatesParity-time (PT)-symmetricarrangements can lead to un-usual optical properties bothin the linear and nonlinearregimes. Here, we reviewrecent developments in thephysics and applicationsof PT-symmetric opticalsystems.
CK-3.4 SUN 14:30Nanowire in PhotonicCrystal Visible Light Source�C. Wilhelm1,2, S. Combrié3,M. Iqbal4, G. Lehoucq3,Q. Xiong4, C. Soci2,4, andA. De Rossi3; 1School ofEEE, Nanyang TechnologicalUniversity, Singapore, Sin-gapore; 2CINTRA, Nanyang
EG-3.4 SUN 14:30Tuning the photon indistin-guishability in semicon-ductor quantum dotsR. Proux1−5, M. Maragkou1−5,E. Baudin1−5, C. Voisin1−5,P. Roussignol1−5, and �C.Diederichs1−5; 1LaboratoirePierre Aigrain, 24 rueLhomond, Paris, France;
CM-3.4 SUN 14:30Monocrystalline siliconpillar created by opticalvortex pulse illumination�F. Takahashi1, S. Takizawa1,H. Fujiwara1, K. Miyamoto1,R. Morita2,3, and T.Omatsu1,3; 1Chiba University,Chiba, Japan; 2HokkaidoUniversity, Sapporo, Japan;
CJ-3.5 SUN 14:30Polarizing Large Mode AreaPhotonic BandGap FiberA. Baz, �L. Bigot, J.-P.Yehouessi, O. Vanvincq, G.Bouwmans, and Y. Quiquem-pois; CNRS - Université Lille 1,Villeneuve d’Ascq, FranceWe report on a polarizing,large mode area, solid-core
CA-3.5 SUN 14:305kW burst-modefemtosecond ampli�ersystem for the EuropeanXFEL pump-probe laserdevelopment�M. Kellert1, M. Pergament1,K. Kruse1, J. Wang1, G.Palmer1, G. Priebe1, L.Wissmann1, U. Wegner1,
CE-3.4 SUN 14:30Optical activity in dielectric8-srs nets�F. Turella1, B. Cumming1, G.Schröder-Turk2, and M. Gu1;1Centre for Micro Photonics,Faculty of Science, Engineer-ing andTechnology, SwinburneUniversity of Technology, Mel-bourne, Australia; 2School of
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higher order soliton dynam-ics in optical �bers. Instead ofbreaking up into several soli-tons, it completely disappearsin a dramatic explosion-likeprocess, being fully irradiatedto dispersive waves.
and tested in the mid-infraredregion at 5.2 microns for the�rst time. Intrinsic Q up to130,000 and losses <0.7dB/cmare shown.
lasers, Hamburg, Germany;3Hamburg center for ultrafastimaging, Hamburg, Germany;4University of Hamburg,Hamburg, GermanyOptical recti�cation usingtilted-pulse-fronts is shownto be a self-limiting process.�e large spectral broadeningof the pump accompanyingTHz generation dramaticallyenhances dispersive e�ectsleading to pulse break-upand termination of terahertzgeneration
Canada; 3Centre de Physique�eorique, CNRS, EcolePolytechnique, Palaiseau,FranceWe show that dispersivewaves can be triggered by astrong pulse from a week co-propagating seed. Employinga seed in the terahertz regionwe show emission of a bluedispersive wave (425 nm).
Italy; 2Dipartimento di �sica,Politecnico di Milano, Milano,Italy; 3Dipartimento di elet-tronica, Politecnico di Milano,Milano, Italy; 4CambridgeGraphene Centre, Universityof Cambridge, Cambridge,United Kingdom; 5Center forNano Science and Technologyat PoliMi, IIT, Milano, ItalySpin and valley dynamics ofmonolayer MoS2 are investi-gated by time-resolved circu-lar dichroism and Faraday ro-tation. �e combination ofthese techniques allows to dis-entangle the time scale of boththe inter- and intra-valley re-laxation processes.
satellite cores arranged in aring around its axis supportsfour non-degenerate helicalBloch modes with dominantOAM orders l = ±1 and ±2.
EA-3.2 SUN 14:15Programming QuantumInterference in ScatteringMaterials�T.A.W. Wolterink, G. Ctis-tis, S.R. Huisman, T.J. Huis-man, A.P. Mosk, and P.W.H.Pinkse; MESA+ Institute forNanotechnology, University ofTwente, Enschede,�e Nether-landsWe demonstrate a methodto program general multiportlinear optical circuits in scat-tering materials. Applied tolight from our bright single-photon source this methodenables adaptive quantum op-tical experiments.
EF-3.4 SUN 14:15Accelerating and lockedRaman solitons inmicro-ring resonators: Rolein supercontinuumgeneration�C. Milian1, A. Gorbach2,M. Taki3, and D. Skryabin2;1Ecole Polytechnique,Palaiseau, France; 2BathUniversity, Bath, UnitedKingdom; 3Universite Lille,Lille, FranceWe show that micro-ring cav-ities with Raman e�ect sup-port locked and acceleratingsolitons that a�ect supercon-tinuum generation
CH-3.3 SUN 14:15Radiocarbon Detection withQuantum Cascade LaserBased Cavity Ring-DownSpectroscopyG. Genoud1, M. Vainio1,H. Phillips2, J. Dean2,�A. Manninen1, and M.Merimaa1; 1VTT TechnicalResearch Centre of Finland,Espoo, Finland; 2NationalPhysical Laboratory, Tedding-ton, United KingdomWe present a real-timeinstrument for radiocarbondetection in carbon dioxide,based on cavity ring-downspectroscopy and mid-infrared quantum cascadelaser. Results for elevatedradiocarbon concentrationsare presented.
CC-3.4 SUN 14:15Terahertz brightness at theextreme: Demonstration of alow frequency 8.3 GV/m λ3THz bullet�M. Shalaby1 and C. Hauri1,2;1PAul Scherrer Institut, Villi-gen, Switzerland; 2EPFL, Lau-sanne, SwitzerlandWe present a THz focusingscheme where high energyTHz pulses are con�ned tothe least possible 3D lightbullet volume of wavelength-cubic with peak �elds up to8.3*GV*m*1 and 27.7*T
EE-3.4 SUN 14:15Dispersive Waves in aSynchronously PumpedPassive Kerr CavityK. Luo, Y. Xu, M. Erkin-talo, and �S. Murdoch; PhysicsDept, University of Auckland,Auckland, New ZealandWe consider theoretically andexperimentally the generationof dispersive waves in a Kerrcavity. A phasematchingrelation predicts dispersivewaves in both dispersionregimes, with dispersive wavefrequency shi�s modi�ed bythe cavity phase detuning.
JSIV-1.3 SUN 14:15Exciton-exciton annihilationand stimulated emission inGraphene Nanoribbons�G. Soavi1, S. Dal Conte2, C.Manzoni2, F. Scotognella1,A. Narita3, X. Feng3, K.Muellen3, and G. Cerullo1,2;1Politecnico di Milano,Milano, Italy; 2IFN-CNR,Milano, Italy; 3Max PlanckInstitute for Polymer Research,Main, GermanyExciton-exciton annihilationin graphene nanoribbons isstudied by means of ultrafastpump-probe spectroscopy.�is process leads to thedelayed formation of a red-shi�ed stimulated emissionsignal, that we assign tobiexcitons.
CI-3.4 SUN 14:15A 3R Regeneration Schemefor Highly Spectral E�cientSignal Waveforms�M. Sorokina, A. Perentos, A.Ellis, S. Turitsyn, and S. Sygle-tos; Aston Institue of Pho-tonic Technologies, Birming-ham, United KingdomWe propose a new regen-eration scheme for highlyspectral e�cient formatsand through numericalsimulations we prove itsnecessity against traditional2R solutions for future highcapacity systems
EA-3.3 SUN 14:30Quantum enhancedabsorption spectroscopy�H. Dinani1,2, M. Gupta3,D. Berry1, and J. Dowling3;1Department of Physicsand Astronomy, MacquarieUniversity, Sydney, Australia;2ARC Centre of Excellence forEngineered Quantum Systems,
EF-3.5 SUN 14:30Adiabatic soliton laserS. Turutsyn1,2 and �A.Bednyakova2,3; 1AstonInstitute of Photonic Tech-nologies, Birmingham, UnitedKingdom; 2Novosibirsk StateUniversity, Novosibirsk,Russia; 3Institute of Com-putational Technologies,
CH-3.4 SUN 14:30Low-noise Applications of aMid-Infrared Supercon-tinuum Source�J. Ramsay1, S. Dupont1, T.Ringsted2, S.B. Engelsen2, andS.R. Keiding1; 1Departmentof Chemistry, Aarhus Uni-versity, Aarhus, Denmark;2Department of Food Science,
CC-3.5 SUN 14:30Generation and NonlinearDistortion of High-EnergyTHz Pulses from LiNbO3Z. Ollmann2, C. Lombosi2,G. Polónyi2, L. Pálfalvi2, J.Hebling1,2, and �J.A. Fülöp1,3;1MTA-PTE High-Field Tera-hertz Research Group, Pécs,Hungary; 2University of Pécs,
EE-3.5 SUN 14:30Acoustic bunching of arandom temporal cavitysoliton patternK. Luo, J.K. Jang, �M. Erkin-talo, S. Coen, and S.G. Mur-doch; Dodd-Walls Centre andPhysics Department, �e Uni-versity of Auckland, Auckland,New Zealand
JSIV-1.4 SUN 14:30Micro�ber-Based, HighlyNonlinear GrapheneSaturable Absorber forGeneration of Rogue Wavesin a Fiber LaserA.-P. Luo, Z.-R. Cai, M. Liu,�Z.-C. Luo, andW.-C. Xu; Lab-oratory of Nanophotonic Func-tional Materials and Devices,
CI-3.5 SUN 14:30Simultaneous Reproductionof Two Datapages forIncreasing Data-TransferRate in Holographic DataStorage�T. Muroi, Y. Katano, N.Kinoshita, and N. Saito; JapanBroadcasting Corporation(NHK), Tokyo, Japan
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Technological University,Singapore, Singapore; 3�alesResearch and Technology,Palaiseau, France; 4Schoolof SPMS, Nanyang Techno-logical University, Singapore,SingaporeWe demonstrate a �exibleplanar fabrication approachfor the integration of semi-conductor nanowires intophotonic crystals. We reportsharp photoluminescencepeaks at well-controlled wave-length in the visible spectralrange, at room temperature
2Ecole Normale Supérieure- PSL Research University,Paris, France; 3CNRS, Paris,France; 4Université Pierreet Marie Curie - SorbonneUniversités, Paris, France;5Université Paris Diderot -Sorbonne Paris Cité, Paris,FranceBy studying the temporal pro-�le of the photon coalescencephenomenon in a HOM ex-periment, we show that the in-distinguishability of photonsemitted by a cw resonantlydriven quantum dot can betuned by the laser.
3CREST, JST, Kawaguchi,JapanWe discover that a sin-gle optical vortex pulseillumination can fabricatemono-crystalline silicon pillarwith a height of >15 um and atip curvature of ~180 nm.
photonic bandgap �ber withhetero-structured cladding.Polarizing behavior is ob-tained together with a 34microns mode �eld diameteron a spectral window largerthan 30 nm.
M. Emons1, J. Morgenweg2,T. Mans2, and M. Lederer1;1European X-ray Free-ElectronLaser Facility GmbH, Albert-Einstein-Ring 19, Hamburg,Germany; 2Amphos GmbH,Kaiserstr. 100, Herzogenrath,Germany�e presented pump ampli�erproduces 1.35ms-bursts of5kW at 10Hz. At intra-burstrep-rates of 100kHz, singlepulses of 50mJ result. Beam�ltering/shaping leads tonearly di�raction limitedGaussian beams with 45mJsingle pulse energy.
Engineering and InformationTechnology, Murdoch Univer-sity, Perth, AustraliaWe present the direct laserfabrication and optical char-acterisation of dielectric 8-srs chiral photonic crystalswith four-fold rotational sym-metry. We experimentallydemonstrate the strong opti-cal activity and absence of cir-cular dichroism predicted bygroup theory.
CK-3.5 SUN 14:45A Small-footprintNanobeam Laser Printed ona Silicon Substrate�I. Karnadi1, J. Son2, J.-Y.Kim2, H. Jang1, S. Lee2,B. Min2, and Y.-H. Lee1;1Department of Physics,KAIST, Daejeon, Korea,South; 2Department of Me-chanical Engineering, KAIST,Daejeon, Korea, SouthA small-footprint nanobeamphotonic crystal laser madeof InGaAsP material is di-rectly integrated on a SiO2/Sisubstrate via transfer-printingprocess.
EG-3.5 SUN 14:45Sub-wavelengthLocalization of a SinglePhoton�G. Yuan1, S. Vezzoli1, C.Altuzarra1, E.T.F. Rogers2,C. Couteau1, C. Soci1, Z.Shen1, and N.I. Zheludev1,2;1Centre for DisruptivePhotonic Technologies,Nanyang Technological Uni-versity, Singapore, Singapore;2Optoelectronics ResearchCentre and Centre for PhotonicMetamaterials, Southampton,United KingdomWe report the �rst experimen-tal demonstration of super-oscillatory behaviors in sin-gle photon regime, where thewave-function of a single pho-ton is localized into lengthscale smaller than the small-est wave length in its Fourierspectrum.
CM-3.5 SUN 14:45Processing of glass withembedded metallicnanoparticles using aradially and azimuthallypolarized picosecond pulsedlaserM. Tyrk, S. Zolotovskaya, W.Gillespie, and �A. Abdolvand;University of Dundee, Dundee,United KingdomWe report on radially and az-imuthally polarized picosec-ond pulsed laser reshapingof silver nanoparticles embed-ded in glass. �is robustmethod allows for a very spe-cial elongation of the origi-nally spherical nanoparticlesin one step.
CJ-3.6 SUN 14:45Low-loss large mode areapixelated andheterostructured BraggFiber�J.-P. Yehouessi, A. Baz, L.Bigot, G. Bouwmans, O.Vanvincq, M. Douay, and Y.Quiquempois; Laboratoire dePhysique des Lasers, Atomes etMolécules, Villeneuve d’Ascq,FranceWe submit a new type ofAll-solid Photonic BandgapFiber with a mode-�elddiameter of 40 micron at1050nm. �e �ber exhibitssingle-mode behavior from1000nm to 1700nm withlosses as low as 25 dB/km.
CA-3.6 SUN 14:45DiPOLE100: A 100 J, 10 Hzcryogenically cooledYb:YAG diode pumpedsolid-state laser�T. Butcher, P. Mason, S.Banerjee, K. Ertel, J. Phillips,J. Smith, M. de Vido, S.Tomlinson, O. Chekhlov, W.Shaikh, C. Hernandez-Gomez,J. Greenhalgh, and J. Col-lier; Central Laser Facility,STFC, Rutherford AppletonLaboratory, Didcot, UnitedKingdomWe present recent per-formance results fromDiPOLE100, a 100 J, 10 HzDPSSL using cryogenicallycooled Yb:YAG multi-slabampli�er technology.
CE-3.5 SUN 14:45photonic spin hall e�ectwith nearly 100% e�ciency�W. Luo1, S. Ma1, S. Xiao1, Q.He1,2, S. Sun3, and L. Zhou1,2;1State Key Laboratory ofSurface Physics and KeyLaboratory of Micro andNano Photonic Structures(Ministry of Education),Fudan University, Shanghai200438, China, Shanghai,China, People’s Republic of(PRC); 2Collaborative Inno-vation Center for AdvancedMicrostructures, Nanjing,China, People’s Republicof (PRC); 3Shanghai Engi-neering Research Center ofUltra-Precision Optical Man-ufacturing, Fudan University,Shanghai, China, People’sRepublic of (PRC)We demonstrate that a gi-ant PSHE with ~100% e�-ciency can be realized at cer-tain meta-surfaces with deep-subwavelength thicknesses.
CD-3.5 SUN 14:45Space and time-resolvedstudy of plasma columnsgenerated by laser�lamentation guidedelectric discharges�G. Point, L. Arantchouk, Y.Brelet, J. Carbonnel, Y.-B.André, A. Mysyrowicz, andA. Houard; Laboratoired’Optique Appliquée - ENSTA,Ecole Polytechnique, CNRS,Palaiseau, FranceWe developed a two-color in-terferometric plasma diagnos-tic for laser �lamentation trig-gered discharges in air. �e in-terferometer is then used oncm-scale discharges to inves-tigate the link between cur-rent waveforms and the elec-tron density.
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ROOM 14c ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2
Macquarie University, Sydney,Australia; 3Hearne Institutefor �eoretical Physics andDepartment of Physics andAstronomy, Louisiana StateUniversity, Baton Rouge,United StatesWe propose an interferomet-ric approach to measure theresonance frequency of a sys-tem of two level atoms. Weshow that by using certaintype ofmultiphoton entangledstates we beat the standardquantum limit.
Novosibirsk, RussiaWe propose a new concept oflaser based on adiabatic am-pli�cation of soliton pulse inthe cavity. Adiabatic change ofthe soliton parameters relaxesthe restriction on the pulseenergy inherent in traditionalsoliton lasers.
University of Copenhagen,Copenhagen, DenmarkUsing a polarization in-dependent pulse-to-pulsenormalization scheme, theapplicability of mid-infraredsupercontinuum sourcesis enhanced remarkably.�e improved sensitivity isdemonstrated in transmissionand re�ection spectroscopy ofgrains, soils and gasses.
Pécs, Hungary; 3ELI-ALPS,ELI-Hu Nk�., Szeged, Hun-gary0.4-mJ THz pulses, suitablefor charged-particle manipu-lation, were generated with0.77% e�ciency in LiNbO3by tilted-pulse-front pump-ing. �e spectral peak isabout 0.2 THz. NonlinearTHz beam distortions wereobserved, caused by THz-induced cascading e�ects.
We report on the experimen-tal observation of temporalcavity soliton bunching ina coherently-driven passive�ber resonator. Hundredsof ultrafast cavity solitonswith random separationsself-organize into orderlybunches through interactionswith transverse acousticwaves.
South China Normal Univer-sity, Guangzhou, China, Peo-ple’s Republic of (PRC)We reported on the obser-vation of rogue waves in a�ber laser mode-locked by amicro�ber-based, highly non-linear graphene saturable ab-sorber. �e results would fur-ther reveal the fundamentalphysics of rogue waves in �berlasers.
We proposed reproductionmethod that can reproducetwo datapages by enter-ing the reference beamswith p-polarization and s-polarization in the hologramssimultaneously. �is methodenables a data-transfer rate oftwice that of the conventionalmethod.
EA-3.4 SUN 14:45Spatial distinguishabilityand induced coherenceA. Heuer, K. Pinkal, and �R.Menzel;University of Potsdam,Potsdam, Germany�e in�uence of the spatialdistinguishability of idler pho-tons on the interference vis-ibility in an induced coher-ence setup was examined. �edistinguishability was accom-plished by mode conversionwith an additional phase plate.
EF-3.6 SUN 14:45Collision between solitonand dispersive wave inphase-mismatchedquadratic nonlinear crystals�X. Liu, B. Zhou, H. Guo, andM. Bache; Technical Univer-sity of Denmark, DK-2800 Kgs.Lyngby, Denmark�rough simulations we showthat a self-defocusing soli-ton colliding with a weakbroadband probe in a phase-mismatched quadratic non-linear crystal e�ciently gen-erates a mid-IR idler. Com-pletely depleting the probe re-lies on exciting a higher-ordersoliton.
CH-3.5 SUN 14:45Broad-band Source forOptical Gas Sensing at 5.6 -5.9 �m�A. Koshkinbayeva1, R.Orobtchouk2, M. Brun1, M.Carras3, and P. Labeye1;1CEA, LETI, MINATECCampus, Grenoble, France;2Institut des Nanotechnolo-gies de Lyon (INL), CNRSUMR5270, Université de Lyon,INSA-Lyon, Villeurbanne,France; 3III-V Lab, Palaiseau,FranceWe present a Si-integratedmid-infrared broad-bandsource composed of a laserarray integrated with anAWG type multiplexer in therange of 1700-1802 cm-1 formultiple gases optical sensor.
CC-3.6 SUN 14:45Strong �eld tunable over theentire THz gap�C. Vicario1, B. Monoszlai1,M. Jazbinsek2, S.-H. Lee3, O.-P. Kwon3, and C.p. Hauri1,4;1SwissFEL Paul ScherrerInstitute, Villigen- PSI,Switzerland; 2Rainbow Pho-tonics, Zurich, Switzerland;3Department of MolecularScience and Technology, AjouUniversity, Suwon, Korea,South; 4Ecole PolytechniqueFederale de Lausanne,Lausanne, SwitzerlandBy optical recti�cation inHMQ-TMS we realizedsingle-cycle MV/cm THzpulses with tunable frequencyover the entire THz gapand duration over the rangebetween 70 fs and 1 ps.
EE-3.6 SUN 14:45Extreme events and phasedynamics in forcedoscillatory media�F. Gustave1, L. Columbo2,F. Prati3, M. Brambilla2, G.Tissoni1, and S. Barland1;1Université de Nice-CNRSUMR7335 Institut NonLinéaire de Nice, Valbonne,France; 2DipartimentoInterateneo di Fisica,Università degli Studi ePolitecnico di Bari, Bari, Italy;3Dipartimento di Scienza eAlta Tecnologia, Universitàdell’Insubria, Via Valleggio 11,Como, ItalyWe experimentally analyzeextreme events in a fast(nanosecond) spatially ex-tended oscillatory mediumwith coherent forcing. Wefocus on the predictability ofindividual events and theiremergence in the (spatio-temporally resolved) opticalphase dynamics.
JSIV-1.5 SUN 14:45Bandgap RenormalizationGoverns the UltrafastResponse of Single-layerMoS2�E.A.A. Pogna1, S. Dal Conte1,M. Marsili2, D. Prezzi2, D.Sangalli3, C. Manzoni1, A.Marini3, D. De Fazio4, M.Bruna4, I. Goykhman4, A.Ferrari4, and G. Cerullo1;1Physics Department - Politec-nico di Milano, Milano, Italy;2CNR- Istituto Nanoscienze,Modena, Italy; 3CNR -Istituto di Struttura dellaMateria, Montelibretti, Italy;4Cambridge Graphene Center,Cambridge, United KingdomComparison of theoreticalsimulations in real time withultrafast transient transmit-tivity measurements allows tounveil the fundamental role ofband gap renormalization toquantatively describe the nonequilibrium optical responseof MoS2 single-layer.
CI-3.6 SUN 14:45Development ofultra-broadband UTC-PDmodule beyond 110 GHzwithout bias circuit�T. Umezawa, K. Akahane, N.Yamamoto, A. Kanno, and T.Kawanishi; National Instituteof Information and Commu-nications Technology, Tokyo,JapanWe report a new ultra-broadband photodetectormodule beyond 110 GHzwithout any bias circuits,using low carrier concen-tration in carrier collectionlayer in UTC structure, inorder to consider large-scalephotonic integration forfuture technology.
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CLEO®/Europe-EQEC 2015 ⋅ Sunday 21 June 2015
ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14b15:30 – 17:00EG-4: Probing NanoscaleElectromagnetic FieldsChair: Erez Hasman, Technion,Haifa, Israel
15:30 – 17:00CM-4: 3D Device LaserWritingChair: Tagashige Omatsu, ChibaUniversity, Chiba, Japan
15:30 – 17:00CJ-4: Characterization andPassive Components forFibre Laser SystemsChair: Matthias Jäger, Leibniz-Institut für Photonische Technolo-gien, Jena, Germany
15:30 – 17:00CA-4: Nanosecond 2�mSolid-state LasersChair: Federico Pirzio, University ofPavia, Pavia, Italy
15:30 – 17:00CE-4: Silicon PhotonicsChair: Kerstin Volz, Philipps-Universität Marburg, Marburg,Germany
15:30 – 17:00CD-4: MIRWavelengthGenerationChair: Mario Bertolotti, La SapienzaUniversita’ di Roma, Roma, Italy
EG-4.1 SUN 15:30Optical Singularities in PlasmonicFields near Single SubwavelengthHoles�A. de Hoogh, N. Rotenberg, andK. Kuipers; FOM Institute AMOLF,Amsterdam,�e NetherlandsWe identify phase and polarizationsingularities in the electric in-plane�eld distribution of the scattering ofsurface plasmon polaritons from asubwavelength hole on a gold �lmthrough both near-�eld measure-ments and theoretical modelling.
CM-4.1 SUN 15:30Flexible tuning of femtosecondwritten �ber Bragg gratings�T.A. Goebel1, C. Voigtländer1,R.G. Krämer1, C. Reinlein2, M.Appelfelder2, A. Tünnermann1,2,and S. Nolte1,2; 1Institute of AppliedPhysics, Abbe Center of Photonics,Friedrich-Schiller-Universität Jena,Jena, Germany; 2Fraunhofer Insti-tute for Applied Optics and PrecisionEngineering, Jena, GermanyWe combine the phase mask tech-nique with a specially designed highpower optimized deformablemirrorfor a �exible tuning of the periodof femtosecond written �ber Bragggratings.
CJ-4.1 SUN 15:30�e Measurement of Fibre CoreLoss using an E�cient, HighPower Mid-Infrared Fibre Laser�S. Crawford1, D.D. Hudson1, andS.D. Jackson2; 1Centre for Ultrahighbandwidth Devices for Optical Sys-tems (CUDOS), Institute of Photon-ics and Optical Science, School ofPhysics, �e University of Sydney,Sydney 2006, Australia; 2MQ Pho-tonics, Department of Engineering,Macquarie University, North Ryde2109, AustraliaA Ho3+Pr3+ co-doped ZBLAN �-bre laser is presentedwith high pow-ered (7.2 W), broadly wavelengthtunable (2825-2975 nm) emission,which is used in the characterisa-tion of core loss in rare-earth doped,double clad �uoride �bres.
CA-4.1 SUN 15:30Femtosecond High EnergyRegenerative Ampli�er Operatingat 1937 nm�A. Wienke1, D. Wandt1, U.Morgner2, J. Neumann1, and D.Kracht1; 1Laser Zentrum Hannovere.V., Laser Development Depart-ment, Ultrafast Photonics Group,Hannover, Germany; 2Institut fürQuantenoptik, Leibniz UniversitätHannover, Hannover, GermanyA regenerative ampli�er based on aTm:YAP crystal generates high en-ergy femtosecond pulses at a wave-length of 1937 nm with an uncom-pressed pulse energy of >0.709 mJ.�e pulses can be compressed to<410 fs.
CE-4.1 SUN (Keynote) 15:30Silicon Photonics: an Enabler forFundamental Science, for theInternet and for the Life Sciences�R. Baets; Ghent University - imec,Ghent, BelgiumIn this keynote talk the rapid devel-opment of the �eld of silicon pho-tonics is reviewed and an outlookis given on its potential to enable abroad range of applications as wellas fundamental science.
CD-4.1 SUN 15:30Deep-Infrared FemtosecondOptical Parametric OscillatorSynchronously-Pumped by aTi:sapphire LaserV. Ramaiah-Badarla1, A. Esteban-Martin1, S.C. Kumar1, K. Devi1,K.T. Zawilski2, P.G. Schuneamann2,and �M. Ebrahim-Zadeh1,3; 1ICFO-�e Institute of Photonic Sciences,Barcelona, Spain; 2BAE Systems,Nashua, United States; 3InstitucioCatalana de Recerca i Estudis Avan-cats (ICREA), Barcelona, SpainWe report a femtosecond OPO forthe deep-IR synchronously-pumpedby a Ti:sapphire laser. Using novelintracavity-cascaded pumping, tun-able generation across 6-8 �m isachieved with high output stabilityand good beamquality at room tem-perature.
EG-4.2 SUN 15:45Visualizing Optical Rogue Wavesat the Nanoscale in ChaoticPhotonic Crystal Cavities�R. van der Wel1, N. Rotenberg1, C.Liu2, A. Di Falco3, A. Fratalocchi2,T. Krauss4, and K. Kuipers1; 1FOMInstitute AMOLF, Amsterdam, �eNetherlands; 2King Abudullah Uni-versity of Science and Technology,�uwal, Saudi Arabia; 3University ofSt. Andrews, St. Andrews, UnitedKingdom; 4University of York, York,United KingdomUsing near-�eld optical microscopywe measure rogue waves insidechaotic photonic crystal cavitiesand study frequency-frequencyand space-space correlations toobtain quantitative parameters todescribe properties such as lossesand coherence.
CM-4.2 SUN 15:45Direct writing of long-period and�ber Bragg gratings in specialty�bers by femtosecond laser pulsesat the wavelength of 1026 nm�A.A. Wolf1, A.V. Dostovalov1, andS.A. Babin1,2; 1Institute of Au-tomation and Electrometry SB RAS,Novosibirsk, Russia; 2NovosibirskState University, Novosibirsk, Russia�ere are presented experimentalresults on direct writing of �berBragg gratings through polyimideprotective coating, as well aslong-period �ber gratings inpolarization-maintaining �ber byfemtosecond laser pulses at thewavelength of 1026 nm.
CJ-4.2 SUN 15:45Spatio-temporal dynamics of aComposite Soliton regime in aPassively Mode Locked FiberLaser�S. Sugavanam1, A. El Taher1,D. Churkin1,2,3, and S. Turitsyn1;1Aston Institute of Photonic Tech-nologies, Aston University, UnitedKingdom; 2Institute of Automationand Electrometry, Novosibirsk, Rus-sia; 3Novosibirsk State University,Novosibirsk, RussiaA stable composite soliton regimeobserved in a passively mode locked�ber laser is characterized using themethod of spatio-temporal dynam-ics. Observed high intensity eventsare attributed to periodic intersec-tions of the pulse complexes.
CA-4.2 SUN 15:45Highly stable and high pulseenergy, double-z-cavity shapedHo:YLF Regenerative Ampli�er�P. Kroetz1,2, A. Ruehl3, G.Chatterjee3, K. Murari1,3,4, H.Cankaya1,3,4,5, A.-L. Calendron1,3,5,F.X. Kärtner1,3,4,5, I. Hartl3,and R.J.D. Miller1,2,5,6; 1CFEL,Hamburg, Germany; 2MPI for theDynamics and Structure of Matter,Hamburg, Germany; 3DESY, Ham-burg, Germany; 4Dep. of Physics,University Hamburg, Hamburg,Germany; 5�e Hamburg Centre forUltrafast Imaging, CUI, Hamburg,Germany; 6Dep. of Physics andChemistry, University of Toronto,Toronto, Canada�e design of a double-z-cavityshapedRegenerative Ampli�er (RA)system is presented. Numerical sim-ulations reveal a highly stable sec-ond stability point that allows highenergy extraction and low-noise op-eration.
CD-4.2 SUN 15:45High peak power opticalparametric ampli�cation of a 7-9�m tunable external-cavityquantum cascade laser source�F. Gutty1, A. Grisard1, C. Larat1,A. Joly1, M. Antier1, D. Papillon1,B. Gérard2, R. Ostendorf3, andE. Lallier1; 1�ales Research &Technology France, Palaiseau,France; 2III-V Lab, Palaiseau,France; 3Fraunhofer Institute forApplied Solid State Physics IAF,Freiburg, GermanyWe demonstrate the ampli�-cation of an EC-QCL tunablefrom 7.5 to 9 microns with anOPA without any moveable partexploiting quasi-phase matchingin orientation-patterned GaAswith an acousto-optically tunablethulium-doped pulsed �ber pump.
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CLEO®/Europe-EQEC 2015 ⋅ Sunday 21 June 2015
ROOM 14c ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON215:30 – 17:00EA-4: OptomechanicsChair: David Hunger, Ludwig-Maximilians-Universität München(LMU), Munich, Germany
15:30 – 17:00CH-4: Bio-medical SensingChair: Laura M. Lechuga, InstitutICN2/CSIC, Bellaterra, Spain
15:30 – 17:00CC-4: THz Coherent Controland SpectroscopyChair: Daniele Brida, University ofKonstanz, Konstanz, Germany
15:30 – 17:00EE-4: Attosecond and HighField PhysicsChair: Howard Milchberg, Univer-sity of Maryland, Maryland, USA
15:30 – 17:00JSIV-2: Graphene Plasmonicsand DevicesChair: �omas Müller, Vienna Uni-versity of Technology, Vienna, Aus-tria
15:30 – 17:00CI-4: Advanced OpticalSolutionsChair: Juan Diego Ania-Castanon,Instituto de Óptica, CSIC, Madrid,Spain
EA-4.1 SUN (Invited) 15:30New Frontiers in QuantumOptomechanics: from levitationto gravitational quantum physics�M. Aspelmeyer; University of Vi-enna, Faculty of Physics, VCQ, Vi-enna, AustriaI will discuss the status of recentnew developments in the �eld ofquantum optomechanics. Speci�-cally, the potential of levitated mas-sive particles in optomechanics ex-periments, and possible future ex-periments at the gravity-quantuminterface.
CH-4.1 SUN (Invited) 15:30A novel label-free biosensingplatform using interference e�ectin an exposed core optical �bre�L. Nguyen1,2, K. Hill1,3, S. Warren-Smith2, and T. Monro2,4,5; 1PlantBiosecurity Cooperative ResearchCentre, Bruce, ACT 2617, Australia;2Institute for Photonics and Ad-vanced Sensing, School of Chemistryand Physics, �e University of Ade-laide, Adelaide SA 5005, Australia;3South Australian Research andDevelopment Institute, UrrbraeSA 5064, Australia; 4Universityof South Australia, Adelaide SA5005, Australia; 5ARC Centre ofExcellence for NanoBio Photonics,�e University of Adelaide, AdelaideSA 5005, AustraliaA novel biosensor using the in-terference e�ect within an exposedcore microstructured optical �bre(ECF), in conjunction with func-tionalization of the �bre core us-ing fuzzy nanoassembly process andbiotin-streptavidin binding is pro-posed and experimentally demon-strated.
CC-4.1 SUN 15:30Coherent control of injectioncurrents in high-quality �lms ofBi2Se3�D. Bas, K. Vargas-Velez, S. Babaki-ray, T. Johnson, P. Borisov, D.Lederman, and A. Bristow; WestVirginia University, Morgantown,United StatesShi� currents and injection currentsare produced and observed in thin-�lm bismuth selenide of varyingthicknesses. Sample thickness, an-gle, and pump intensity studies arecompared with known signatures toidentify surface state contribution.
EE-4.1 SUN (Tutorial) 15:30Population trapping,�lamentation and applications�S.L. Chin; Center for Optics, Pho-tonics and Laser (COPL), Laval Uni-versity, Quebec City, Canada�e contribution has been with-drawn by the authors.
JSIV-2.1 SUN (Invited) 15:30Two-Dimensional Optics withGraphene Plasmons�R. Hillenbrand; CIC nanoGUNEand UPV/EHU, San Sebastián,Spain; IKERBASQUE, BasqueFoundation for Science, Bilbao,SpainNear-�eld microscopy is employedto demonstrate the re�ection, re-fraction and focusing of propagat-ing graphene plasmons launched bymetal tips and tailored metal anten-nas, constituting an essential step forthe development of future grapheneplasmonic circuits.
CI-4.1 SUN (Invited) 15:30Passive ampli�cation andreal-time averaging of repetitivewaveforms by Talbot e�ect�J. Azana1, R. Maram1, J. VanHowe1,2, and M. Li1,3; 1Institut Na-tional de la Recherche Scienti�que(INRS) * Energie, Matériaux et Télé-communications, Montreal, Canada;2Department of Physics and Astron-omy, Augustana College, Rock Is-land, United States; 3State Key Labo-ratory on Integrated Optoelectronics,Institute of Semiconductors, ChineseAcademy of Sciences, Beijing, China,People’s Republic of (PRC)We review recent work on a methodfor intensity ampli�cation ofrepetitive signals without usingactive gain. �is passive ampli�erimproves random intensity noisepresent on the input signal similarlyto a real-time averaging process.CC-4.2 SUN 15:45
Spin wave excitation andmanipulation in cantedantiferrimagnetics with THzpulses�G.-H. Ma, Z. Jin, J. Jiang, and S.Cao; Department of Physics, Shang-hai University, Shanghai, China,People’s Republic of (PRC)�e contribution has been with-drawn by the authors.
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ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a ROOM 14bEG-4.3 SUN 16:00Near-�eld characterization ofdisordered nano-materials�V. Parigi1, E. Perros1, A. Maitre2,3,R. Carminati1, V. Krachmalnico�1,and Y. DeWilde1; 1ESPCI ParisTech,PSL Research University, CNRS,Institut Langevin, Paris, France;2Sorbonne Universités, UPMCUniv. Paris 06, UMR 7588, Institutdes NanoSciences de Paris, Paris,France; 3CNRS, UMR 7588, Institutdes NanoSciences de Paris, Paris,FranceTailoring light-matter interactionsat the nano-scale require appro-priate characterisation tools: wewill show experimental results ofspatial characterization of di�erentvolume-disordered dielectric sam-ples from correlations in near-�eldspeckle patterns measured by scan-ning optical microscopy
CM-4.3 SUN 16:00Femtosecond Laser Written FibreBragg Gratings with ArbitraryRe�ection and Dispersion Pro�les�S. Antipov1,2, M. Ams1,2, R.Williams2, A. Fuerbach1,2, and M.Withford1,2; 1Centre for Ultrahigh-bandwidth Devices for OpticalSystems (CUDOS), Sydney, Aus-tralia; 2MQ Photonics ResearchCentre, Sydney, AustraliaWe report on a novel femtosec-ond laser core-scanning techniquethat enables the inscription of Fi-bre Bragg gratings (FBGs) with tai-lored re�ection and dispersion pro-�les into optical �bres with arbitrarycore size.
CJ-4.3 SUN 16:00Novel Angle-ResolvedInterrogation Method forDouble-Clad Doped Fibers andHigh-Power Fiber LaserComponents�G.Y. Chen1, C.A. Codemard2, J.S.Chan1, P.M. Gorman2, and M.N.Zervas1,2; 1Optoelectronics ResearchCentre, University of Southampton,Southampton, United Kingdom;2Advanced Laser Laboratory,SPI Lasers, Southampton, UnitedKingdomFor the �rst time an angle-resolvedmethod is exploited to deliver accu-rate information of the relative con-tribution of modes towards pumpabsorption and optical loss for thedesign of multimode �bers and �berlaser components.
CA-4.3 SUN (Invited) 16:002 �mWavelength, 39 mJ Energy,Picosecond Ho:YLF CryogenicChirped Pulse Ampli�er forMid-Infrared OPCPA�M. Hemmer1, D. Sánchez1, M.Jelínek2, V. Smirnov3, H. Jelinkova2,V. Kubecek2, and J. Biegert1,4;1ICFO-Institut de Ciencies Fo-toniques, Mediterranean TechnologyPark, Castelldefels, Barcelona,Spain; 2Czech Technical Universityin Prague, Faculty of Nucl. Sci-ences and Phys. Eng., Brehová 7,11519 Prague 1, Czech Republic;3OptiGrate Corp., 562 S. EconCircle, Oviedo, Florida 32765,United States; 4ICREA - InstitucióCatalana de Recerca i EstudisAvançats, Barcelona, SpainWe report on a 2 um wavelengthchirped pulse ampli�er system de-livering optical pulses with 39 mJenergy, 10 ps duration at 100Hz rep-etition rate. �e system is ideallysuited for pumping mid-IR OPC-PAs.
CD-4.3 SUN 16:00>100 mW, femtosecondmid-infrared optical parametricoscillator at 7 um�S. Chaitanya Kumar1, J. Krauth2,A. Steinmann2, K.T. Zawilski3, P.G.Schunemann3, H. Giessen2, andM. Ebrahim-Zadeh1,4; 1ICFO-�eInstittute of Photonic Sciences,Barcelona, Spain; 24th PhysicsInstitute and Research CenterSCOPE, University of Stuttgart,Stuttgart, Germany; 3BAE Systems,Incorporated, New Hampshire,United States; 4Institucio Catalanade Recerca i Estudis Avancats(ICREA), Bercelona, SpainWe report a mid-infrared femtosec-ond OPO based on CdSiP2 tun-able across 6786-7069 nm, generat-ing record power of 110-mW at 7um, with passive stability <3% rms(1-hour) in power and <0.1% rms(15-min) in wavelength.EG-4.4 SUN 16:15
Casimir-Polder interaction as ahighly-selective probe of thenear-�eld thermal emissionJ.C.d.A. Carvalho1, P. Chaves deSouza Segundo2, �A. Laliotis1, I.Maurin1, M. Oriá3, M. Chevrollier3,M. Ducloy1, and D. Bloch1; 1Lab.de Physique des Lasers, CNRS, Univ.Paris 13, Villetaneuse, France; 2Univ.Federal de Campina Grande, Cuité,PB, Brazil; 3Univ. Federal deParaíba, João Pessoa, BrazilAtomic re�ection spectroscopyprobes the temperature-dependenceof the Casimir-Polder interaction.�rough the coupling with surfaceresonances, the atom-surfaceinteraction can increase or decreasewith temperature, and the atomselectively absorb thermal energy
CM-4.4 SUN 16:15Arbitrary Waveplate Operationsin Integrated Optics�G. Corrielli1, A. Crespi1, R.Geremia1, L. Sansoni2,3, A.Santinelli3, R. Ramponi1, P.Mataloni3, F. Sciarrino3, and R.Osellame1; 1Consiglio Nazionaledelle Ricerche- Istituto di Fotonicae Nanotecnologie, Milano, Italy;2Integrated Quantum Optics,University of Paderborn, Paderborn,Germany; 3Università La Sapienza,dipartimento di �sica, Roma, ItalyWe propose a method for the fabri-cation of waveplates with arbitraryoriented optical axes in femtosec-ond laser written optical circuitsand we demonstrate the capabilityof performing arbitrary rotations ofpolarization encoded qubits on chip.
CJ-4.4 SUN 16:15Coherence Evaluation of OctaveSpanning Supercontinuum UsingCarbon Nanotube Fiber Laser andSimilariton Ampli�erY. Nomura1, Y. Sakakibara2, E.Omoda2, H. Kataura2, and �N.Nishizawa1; 1Nagoya University,Nagoya, Japan; 2AIST, Tsukuba,JapanOctave spanning coherent super-continuum with good �atness wasgenerated stably with carbon nan-otube �ber laser, simlariton ampli-�er, and normal dispersion highlynonlinear �ber. Coherence proper-ties of generated SCs were examinedwith heterodyne beat measurement.
CE-4.2 SUN 16:15A poly-Si on LiNbO3 photonicplatformG. Martinez-Jimenez1, G. Zisis1,F. Yohann1, H. Noel1, D. Grech2,H.M.H. Chong2, A.C. Peacock1,and �S. Mailis1; 1. OptoelectronicsResearch Centre, University ofSouthampton, Southampton, UnitedKingdom; 2School of Electronic andComputer Science, University ofSouthampton, Southampton, UnitedKingdomWe propose a poly-Silicon-on-lithium niobate photonic materialplatform realized by post annealing,using c.w. visible lasers, of thinamorphous Si �lms deposited onLiNbO3 single crystal substratesfor applications in the near/mid IRspectral region
CD-4.4 SUN 16:15Wavelength tuning of opticalparametric oscillation inwhispering gallery resonators forinfrared spectroscopy�S.-K. Meisenheimer1,2, J.U.Fuerst1, K. Buse1,2, and I. Breunig1;1Department of MicrosystemsEngineering - IMTEK, Universityof Freiburg, Freiburg, Germany;2Fraunhofer Institute for PhysicalMeasurement Techniques, Freiburg,GermanyControlled wavelength tuning inwhispering gallery resonators over100 nm is achieved by keeping thepump mode �xed. Radial poling oflithiumniobate with a period of 30.2�m allows quasi-phase-matching inthe infrared.
EG-4.5 SUN 16:303D LDOS mapping of a resonantoptical antenna using single�uorescent molecules�A. Singh1, P.M.d. Roque1, G.Calbris1, J.T. Hugall1, and N.F.v.Hulst1,2; 1ICFO - Institut deCiencies Fotoniques, Castelldefels(Barcelona), Spain; 2ICREA -
CM-4.5 SUN 16:30Direct Laser Writing of VolumeFresnel Zone Plates in Silicon�A. Turnali1, O. Tokel2, I. Pavlov2,and F.Ö. Ilday1,2; 1Department ofElectrical and Electronics Engineer-ing, Bilkent University, Ankara,Turkey; 2Department of Physics,Bilkent University, Ankara, Turkey
CJ-4.5 SUN 16:30Optimized Yb-doped Fibers andJoining Technology for E�cientEnd Pumped Monolithic HighPower Fiber Oscillators�A. Liem1, N. Haarlammert1, C.Matzdorf2, J. Nold1, S. Kuhn1, L.Kido1, V. Reichel1, T. Schreiber1, R.Eberhardt1, and A. Tünnermann1,2;
CA-4.4 SUN 16:30Passively Q-Switched Tm3+:LiGdF4Laser Using Cr2+:ZnSe asSaturable Absorber�B. Oreshkov1,3, S. Veronesi2, M.Tonelli2,3, A. di Lieto2,3, V. Petrov1,U. Griebner1, X. Mateos5, and I.Buchvarov4; 1Max Born Institute forNonlinear Optics and Short Pulse
CE-4.3 SUN 16:30E�ect of Deposition Temperatureon the Propagation Loss ofPoly-Silicon Waveguides UsingHot Wire-CVD�T. Ben Masaud1,2, A. Tarazona3,R. Petra1, G. Mashanovich2, G.Reed2, and H. Chong1; 1Electronicsand Computer Science, University
CD-4.5 SUN 16:30Generation of Ultra-short Mid-IRPulses by Four-Wave Mixing inMetalized Waveguides�T. Flöry1, P. Malevich1, A. Pugzlys1,A. Voronin2, A. Zheltikov2,3, and A.Baltuska1; 1Photonics Institute Vi-enna University of Technology, Vi-enna, Austria; 2Physics Department,
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ROOM 14c ROOM EDISON ROOM EINSTEIN ROOM HERTZ ROOM MAIMAN ROOM NEWTON2EA-4.2 SUN 16:00Measurement-based control of amechanical oscillator at itsthermal decoherence rate�V. Sudhir, D. Wilson, N. Piro, R.Schilling, A. Ghadimi, and T. Kip-penberg; Ecole Polytechnique Fed-eral de Lausanne (EPFL), Lausanne,SwitzerlandCavity-enhanced interferometry isused to resolve the displacement ofa 4.3MHz nanobeam oscillator withan imprecision 40dB below that atthe standard quantum limit. �ismeasurement is used to feedbackcool it to 5.3 quanta.
CH-4.2 SUN 16:00Detecting Single MoleculeInteractions withPlasmon-enhanced OpticalMicrocavities�F. Vollmer, M. Baaske, andM. Fore-man; Max Planck Institute for theScience of Light, Erlangen, GermanyUsing an optical microcavity andgold nanorods, we have ampli�edthe interaction of light with DNA tothe extent that we can now track in-teractions between individual DNAmolecules.
CC-4.3 SUN (Invited) 16:00Local THz Resonances inSemiconductors: Active Controlof Near-Fields, THz Extinctionand Beaming�J. Gomez Rivas1,2, G. Georgiou1,and A. Bhattacharya1; 1Centerfor Nanophotonics, FOM InstituteAMOLF, Amsterdam, �e Nether-lands; 2COBRA Research Institute,Eindhoven University of Technology,Eindhoven,�e NetherlandsWe demonstrate the THz near-�eldenhancement of metallic bowtie an-tennas. To achieve full control ofthese �elds, we create plasmonic an-tennas in unstructured surfaces bythe photo-excitation of a semicon-ductor layer with a shaped beam.
JSIV-2.2 SUN 16:00Phonon-enhanced graphenephotoresponse for mid-infraredlight�M. Badioli1, A. Woessner1, K.-J.Tielrooij1, S. Nanot1, G. Navickaite1,T. Stauber2, F.J. García de Abajo1,3,and F.H.L. Koppens1; 1ICFO - Insti-tut de Ciències Fotòniques, Castellde-fels (Barcelona), Spain; 2Instituto deCiencia de Materiales de Madrid(CSIC), Madrid, Spain; 3ICREA - In-stitució Catalana de Recerca i Es-tudis Avançats, Barcelona, SpainCombining spectrally and spatiallyresolved photocurrent and trans-mission measurements in the mid-infrared, we show how the graphenephotorespose can be strongly en-hanced via the excitation of bulk andsurface phonons of the substrate.
CI-4.2 SUN 16:00Spectral Sideband Splitting inStrongly Dispersion OscillatingFibersC. Finot1, F. Feng1, P. Morin1, Y.Chembo2, A. Sysoliatin3, and �S.Wabnitz4; 1Laboratoire Interdisci-plinaire Carnot de Bourgogne, Dijon,France; 2FEMTO-ST/Optics depart-ment, Besançon, France; 3Fiber Op-tics Research Center, Moscow, Rus-sia; 4Dipartimento di Ingegneriadell*Informazione, Brescia, FranceWe experimentally and theoret-ically demonstrate the spectralsplitting experienced by quasi-phase matched gain sidebands inthe strongly dispersion managedregime of dispersion oscillating�bers. Application to pulse doubletgeneration with continuouslytunable delay is discussed.
EA-4.3 SUN 16:15Photonic Crystals on High-QMicromechanical Membrane forDispersive Cavity Optomechanics�I. Krasnokutska1, X. Chen1, K.Makles1, R. Braive2, S. Deleglise1,T. Jacqmin1, T. Briant1, P.-F.Cohadon1, I. Robert-Philip2, andA. Heidmann1; 1Laboratory KastlerBrossel, Paris, France; 2Laboratoryfor Photonics and Nanostructures,Marcoussis, FranceWe enhance dispersive optome-chanical coupling by using photoniccrystal membrane in the middle of ahigh-�nesse cavity. �is membraneexhibits high mechanical Q-factor,99.91% of re�ectivity and 300 ppmof scattering loss.
CH-4.3 SUN 16:15Optical trace gas detection inhuman breath for diseasediagnosis�M. Azhar1, D. Marchenko1,J. Mandon1, S. Cristescu1, M.Boerkamp2, J. Mink2, and F.Harren1; 1Radboud University,Nijmegen, �e Netherlands; 2VTecLasers and Sensors, Eindhoven, �eNetherlandsA compact, optical spectrometer fortrace gas detection in human breathis reported. Biomarkers like Hydro-gen cyanide have been detected inhuman breath at parts per billionlevels-o�ering a potential for non-invasive disease diagnosis.
JSIV-2.3 SUN 16:15On-chip graphene optoelectronicdevices for optical interconnects�D. Englund1, R.-J. Shiue1, Y. Gao2,D. Efetov1, C. Peng1, and J. Hone2;1Massachusetts Institute of Tech-nology, Cambridge, United States;2Columbia University, New York,United StatesWe report on hybrid graphene-silicon photonic optoelectronicdevices for optical interconnects,including high-speed nanocavity-integrated graphene modulators,and high-responsivity and broad-band photodetectors operating inexcess of 50 GHz.
CI-4.3 SUN 16:15Fast and Chaotic WDMAll-Optical PolarizationScramblerM. Guasoni, P.-Y. Bony, �M. Gilles,A. Picozzi, and J. Fatome; Labora-toire Interdisciplinaire Carnot deBourgogne (ICB), CNRS, Dijon,FranceWe report a simple and e�ective all-optical polarization scrambler basedon the nonlinear interaction in anoptical �ber between a signal beamand its backward replica generatedby a re�ective loop at the �ber end.
EA-4.4 SUN 16:30Progress toward cooling a micro-gram-scale optomechanical reson-ator to its quantum ground state�L. Neuhaus, S. Zerkani, A. Kuhn,S. Chua, T. Jacqmin, S. Deléglise,T. Briant, P.-F. Cohadon, and A.Heidmann; Laboratoire KastlerBrossel, UPMC, ENS, CNRS, Collègede France, Paris, FranceWe present an optomechanical sys-
CH-4.4 SUN 16:30In-�ber silicon microsphere as ahybrid Fabry-Pérot micro-cavity�L. Xiao1, N. Healy1, T. Hawkins2,M. Jones2, J. Ballato2, U. Gibson3,and A. Peacock1; 1OptoelectronicsResearch Centre, Univ. of Southamp-ton, Southampton, United Kingdom;2�e Center for Optical Materials
CC-4.4 SUN 16:30Sensitivity Enhancement forMicroorganism Detection withTerahertz Metamaterial Sensors�S.J. Park and Y.H. Ahn; Ajou Uni-versity, Suwon, Korea, SouthWe demonstrate that THz metama-terials can work as e�cientmicroor-ganism detectors both in aqueous
EE-4.2 SUN 16:30Breakdown of the DipoleApproximation in Strong-FieldIonization�A. Ludwig1, J. Maurer1, B.W.Mayer1, C.R. Phillips1, L.Gallmann1,2, and U. Keller1;1ETH Zürich, Zürich, Switzer-land; 2University of Bern, Bern,
JSIV-2.4 SUN 16:30Graphene Enabled Silicon RingResonators for PhotonicNetwork-on-Chip�J.A. Lazaro1, J. Gonzalez1, J.A.Altabas2, and A. Lerin1; 1UniversitatPolitecnica de Catalunya, Barcelona,Spain; 2Aragon Institute of Engi-neering Research (I3A), University of
CI-4.4 SUN 16:30SOA-based, Idler-free PhaseQuantiserR. Kakarla1, �K. Bottrill2, F.Parmigiani2, D. Venkitesh1, andP. Petropoulos2; 1Indian Instituteof Technology Madras, Chennai,India; 2Optoelectronics ResearchCentre, University of Southampton,
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Institució Catalana de Recerca iEstudis Avançats, Barcelona, SpainBy scanning a resonant dipole an-tenna in the near-�eld of single�uorescent molecules and measur-ing �uorescence lifetime of themolecules, we are able tomap 3D lo-cal density of optical states aroundthe antenna.
Silicon-photonics components arefabricated on Si surfaces. Wepresenta maskless, single-step laser writingmethod for creating Fresnel zoneplates deeply buried in Si. �is isthe �rst realisation of any optical el-ement inside Si.
1Fraunhofer Institute for AppliedOptics and Precision Engineering,Jena, Germany; 2Friedrich SchillerUniversity Jena, Institute of AppliedPhysics, Jena, GermanyAmethod for analyzing splice lossesbased on refractive index pro�lemeasuring is presented and ap-plied to an e�cient, single mode1kW monolithic �ber laser with anYtterbium-doped �ber fabricated atthe Fraunhofer IOF.
Spectroscopy, Berlin, Germany;2NEST Istituto Nanoscienze - CNR,Pisa, Italy; 3Dipartimento di Fisicadell’Università di Pisa, Pisa, Italy;4Faculty of Physics, So�a University,So�a, Bulgaria; 5Física i Cristallo-gra�a de Materials i Nanomaterials(FiCMA-FiCNA), Universitat Rovirai Virgili (URV), Tarragona, SpainWe demonstrate e�cient, passivelyQ-switched laser operation, basedon Tm3+:LiGdF4 and Cr2+:ZnSe. �epolarized emission was centeredat 1876nm, with pulse parametersof 13ns (duration), 467�J (energy)and 37kW (peak power) at 350Hz.
of Southampton, Southampton,United Kingdom; 2OptoelectronicResearch Centre, University ofSouthampton, Southampton, UnitedKingdom; 3Echerkon TechnologiesLtd, Crawley, United KingdomIn this investigation of the e�ectof temperature deposition, using ahot-wire chemical vapour deposi-tion process, on the propagation lossof sub-micron poly-Si waveguides at1550 nm, temperatures below 300oC produced the lowest loss.
International Laser Center, M.V.Lomonosov Moscow State Univer-sity, Moscow, Russia; 3Departmentof Physics and Astronomy, TexasA&MUniversity, College Station TX,United StatesAbstract: 2.7-�m microjoule fem-tosecond pulses are generated in ametal coated hollow �ber thru four-wave-mixing parametric ampli�ca-tion. Numerical simulations pre-dict generation of few-cycle opticalpulses with the central wavelengthextending beyond 10 �m.
EG-4.6 SUN 16:45Strong modi�cation of themagnetic local density of opticalstate through magneticnanoantennas�M. Mivelle1, T. Grosjean2, U.Fischer3, G. Burr4, and M. Garcia-Parajo1,5; 1ICFO, Barcelona, Spain;2FEMTO-ST, Besançon, France;3University of Münster, Munster,Germany; 4IBM, San Jose, UnitedStates; 5ICREA, Barcelona, SpainWe theoretically describe howone can achieve unprecedentedenhancement of both the total andradiative decay rate of a magneticdipole moment by using resonatingnanoantennas designed to stronglyenhance the optical magnetic �eld.
CM-4.6 SUN 16:45Femtosecond laser volumestructuring of crystals using highrepetition rates and burst pulses�F. Dreisow and S. Nolte; FriedrichSchiller Universität Jena - Institute ofApplied Physics, Jena, GermanyWe report on local structuring ofcrystals by femtosecond lasers. Wefound that high repetition rate burstmode processing yields less cracksand reduced stress �elds. �eprogress towards local melting isdiscussed.
CJ-4.6 SUN 16:45Axicons for Mode Conversion inHigher-Order Mode FIbre Lasers�J. Nicholson, A. DeSantolo, P.Westbrook, R. Windeler, T. Kremp,C. Headley, and D. DiGiovanni;OFS Laboratories, Somerset, UnitedStatesWe demonstrate axicons for modeconversion in higher-order mode�ber lasers. �e LP0,14 mode of anErbium doped higher-order mode�ber ampli�er is converted with85% e�ciency to a beam with M^2< 1.3.
CA-4.5 SUN 16:45Q-switching of a Tm,Ho:KLu(WO4)2Microchip Laser at 2061 nm by aGraphene-Based Saturable Absorber�J.M. Serres1, X.Mateos1, P. Loiko1,2,V. Jambunathan1,3, K. Yumashev2,V. Petrov4, U. Griebner4, M. Aguiló1,and F. Díaz1; 1Univ. Rovira i Vir-gili, Tarragona, Spain; 2Center forOptical Materials and Technologies,Belarusian National Technical Univ.,Minsk, Belarus; 3HiLASE Centre,Inst. of Physics ASCR, Prague, CzechRepublic; 4Max Born Inst. for Non-linear Optics and Short Pulse Spec-troscopy, Berlin, GermanyA diode-pumped Tm,Ho:KLu(WO4)2microchip laser passively Q-switched with graphene generated amaximum average output power of74 mW with M2 < 1.1 at 2061 nm.�e shortest pulse duration was 201ns.
CE-4.4 SUN 16:45All-Optical Formation of CoherentDark States in Single Silicon-Va-cancy Color Centers in Diamond�J.N. Becker1, B. Pingault2, C.Hepp2, C. Schulte2, C. Arend1,M. Markham3, M. Atatüre2, andC. Becher1; 1Fachrichtung 7.2(Experimentalphysik), Univ. desSaarlandes, Saarbrücken, Germany;2Atomic, Mesoscopic and OpticalPhysics Group, Cavendish Lab.,Univ. of Cambridge, Cambridge,United Kingdom; 3Element Six Ltd.,Global Innovation Centre, Didcot,United KingdomWe present all-optical formation ofcoherent ground state spin superpo-sitions of silicon vacancy color cen-ters in diamond as well as a mea-surement of their characteristic co-herence time using coherent popu-lation trapping.
CD-4.6 SUN 16:45Liquid-�lled �ber capillaries formid-IR supercontinuumgeneration�S. Kedenburg, T. Steinle, T. Gissibl,A. Steinmann, and H. Giessen; 4thPhysics Institute and Research Cen-ter SCOPE, University of Stuttgart,Stuttgart, GermanyWe demonstrate supercontinuumgeneration in �ber capillaries in�l-trated with the highly nonlinear liq-uid CS2 at di�erent pump wave-lengths. �e generated supercon-tinua exhibit a record width of over1200 nm for a 5 �m core diameter.
17:15 – 18:45PL-1: ECBO-CLEO/Europe 2015International Year of Light Event and PlenaryTalksChair: Peter E. Andersen, DTU Fotonik - Technical Uni-versity of Denmark, Roskilde, Denmark
PL-1.1 SUN (Plenary) 17:15Far-�eld Optical Nanoscopy: Principles and RecentAdvancements�S.W. Hell; Max Planck Institute for Biophysical Chem-istry, Göttingen, GermanyProf. Stefan W. Hell will discuss on far-�eld opticalnanoscopy: principles and recent advancements.
PL-1.2 SUN (Plenary) 18:00Imaging Life at High Spatiotemporal Resolution�E. Betzig; Janelia Research Campus, HHMI, Ashburn,VA, United StatesMicroscopes must di�erentiate to handle the compet-ing demands of high spatial resolution, high speed, non-invasiveness, and deep penetration into tissues. I willdiscuss a number of microscopes that balance thesetradeo�s in di�erent ways.
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tem made from a quartz micropil-lar in a cryogenic Fabry-Perot cavity.A�er stabilizing our system againsta thermo-mechanical instability, weexpect to feedback-cool our me-chanical resonator to its quantumground state.
Science and Engineering, Technolo-gies (COMSET), Dep. of MaterialScience and Engineering, Clemson,United States; 3Dep. of Physics, Nor-wegian Univ. of Science and Technol-ogy, Trondheim, NorwayA silicon microsphere was fabri-cated inside a �ber forming a hybridFabry-Pérot microcavity. �e largedi�erence in indices and thermal-optic coe�cients of the sphere andits silica cladding are exploited forhigh-sensitivity temperature sensing.
and ambient conditions. �e sensi-tivity has been studied as a functionof substrate dielectric constant, gapsize and metal thickness.
SwitzerlandWe experimentally proof the break-downof the dipole approximation inthe long-wavelength limit at moder-ate intensities. �e breakdownman-ifests itself as asymmetries in pho-toelectron momentum distributionsdue to magnetic �eld e�ects.
Zaragoza, Zaragoza, SpainWe propose graphene Siliconwaveguides in ring-resonatorstructures for tuneable �lters andwavelength-routers for futurephotonic Network-on-Chip (NoC).Analytical model shows up to2.8THz FSR adequate for 14WDM channels at 200GHz with6.1(0.17)dB drop-(passing-)losses.
Southampton, United KingdomWedemonstrate 4-level phase quan-tisation using SOAs, regeneratinga 10GBaud QPSK signal contami-nated with broadband phase noise.Preliminary results show a reduc-tion of phase noise by 50% and animprovement in receiver sensitivityof 1dB.EA-4.5 SUN 16:45
One and two-mode squeezing ofthermal �uctuations in a cavityopto-mechanical system byparametric modulation of theoptical springA. Pontin1,2, M. Bonaldi3,4, A.Borrielli3,4, F.S. Cataliotti1,2,8, L.Marconi1, F. Marino2,5, G. Pand-raud6, G.A. Prodi4,7, E. Serra4,6, and�F. Marin1,2,5,8; 1Dip. di Fisica e As-tronomia, Univ. di Firenze, Firenze,Italy; 2Istituto Nazionale di FisicaNucleare, Sezione di Firenze, SestoFiorentino (FI), Italy; 3Materialsfor Electronics and Magnetism,Nanoscience-Trento-FBK Division,Povo (TN), Italy; 4Istituto Nazionaledi Fisica Nucleare, Trento Inst. forFundamental Physics and Applica-tion, Povo (TN), Italy; 5CNR-INO,Firenze, Italy; 6Dept. of Microelec-tronics and Computer Engineering/ECTM/DIMES, Del� Univ. ofTechnology, Del�, �e Netherlands;7Dip. di Fisica, Univ. di Trento,Povo (TN), Italy; 8European Lab. forNon-Linear Spectroscopy (LENS),Sesto Fiorentino (FI), ItalyWe report the experimental obser-vation of two-mode squeezing be-tween oscillation modes of a ther-mal micro-oscillator. �e e�ect isobtained by parametric modulationof the optical spring in a cavity op-tomechanical system.
CH-4.5 SUN 16:45Nanoscuptured thin �lms basedSERS nanobiosensor for highlysensitive and speci�c detection ofE. coli�S.K. Srivastava1, H.B. Hamo2,A. Kushmaro2,3, R.S. Marks2,3, C.Grüner4, B. Rauschenbach4,5, and I.Abdulhalim1,3; 1Dep. of Electro opticEngineering and Ilse Katz Inst. forNanoscale Science and Technology,Ben Gurion Univ. of the Negev, BeerSheva, Israel; 2�e Avram and StellaGoldstein-Goren Dep. of Biotech-nology Engineering, Ben GurionUniv., Beer Sheva, Israel; 3School ofMaterials Science and Engineering,Nanyang Technological Univ.,Singapore, Singapore; 4Leibniz Inst.of Surface Modi�cation, Leipzig,Germany; 5Univ. Leipzig, Inst. forExperimental Physics II, Leipzig,GermanyWe have fabricated and character-ized a SERS nanobiosensor utilizingnanosculptured thin �lms of silverfor highly speci�c and sensitive de-tection of E. coli. Sensor can de-tect bacterial concentrations up tothe levels of single bacterium.
CC-4.5 SUN 16:45Mid- and far-infrared digitalholography with quantum cascadelasers�M. Ravaro1,2, M. Locatelli1,L. Consolino1,2, S. Bartalini1,2,M.S. Vitiello1,3, R. Cicchi1,2, F.Pavone1,2,4, and P. De Natale1,2;1INO, Istituto Nazionale di Ottica-CNR, Florence, Italy; 2LENS,European Laboratory for NonLinearSpectroscopy, Sesto Fiorentino, Italy;3NEST-CNR, Istituto Nanoscienzeand Scuola Normale Superiore, Pisa,Italy; 4Dipartimento di Fisica eAstronomia, Università di Firenze,Florence, ItalyWe report on our recent resultsof real time speckle and transmis-sion digital holography in the mid-IR and Terahertz spectra, based onquantum cascade lasers combinedwith a high-sensitivity microbolo-metric thermocamera.
EE-4.3 SUN 16:45Slow Fragmentation a�erUltrafast Laser Field Ionization�S. Larimian1, S. Erattupuzha1,E. Lötstedt2, T. Szidarovszky2, R.Maurer1, S. Roither1, M. Schö�er1,D. Kartashov1, A. Baltuška1, K.Yamanouchi2, M. Kitzler1, and X.Xie1; 1Photonics Institute, ViennaUniversity of Technology, Vienna,Austria; 2Department of Chemistry,School of Science, �e University ofTokyo, Tokyo, AustriaWe report experimental observationof “slow” fragmentation from ethy-lene molecules on nanosecond oreven microsecond timescale a�ertheir interaction with femtosecondlaser pulses. Our results indicatethat such process originates frommeta-stable intermediate states.
JSIV-2.5 SUN 16:45Single-molecule study for agraphene-based nano-positionsensor�G. Mazzamuto1,2, A. Tabani1, S.Pazzagli2, S. Rizvi1, A. Raserbat-Plantey5, K. Schaedler5, G.Navickaite5, L. Gaudreau5, F.Cataliotti1,2,3, F. Koppens5, and C.Toninelli1,3,4; 1LENS and Universitàdi Firenze, Sesto Fiorentino, Italy;2Dipartimento di Fisica ed Astrono-mia, Univ. Firenze, Sesto Fiorentino,Italy; 3QSTAR, Firenze, Italy; 4INO -Istituto Nazionale di Ottica, Firenze,Italy; 5ICFO - Institut de CienciesFotoniques, Castelldefels, SpainIn this study we lay the ground-work for a graphene-based funda-mental ruler at the nanoscale, rely-ing on the e�cient energy-transfermechanism between single organicquantum emitters (Dibenzoterry-lene molecules) and a graphenemonolayer.
CI-4.5 SUN 16:45Recon�gurable coupled ringresonator waveguide-basedbandpass �lter for signalprocessingC. Taddei1, L. Zhuang1,2, M.Hoekman3, C.G.H. Roelo�zen4, and�K.-J. Boller1; 1MESA+ Institutefor Nanotechnology, University ofTwente, Enschede, �e Netherlands;2Monash Electro-Photonics Labora-tory, Monash University, Clayton,Australia; 3Lionix B.V., Enschede,�e Netherlands; 4Satrax B.V.,Enschede,�e NetherlandsWe demonstrate an advanced pho-tonic �lter integrated in a Si3N4-SiO2 waveguide chip. �e recon-�gurable �at-top optical �lter pro-vides a record-narrow, record-�atand high-contrast pass-band for the�rst all-optical selection of singlesatellite channels.
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HALL B012:30 – 13:30CA-P: CA Poster Session
CA-P.1 SUNHigh Average Power kW-scale Yb:YAG�in-diskRegenerative Ampli�er�T. Nubbemeyer1, M. Gorjan1,2, A. Alismail1, M.Ue�ng1, H.G. Barros1, T. Metzger3, D. Sutter4, Z.Major1,2, and F. Krausz1,2; 1Department für Physik,Ludwig-Maximilians-Universität München, Garching,Germany; 2Max-Planck-Institut für Quantenoptik,Garching, Germany; 3TRUMPF Scienti�c Lasers GmbH+ Co. KG, München-Unterföhring, Germany; 4TRUMPFLaser GmbH, Schramberg, GermanyScaling of a thin-disk Yb:YAG CPA ampli�er to high av-erage powers is investigated. We demonstrate a pulseenergy of 170mJ at 1kHz and >1kW average power at100kHz repetition rate.
CA-P.2 SUNDirectly diode-side-pumped Alexandrite slab lasersin the bounce geometry and optical vortex generation�G.�omas1, A.Minassian2, andM.Damzen1; 1ImperialCollege London, London, United Kingdom; 2Unilase Ltd,London, United KingdomWe present results of a diode-side-pumped Alexandritelaser in the bounce geometry. In compact cavity con�g-uration, 12W output power is demonstrated. Addition-ally, we report direct vortex generation from a vibroniclaser for the �rst time.
CA-P.3 SUNNovel Technique for Transverse Mode Switching in aNd:YAG Laser�D. Kim and J.W. Kim; Hanyang University, Ansan, Ko-rea, SouthA simple method to control the generated transversemode in a solid state laser system coupled with the sec-ondary cavity is reported. Using this approach, we caneasily switch the mode between TEM00 and LG01.
CA-P.4 SUNTopological E�ects in Phase Locking of Lasers�V. Pal, C. Tradonsky, R. Chriki, G. Barach, A.A. Friesem,and N. Davidson; Department of Physics of Complex Sys-tems, Weizmann Institute of Science, Rehovot, IsraelExperimental and calculated results demonstratingtopological e�ects in phase locking a ring array of lasersare presented. �e e�ects occur with an odd number oflasers but not with an even number.
CA-P.5 SUNE�cient Q-switched Ho: GdVO4 Laser At RoomTemperature�Y. Ding, Y. Ju, B. Yao, and Y. Li;Harbin Institute of Tech-nology, Harbin, China, People’s Republic of (PRC)We demonstrated a novel solid-state laser, a room tem-perature Q-switched Ho: GdVO4 laser at 2�moperationpumped by a 1942nm Tm-�ber laser.
CA-P.6 SUNNarrow-band zero-phonon-line pumped e�cientcryogenic Yb:YAG laser�V. Jambunathan1, L. Horackova1,2, P. Navratil1,2, A.Lucianetti1, and T. Mocek1; 1HiLASE Center, Instituteof Physics ASCR, Dolní Břežany, Czech Republic; 2CzechTechnical University in Prague, Prague, Czech RepublicCryogenic laser performance of Yb:YAG pumped byVBG stabilized narrow band �ber coupled diode laserat 969 nm is presented. A maximum output power of6.54W with a slope e�ciency 64.6% at 140K is achieved.
CA-P.7 SUNDi�erent pro�les of fundamental mode from conicalrefraction lasers�Y. Loiko1, A. Turpin2, G. Sokolovskii3, J. Mompart2, andE. Rafailov1; 1Optoelectronics and Biomedical Photon-ics Group, AIPT, Aston University, Birmingham, UnitedKingdom; 2Departament de Física, Universitat Autònomade Barcelona, Bellaterra, Spain; 3Io�e Physico-TechnicalInstitute, St Petersburg, RussiaFor the �rst time, we report the fundamental mode with�at-top, crescent and involving optical-singularity trans-verse pro�le from conical refraction lasers. We discussthe parameters that a�ect the output patterns.
CA-P.8 SUNOptical Ampli�cation in Anisotropic Yb:FAP LaserCeramics�Y. Sato, J. Akiyama, and T. Taira; Institute for MolecularScience, Okazaki, JapanFluorescence from anisotropic Yb:FAP laser ceramicswas ampli�ed to 2.8 times by constructing an optical res-onator. �is ampli�cation indicates that the laser-diodepumping formed the optical gain comparable to the op-tical loss in Yb:FAP ceramics.
CA-P.9 SUNExtreme Linewidth Broadening in a Nd:YLiF4-KGWIntracavity Raman Laser�D. Geskus1,4, J. Jakutis-Neto2, D. J. Spence3, H. M. Pask3,and N. U. Wetter4; 1Department of Materials and NanoPhysics, KTH - Royal Institute of Technology, Kista, Swe-den; 2Instituto de Estudos Avançados, IEAv-DCTA, SãoJosé dos Campos, SP, Brazil; 3MQ Photonics, Department
of Physics and Astronomy, Macquarie University, Sydney,Australia; 4Centro de Lasers e Aplicações, IPEN/SP, SãoPaulo, SP, BrazilLinewidth broadening of up to 4 nm of the fundamental�eld has been observed in a intracavity Nd:YLF-KGWRaman laser. Nine laser con�gurations have been ana-lyzed to identify the responsible processes using a math-ematical model.
CA-P.10 SUNSelf-Sustained Pulsations in an Intra-Cavity Pumped�in-Disk Laser�C. Vorholt and U. Wittrock; Photonics Laboratory,Muenster University of Applied Science, Steinfurt, Ger-manyWe examine the laser dynamics in an intra-cavitypumped thin-disk laser. Experimental and numerical in-vestigations show that — depending on a single param-eter — the laser exhibits either self-sustained pulsations,chaotic oscillations, or continuous-wave operation.
CA-P.11 SUNParasitic Noise Suppression in a Double-Pass RingAmpli�er�V. Polyakov; ITMO University, Saint-Petersburg, Russia�e way to suppress the parasitic oscillations and spatialnoise in double-pass ring Nd:YAG ampli�er with polar-ization decoupling is discussed. We used 4mm diameteractive rod and 3.6 kW total optical pump power.
CA-P.12 SUN260 MHz, MW-level thin-disk oscillator�J. Zhang1,2, N. Lilienfein1,3, J. Brons1, M. Seidel1, D.Bauer4, D. Sutter4, V. Pervak3, Z. Wei2, A. Apolonski1,3,O. Pronin3, and F. Krausz1,3; 1Max-Planck-Instituteof Quantum Optics, Garching, Germany; 2Beijing Na-tional Laboratory for Condensed Matter Physics and In-stitute of Physics, Chinese Academy of Sciences, Beijing,China, People’s Republic of (PRC); 3Ludwig-Maximilians-University Munich, Garching, Germany; 4TRUMPF-Laser GmbH and Co. KG, Schramberg, GermanyA Kerr-lens mode-locked Yb:YAG thin-disk oscillatordelivering 215-fs pulses with 75-W average power at arepetition rate of 260 MHz is presented.
CA-P.13 SUNHundred-J-Level, Nanosecond-Pulse Nd:glass LaserSystem with High Beam Quality�S. Li1, Y. Wang1, Z. Lu1, L. Ding1,2, Y. Chen1, P. Du1, Z.Zheng1, D. Ba1, H. Yuan1, C. Zhu1, Z. Bai1, Z. Liu1, andC. Cui1; 1Harbin Institute of Technology, Harbin, China,People’s Republic of (PRC); 2China Academy of Engineer-ing Physics, Mianyang, China, People’s Republic of (PRC)A 100-J-level Nd:glass laser system in nanosecond-scale
pulse-width has been constructed. �e laser system op-erates at the wavelength of 1053 nm and 351 nm withhigh beam quality.
CA-P.14 SUNPhase Bounding in Self-mode-locked Nd:YVO4 Laserwith Intracavity SHG�A. Kovalev1, V. Polyakov1, and O. Orlov2; 1ITMO Uni-versity, Saint Petersburg, Russia; 2D.I. Mendeleyev Insti-tute for Metrology, Saint Petersburg, RussiaWe report on a new experimentally achieved regime ofmode-locked operation in Nd:YVO4/KTP laser whichimplies output power modulation on solely second har-monic of the laser occurring from bounded phase varia-tions.
CA-P.15 SUNHigh peak power thermally bondedEr3+,Yb3+:glass/Co2+: MgAl2O3 microchip laser�J. Mlynczak, N. Belghachem, and K. Kopczynski; Insti-tute of Optoelectronics, Military University of Technology,Warsaw, Poland�e highest, ever reported, peak power of 7.68 kW inpassively q-switched microchip laser made of thermallybonded active medium Er3+,Yb3+:glass and saturableabsorber Co2+: MgAl2O3 was achieved.
CA-P.16 SUNLow-�reshold Solid-State Pulsed Laser withLarge-Size Topological InsulatorJ.-L. Xu1, C.-Y. Tu1, and �C.-K. Lee2; 1Key Laboratory ofOptoelectronic Materials Chemistry and Physics of CAS,Fujian Institute of Research on the Structure of Matter,Chinese Academic of Sciences, Fuzhou, China, People’sRepublic of (PRC); 2Department of Photonics, NationalSun Yat-sen University, Kaohsiung, Taiwan, China, Re-public of (ROC)�e contribution has been withdrawn by the authors.
CA-P.17 SUNUn-cooled diode-pumped 2-�m laser for space-bornelidar�P. Meng1, Y. Tao1, and B. Yao2; 1Beijing Institute ofSpace Mechanics & Electricity, Beijing, China, People’sRepublic of (PRC); 2National Key Laboratory of TunableLaser Technology, Harbin Institute of Technology, Harbin,China, People’s Republic of (PRC)Uncooled Ho:YAG laser resonantly pumped by un-cooled diode-pumped Tm:YLF laser for space-borne li-dar was investigated experimentally for the �rst time.9.18W laser output at 2.09�mwas obtained under diode-pumped power of 51.5W at 792nm.
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HALL B0CA-P.18 SUNResonantly pumped 1645nm and 1617nmQ-switched Er:YAG ceramic lasersQ. Ye1, S. Wang1, Y. Shi1, M. Gao1, �C. Gao1, and J.Zhang2; 1Beijing Institute of Technology, Beijing, China,People’s Republic of (PRC); 2Jiangsu Normal University,Xuzhou, China, People’s Republic of (PRC)Fiber laser resonantly pumped Q-switched Er:YAG ce-ramic lasers with the wavelengths of 1645 nm and 1617nm were studied. Experimental results were comparedwith the results obtained fromQ-switched Er:YAG crys-tals lasers.
CA-P.19 SUNMulti-Wavelength Yb3+:GdAl3(BO3)4 PassivelyQ-switched Solid-State Laser with TopologicalInsulator Bi2Te3 as Saturable AbsorberY.-J. Sun1, J.-L. Xu1, C.-Y. Tu1, and �C.-K. Lee2; 1KeyLaboratory of Optoelectronic Materials Chemistry andPhysics of CAS, Fujian Institute of Research on the Struc-ture of Matter, Chinese Academic of Sciences, Fuzhou,China, People’s Republic of (PRC); 2Department of Pho-tonics, National Sun Yat-sen University, Kaohsiung, Tai-wan, China, Republic of (ROC)�e contribution has been withdrawn by the authors.
CA-P.20 SUNHigh-order mode excitation in end-pumpedsolid-state lasers around cavity degeneracy lengthsN. Barré, �M. Romanelli, and M. Brunel; Institut dePhysique de Rennes, Rennes, FranceWe study experimentally and numerically the crucialrole of cavity degeneracy and thermal lensing in high-order mode excitation, and show that pure high-ordermodes with circular or elliptical nodal lines cannot beexcited.
CA-P.21 SUNRegenerative ampli�cation in Yb3+-doped fusedsilica�F. Roeser1, M. Loeser1,2, M. Siebold1, D. Albach1, S.Grimm3, A. Langner4, G. Schötz4, and U. Schramm1,2;1Helmholtz-Zentrum Dresden-Rossendorf, Dresden, Ger-many; 2Technische Universität Dresden, Dresden, Ger-many; 3Institute of Photonic Technology, Jena, Germany;4Heraeus Quarzglas GmbH & Co. KGH, Hanau, Ger-manyWe report to our knowledge the �rst short pulse gener-ation experiment in bulk volume Yb-doped fused silicautilizing a Q-switched cavity.
CA-P.22 SUNTowards GW peak power from a Kerr-lensmode-locked thin-disk oscillator�J. Brons1, V. Pervak1,2, D. Bauer3, D. Sutter3, V.Kalashnikov4, A. Apolonski1,2, O. Pronin1, and F.Krausz1,2; 1Max-Planck Institut für Quantenoptik,Garching, Germany; 2Ludwig-Maximilians-UniversitätMünchen, Garching, Germany; 3TRUMPF Laser GmbH,Schramberg, Germany; 4Aston University, Birmingham,United KingdomA geometrical power-scaling procedure for KLMoscilla-tors has been reported resulting in 270 W, 38 MW froman Yb:YAG thin-disk oscillator. We describe the scal-ing steps and progress on reaching several hundredMWoutput-peak-power.
CA-P.23 SUNPassively Mode-Locked 640-nm Pr:YLF LaserPumped by InGaN Laser Diodes�R. Kariyama, H. Tanaka, K. Iijima, K. Hirosawa, and F.Kannari; Keio University, Kanagawa, JapanWe achieved the �rst diode-pumped mode-lock Pr:YLFlaser. �e average output power reaches 68 mW at 640nm with a pulse width of 15 ps and a repetition rate of108 MHz.
CA-P.24 SUNTemperature In�uence on Diode-pumped TunableTm:BaF2 Laser�J. Sulc1, M. Nemec1, M. Fibrich1, H. Jelinkova1,M.E. Doroschenko2, V.A. Konyushkin2, and V.V. Osiko2;1Czech Technical University in Prague, Prague, Czech Re-public; 2AM Prokhorov General Physics Institute of RAS,Moscow, Russia�e performance and tunability of a newly developedTm:BaF2 laser was investigated. �e temperature inde-pendent (80 – 280K) laser tuning range extended from1822 nm up to 1948 nm.
CA-P.25 SUNRoom temperature, diode-side-pumped, passivelyQ-switched Yb:LuAG slab laser�M. Kaskow1, J.K. Jabczynski1, W. Zendzian1, J. Sulc2,M. Nemec2, and H. Jelinkova2; 1Institute of Optoelectron-ics, Military University of Technology, Warsaw, Poland;2Faculty of Nuclear Sciences and Physical Engineering,Czech Technical University, Prague, Czech RepublicE�cient, diode-side pumped Yb:LuAG slab laser wasdemonstrated with 100 mJ of output energy in free run-ning. 10.1 mJ energy, 2.5 MW peak power was obtainedin passively Q-switched regime at 1030.5 nm.
CA-P.26 SUNE�cient power scaling at 1342 nm wavelength withcomposite multiple Nd-doped vanadate crystal�A. Rodin1,2, M. Grishin1,2, and A. Michailovas1,2;1Center for Physical Sciences and Technology, Vilnius,Lithuania; 2UAB Ekspla, Vilnius, LithuaniaPower scaling in regenerative ampli�er at 1342nm isachieved using composite di�usion-bonded Nd:YVO4rod pumped at 880nm. Output power of 10 and 17.5Wwith M2~1.1 delivered in 13ps and CW at 15% and 26%e�ciency
CA-P.27 SUNHigh brightness diode-pumped organic solid-statelaserZ. Zhao1,2, O. Mhibik1,2, M. Nafa1,2, S. Chenais1,2, and�S. Forget1,2; 1Université Paris 13, Sorbonne Paris Cité,Laboratoire de Physique des Lasers, Villetaneuse, France;2CNRS, UMR 7538, LPL, Villetaneuse, FranceHigh-power, di�raction-limited organic solid-state laseroperation has been achieved in a vertical external cavitysurface-emitting organic laser (VECSOL), pumped by alow-cost compact blue laser diode, leading to a recordpower-brightness of 8.9 TW/m2/sr.
CA-P.28 SUNSingle source pumped MOPA for Q-switched pulsesin the 2 �m spectral range�I. Rohde1, D. �eisen-Kunde2, and R. Brinkmann1,2;1Institut für Biomedizinische Optik, Lübeck, Germany;2Medical Laser Center Lübeck, Lübeck, GermanyIn order to increase the energy of a Q-switched Ho:YAGlaser pulses with durations stretched to several hundrednanoseconds, a master oscillator power ampli�er systempumped by a single source was designed for medical ap-plications.
CA-P.29 SUNDiode-Pumped Laser Emission from DepressedCladding Waveguides Inscribed in Nd-doped Mediaby Femtosecond Laser Writing Technique�G. Salamu1, N. Pavel1, T. Dascalu1, F. Jipa2, and M.Zam�rescu2; 1National Institute for Laser, Plasma andRadiation Physics, Solid-State Quantum Electronics Lab-oratory, Bucharest 077125, Romania; 2National Institutefor Laser, Plasma andRadiation Physics, Solid-State LaserLaboratory, Bucharest 077125, RomaniaDepressed cladding waveguides were inscribed inNd:YAG and Nd:YVO4 laser media by direct opticalwriting with a femtosecond-laser beam. Continuous-wave laser emission at 1.06 microns was obtained underthe pump with �ber-coupled diode lasers.
CA-P.30 SUNLaser Properties of Yb:YGAG Ceramic inComparison with Crystalline Yb:YAG�J. Mužík1,2, V. Jambunathan2, M. Jelínek1, V. Kubeček1,T. Miura2, A. Endo2, and T. Mocek2; 1Czech TechnicalUniversity, Faculty of Nuclear Sciences and Physical Engi-neering, Praha, Czech Republic; 2HiLASE center, Instituteof Physics AS CR, v.v.i., Dolní Břežany, Czech Republic�e laser performance of Yb-doped mixed garnetY3Ga2Al3O12 ceramic at room temperature was investi-gated and compared with crystalline Yb:YAG under thesame conditions. �e obtained results show very goodproperties of this new active material.
CA-P.31 SUNGraphene-Based Q-Switching of a CompactPassively-Cooled Yb:YAG Laser�J.M. Serres1, V. Jambunathan1,2, A. Lucianetti2, T.Mocek2, X. Mateos1, P. Loiko1,3, K. Yumashev3, V.Petrov4, U. Griebner4, M. Aguiló1, and F. Díaz1; 1Univ.Rovira i Virgili, Tarragona, Spain; 2HiLASE Centre, Inst.of Physics ASCR, Praha, Czech Republic; 3Center forOptical Materials and Technologies, Belarusian NationalTechnical Univ., Minsk, Belarus; 4MaxBorn Inst. for Non-linearOptics& Short Pulse Spectroscopy, Berlin, GermanyA diode-pumped passively Q-switched Yb:YAG laserwith graphene generated a maximum average outputpower of 185 mW. �e shortest pulse duration was 228ns at a pulse repetition frequency of 285 kHz.
CA-P.32 SUNEvaluation of co-doped Lu3+, Nd3+: GdCa4O(BO3)3single crystal, a potential self-doubling material withemission in green spectral range�C.A. Brandus1,2, L. Gheorghe1, A. Achim1, G. Stanciu1,and T. Dascalu1; 1National Institute for Laser, Plasmaand Radiation Physics, Bucharest, Romania; 2Faculty ofPhysics, University of Bucharest, Bucharest, RomaniaEnhanced laser emission at fundamental wavelengthof 1.06 �m is obtained from a co-doped ZX cutLu3+,Nd3+:GdCa4O(BO3)3 single crystal as comparedto XY cut Nd3+:GdCa4O(BO3)3. �e laser results aresustained by the measured spectroscopic data.
CA-P.33 SUNHigh power kHz cryogenic Yb:YAG CPA laser system�E. Perevezentsev, I. Mukhin, I. Kuznetsov, and O.Palashov; Institute of Applied Physics of the RussianAcademy of Sciences, Nizhny Novgorod, Russia80mJ at 500Hz is achieved from the cryogenic Yb:YAGdisk ampli�er with a 3ns Q-switched seed laser. New1ns chirped-pulse front-end consisting of a femtosecondlaser, CVBG stretcher and regenerative ampli�er will beimplemented soon
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HALL B0CA-P.34 SUNPower scalable spectral broadening in bulk crystalswith more than 100 W average power�J. Brons1, M. Seidel1, V. Pervak1,2, A. Apolonski1,2,O. Pronin1, and F. Krausz1,2; 1Max-Planck-Institutfür Quantenoptik, Garching, Germany; 2Ludwig-Maximilians-Universität München, Garching, GermanyPower-scalable spectral broadening in bulk crystals isdemonstrated. Pulses at 100-W average-power level arecompressed to 120-fs in a single stage. A spectrum with60-fs Fourier-limit is generated in a second stage.
CA-P.35 SUNFemtosecond Laser Damage at kHz and MHzRepetition RatesB.J. Nagy1, L. Vámos1, D. Oszetzky1, P. Rácz1, L. Gallais2,and �P. Dombi1; 1Wigner Research Centre for Physics, Bu-dapest, Hungary; 2Institut Fresnel, CNRS, Aix-MarseilleUniversité, Ecole Centrale Marseille, Marseille, FranceWe report comparative femtosecond laser induced dam-age threshold measurements at kHz and MHz repetitionrates with the same setup. We saw over 2.7 times higherLIDT in the kHz region explained by thermally assisteddamage.
CA-P.36 SUNLaser-diode-pumped, Q-Switched Tm:YAG Laserwith 128 mJ Pulse Energy�M. Yumoto, N. Saito, and S. Wada; RIKEN,Wako, JapanLaser-diode-pumped, Q-switched Tm:YAG laser withhigh pulse energy and high beam quality was demon-strated. Pulse energy reached 128 mJ with pulse widthof 160 ns at a repetition rate of 10 Hz.
CA-P.37 SUNInvestigation of optimal conditions for collinearparametric Raman comb generation in calcite under532 and 1064 nm picosecond laser pumpingS. Smetanin1, �M. Jelinek2, V. Kubecek2, and H.Jelinkova2; 1Prokhorov General Physics Institute of Rus-sian Academy of Sciences, Moscow, Russia; 2Czech Tech-nical University in Prague, FNSPE, Prague, Czech Repub-lic�e optimal conditions of low-threshold collinear para-metric Raman-comb generation in calcite under 20-ps laser excitation are demonstrated. Combs from2nd-anti-Stokes to 4th-Stokes under 532-nm pumpingor from 5th-anti-Stokes to 4th-Stokes under 1064-nmpumping were generated.
CA-P.38 SUNEnergy Transfer in Tm,Ho:KY(WO4)2 Laser Crystal�S. Kurilchik1,2, V. Kisel1, A. Yasukevich1, and N.Kuleshov1; 1Center for Optical Materials and Technolo-gies, BelarusianNational Technical University, Minsk, Be-larus; 2Kazan Federal University, Kazan, RussiaParameters of the energy transfer between thulium andholmium ions in Tm,Ho:KY(WO4)2 crystal were evalu-ated from the measurements of �uorescence decay dy-namics. �e results are in a good agreement with thepredictions of Förster-Dexter theory.
CA-P.39 SUN�e Schawlow-Townes Linewidth - A�reefoldApproximation�M. Pollnau1 and M. Eichhorn2; 1KTH - Royal Instituteof Technology, Stockholm, Sweden; 2French-German Re-
search Institute of Saint-Louis ISL, Saint Louis, FranceConsidering spontaneous emission in the photon rateequation, we derive the correct laser linewidth below andabove threshold. �e Schawlow-Townes equation con-tains a three-fold approximation and does not representa lower limit to the linewidth.
CA-P.40 SUNTransform-Limited Ultrashort Pulse Generation byχ(2)-Lens Mode-Locking of Nd:LuYAG Laser withInhomogeneously Broadened Gain BandwidthV. Aleksandrov1, H. Iliev2, �I. Buchvarov1,3, X. Xu4, andJ. Xu4; 1Physics Department, So�a University, 5 JamesBourchier Blvd., So�a, Bulgaria; 2IBPhotonics Ltd., 19APlovdivsko pole Str., So�a, Bulgaria; 3Laser Engineer-ing and Biomedical Optics Dept., ITMO University, St.-Petersburg, Russia; 4Key Laboratory of Transparent andOpto-functional Inorganic Materials, Shanghai Instituteof Ceramics, Chinese Academy of Sciences, Shanghai,China, People’s Republic of (PRC)We demonstrate χ(2)-lens mode-locking of a Nd-dopedmixed aluminium garnet (Nd:Lu1.5Y1.5Al5O12) laserwith inhomogeneously broadened gain bandwidth. 2.4ps transform-limited pulses with output power of 290mW at 120 MHz repetition rate are obtained.
CA-P.41 SUNCascade-like and four-wave-mixing second Stokesgeneration at nonlinear cavity dumping ofsub-nanosecond Nd:SrMoO4 self-Raman laser�M. Jelinek1, V. Kubecek1, H. Jelinkova1, L. Ivleva2, S.Smetanin2, and A. Shurygin3; 1Czech Technical Univer-sity in Prague, Prague, Czech Republic; 2Prokhorov Gen-
eral Physics Institute of Russian Academy of Sciences,Moscow, Russia; 3Kovrov State Technological Academy,Kovrov, Czech RepublicCascade-like and four-wave-mixing self-Raman gener-ation of the 1.3-um 2nd-Stokes in the LD-pumped Q-switched Nd:SrMoO4 laser with strong 2nd Stokes pulseshortening down to 280 ps (10-times shorter than thefundamental 1.06-um pulse duration) is demonstrated.
CA-P.42 SUNProspects for Tapered-Diode Pumped Cr:LiCAFRegenerative Ampli�ers�U. DEMIRBAS; Antalya International University, An-talya, TurkeyDetailed simulation results have shown that, Cr:LiCAFregenerative ampli�ers pumped by two state-of-the-art1-W tapered diodes have the potential to produce pulseswith 100-microjoule energy and 2-GW peak power atrepetition rates up to 8-kHz.
CA-P.43 SUNSingle Shot to 1 kHz Repetition Rate Operation of355 nm Passively Q-Switched Microchip Laser Usinga Parameter Matrix�R. Bhandari, N. Ishigaki, S. Uno, and K. Tojo; ShimadzuCorporation, Atsugi, JapanWe describe a new method for operation enhancementof a 355 nm passively Q-switched microchip laser usinga parameter matrix. We obtain single shot to 1 kHz repe-tition rate, multi-kW peak power, picosecond pulse out-put.
12:30 – 13:30CC-P: CC Poster SessionCC-P.1 SUNQuantitative Measurement of Permeabilization inLiving Cells by Terahertz Attenuated Total Re�ection�M. Grognot and G. Gallot; Ecole polytechnique,Palaiseau, FranceUsing attenuated total re�ection technique in the ter-ahertz domain, we demonstrate non-invasive, non-staining real time measurements of cytoplasm leakageduring permeabilization of live MDCK cells by saponinat low concentration.
CC-P.2 SUNLarge spectral broadening by cross-phase modulationwith intense THz �eld�C. Vicario1, M. Shalaby1, and C.P. Hauri1,2; 1SwissFELPaul Scherrer Institute, Villigen- PSI, Switzerland; 2Ecole
Polytechnique Federale de Lausanne, Lausanne, Switzer-landGV/m single-cycle THz induces nonlinear cross-phasemodulation in electro-optical crystal leading to centralwavelength shi� and threefold spectral broadening of theco-propagating laser pulse.
CC-P.3 SUNHighly E�cient Ultra-Broadband THzWaveGeneration in New Acentric Core Nonlinear OrganicCrystal�B.J. Kang1, S.H. Lee2, W.T. Kim1, O.-P. Kwon2, and F.Rotermund1; 1Department of Energy Systems Research &Department of Physics, Ajou University, Suwon, Korea,South; 2Department ofMolecular Science andTechnology,Ajou University, Suwon, Korea, SouthHighly e�cient ultra-broadband THz wave generationis demonstrated in new acentric core organic crystals bynear-infrared pumping. By optimized phase-matching
condition, we achieve 200-kV/cm THz electric �eld withupper cut-o� frequencies beyond 10 THz.
CC-P.4 SUNSub-wavelength circular plasmonic patch resonatorsin the THz regime�C.G. Derntl, D. Bachmann, K. Unterrainer, and J.Darmo;ViennaUniversity of Technology, Vienna, AustriaWe present plasmonic circular patch resonators withstructured dielectric appropriate for the strong couplingto quantum systems. It is perfectly suited to study inter-subband cavity polariton states, cyclotron states in 2DEGand coupled plasmonic resonators.
CC-P.5 SUNErrors in the Quantitative Determination ofTerahertz Optical Properties in Time-DomainTerahertz Spectroscopy�Q. Liang1, G. Klatt2, N. Krauss1, O. Kukharenko3, and T.
Dekorsy1; 1Department of Physics and Center for AppliedPhotonics, University of Konstanz, Konstanz, Germany;2Laser Quantum GmbH, Konstanz, Germany; 3Facultyof Physics, National Taras Shevchenko University of Kyiv,Kyiv, UkraineWe demonstrate theoretically and experimentally focusdisplacement correction in a four-mirror set-up of THztime-domain spectroscopy. �e corrections agree quan-titatively with the values from a two-mirror set-up, andcan improve the precision in material characterization.
CC-P.6 SUNTerahertz Waves for Ancient ManuscriptsConservation�M. Missori1, J. Bagniuk2, M. Clerici3,4, J. Lojewska2, M.Misiti5, L. Peters6, R. Morandotti4, A. Mosca Conte7, O.Pulci7, L. Teodonio1,5,7, C. Violante7, and M. Peccianti6;1ISC-CNR, Rome, Italy; 2Jagiellonian Univ., Krakow,Poland; 3Heriot-Watt Univ., Edinburgh, United Kingdom;
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HALL B04INRS-EMT, Montreal, Canada; 5ICRCPAL, MIBACT,Rome, Italy; 6Univ. of Sussex, Brighton, United Kingdom;7ETSF, Univ. di Roma Tor Vergata, Roma, ItalyWe report on the development of a novel non-destructive microscopy approach, based on TerahertzTime-Domain-Spectroscopy, capable of assessing thestate of degradation of ancient manuscripts via electro-magnetic molecular �ngerprint detection.
CC-P.7 SUNSub-THz generation from DAST crystal pumped byan is-BBO-OPG system�Y. Tokizane1, Y. Miyake1,2, K. Nawata1, S. Fan1, S.Hayashi1, T. Notake1, A. Sato2, Y. Takida1, and H.Minamide1; 1Riken, Sendai, Japan; 2Tohoku Institute ofTechnology, Sendai, JapanWe demonstrated sub-THz generation from a DASTcrystal pumped by is-BBO-OPG outputs seeded at1323.2 nm and 1325.8 nm. �e output frequency wasmeasured using Fabry-Perot etalon as 0.47 THz.
CC-P.8 SUNReconstruction of ultra-broadband THz electric �elddistorted by electo-optic sampling�A.D. Koulouklidis1,2, V.Y. Fedorov1, and S.Tzortzakis1,2,3; 1Institute of Electronic Structure andLaser (IESL), Foundation for Research and Technology- Hellas (FORTH), Heraklion, Greece; 2Department ofMaterials Science and Technology, University of Crete,Heraklion, Greece; 3Science Program, Texas A&M Uni-versity at Qatar, Doha, QatarWe present a simple experimental procedure coupledwith a comprehensive model allowing one restoring thereal ultra-broadband THz electric �eld generated bytwo-color �lamentation, which was distorted by electro-optic sampling.
CC-P.9 SUNSimple and distortion free optical sampling of THzpulses near zero optical transmission point�M. Cornet1,2, J. Degert1,2, E. Abraham1,2, and E.Freysz1,2; 1Université de Bordeaux, LOMA, Talence,France; 2CNRS, LOMA, Talence, FranceA simple and distortion-free method to sample THz
pulses in zinc-blende crystals is proposed and experi-mentally demonstrated in a <110> cut ZnTe. Compar-ison of its performances with other techniques is given.
CC-P.10 SUNSpectral analysis of the optical pulses produced bythe interaction of optical and THz pulses in a ZnTecrystal�M. Cornet1,2, J. Degert1,2, E. Abraham1,2, and E.Freysz1,2; 1Université de Bordeaux, LOMA, Talence,France; 2CNRS, LOMA, Talence, France�e spectra of optical pulses produced in ZnTe crystalsduring the interaction of THz pulses in the 100 kV/cmrange and optical pulses are shown to result from cross-phase modulation, sum and di�erence frequency mix-ing.
CC-P.11 SUNTHz Generation from DAST crystal Pumped byChirp-controlled Femtosecond Pulses fromDouble-clad Yb-doped Fiber Ampli�er�J. Hamazaki, N. Sekine, A. Kasamatsu, and I. Hosako;National Institute of Information and CommunicationsTechnology, Tokyo, JapanTo generate a high-power broadband THz pulse e�-ciently, optical recti�cation e�ect using DAST crystaland chirp-controlled femtosecond pump pulses is used.E�ects of the pump pulse chirp in the THz pulse gener-ation are investigated.
CC-P.12 SUNReal time monitoring of terahertz E-�eld vectorwaveform�A. Kasatani, N. Yasumatsu, K. Oguchi, and S.Watanabe;Department of Physics, Faculty of Science and Technology,Keio University, Kanagawa, JapanWe developed a high-speed terahertz polarimeter basedon an electro-optic sampling setup using an electro-opticmodulator. We get terahertz electric-�led vector infor-mation within 1 ms and its waveform within 100 ms atthe fastest condition.
CC-P.13 SUNDouble-metal Schottky enhanced THz emitters�P. Gow, D. McBryde, S. Berry, M. Barnes, and V. Apos-
tolopoulos; University of Southampton, Southampton,United KingdomLateral photo-Dember based THz emitters utilising adouble-metal geometry are demonstrated and charac-terised. It is found a metal pairing of copper and chromegive the largest peak-to-peak THz output at a tempera-ture of 150 K.
CC-P.14 SUNBeam Cleaning in Terahertz Quantum CascadeLasers by Coupling to Flexible Polystyrene\SilverCoated HollowWaveguides�R. Wallis1, R. Degl’Innocenti1, D. Jessop1, Y. Ren1, A.Klimont1, Y. Shah1, O. Mitrofanov2, C. Bledt3, J. Melzer3,J. Harrington3, H. Beere1, and D. Ritchie1; 1Universityof Cambridge, Cambridge, United Kingdom; 2UniversityCollege London, London, United Kingdom; 3Rutgers Uni-versity, New Jersey, United StatesWe couple a metal-metal terahertz quantum cascadelaser to a polystyrene/silver coated hollowwaveguide us-ing a novel copper waveguide monolithically integratedinto the mounting block. A coupling e�ciency of >70%and Gaussian-like emission were recorded.
CC-P.15 SUNVisualization of Extended-Drude Response ofPhotoexcited Carriers in InSb by UltrabroadbandInfrared Time-Domain Spectroscopy�E. Matsubara1,2, T. Morimoto2, M. Nagai2, and M.Ashida2; 1Osaka Dental University, Osaka, Japan;2Osaka University, Osaka, JapanUsing air-plasma based ultrabroadband infrared time-domain spectroscopy, we observed photoinduced opticalconductivity spectra in InSb, which are well explained bythe extended Drude model with energy-dependent scat-tering time and e�ective mass of electrons.
CC-P.16 SUNAir Nonlinearity triggered by an ultra-intense sub-5THz light bullet�M. Shalaby1 and C. Hauri1,2; 1Paul Scherrer Institute,Villigen, Switzerland; 2EPFL, Lausanne, SwitzerlandWe present an experiment where ultraintense low fre-quency THz bullet turns air into a nonlinear medium.
Both instantaneous and delayed dynamics were ob-served.
CC-P.17 SUNTerahertz properties of liquid crystals doped withferroelectric BaTiO3 nanopartecles prepared by thesol-gel processU. Chodorow1, �E. Mavrona2,3, O. Chojnowska4, K.Garbat4, M. Walczakowski5, S. Saitzek3, J.-f. Blach3,V. Apostolopoulos2, M. Kaczmarek2, and J. Parka1,6;1Military University of Technology, Warsaw, Poland;2University of Southampton, Southampton, United King-dom; 3Université d’Artois, Lens, France; 4Military Univer-sity of Technology, Warsaw, Poland; 5Military Universityof Technology, Warsaw, Poland; 6Warsaw University ofTechnology, Warsaw, PolandWe present results of terahertz measurements of liq-uid crystal ferroelectric nanoparticles suspensions. Itshows that addition of ferroelectric nanoparticles to liq-uid crystal hosts improves birefringence of the mate-rial without additional time-consuming and expensivechemical synthesis.
CC-P.18 SUNCompressive Sensing Imaging with a GrapheneModulator at THz Frequency in Transmission ModeV.A. Özkan1, T. Takan1, N. Kakenov2, O. Balci2, C.Kocabaş2, and �H. Altan1; 1Middle East Technical Univ.,Ankara, Turkey; 2Bilkent Univ., Ankara, TurkeyWe demonstrate compressive sensing with a uniquegraphene based optoelectronic device which allows us tomodulate the THz �eld through an array of columns orrows distributed throughout its face
CC-P.19 SUNNonlinear-Optical Calibration of the Terahertz WaveSpectral Brightness�V. Kornienko, G. Kitaeva, A. Penin, A. Tuchak, and P.Yakunin; Faculty of Physics, Lomonosov Moscow StateUniversity, Moscow, Russia�e experimental procedure for measuring the value ofthe terahertz wave spectral brightness is discussed. �emethod is based on the use of spontaneous parametricdown-conversion under the non-linear optical terahertzwave detection.
12:30 – 13:30CL-P: CL Poster Session
CL-P.1 SUNDevelopment of LED based UV-A emission systemand a photosensitive substance for clinicalapplication in corneal radiation.
�A. Mota1, A. Orlandi1,2, A. Cestari1, G. Rossi1, J.Castro2, M. Stefani1, T. Ortega2, and T. Rosa1; 1OptoEletrônica S/A, São Carlos, Brazil; 2Instituto de Física deSão Carlos at São Paulo University, São Carlos, Brazil�e contribution has been withdrawn by the authors.
CL-P.2 SUNEngineered SERS substrate for small organicmolecule detection�I. Mannelli1, D. Janner1, K.Meissner1, and V. Pruneri1,2;1ICFO - Institut de Ciencies Fotoniques, Castelldefels,Spain; 2ICREA - Institució Catalana de Recerca i EstudisAvançats, Barcelona, Spain
A new SERS substrate for the detection of small organicmolecules with relevance to food industry has been engi-neered by using a simple and low cost procedure, basedon growing nanoparticles directly on the surface.
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HALL B0CL-P.3 SUNMechanism of Fluorescence Quenching in theWater-Dispersible Nd3+ Doped NanocrystalsSuitable for Bioimaging in the Near IR SpectralRange�Y. Orlovskii1,2, A. Vanetsev1, K. Kaldvee1, L. Puust1, A.Baranchikov3, E. Samsonova1, A. Ryabova2, S. Lange1,I. Sildos1, J. Kikas1, R. Steiner4, and V. Loschenov2;1University of Tartu, Tartu, Estonia; 2Prokhorov GeneralPhysics Institute RAS, Moscow, Russia; 3Kurnakov Insti-tute of General and Inorganic Chemistry RAS, Moscow,Russia; 4Institut für Lasertechnologien in der Medizinund Messtechnik an der Universität Ulm, Ulm, GermanyWe study �uorescent quenching of water-dispersibleNd-doped nanocrystals for near-IR bioimaging, employingthe energy transfer probe to compare di�erent hosts. Werevealed the volume location of the -OH quenchers andthe weakest quenching in KY3F10.
CL-P.4 SUNα-Glucose SERS using Multi-branched GoldNanostructures in Water�A. Ceja-Fdez1, T. López-Luke1, A. Torres-Castro2, J. Z.Zhang3, and E. De la Rosa1; 1Centro de Investigacionesen Optica, A. C., León, Mexico; 2Universidad Autonomade Nuevo León, Monterrey, Mexico; 3University of Cali-fornia, Santa Cruz, United StatesIn this work, Multi-branched gold nanostructures ob-tained by a seed-mediated method, were coated with sil-ica and analyzed as substrates to detect low concentra-tions of α-Glucose in water solution, obtaining promis-ing results for SERS applications.
CL-P.5 SUNFemtosecond Versus Picosecond Pulses ForLaser-Induced Transfer Of Biomaterials�R. Devillard1,2,3, S. Petit1, J.C. Delagnes1, O.Kerouredan2, F. Deloison3, and E. Cormier1; 1CNRS-CELIA, Université de Bordeaux, Bordeaux, France;2INSERM U1026, Université de Bordeaux, Bordeaux,France; 3Alphanov, Talence, FranceLaser assisted bioprinting and needle free injections canbe achieve by laser induced forward transfer modi�edtechnics. To assess in�uence of pulse duration, we usedtime resolved imaging technique to characterize jet for-mation.
CL-P.6 SUNOut-of-Plane Plasmonic Structures for SpectroscopicInvestigation and Potential Recording of NeuronalNetworksG.C. Messina, M. Dipalo, �P. Zilio, H. Amin, R. La Rocca,V. Shalabaeva, L. Berdondini, and F. De Angelis; IIT - Is-tituto Italiano di Tecnologia, Genova, Italy
�ree-dimensional plasmonic nanocylinders integratedonMulti ElectrodeArrays are used for investigating neu-ronal cells through Enhanced Spectroscopy and poten-tial recording. �e peculiar geometry of the nanostruc-tures demonstrated valid performances in both cases.
CL-P.7 SUNUse of a supercontinuum laser source with lowtemporal coherence for elastic scattering light sheetmicroscopy�D. Merino1, O. Olarte1, J.L. Cruz2, A. Díez2, Y.Barmenkov3, M. Andrés2, P. Pérez4, and P. Loza-Alvarez1;1ICFO, �e Institute of Photonic Sciences, Castelldefels,Spain; 2ICMUV, Universidad de Valencia, Burjassot,Spain; 3Centro de Investigaciones en Óptica, Leon, Mex-ico; 4FYLA LASER SL, Valencia, SpainLight Sheet microscopy is usually based in �uorescencetechniques. We present the use of a FYLA SC500 super-continuum source as a candidate to reduce the e�ect ofspeckle on a elastic scattering light sheet microscope.
CL-P.8 SUNSapphire Microspheres: Possible Applications toBiosensing�M.S. Murib1, W. Yeap2, D. Martens3, L. Michiels4, M.J.Schöning5, W. De Ceuninck6, K. Haenen7, P. Bienstman8,A. Serpengüzel9, and P. Wagner10; 1Hasselt Univer-sity, Institute for Materials Research, Hasselt, Belgium;2Hasselt University, Institute for Materials Research, Has-selt, Belgium; 3Gent University, Department of Informa-tion Technology, INTEC, Gent, Belgium; 4Hasselt Uni-versity, Biomedical Research Institute, Hasselt, Belgium;5Aachen University of Applied Sciences, Institute of Nano-and Biotechnologies, Jülich, Germany; 6Hasselt Univer-sity, Institute for Materials Research, Hasselt, Belgium;7Hasselt University, Institute for Materials Research, Has-selt, Belgium; 8Gent University, Department of Informa-tion Technology, INTEC, Gent, Belgium; 9Koç Univer-sity, Microphotonics Research Laboratory, Department ofPhysics, Istanbul, Turkey; 10Hasselt University, Institutefor Materials Research, Hasselt, BelgiumWhispering gallery modes were monitored before thesapphire was functionalized with DNA and a�er it wasfunctionalized with ssDNA and dsDNA. It is shown thatssDNA is more uniformly oriented on the sapphire sur-face than dsDNA.
CL-P.9 SUNVisible Fluorescent of Peptide Beta Sheets NanowiresG. Rosenman1 and �A.Handelman2; 1Tel Aviv University,Tel Aviv, Ramat Aviv, Israel; 2Holon Institute of Technol-ogy, Holon, Israel�e contribution has been withdrawn by the authors.
CL-P.10 SUNProbing in-vitro dynamics of microtubules in livingneurons with second harmonic imaging�D. Marie1, M.-R. Carlos1, R. Sylvie1, J. Pascal2, M.Pierre2, and M. Pierre3; 1Laboratory of tundamentalbiophotonics Ecole Polytechnique Federale de Lausanne,Lausanne, Switzerland; 2laboratory of neuroenergeticsand celular dynamics Ecole Polytechnique Federale deLausanne, Lausanne, Switzerland; 3division of biologi-cal and environmental sciences and engineering KAUST,�uwal, Saudi ArabiaWe developed a wide-�eld second harmonic imagingmethod with high throughput and low �uence thatcan be used to probe dynamics in living cells (i.e.microtubule-built neuronal structures) with image ac-quisition times of 50 microseconds.
CL-P.11 SUNMonolithic Opto�uidic Constriction Chip forCellular Squeezing Studies�G. Nava1,2, R. Martinez Vazquez3, T. Yang1, F.Bragheri3, P. Paiè3,4, P. Minzioni1, A. Pietra1, M.Veglione5, C. Mondello5, R. Osellame3,4, and I.Cristiani1; 1Dipartimento di Ingegneria Industriale edell’Informazione, Università di Pavia, Pavia, Italy;2Department of Biomedical Science and TranslationalMedicine, Università di Milano, Milano, Italy; 3Istitutodi Fotonica e Nanotecnologie (IFN)-CNR, Milano, Italy;4Dipartimento di Fisica, Politecnico di Milano, Milano,Italy; 5Istituto di Genetica Molecolare (IGM)-CNR,Pavia, ItalyWe report about a double-Y shapedmicro�uidic chip re-alized by fs-laser micromachining and including a con-striction embedded in one of the output branches. �echip allows studying single-cell passive-squeezing abil-ity, and even drugs-induced changes.
CL-P.12 SUNProbing the structure of collagen in tissues: Forwardversus Backward Polarization-resolved SHGmicroscopyC. Teulon, I. Gusachenko, G. Latour, and �M.-C. Schanne-Klein; Lab. for Optics and Biosciences, Ecole Polytech-nique, CNRS, Inserm, Palaiseau, FrancePolarization-resolved second harmonic microscopy isused for probing collagen structure in intact tissues. �e-oretical analysis, vectorial numerical simulations and ex-periments were performed to understand how geomet-rical parameters a�ect polarization-resolved measure-ments in homogeneous collagen-rich tissues.
CL-P.13 SUNDetection of mRNA by bi-color imaging based onPMMA nanoparticles and molecular beacons inhuman cancer cells�B. Adinol�1, M. Pellegrino2, A. Giannetti1, S. Tombelli1,C. Trono1, G. Sotgiu3, G. Varchi3, and F. Baldini1;1Istituto di Fisica Nello Carrara CNR, Sesto Fiorentino,Italy; 2Dipartimento di Ricerca Traslazionale e delleNuove Tecnologie in Medicina e Chirurgia, Università diPisa, Pisa, Italy; 3Istituto per la Sintesi Organica e la Fo-toreattività CNR, Bologna, ItalyIn this work, we demonstrate that molecular beacons,together with PMMA nanoparticles, can play a funda-mental role in achieving quantitative information on in-tracellular events acting not only as on-o� elements butalso as sensing probe.
CL-P.14 SUNInnovative Fibre Probe for Laser Ablation of TumourCells�Y. Liu1, R. Gassino1, H. Yu1, A. Braglia1, A. Vallan1,D. Tosi2, M. Konstantaki3, S. Pissadakis3, and G.Perrone1; 1Politecnico di Torino, Dept. of Electronics andTelecommunications, Torino, Italy; 2Nazarbayev Univer-sity, School of Engineering, Astana, Kazakhstan; 3IESL-FORTH, Heraklion, Greece�e paper presents the concept of a newminiaturized all-�bre probe, which combines the delivery of high powerlaser beams and temperature transducers, and providessome results about the characterization of �rst proto-types.
CL-P.15 SUNInfrared spectroscopy with graphene plasmons�A. Marini1, I. Silveiro1, and J. Garcia de Abajo1,2;1ICFO-Institut de Ciencies Fotoniques, Castelldefels,Spain; 2ICREA-Institucio Catalana de Recerca i EstudisAvancats, Barcelona, SpainWe investigate the e�ciency of graphene-based infraredsensors �nding that, thanks to the outstanding tunabil-ity of graphene through externally applied gate voltage,broadband infrared spectroscopy can be achieved.
CL-P.16 SUNLaser Engineering of Various Porous Materials forFabrication of Paper-Based Micro�uidic Devices�P. He, I. Katis, R. Eason, and C. Sones; OptoelectronicsResearch Centre, University of Southampton, Southamp-ton, United KingdomWe report the successful demonstration of a laser-baseddirect-write technique for patterning of various porousmaterials in order to fabricate more diversi�ed and mul-tifunctional paper-based micro�uidic devices that �ndapplications in a�ordable point-of-care medical diag-nostics.
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HALL B0CL-P.17 SUNExtremely compact digital lensless holographymicroscopy for getting multispectral images ofbiological samplesO. Mendoza-Yero1, M. Carbonell-Leal1, E. Tajahuerce1,�J. Lancis1, and J. Garcia-Sucerquia2; 1Universitat JaumeI, Castellón, Spain; 2Universidad Nacional de Colombia-
Sede Medellin, Medellin, ColombiaA robust and compact digital lensless holography mi-croscopy able to get multispectral images of biologicalsamples is presented. Spatial resolutions of few microm-eters are achieved. Multispectral images allows obtain-ing information on re�ectance/absorbance of speci�c re-gions.
CL-P.18 SUNDNA-origami structures for nanophotonics:enhancing �uorescence�A. Puchkova, G. Acuna, C. Vietz, B. Wuensch, E. Pibiri,B. Lalkens, D. Wang, and P. Tinnefeld; Institute for Phys-ical &�eoretical Chemistry, Braunschweig University ofTechnology, Braunschweig, Germany
We employ DNA-Origami as a platform where metallicnanoparticles and single organic �uorophores can be or-ganizedwith nanometer precision. �ese nano-antennasbased on nanoparticles dimers produce �uorescence en-hancement of three orders of magnitude.
12:30 – 13:30CM-P: CM Poster Session
CM-P.1 SUNLocalized nanoclusters in PDMS induced byfemtosecond pulses�A.M. Alshehri1,3, K.L.N. Deepak1, D.T. Marquez2,S. Desgreniers1, and V.R. Bhardwaj1; 1Departmentof Physics, University of Ottawa, Ottawa, Canada;2Department of Chemistry, University of Ottawa, Ottawa,Canada; 3Department of Physics, King Khalid University,Abha, Saudi ArabiaWe demonstrate formation of localized carbonaceousand siliconaceous clusters, con�ned to the modi�ed re-gion when polydimethylsiloxane is irradiated by fem-tosecond pulses. �e embedded clusters produced broadphotoluminescence and Raman spectra indicated for-mation of quasi-crystalline silicon clusters.
CM-P.2 SUNHigh Density Data Storage In Transparent PlasticsUsing Femtosecond Laser Microstructuring�K. Deepak1, A. Alshehri1, S. Hadjiantoniou1, D.Marquez2, T. Scaiano2, A. Pelling1, and R. Bhardwaj1;1Dept. of Physics, University of Ottawa, Ottawa, Canada;2Dept. of Chemistry, University of Ottawa, Ottawa,CanadaWe report high data storage ~ 66 GB/cm3 in Poly(methylmethacrylate) by utilizing locally con�ned �uo-rescent data bits fabricated by a femtosecond (fs) laser.
CM-P.3 SUNPulsed laser assisted decoration of 2D materials withplasmonic nanoparticles�M. Sygletou1,2, C. Petridis3, E. Kymakis3, C. Fotakis1,2,and E. Stratakis1,2; 1Institute of Electronic Structure andLaser, Foundation for Research & Technology, Heraklion,Greece; 2University of Crete, Heraklion, Greece; 3Centerof Materials Technology and Photonics & Electronic Engi-neering Department, Technological Educational Institute(TEI) of Crete, Heraklion, GreeceIn the present study we address a novel, facile, simpletop-down, laser technique for the e�ective optical in-
duced decoration of two - dimensional (2D) nanosheets(NS) with metal (Ag, Au) nanoparticles (NPs).
CM-P.4 SUNEnhancement of Properties of Heat Transfer Fluidsby In-situ Fabrication of Gold Nanoparticles byPulsed Laser Ablation in Liquids�R. Torres-Mendieta1, R. Mondragón2, E. Juliá2, O.Mendoza-Yero1, P. Andrés3, and J. Lancis1; 1GROCUJI, Institut de Noves Tecnologies de la Imatge (INIT),Universitat Jaume I., Castellón de la Plana, Spain;2Departamento de Ingeniería Mecánica y Construcción,Universitat Jaume I., Castellón de la Plana, Spain;3Departament d’Óptica, Universitat de València, Burjas-sot Valencia, SpainWe fabricated gold nanoparticles into a heat transfer�uid used in real solar power plants, obtaining a stablenano�uid which still presents an enhancement in ther-mal conductivity of 3.6% making it suitable for appliedtechnology
CM-P.5 SUNFabrication of Fluorescent Silver Nanoclusters-basedMicro-Label in Polymers�P. kunwar1, J. Hassinen2, G. Bautista1, R. H.A. Ras2, andJ. Toivonen1; 1Tampere University of Technology, Tam-pere, Finland; 2Aalto University, Espoo, FinlandWe demonstrate the fabrication of �uorescent micro-labels by generating silver nanoclusters in polymer �lm.�e as-formed micro-labels can be used for special au-thenticity markings due to it’s small size and uniqueemission signature.
CM-P.6 SUNPlasmonics for rapid laser micro-joining ofdielectricsS. Zolotovskaya1, Z. Wang2, and �A. Abdolvand1;1University of Dundee, Dundee, United Kingdom;2Bangor University, Bangor, United KingdomA joint strength of 12.5MPawas achieved upon nanosec-ond pulsed laser irradiation (0.13 J/cm2) of a 1-mm thickglass with embedded spherical silver nanoparticles (30-40 nm in diameter) to a 1-mm thick clear glass.
CM-P.7 SUNLow loss ZBLAN waveguides for mid-infraredastronomical interferometry�S. Gross1,2, N. Jovanovic3, A. Sharp1, M. Ireland4, J.Lawrence5, and M.J. Withford1,2; 1MQ Photonics Re-search Centre, Dept. of Physics and Astronomy, Mac-quarie University, Sydney, Australia; 2Centre for Ul-trahigh bandwidth Devices for Optical Systems (CU-DOS), Sydney, Australia; 3National Astronomical Obser-vatory of Japan (NAOJ), Subaru Telescope, Hilo, UnitedStates; 4Research School of Astronomy & Astrophysics,Australian National University, Canberra, Australia;5Australian Astronomical Observatory (AAO), Sydney,AustraliaWe present femtosecond laser written mid-infraredwaveguides in ZBLAN glass based on a depressedcladding geometry. �e single-mode waveguides featurelow losses (0.3 dB/cm) and circular mode-pro�les mak-ing them ideal for future astronomical interferometers.
CM-P.8 SUNUltrafast laser inscribed waveguides for mid-infraredinterferometry: Experimental study of suitable hostmaterialsA. Arriola1,2, �S. Gross1,2, T. Gretzinger1,2, M. Ams1,2,H. Ebendor�-Heidepriem3, J. Sanghera4, M. Ireland5,P. Tuthill6, and M. Withford1,2; 1Centre for Ultrahighbandwidth Devices for Optical Systems (CUDOS), Syd-ney, Australia; 2MQ Photonics Research Centre, Dept.of Physics and Astronomy, Macquarie University, Syd-ney, Australia; 3School of Physical Sciences, ARC Centreof Excellence for Nanoscale BioPhotonics, University ofAdelaide, Adelaide, Australia; 4US Naval Research Lab-oratory, Code 5623, 4555 Overlook Ave., SW, Washing-ton, DC 20375, Washington DC, United States; 5ResearchSchool of Astronomy & Astrophysics, Australian NationalUniversity, Canberra, Australia; 6Sydney Institute for As-tronomy (SIfA), School of Physics, University of Sydney,Sydney, Australia�e mid-infrared wavelength region is of special interestfor direct detection of exoplanets using stellar interfer-ometry. We report on an experimental study of suitablehost materials to inscribe mid-infrared waveguides us-ing a femtosecond laser.
CM-P.9 SUNFemtosecond laser micro fabricated structures forwavelength selective light harvesting for lab on chipapplications�S.S. Guduru1,2, F. Scotognella2, L. Criante1, R. MartinezVázquez2, R. Ramponi3, andK.C. Vishnubhatla1; 1Centerfor Nanoscience and Technology,Istituto Italiano di Tec-nologia, Milano, Italy; 2Dipartimento di Fisica, Politec-nico di Milano, Milano, Italy; 3CNR-Istituto di Fotonica eNanotecnologie, Milano, ItalyWavelength selective light harvesting in integrated chipfabricated by femtosecond laser micromachining, wherewe excite the analyte in a microchannel and collect �uo-rescence by Fresnel lenses while �ltering residual excita-tion by 1D Photonic crystal.
CM-P.10 SUNWavelength stabilization of laser diodes by ultrashortpulse written Volume-Bragg-Gratings�D. Richter1, C. Voigtländer1, R.G. Krämer1, J.U.�omas1, H. Zimer2, A. Tünnermann1,3, and S. Nolte1,3;1Institute of Applied Physics, Abbe Center of Photon-ics, Friedrich Schiller University Jena, Jena, Germany;2TRUMPF Laser GmbH + Co. KG, Schramberg, Ger-many; 3Fraunhofer Institute for Applied Optics and Pre-cision Engineering, Jena, GermanyWe present our results of spectral stabilizing laser diodeswith ultrashort pulse written fused silica VBGs. Wedemonstrate a lower load dependent spectral shi� of thespectrum due to less internal absorption by the grating.
CM-P.11 SUNLaser based microfabrication of micro�uidic chipson soda-lime glass for circulating tumour cell capture�D. Nieto1, R. Couceiro2, R. López-López2, M. Abal2, andM.T. Flores-Arias1; 1Microoptics andGRINOptics Group,Applied Physics Department, Faculty of Physics, Santiagode Compostela, Spain; 2Translational Medical Oncology;Health Research Institute of Santiago (IDIS); FundacionRamon Dominguez, SERGAS, Santiago de Compostela,SpainWe present a hybrid laser process composed for a laserdirect write technique and a CO2 laser based thermaltreatment for fabricating micro�uidics chips for circu-lating tumour cell capture.
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HALL B0CM-P.12 SUNFabrication and optimization of microlens arrays onsoda-lime glass materials using a Ti:sapphire laserand sol-gel coating�D. Nieto, A.I. Gomez-Varela, and M.T. Flores Arias;Mi-crooptics and GRIN Optics Group, Applied Physics De-partment, Faculty of Physics, University of Santiago deCompostela, Santiago de Compostela, SpainWe present a simple, repeatable and non-contaminantmethod for fabricatingmicrooptical elements. It consistson depositing hybrid SiO2 coatings via sol-gel route ontomicrolens arrays fabricated using a Ti:Sapphire laser op-erating at 1030 nm.
CM-P.13 SUNReversible Deformations of PolymericMicrostructures Induced by Changing theSurrounding Liquid Medium�S. Rekstyte1,2, V. Mizeikis2, and M. Malinauskas1;1Laser Research Center, Vilnius University, Vilnius,Lithuania; 2Research Institute of Electronics, ShizuokaUniversity, Hamamatsu, JapanWe present a novel method for creating solvent-sensitivemechano-�uidic sensors by utilizing reversible deforma-tions of polymeric structures, fabricated usingmultipho-ton polymerization technique. A functionalmicrodevicesensitive to solvent type or composition is demonstrated.
CM-P.14 SUNExploring Silicon Vibration Resonance InMicromachining Applying Temporal ShapedFemtosecond Laser Pulses�G.F.B.d. Almeida, R.J. Martins, A.J.G. Otuka, and C.R.
Mendonça; Instituto de Física de São Carlos, Universi-dade de São Paulo, São Carlos, BrazilWe report pulse shaping applied in femtosecond lasermicromachining and demonstrated how distinct pulsetrains are able to control the microstructuring processin silicon by analyzing its laser-induced periodic surfacestructures.
CM-P.15 SUNDicing of a sapphire wafer using sub-picosecondpulses at a wavelength of 800 nm�S. Kolpakov, N. Gordon, A. Yadav, H. Kbashi, I. Titkov, E.Rafailov, and K. Zhou; Aston Institute of Photonic Tech-nologies, Aston University, Birmingham, United KingdomWe have demonstrated dicing of sapphire wafers of up to350 um width using femto-second near infrared pulseswith the wavelength of 800 nm. �e kerf width was mea-sured to be ~40 micrometers.
CM-P.16 SUNLaser Induced Forward Transfer technique as a toolfor the surface wetting properties characterization.�M.Chatzipetrou1, K. Ellinas2, E. Gogolides2, A. Tserepi2,and I. Zergioti1; 1National Technical University of Athens,Athens, Greece; 2Institute of Nanoscience and Nanotech-nology, NCSR Demokritos, Athens, Greece�e contribution has been withdrawn by the authors.
CM-P.17 SUNMulti-Shot Laser Ablation and Digital MicromirrorDevice Mask Translation for Sub-di�raction-limitMachining Resolution�D. Heath, B. Mills, J. Grant-Jacob, M. Feinaeugle, and
R. Eason; Optoelectronics Research Centre, University ofSouthampton, Southampton, United KingdomWe present a rapid fabrication technique for the laser-machining of material with sub-di�raction-limit resolu-tion, achieved through spatial light intensity modulationby a digital micromirror device of multiple 1mJ 800nm150fs pulses.
CM-P.18 SUNMathematical Model of Nonlinear Laser Lithography�Ö. Yavuz1, E. Ergecen2, O. Tokel3, I. Pavlov3, andF.Ö. Ilday1,3; 1Department of Electrical and Electron-ics Engineering, Bilkent University, Ankara, Turkey;2Department of Electrical and Electronics Engineer-ing, Middle East Technical University, Ankara, Turkey;3Department of Physics, Bilkent University, Ankara,TurkeyNonlinear laser lithography (NLL) emerged as a novelsurface structuring method allowing long-range peri-odic order. NLL depends on the interplay of three mech-anisms (nonlinearity and feedback mechanisms). Wepresent a mathematical formalism for NLL.
CM-P.19 SUNOptically Mapping the Oxidation of SrTiO3 Plasmasfor Stoichiometric Growth of Crystalline Films byPulsed Laser Deposition�K. Orsel1, R. Groenen2, B. Bastiaens1, G. Koster2, G.Rijnders2, and K. Boller1; 1Laser Physics and Nonlin-ear Optics, MESA+ Research Institute for Nanotechnol-ogy, University of Twente, Enschede, �e Netherlands;2Inorganic Materials Science, MESA+ Research Institutefor Nanotechnology, University of Twente, Enschede, �e
NetherlandsWe employ laser induced �uorescence and absorptionspectroscopy, for spatiotemporal mapping of species inSrTiO3 plasmas for pulsed laser deposition. Correlationwith X-ray di�raction reveals that stoichiometric growthrequires complete Ti and Sr oxidation.
CM-P.20 SUNDynamics of laser printing of conductive inks at highvelocityD. Puerto1, E. Biver2, A.-P. Alloncle1, and �P. Delaporte1;11Aix-Marseille University, CNRS, LP3 laboratory, Mar-seille, France; 2Oxford Lasers, Oxford, United KingdomHydrodynamics of the formation and propagation of liq-uid jets when laser printing of silver nanoparticle inksis performed at high velocity, up to 1MHz, is studied.In�uence of ink viscosity and silver contents is investi-gated.
CM-P.21 SUNTransient waveguiding e�ects during glass processingby bursts of ultrashort laser pulses.�K. Mishchik1, C. Javaux Léger2, O. Dematteo Caulier1,S. Skupin1, B. Chimier1, G. Duchateau1, A. Bourgeade3,R. Kling2, C. Hönninger4, and J. Lopez1; 1CELIA,Université Bordeaux CNRS CEA, Talence, France;2ALPhANOV, Talence, France; 3CEA/CESTA, Le Barp,France; 4Amplitude Systèmes, Pessac, FranceWe have used bursts of femtosecond laser pulses for bulkmodi�cation of glasses. �e small time interval of 25ns between subsequent pulses causes transient thermalwaveguiding e�ects resulting in high aspect ratio volumemodi�cations.
12:30 – 13:30EE-P: EE Poster Session
EE-P.1 SUNPicosecond laser �lamentation in airA. Schmitt-Sody1, H. Kurz2, L. Bergé3, S. Skupin4, and �P.Polynkin5; 1Air Forcr Research Laboratory, Albuquerque,United States; 2Institut fur Quantenoptik, Leibniz Uni-versitat, Hannover, Germany; 3CEA, DAM, DIF, 91297,Arpajon, France; 4Univ. Bordeaux - CNRS - CEA, Cen-tre Lasers Intenses et Application, UMR 5107, Talence,France; 5College of Optical Sciences, University of Ari-zona, Tucson, United StatesWe show that in picosecond laser �lamentation in air,impact ionizationmechanism facilitates the formation ofdense yet continuous plasma channels. At a given pulseduration, optical �uence is independent on the pulse en-ergy.
EE-P.2 SUNSuper�lamentation in water: from femtoseconds tomicroseconds�F. Potemkin, E. Mareev, A. Podshivalov, and V. Gordi-enko; Faculty of Physics and International Laser CenterM.V. Lomonosov Moscow State University, Moscow, Rus-siaWe report whole life cycle of super�lament excited intight focusing beams in water. Extreme energy deliveryachieved under super�lamention is re�ected in strongpost-e�ects (cavitation bubbles and shock waves), whichcan completely characterize super�lament.
EE-P.3 SUNFilamentation of femtosecond Bessel beams withshaped longitudinal pro�les�I. Ouadghiri Idrissi, C. Xie, R. Giust, L. Furfaro,L. Froehly, J.M. Dudley, and F. Courvoisier; Institut
FEMTO-ST, UMR 6174 CNRS University of Franche-Comte, Besancon, FranceWe introduce a novel approach to control the competi-tion between the linear growth rate of on-axis intensityof a Bessel beam and the growth rate of nonlinearities byinitial spatial shaping in direct space.
EE-P.4 SUNUnderdense channels generated in air by energeticfemtosecond laser pulses�G. Point1, C. Milian2, A. Couairon2, A. Mysyrowicz1,and A. Houard1; 1Laboratoire d’Optique Appliquée -ENSTA, Ecole Polytechnique, CNRS, Palaiseau, France;2Centre de Physique �éorique - Ecole Polytechnique,CNRS, Palaiseau, FranceFormation of underdense channels in air using laser �l-amentation is studied interferometrically. Using a 5 mJpulse, we report an initial air temperature of 1400 K.Such channels can last more than 90 ms.
EE-P.5 SUNSpectral phase transfer from NIR to deep UVfemtosecond pulses via four-wave mixing in argon onhollow core waveguide�J. de Paula Siqueira, S. Carlos Zilio, C. Renato Men-donça, and L. Misoguti; Instituto de Física de São Carlos,São Carlos, BrazilIn this work, we report on the spectral π-step phasetransfer from near infrared to deep UV femtosecondpulses by four-wave mixing in argon using the broad-band phase-matched guided wave technique.
EE-P.6 SUNStatistical Description of Capillary-BasedHigh-Harmonic Generation�A.W. Degen-Kni�on, W.S. Brocklesby, and P. Horak; Op-toelectronics Research Centre, University of Southampton,Southampton, United Kingdom
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CLEO®/Europe-EQEC 2015 ⋅ Sunday 21 June 2015
HALL B0We develop a computationally e�cient approach to ap-proximately predict XUV spectra from gas-�lled cap-illaries by high-harmonic generation of intense near-infrared pump laser pulses. Simulation times are a hun-dred times shorter than for explicit simulations.
EE-P.7 SUNCharge-carriers photogeneration and dynamics insemiconducting carbon nanotubes�G. Soavi1, F. Scotognella1, D. Brida2, T. Hefner3, T.Hertel3, G. Lanzani4, and G. Cerullo1,5; 1Dipartimento diFisica, Politecnico di Milano, Milano, Italy; 2Departmentof Physics and Center of Applied Photonics, University ofKonstanz, Konstanz, Germany; 3Inst. for Physical and�eoretical Chemistry Dept. of Chemistry and Pharmacy,University of Wuerzburg, Wuerzburg, Germany; 4IstitutoItaliano di Tecnologia, Milano, Italy; 5IFN-CNR, Milano,ItalyWe study the photogeneration and the spectroscopicsignatures of charge-carriers in semiconducting carbonnanotubes. We demonstrate that also low-energy pho-tons (i.e. well below the optical band gap) can directlyexcite the electronic transitions.
EE-P.8 SUNObservation of High-Lying Rydberg States in StrongField Interaction�S. Larimian1, S. Erattupuzha1, R. Maurer1, C. Lemell2,S. Nagele2, S. Yoshida2, J. Burgdörfer2, A. Baltuška1, M.Kitzler1, and X. Xie1; 1Photonics Institute, Vienna Uni-versity of Technology, Vienna, Austria; 2Institute for�e-oretical Physics, Vienna University of Technology, Vienna,AustriaWe report direct observation of weak DC �eld ioniza-tion of electrons from high-lying Rydberg states whichhave been recaptured by the ionic core a�er strong �eldionization from atoms and molecules.
EE-P.9 SUNQuantitative Analysis of l = 2 Radially PolarizedUltrashort Pulses by Using Extended StokesParameters�M. Suzuki1, K. Yamane1,2, K. Oka1, Y. Toda1,2, and R.Morita1,2; 1Hokkaido University, Sapporo, Japan; 2JST,CREST, Sapporo, JapanUsing the extended Stokes parameters and the degree ofpolarization de�ned for the spatial distribution, we per-form full quantitative characterizataion of the polariza-tion states of l = 2 radially polarized ultrashort pulses inthe whole spectral range.
EE-P.10 SUNOptical Event Horizons in a Dispersion VaryingOptical Fiber�S. Wang1,2, A. Mussot1, M. Conforti1, A. Bendahmane1,X. Zeng2, and A. Kudlinski1; 1PhLAM/IRCICA, CNRS-Universite Lille 1, UMR 8523/USR 3380, Lille, France;2�e Key Lab of Specialty Fiber Optics and Optical AccessNetwork, Shanghai University, Shanghai, China, People’sRepublic of (PRC)We experimentally investigate optical event horizons ina dispersion varying �ber with a single input pulse. Itsplits into a soliton and a DW which collides it due tothe dispersion variation of the �ber.
EE-P.11 SUNTunable Mid-infrared Radiations in Quadratic Mediathrough Near-infrared Soliton Interactions withSecond-harmonic Resonances�H. Guo1, X. Liu1, X. Zeng2, B. Zhou1, and M. Bache1;1Group of Ultrafast Nonlinear Optics, DTUFotonik, Tech-nical University of Denmark (DTU), Kgs. Lyngby, Den-mark; 2Key Laboratory of Special Fiber Optics andOpticalAccess Networks, Shanghai University, Shanghai, China,People’s Republic of (PRC)Mid-IR radiation in periodically poled lithium niobateis investigated, through the four-wave-mixing betweenfundamental soliton wave and CW second-harmonicresonance. �e scheme is single-pumped. �e radiationis intense and tunable in 3-6 micron by QPM.
EE-P.12 SUNEmission of quasi-resonant radiations in dispersionoscillating �bers�M. Conforti1, S. Trillo2, A. Mussot1, and A.Kudlinski1; 1PhLAM/IRCICA, CNRS-Université Lille1, UMR 8523/USR 3380, Villeneuve d’Ascq, France;2Dipartimento di Ingegneria, Università di Ferrara,Ferrara, ItalyWe report experimental demonstration of the generationof multiple resonant radiations in dispersion oscillating�bers. �ey are generated when pumping both in nor-mal and anomalous dispersion regime, thanks to quasi-phase-matching supported by periodic dispersion.
EE-P.13 SUNGeneration and Characterization of ultrashort AiryPulses�N. Becker1, F. Eilenberger2, and T. Pertsch1; 1Institute ofApplied Physics, Jena, Germany; 2Fraunhofer Institute for
Applied Optics and Precision Engineering IOF, Jena, Ger-manyWe tailor ultrashort Airy pulses with high precision us-ing a pulse shaper. �eir propagation behaviour and self-acceleration properties are mapped in a �exible, singlebeam experiment.
EE-P.14 SUNExperimental demonstration of extreme pulseinteraction in the optical event horizons scenario�A. Tajalli1, A. Pape1, I. Babushkin1, G. Steinmeyer2, U.Morgner1, andA.Demircan1; 1Institute forQuantumOp-tics, Liebniz Universität Hannover, 30167 Hannover, Ger-many; 2Max Born Institute, 12489 Berlin, GermanyWe present experimental realization of controlling tra-jectories of optical solitons in supercontinuum by con-cept of optical event horizon. �is enables not only tomanipulate the soliton properties but also the global su-percontinuum dynamics.
EE-P.15 SUNCoherent Dynamics of Uniaxially-Strained GaNExcitons Excited by Cylindrically Polarized Pulses�K. Shigematsu1, S. Morimoto1, M. Suzuki1, K.Yamane1,2, R. Morita1,2, and Y. Toda1,2; 1Departmentof Applied Physics, Hokkaido University, Sapporo, Japan;2Core Research for Evolutionary Science and Technology,Japan Science and Technology Agency, Tokyo, JapanA novel four-wave mixing (FWM) spectroscopy usingcylindrically polarized pulses is demonstrated to studycoherent dynamics of polarized excitons in uniaxially-strained GaN �lms. Spatiotemporal polarization anal-ysis of FWM signals provides information on exciton-exciton interactions.
EE-P.16 SUNDi�erential ultrafast all-optical switching of theresonances of a micropillar cavity�H. �yrrestrup1, E. Yüce1, G. Ctistis1, J. Claudon2,3, J.-M. Gérard2,3, and W.L. Vos1; 1Complex Photonics Sys-tems (COPS), MESA+ Institute for Nanotechnology, Uni-versity of Twente, Enschede,�e Netherlands; 2UniversityGrenoble Alpes, INAC-SP2M, Nanophysics and Semi-conductors Lab, Grenoble, France; 3CEA, INAC-SP2M,Nanophysics and Semiconductors Lab, Grenoble, FranceWe perform frequency- and time-resolved all-opticalswitching of GaAs-AlAs micropillar cavities using an ul-trafast pump-probe setup. Di�erent pillar modes exhibitdi�erent frequency shi�s, which is well modelled by thespatial di�usion and recombination of carriers.
EE-P.17 SUNSnapshots of the retarded interaction of chargecarriers with ultrafast �uctuations in cuprates�S. Dal Conte1, L. Vidmar2, D. Golez2, M. Mierzejewski3,G. Soavi1, S. Peli4, F. Ban�4, G. Ferrini4, R. Comin5,B. Ludbrook5, L. Chauviere5, N. Zhigadlo6, H. Eisaki7,M. Greven8, S. Lupi9, A. Damascelli5, D. Brida1, M.Capone10, J. Bonca2, G. Cerullo1, and C. Giannetti4;1IFN-CNR, Milano, Italy; 2J. Stefan Institute, Ljubljana,Slovenia; 3Institute of Physics, University of Silesia, Ka-towice, Poland; 4Department of Physics, Università Cat-tolica del Sacro Cuore, Brescia, Italy; 5Department ofPhysics and Astronomy, University of British Columbia,Vancouver, Canada; 6Laboratory for Solid State Physics,ETH, Zurich, Switzerland; 7Nanoelectronics Research In-stitute, National Institute of Advanced Industrial Scienceand Technology, Tsukuba, Japan; 8School of Physics andAstronomy, University of Minnesota, Minneapolis, UnitedStates; 9CNR-IOM Dipartimento di Fisica, Università diRoma La Sapienza, Roma, Italy; 10CNR-IOMDemocritosNational Simulation Center and SISSA, Trieste, ItalyWe measure the transient re�ectivity of an high-Tc su-perconductor with an unprecedented temporal resolu-tion (~20fs) demonstrating that the dynamics of the car-riers can be described in terms of a retarded interactionwith short-range antiferromagnetic �uctuations.
EE-P.18 SUNPhotodissociation of 1,2-Butadiene Studied byTime-Resolved Molecular Orbital SpectroscopyUsing Single-Order High Harmonic PulsesR. Iikubo1, T. Fujiwara1, �T. Sekikawa1, Y. Harabuchi2,T. Taketsugu2, and Y. Kayanuma3; 1Department ofApplied Physics, Hokkaido University, Sapporo, Japan;2Department of Chemistry, Hokkaido University, Sap-poro, Japan; 3Materials and Structures Laboratory, TokyoInstitute of Technology, Tokyo, JapanWide range of time-resolved photoelectron spectroscopyby single-order high harmonic speci�es the breakingbond in 1,2-butadiene upon dissociation. A�er coher-ent oscillation in the femtosecond regime, the moleculesdissociate with a time constant of 1.1 ns.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13b8:00 – 8:45ED-1a: Frequency Combs IChair: Stephan Schiller, Heinrich-Heine-Universität Düsseldorf, Düsseldorf, Germany
8:00 – 8:45EG-5a: Interaction of Electronswith Optical Near-�elds IChair: Nahid Talebi, Max Planck Institute forIntelligent Systems, Stuttgart, Germany
8:00 – 8:45CM-5a: Fundamental Aspects ofLaser Matter Interaction IChair: Marta Castillo, CSIC, Madrid, Spain
8:00 – 8:45CK-4a: Quantum InformationProcessing IChair: Alexander Szameit, Friedrich-Schiller-Universität Jena Institute of AppliedPhysics, Jena, Germany
8:00 – 8:45CA-5a: Microchip Lasers IChair: Mauro Tonelli, Universita’ di Pisa,Pisa, Italy
ED-1a.1 MON 8:00Coherent Broadening of a MicroresonatorFrequency Comb to an Optical Octave forf-2f Self-Referencing�P. Del’Haye1, A. Coillet1, K. Beha1, D.Cole1, H. Lee2, K. Vahala2, S. Papp1, andS. Diddams1; 1NIST, Boulder, United States;2Caltech, Pasadena, United StatesWe present results on coherent broadeningof a 16.4 GHz microresonator-based opti-cal frequency comb to an octave (1111nmto 2222nm) for f-2f self-referencing. Coher-ence is shown by generating beat notes withan 1111 nm laser.
EG-5a.1 MON 8:00Quantum Coherent Interaction ofElectrons with Optical Near-�elds in anUltrafast Electron MicroscopeA. Feist, �K.E. Echternkamp, J. Schauss, S.V.Yalunin, S. Schäfer, and C. Ropers; IV. PhysicsInstitute, Georg-August-Universität Göttin-gen, Göttingen, GermanyWe study photon-induced scattering of swi�electrons with con�ned light in an ultrafasttransmission electron microscope (UTEM).�e �uence-dependent sideband populationin the kinetic energy spectra evidences thequantum coherent manipulation of the elec-tron momenta.
CM-5a.1 MON 8:00Modeling dielectric material modi�cationby trains of fs laser pulsesO. Dematteo Caulier1, B. Chimier1, S.Skupin1, A. Bourgeade1, �K. Mishchik1, C.Javaux2, R. Kling2, C. Hönninger3, J. Lopez1,V. Tikhonchuk1, and G. Duchateau1; 1Univ.Bordeaux-CNRS-CEA, Centre des Lasers In-tenses et Applications, UMR 5107, Talence,France; 2ALPHANOV, rue François Mitter-rand, Talence, France; 3AMPLITUDE SYS-TEMES, Cité de la photonique, Pessac, FranceWe show that by taking into account non-linear pulse propagation e�ects, heat di�u-sion, and heat accumulation, it is possible toexplain size and shape of dielectric materialmodi�cations induced by trains of fs laserpulses.
CK-4a.1 MON 8:00Single photon emission in colloidalInP\ZnS quantum dotsA.Guille, �M.Tessier, Z. Hens, and E. Brainis;University of Ghent, Gent, BelgiumWe present results on single InP\ZnS core-shell quantum dots. We show that they canbe e�cient single photons sources and wediscuss the creation of non radiative recom-bination centers at high excitation �uence.
CA-5a.1 MON (Invited) 8:00Monoclinic Double Tungstate MicrochipLasers at 1 and 2 um�X. Mateos1, J.M. Serres1, P. Loiko1,2,K. Yumashev2, N. Kuleshov2, V. Petrov3,U. Griebner3, M. Aguiló1, and F. Díaz1;1Universitat Rovira i Virgili, Tarragona,Spain; 2Center for Optical Materials andTechnologies, Belarusian National TechnicalUniversity, Minsk, Belarus; 3Max BornInstitute for Nonlinear Optics and ShortPulse Spectroscopy, Berlin, Germany�e present talk reviews recent experimen-tal studies of thermal lensing and highly ef-�cient laser operation achieved inmicrochipcon�gurations. �e e�orts were focused onKLuW doped with Yb3+, Tm3+ or Ho3+ions.
ED-1a.2 MON 8:15Counting the Cycles of Light Using anOptical Microresonator�J. Jost1, T. Herr1,2, C. Lecaplain1, E. Lucas1,V. Brasch1, M. Pfei�er1, and T. Kippenberg1;1École Polytechnique Fédérale de Lausanne(EPFL), Lausanne, Switzerland; 2Centre Su-isse d’Electronique et de Microtechnique(CSEM), Neuchatel, SwitzerlandMicroresonator based optical frequencycombs have the potential to greatly extendoptical frequency measurements. Herewe demonstrate the �rst self-referencedmicroresonator based optical comb suitablefor optical frequencymetrology applications
EG-5a.2 MON 8:15Mapping THz near-�elds with nanotipstreaking�L. Wimmer, G. Herink, K.E. Echternkamp,S.V. Yalunin, and C. Ropers; IV. Physical In-stitute, Georg-August University Göttingen,Göttingen, GermanyWe demonstrate nanotip streaking usingnear-infrared pulses and single-cycle THZ-transients to map the nanotip near-�eld.�is scheme allows for the control of thephotoelectron energy spectra and the time-resolved study of hot carrier dynamics.
CM-5a.2 MON 8:15Modelling of Nanostructures Formationand Space Charge Separation inSilver-Doped Phosphate Glass under aTrain of Femtosecond Laser Pulses�E.O. Smetanina1, B. Chimier1, Y. Petit2, T.Cardinal2, L. Canioni1, and G. Duchateau1;1Université de Bordeaux, Centre National dela Recherche Scienti�que, Commissariat à l’Énergie Atomique et aux Énergies Alterna-tives, Centre Lasers Intenses et Applications,Unités Mixtes de Recherche 5107, Talence,France; 2Centre National de la Recherche Sci-enti�que, Université de Bordeaux, Institutde Chimie de la Matière Condensée de Bor-deaux, UPR 9048, Pessac, FranceWe present the 1D numerical simulation ofnanostructures formation under femtosec-ond laser pulse irradiation of silver-dopedphosphate glass. �e model includes pho-toionization and laser heating of sample, dif-fusion, kinetic reactions and photodissocia-tion of silver species.
CK-4a.2 MON 8:15Novel physics in photonic crystalnanolasers : Dynamics and Coherence�A. Lebreton1, I. Abram1, R. Braive1, N.Belabas1, I. Sagnes1, F.Marsili2, V.B. Verma2,S.W. Nam2, T. Gerrits2, I. Robert-Philip1, M.Stevens2, and A. Beveratos1; 1CNRS-LPN,Marcoussis, France; 2National Institute ofStandards and Technology, Boulder, UnitedStates�e large discretization noise in nanolasersdue to the small numbers of dipoles and pho-tons, results in large pulse-to-pulse jittersand large amplitude �uctuations of the co-herent output, as demonstrated by interfero-metric photon-correlation.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 14a ROOM 14b ROOM CURIE ROOM EDISON ROOM EINSTEIN8:00 – 8:45CE-5a: Semiconductor Technologyand SemiconductorCharacterization IChair: Michael Jetter, University of Stuttgart,Stuttgart, Germany
8:00 – 8:45CD-5a: Applications ofNonlinearities IChair: Mario Bertolotti, La Sapienza Univer-sita’ di Roma, Roma, Italy
8:00 – 8:45EF-4a: Extreme Events in Optics IChair: Massimo Giudici, INLN, Université deNice, Nice, France
8:00 – 8:45JSII-1a: Opto�uidic BiosensorsChair: Hatice Altug, EPFL, Lausanne,Switzerland
8:00 – 8:45EE-5a: Material Dynamics onUltrafast Time Scale IChair: Fabio Biancalana, School of Engineer-ing and Physics Heriot-Watt University, Ed-inburgh, United Kingdom
CE-5a.1 MON 8:00Ultrafast Exciton Dynamics in DoublyEmitting Asymmetric GiantPbS/CdS/CdS Nanocrystals�G. Sirigu1, A. Camellini1, H. Zhao2,3,A. Parisini4, F. Rosei3,5, V. Morandi4,A. Vomiero2,3,6, and M. Zavelani-Rossi1;1Dipartimento di Fisica, IFN-CNR, Politec-nico di Milano, Milano, Italy; 2CNR INOSENSOR Lab, Brescia, Italy; 3INRS Centrefor Energy, Materials and Telecommuni-cations, Varennes, Canada; 4CNR IMMSection of Bologna, Bologna, Italy; 5CSACSMcGill University, Montreal, Canada; 6LuleaUniversity of Technology, Lulea, SwedenWe present novel asymmetric giantcore/shell/shell PbS/CdS-Zincblende/CdS-Wurtzite nanocrystals with dual coloremission, originating from PbS core andCdS-Wurtzite states, and we study theultrafast exciton dynamics.
CD-5a.1 MON 8:00Nonlinear Figure-of-merit Measurementof Waveguides Using a Top-hatDispersive-scan TechniqueS. Serna1,2 and �N. Dubreuil1; 1LaboratoireCharles Fabry, Institut d’Optique, CNRS,Univ Paris Sud, Palaiseau, France; 2Institutd’Electronique Fondamentale, UniversitéParis-Sud 11, CNRS UMR 8622, Orsay,France�e �rst nonlinear waveguide characteriza-tion using a top-hat Dispersive-scan tech-nique, a temporal analogue of the spatialZ-scan method, is reported. It allows thenonlinear �gure-of-merit measurement ofnanowires independently of the coupling ef-�ciency.
EF-4a.1 MON 8:00Nonlinear Time Series Analysis ofMulti�laments�S. Birkholz1, C. Brée2, A. Demircan3, E.Nibbering1, and G. Steinmeyer1; 1Max-Born-Institut für Nichtlineare Optik undKurzzeitspektroskopie, Berlin, Germany;2Weierstraß-Institut für Angewandte Analy-sis und Stochastik, Berlin, Germany; 3Institutfür Quantenoptik, Leibniz UniversitätHannover, Hannover, GermanyWe perform a nonlinear time series analy-sis on prominent rogue event systems. Ourresults show striking similarities betweenthe Draupner ocean wave and multi�la-ments: both bear determinism, indicatingpredictability of rogue events within thesesystems.
JSII-1a.1 MON 8:00Single-Cell Optical Stretching and Sortinginto an Integrated Micro�uidic DeviceP. Paiè1,2, �T. Yang3, G. Nava3,4, F. Bragheri2,R. Martinez Vazquez2, P. Minzioni3, M.Veglione5, M. Di Tano5, C. Mondello5, R.Osellame1,2, and I. Cristiani3; 1Dipartimentodi Fisica, Politecnico di Milano, Milano, Italy;2Istituto di Fotonica e Nanotecnologie (IFN)-CNR, Milano, Italy; 3Dipartimento di Ingeg-neria Industriale e dell’Informazione, Uni-versità di Pavia, Pavia, Italy; 4Departmentof Biomedical Science and TranslationalMedicine, Università di Milano, Milano,Italy; 5Istituto di GeneticaMolecolare (IGM)-CNR, Pavia, ItalyWedescribe the fabrication and validation ofa micro-opto�uidic chip, realized by fs-laserirradiation, which allows performing singlecells sorting-and-collection on the basis ofcells mechanical properties with high accu-racy and without a�ecting cells viability
EE-5a.1 MON 8:00Ultrafast Hole Relaxation and TransientBiexciton Absorption in SingleCdSe/ZnSe Quantum Dots�C. Hinz, C. Traum, J. Haase, B. Bauer, A.Leitenstorfer, and D.V. Seletskiy; UniversitätKonstanz, Department of Physics, Konstanz,GermanyFew-fermion dynamics in single CdSe/ZnSequantum dots is studied by two-colorpump-probe measurements on femtosec-ond timescales. Ultrafast hole relaxationand induced absorption into biexciton statesare observed when pumping p-p and d-stransitions.
CE-5a.2 MON 8:15Spatial Mapping of Exciton Lifetimes inSingle ZnO Nanowires�F. Güell1, J.S. Reparaz2, G. Callsen2,M.R. Wagner2, A. Ho�mann2, and J.R.Morante1,3; 1Universitat de Barcelona,Barcelona, Spain; 2Technische Universität,Berlin, Germany; 3Institut de Recerca enEnergia de Catalunya, Barcelona, Spain�e spatial dependence of the exciton life-times reveals that the free exciton and boundexciton lifetimes show a maximum at thecenter while they decrease by 30% towardsthe tips of single ZnO nanowires.
CD-5a.2 MON 8:15Collapse Arrest in Instantaneous KerrMedia via Parametric Interactions�A. Pasquazi1, M. Peccianti1, M. Clerici2,3,C. Conti4, and R. Morandotti2; 1Universityof Sussex, Brighton, United Kingdom; 2INRS-EMT, Varennes, Canada; 3Herriot-Watt Uni-versity, Edinburg, United Kingdom; 4ISC-Sapienza, Rome, ItalyWe demonstrate a four wave mixing interac-tion based on four wave mixing that can ar-rest the collapse and stabilize solitary propa-gation in a pure Kerr material by controllingthe wavelength of the interacting beams.
EF-4a.2 MON 8:15Control of Rogue Waves in OpticallyInjected Semiconductor LasersJ. Ahuja1, B. Nalawade1, S. Perrone2, J.Zamora-Munt2, R. Vilaseca2, and �C.Masoller2; 1Indian Institute of TechnologyGuwahati, Guwahati, India; 2Departamentde Fisica i Enginyeria Nuclear, UniversitatPolitecnica de Catalunya, Terrassa, SpainIn optically injected semiconductor lasersrogue waves can be suppressed by cur-rent modulation of appropriated frequency.When not suppressed, the modulation pro-vides a safe phase-window in which RWs areunlikely to occur
JSII-1a.2 MON 8:15Optimization Study of BimodalWaveguide Interferometric Biosensors�D. Grajales and L.M. Lechuga; Nanobiosen-sors and Bioanalytical Applications Group,Institut Català de Nanociència i Nan-otecnologia (ICN2) CSIC & CIBER-BBN,Barcelona, SpainPhotonic biosensors based on evanescentwave detection principle can a�ord quick,precise, cheap and reliable diagnostic toolsfor point-of-care solutions. An optimizedbimodal interferometer sensor is proposed.
EE-5a.2 MON 8:15Ultrafast Pseudospin Dynamics ofCarriers in Graphene�A. Grupp1, M. Trushin1, G. Soavi1, A.Budweg1, D. De Fazio2, U. Sassi2, A.Lombardo2, A. Ferrari2, W. Belzig1, A.Leitenstorfer1, and D. Brida1; 1Departmentof Physics and Center for Applied Photon-ics, University of Konstanz, Konstanz, Ger-many; 2Cambridge Graphene Centre, Cam-bridge, United KingdomPseudospin-selective ultrafast optical excita-tion is studied in graphene. We observe theevolution of anisotropy in momentum spaceas a function of excited carrier density. Ouranalytical model can well describe the re-sults.
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ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13bED-1a.3 MON 8:30Towards self-referencing a 10 GHzElectro-Optic Frequency Comb�K. Beha, D.C. Cole, F.N. Baynes, P. Del’Haye,A. Rolland, T.M. Fortier, F. Quinlan, S.A.Diddams, and S.B. Papp; Institute for Stan-dards and Technology, Boulder, United StatesWe generate a coherent, octave-spanningfrequency comb via electro-optic modula-tion of a 1550 nm laser and spectral broad-ening. �is comb allows o�set frequency de-tection, and generation of ultrastable 10GHzmicrowaves.
EG-5a.3 MON 8:30Holographic Control of Free-electronLight EmissionG. Li1,2, �B. Clarke1, J. So1, K.F.MacDonald1,X. Chen2, W. Lu2, and N.I. Zheludev1,3;1University of Southampton, Southampton,United Kingdom; 2Shanghai Institute of Tech-nical Physics, Shanghai, China, People’s Re-public of (PRC); 3Nanyang TechnologicalUniversity, Singapore, SingaporeWe demonstrate experimentally that holo-graphic nanostructures can be employed tocontrol the wavefront - the direction, spec-tral composition and phase pro�le of lightemission stimulated by free electron injec-tion into plasmonic and dielectric media.
CM-5a.3 MON 8:30Imaging Energy Deposition ofFemtosecond Pulses in Raman-ActiveMaterials�S. Minardi1, C. Milián2, D. Majus3, A.Gopal4, G. Tamošauskas3, A. Couairon2,T. Pertsch1, and A. Dubietis3; 1Institute ofApplied Physics, Jena, Germany; 2Centrede Physique �éorique, Palaiseau, France;3Department of Quantum Electronics, Vil-nius, Lithuania; 4Institute of Quantum Elec-tronics, Jena, GermanyWe investigate the energy deposition dy-namics of focused femtosecond pulses inwa-ter with a new diagnostic based on inverseRaman scattering. We show that the ioniza-tion threshold of water is 8eV, rather than6.5eV.
CK-4a.3 MON 8:30On-chip realization of Hadamard andPauli-X gates for polarization-encodedqubits�R. Heilmann, R. Heilmann, R. Heilmann,and A. Szameit; Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, GermanyWe demonstrate an integrated arbitrarywave plate operation including Hadamardand Pauli-X gate operation for polarization-encoded qubits solving the problem of on-chip polarization state modulation in fem-tosecond laser-written circuits for quantumoptics.
CA-5a.2 MON 8:30Vibronic 2.1 �mYb,Tm:KLu(WO4)2Microchip Laser�P. Loiko1,2, J.M. Serres2, X. Mateos2, K.Yumashev1, N. Kuleshov1, V. Petrov3, U.Griebner3, M. Aguiló2, and F. Díaz2; 1Centerfor Optical Materials and Technologies,Belarusian National Technical University,Minsk, Belarus; 2Física i Cristallogra�ade Materials i Nanomaterials (FiCMA-FiCNA), Universitat Rovira i Virgili (URV),Tarragona, Spain; 3Max Born Institutefor Nonlinear Optics and Short PulseSpectroscopy, Berlin, GermanyCW Yb,Tm:KLuW microchip laser diode-pumped at 978 nm is realized. Electron-phonon coupling allows for laser genera-tion at 1.96-2.09 �m. �e maximum outputpower is 140mWwith the slope e�ciency of16
9:00 – 11:00PL-2: 2015World of Photonic CongressOpening and Plenary Talk
In the honour of the UN proclaimed 2015 InternationalYear of Light and Light-Based Technologies, the cere-mony dedicated to “Light solutions for the Society Chal-lenges of our World” will start with a couple of welcomeaddresses, short invited talks and will be followed by aPlenary Talk.
09:00 – 10:00
Words of Welcome by Reinhard Pfei�er, Deputy CEO,Messe München International.Welcome Address by Flavia Schlegel,Assistant Director-General for Natural Sciences, UNESCO.
International Year of Light – �e European Perspec-tive by Günther Oettinger, Commissioner Digital Econ-omy & Society.
International Year of Light – �e American Perspec-tive by Lawrence S. Goldberg, Senior Engineering Ad-visor, Division of Electrical, Communications and CyberSystems (ECCS) National Science Foundation.International Year of Light – �e African Perspec-tive by Yanne K. Chembo, ERC Starting Grand Laure-ate, Centre National de la Recherche Scienti�que (CNRS)Paris, African Physical Society.
Moderation: JohnDudley,Université de Franche-Comté,Besançon, France, Chairman of the International Year ofLight Steering Committee
PL-2.1 MON (Plenary) 10:00High Performance Quantum Cascade Lasers from theMid-IR to the Far-IR and their impact on Science andTechnology�F. Capasso;Harvard University, Cambridge, MA, UnitedStatesSince their invention in 1994 Quantum Cascade Lasers,thanks to their fundamentally new design principles,have opened up the mid-IR to far-IR spectrum (3-300�m) to major advances in science and technology.
Session Chair: PatrickGeorges, Institut d’Optique Grad-uate School, Laboratoire Charles Fabry, Palaiseau, France
ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 14a ROOM 14b11:15 – 12:45CJ-5: Mid-IR FibreLaser Systems IChair: Stuart Jackson, Mac-quarie University, Sydney,Australia
11:15 – 12:45ED-2: Combs andPrecision MeasurementChair: Pascal Del’Haye, NIST,Boulder, USA
11:15 – 12:45EG-6: Cavity AssistedInteractionsChair: Ilja Gerhardt, Univer-sity Stuttgart, Stuttgart, Ger-many
11:15 – 12:45CM-6: Laser VolumeMicro and Nanostruc-turingChair: Yves Bellouard, EPFL,Lausanne, Switzerland
11:15 – 12:45CK-5: NonlinearMicro/NanophotonicsChair: Peter G. R. Smith,ORC, University of Southamp-ton, Southampton, UnitedKingdom
11:15 – 12:45CE-6: Nanomaterials forPhotonic ApplicationsChair: Pascal Loiseau, Labora-toire de Chimie de la MatièreCondensée de Paris, Paris,France
11:15 – 12:45CD-6: FrequencyConversion andApplicationsChair: Cornelia Denz, Univer-sity of Münster, Münster, Ger-many
CJ-5.1 MON 11:15Double Pass Gain inHelium- Xenon Dischargesin Hollow Optical Fibres at3.5�mA. Love1, S. Bateman1, W.
ED-2.1 MON 11:15Ramsey-Comb Spectroscopyin the Deep UltravioletSpectral Region�R. Altmann, L. Dreissen, S.Galtier, and K. Eikema; Vrije
EG-6.1 MON 11:15A sub-λ3 mode volume can-tilever-based Fabry-PérotmicrocavityH. Kelkar1, D. Wang1, B.Ho�mann1, S. Christiansen1,2,
CM-6.1 MON 11:15Direct writing of nanostruc-tures embedded in variousmaterials using femtosecondlaser�Y. Shimotsuma1, T. Sei1, M.
CK-5.1 MON (Invited) 11:15Photonic Crystal NonlinearWaveguides: CompressingNonlinear Fiber Optics on aChip�A. De Rossi and S. Combrié;
CE-6.1 MON 11:15Eco-Friendly FluorescentNanomaterials for E�cientLightingP.-C. Shen1,2, K.-Y. Chen1, and�C.-F. Lin1,2,3,4; 1Graduate
CD-6.1 MON 11:15400 THz bandwidth super-continuum generation intapered tellurite suspendedcore �ber�J. Picot-Clemente1, C.
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ROOM 14a ROOM 14b ROOM CURIE ROOM EDISON ROOM EINSTEINCE-5a.3 MON 8:30Fabrication and Optical Properties ofAlGaAs/GaAs Nanowire/Quantum-WellHeterostructures�X. Yan, X. Zhang, Y. Wu, W. Wei, J. Li,and X. Ren; Beijing University of Posts andTelecommunications, Beijing, China, People’sRepublic of (PRC)AlGaAs/GaAs nanowire/quantum-well het-erostructures were fabricated. Fabry-Perotmodes were observed in the quantum wellspectra region, indicating that the well andnanowire act as the gain and cavity, respec-tively. �e structure is promising for in-frared nanolasers.
CD-5a.3 MON 8:30Simultanuous Generation andEnhancement of THG and SHG in aStable Micro�bre Knot Resonator�R. Ismaeel, T. Lee, and G. Brambilla; Op-toelectronics research center, Southampton,United Kingdom�e Simultaneous generation of third andsecond harmonics is demonstrated in Mi-cro�ber knot resonators. �is techniqueprovides a stable con�guration which im-proves e�ciencies of the THG and SHG by24 and 6 times respectively.
EF-4a.3 MON 8:30Extreme Events in a Broad AreaSemiconductor Laser with SaturableAbsorber�S. Barbay1, F. Selmi1, Z. Loghmari1, S.Coulibaly2, and M. Clerc3; 1Laboratoirede Photonique et de Nanostructure, CNRS-UPR20, Marcoussis, France; 2Laboratoire dePhysique des Lasers, Atomes et Molécules,CNRS-UMR8523, Villeneuve d’Ascq, France;3Departamento de Física, Universidad deChile, Santiagio, ChileWe present experimental and numerical re-sults on extreme events generation in a spa-tially extended VCSEL with integrated sat-urable absorber. We analyze the role of spa-tial coupling and spatio-temporal chaos inthe generation of extreme events.
JSII-1a.3 MON 8:30Opto�uidic-Plasmonic HandheldBiosensor for High-�roughput andLabel-Free Monitoring of MolecularInteractions�A. Coskun1,3, A. Cetin2,5, D. Etezadi2,5,B. Galarreta2,4, D. Alvarez2, H. Altug2,5,and A. Ozcan1; 1University of CaliforniaLos Angeles (UCLA), Los Angeles, UnitedStates; 2Boston University, Boston, UnitedStates; 3California Institute of Technology,Pasadena, United States; 4Ponti�cia Univer-sidad Catolica del Peru, Lima, Peru; 5EcolePolytechnique Federale de Lausanne (EPFL),Lausanne, SwitzerlandWe demonstrate an opto�uidic-plasmonicbiosensor, weighing 40 g and 7.5 cm inheight, which integrates micro�uidics, plas-monic sensor technology and dual-colorlensfree imaging for real-time monitoring ofbiomolecular binding events in point of caresettings.
EE-5a.3 MON 8:30Carrier-Envelope Phase SensitivePhotoemission from Resonant andO�-Resonant Plasmonic Nanoparticles�W. Putnam1, R. Hobbs1, Y. Yang1, K.Berggren1, and F. Kärtner1,2; 1MassachusettsInstitute of Technology, Camrbidge, UnitedStates; 2DESY and University of Hamburg,Hamburg, GermanyPhotoemission from resonant and o�-resonant plasmonic nanoparticle arrays isinvestigated. We �nd the photoemissioncurrent is sensitive to the carrier-envelopephase and explore the dependence of thissensitivity on the resonant wavelength ofthe nanoparticles.
ROOM 21 ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM NEWTON2 ROOM ROENTGEN NOTES11:15 – 12:45EB-1: Quantum Statesand CharacterizationChair: Gregor Weihs, Univer-sity of Innsbruck, Innsbruck,Austria
11:15 – 12:45EF-5: Turbulence, Op-tical RogueWaves andModulation Instabilitiesin Optical FibresChair: Stéphane Barland,INLN, Université de Nice,Nice, France
11:15 – 12:45JSII-2: IntegratedOn-Chip DiagnosticsChair: Laura Lechuga, ICN2and CSIC, Barcelona, Spain
11:15 – 12:45JSIII-1: Laser DrivenAccelerationChair: Victor Malka, Lab-oratoire Optique AppliquéeANSTA/X/CNRS, Paris,France
11:15 – 12:45CI-5: OpticalComputing, DataProcessing, RoFChair: Marc Haelterman,Université Libre de Bruxelles,Bruxelles, Belgium
11:15 – 12:45CA-6: Diode-pumpedUV, Visible and NIRSolid-state LasersChair: Mauro Tonelli, Univer-sita’ di Pisa, Pisa, Italy
EB-1.1 MON 11:15Quantum tomography withinitial system-environmentcorrelationsM. Ringbauer1,2, C. Wood3,K. Modi4, A. Gilchrist5, A.
EF-5.1 MON (Invited) 11:15Optical Wave Turbulence inFibre Lasers�S. Turitsyn; Aston Institute ofPhotonic Technologies, Birm-ingham, United Kingdom
JSII-2.1 MON (Invited) 11:15Chip-based Raman spectro-scopy for biomedicaldiagnosis�J. Popp; Leibniz Institute ofPhotonic Technology e.V., Jena,
JSIII-1.1 MON (Invited) 11:15Laser wake�eld accelerationof multi-GeV electronbeams with PW laser pulses�H.T. Kim1,2, K.H. Pae1,V.B. Pathak1, K. Nakjima1,
CI-5.1 MON 11:15Information processingusing a photonic reservoircomputer based on a coher-ently driven passive cavitywith an analog readout layer
CA-6.1 MON 11:15Diode pumping of ultrafastTi:Sapphire lasers: powerscaling to 200 mW in 68 fsand �rst noise analysis�K. Gürel1, V.J. Wittwer1, M.
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ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 14a ROOM 14b
Belardi1, C. Webb2, and �W.Wadsworth1; 1University ofBath, Bath, United Kingdom;2University of Oxford, Oxford,United KingdomGain is observed in a doublepass of a Helium-Xenon gasDC discharge in a 90cm long�exible hollow core�bre. Out-put at 3.5�m increases withdischarge current up to themaximum of 0.55mA.
Universiteit, Amsterdam, �eNetherlandsRamsey-comb spectroscopyenables ultra-high precisionspectroscopy with high-power frequency comb laserpulses. We are now extendingthis method to the deep-UVfor precision spectroscopyof krypton and molecularhydrogen.
�S. Götzinger1, and V.Sandoghdar1; 1Max PlanckInstitute for the Science ofLight, Erlangen, Germany;2Helmholtz Centre Berlin forMaterials and Energy, Berlin,GermanyA tunable Fabry-Pérot micro-cavity with 2.6 �m curva-ture mirror and 0.4 numeri-cal aperture is fabricated. Westudy the e�ect of a nanopar-ticle on the cavity modes anddiscuss the coupling of singlemolecules.
Sakakura2, and K. Miura1;1Department of MaterialChemistry, Graduate School ofEngineering, Kyoto University,Kyoto, Japan; 2Society-Academia Collaboration forInnovation, Kyoto University,Kyoto, Japan�e photo-induced periodicnanostructures embedded invarious materials can open anew opportunity to developavant-garde devices such as a5D optical storage, polariza-tion imaging sensor, thermo-electric conversion elements.
�ales Research and Technol-ogy, Palaiseau, Francewe brie�y review the achieve-ments of the GaInP photoniccrystal technology for on-chipnonlinear optics
Inst. of Photonics and Opto-electronics, Nat. Taiwan Univ.,Taipei, China, Republic of(ROC); 2Innovative PhotonicsAdvanced Research Center, Nat.Taiwan Univ., Taipei, China,Republic of (ROC); 3GraduateInst. of Electronics Engineering,Nat. Taiwan Univ., Taipei,China, Republic of (ROC);4Dep. of Electrical Engineer-ing, Nat. Taiwan Univ., Taipei,China, Republic of (ROC)Advanced rare-earth-freelight- conversion nanoma-terials for LED lighting aredeveloped. Unlike the con-ventional phosphors that relyon rare-earth metals, our pro-posed nanotechnology-basedmaterials are constructed byintegrating II-VI semicon-ductor nanoparticles withpolymeric materials.
Strutynski1, F. Amrani1, B.Kibler1, F. Désévédavy1, J.-C.Jules1, G. Gadret1, D. Deng2,T. Cheng2, Y. Ohishi2, andF. Smektala1; 1LaboratoireInterdisciplinaire Carnot deBourgogne, UMR 6303 CNRS-Université de Bourgogne,Dijon, France; 2ResearchCenter for Advanced PhotonTechnology, Toyota Tech-nological Institute, Nagoya,JapanWe demonstrate 400-THz(0.6-3.3 um) bandwidth SCgeneration in a 10 cm-longsample of tapered telluritesuspended core �ber pumpedby femtosecond pulses withnJ-level energy.
CJ-5.2 MON 11:30Femtosecond mode-lockedpulses from a mid-infrared�ber laser�T. Hu1, S. Jackson2, andD. Hudson1; 1Centre forUltrahigh bandwidth Devicesfor Optical Systems, Universityof Sydney, Sydney, Australia;2MQ Photonics, MacquarieUniversity, Sydney, AustraliaWe report 497 fs pulses froma mode-locked �ber laser op-erating in the mid-infrared at2.8 microns, measured usinga Frequency Resolved OpticalGating method, for applica-tions in mid-infrared photon-ics.
ED-2.2 MON 11:30Dual-comb intracavity highharmonic generation forprecision spectroscopy inthe XUVD. Carlson, T.-H. Wu, and�R.J. Jones; University of Ari-zona, Tucson, United StatesWe show two high power 100fs frequency combs can becoupled to the same enhance-ment cavity for potentiallysimplifying dual-comb spec-troscopy in the XUV and fortime-resolved measurementsof optical nonlinearities.
EG-6.2 MON 11:30Cavity-enhanced ScanningRaman-Imaging ofIndividual CarbonNanotubes�T. Hümmer1,2, M.S.Hofmann1, J. Noe1, A.Högele1, T.W. Hänsch1,2,and D. Hunger1,2; 1Ludwig-Maximilians-Universität,München, Germany;2Max-Planck-Institut fürQuantenoptik, Garching,GermanyWe use fully tunable �ber-based optical Fabry-Pérot mi-crocavities with small modevolumes and high quality fac-tors to detect Raman scatter-ing of individual carbon nan-otubes strongly enhanced bythe Purcell e�ect.
CM-6.2 MON 11:30Femtosecond pulse inducednanostructures in ULE glass�F. Zimmermann1, A. Plech2,S. Richter1, A. Schmitt1,A. Tünnermann1,3, and S.Nolte1,3; 1Institute of AppliedPhysics, Abbe Center ofPhotonics, Friedrich-Schiller-University, Jena, Germany;2Institue for SynchrotronRadiation, Karlsruhe Instituteof Technology, Karlsruhe,Germany; 3Fraunhofer Insti-tute for Applied Optics andPrecision Engineering, Jena,GermanyWe report on ultrashort pulseinduced nanostructures in thebulk of ULE glass. Due to thematerial composition the glassmore likely decomposes intonanometric sheets resulting inincreased form-birefringencein contrast to pristine silica.
CE-6.2 MON 11:30Designing oxynitridenanostructured thin �lms toenhance europium whitelight emission for e�cientsolid state emitters.�I. Camps, A. Mariscal, andR. Serna; Laser ProcessingGroup, Institute of Optics,CSIC, Madrid, SpainWe report the visible broad-band emission of Eu ionsembedded in two di�erentmatrices: a-Al2O3 andSiAlON. �e host natureand the dopant distributiondetermined its oxidation stateand thus the emission spectralshape.
CD-6.2 MON 11:30Dynamics of Phase SensitiveAmpli�cation beyond thelinear limit�A. Martin1,2, S. Combrié3, G.Lehoucq3, and A. de Rossi3;1Université Paris-Sud, Orsay,France; 2Laboratoire de Pho-tonique et de Nanostructures(CNRS UPR20), Marcoussis,France; 3�ales Research andTechnology, Palaiseau, FranceWe accurately measurephase-sensitive ampli�cationin a semiconductor photonicnanowaveguide. In thestrong nonlinear regimethe sinusoidal dependenceon the phase is no longerrespected, consistently withpredictions from generalizedSchroedinger equation.
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ROOM 21 ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM NEWTON2 ROOM ROENTGEN NOTES
White1,2, and �A. Fedrizzi1,2;1Centre for EngineeredQuantum Systems, Schoolof Mathematics and Physics,University of Queensland,Brisbane, Australia; 2Centrefor Quantum Computing andCommunication Technology,School of Mathematics andPhysics, University of Queens-land, Brisbane, Australia;3Institute for QuantumComputing and Departmentof Physics and Astronomy,University of Waterloo,Ontario, Canada; 4School ofPhysics, Monash University,Melbourne, Australia; 5Centrefor Engineered Quantum Sys-tems, Department of Physicsand Astronomy, MacquarieUniversity, Sydney, AustraliaConventional tomographicmethods do not fully capturethe interplay between aquantum system and itsenvironment. We exper-imentally reconstruct anovel super-channel whichfully characterizes initialcorrelations and dynamicsof photons in a simulatedenvironment.
I will overview recent progressin studies of optical wave tur-bulence in �bre lasers. Recenttheoretical, numerical and ex-perimental results includingtransition from quasi-stablelasing regimes to strongly de-veloped wave turbulence willbe presented.
Germany; Institute of Physi-cal Chemistry &Abbe Centerof Photonics, Friedrich SchillerUniversity, Jena, GermanyWe will present the combina-tion of Raman spectroscopywith specially tailored chip-based sampling approachesfor biomedical diagnosislike rapid identi�cation ofpathogens embedded in com-plex matrices, identi�cationof circulating tumor cells andtherapeutic drug monitoring.
I.J. Kim1,2, S.K. Lee1,2,J.H. Sung1,2, T.M. Jeong1,2, F.Sylla3, A. Lifschitz4, V.Malka4,and C.H. Nam1,5; 1Centerfor Relativistic Laser Science,IBS, Gwangju, Korea, South;2Advanced Photonics ResearchInstitute, GIST, Gwangju,Korea, South; 3SourceLAB-Laser Plasma Technologies,LOA, Palaiseau, France;4Laboratoire d’Optique Ap-pliquée, ENSTA ParisTech,CNRS UMR7639, ÉcolePolytechnique, Palaiseau,France; 5Department ofPhysics and Photon Science,GIST, Gwangju, Korea, SouthWe present a coherent con-trol method of laser wake-�eld acceleration processes toachieve stablemulti-GeV elec-tron beams using PW laserpulses.
�Q. Vinckier, F. Duport, A.Smerieri, M. Haelterman, andS. Massar; Université Libre deBruxelles, Bruxelles, BelgiumWe study numerically a re-alistic model of an originalautonomous implementationof a photonic neural net-work in order to demonstrateits high potential to processhigh-bandwidth signals witha strikingly low power con-sumption.
Ho�mann1, C.J. Saraceno1,2,S. Hakobyan1, B. Resan3, A.Rohrbacher3, K. Weingarten3,S. Schilt1, and T. Südmeyer1;1Laboratoire Temps-Fréquence, Université deNeuchâtel, Neuchâtel, Switzer-land; 2Institute for QuantumElectronics, ETH Zurich,Zurich, Switzerland; 3JDSUUltrafast Lasers AG, Schlieren,SwitzerlandWe present the highestaverage power from a diode-pumped Ti:Sapphire laser.Using SESAM-modelockingwe obtain 200-mW in 68-fspulses at 378-MHz. Towardsthe stabilization of this laser,we analyzed its intensity andphase noise characteristics.
EB-1.2 MON 11:30Characterizing anEntangled-Photon Sourcewith Classical Detectors andMeasurements�L. Rozema1, C. Wang2,D. Mahler2, A. Hayat2, A.Steinberg2, J. Sipe2, and M.Liscidini3; 1University ofVienna, Vienna, Austria;2University of Toronto,Toronto, Canada; 3Universitadegli Studi di Pavia, Pavia,ItalyWe experimentally demon-strate the reconstructionof the polarization stateof entangled photon pairsby stimulated emissiontomography.
CI-5.2 MON 11:30Bu�ering Data in aTime-Delayed Neuron-likeRegenerative OptoelectronicPulse Generator�B. Romeira1,2, R. Avo1, J.Figueiredo1, and J. Javaloyes3;1CEOT, Departamento deFísica, Universidade doAlgarve,, Faro, Portugal;2COBRA Research Institute,Eindhoven University ofTechnology, Eindhoven, �eNetherlands; 3Departament deFisica, Universitat de les IllesBaleares, Palma, SpainWe demonstrate, experi-mentally and theoretically,an optoelectronic pulsegenerator operating in aneuron-like excitable regimeand submitted to delayedfeedback, which enablesrobust regenerative signalbu�ering including writing,storage, and reshaping of datasignals.
CA-6.2 MON 11:30Power Scaling ofModelocked Ti:sapphireLaser Pumped by HighPower InGaN Green LaserDiode�H. Tanaka, R. Sawada, R.Kariyama, A. Hosaka, K. Hiro-sawa, and F. Kannari; Depart-ment of Electronics and Electri-cal Engineering, Keio Univer-sity, Yokohama, JapanWe demonstrate a power-scaling of a modelockedTi:sapphire laser pumped byhigh power InGaN-green-LDs, and the maximumoutput power of 44.8 mW wasobtained with the spectrumwidth of 9.2 nm.
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ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 14a ROOM 14bCJ-5.3 MON (Invited) 11:45Fiber lasers at 3 microns andbeyond�R. Vallee, M. Bernier, V.Fortin, A. Haboucha, S. Duval,J.-C. Gauthier, and F. Jobin;Center for Optics Photonicsand Lasers, Quebec, CanadaMid-infrared �ber lasersbased on rare-earth activeions as well as Raman gainare reviewed with respect tofuture challenges in termsof extended wavelengthcoverage as well as averageand peak power scaling.
ED-2.3 MON 11:45High-precisionspectroscopic system basedon a frequency-comb-assisted quantum cascadelaser at around 8.6 �mA. Gambetta1, M. Cassinerio1,N. Coluccelli1, E. Fasci2, A.Castrillo2, D. Gatti1, M.Marangoni1, L. Gianfrani2, P.Laporta1, and �G. Galzerano1;1Istituto di Fotonica eNanotecnologie - CNR andDipartimento di Fisica Politec-nico di Milano, Milano, Italy;2Dipartimento di Matematicae Fisica - Seconda Universitàdi Napoli, Caserta, ItalyWe report on metrological-grade spectroscopic systembased on a quantum cascadelaser, tunable in the wave-length range from 8.56 to 8.63�m, directly phase-locked toa tooth of a mid-IR frequencycomb.
EG-6.3 MON 11:45Coupling nano-antennas tomicrocavities: radiativeinteractions cause strongand tunable frequency shi�s�F. Ruesink, H. Doeleman, R.Hendrikx, F. Koenderink, andE. Verhagen; FOM InstituteAMOLF, Amsterdam, �eNetherlandsWe demonstrate strong fre-quency shi�s in a hybrid sys-tem that couples plasmonicnano-antennas to a high-Qmicrocavity. We recognize ra-diative antenna-cavity inter-actions to be responsible forboth anomalous cavity blue-shi�s and linewidth narrow-ing.
CM-6.3 MON 11:45Functional BirefringentElements Imprinted byFemtosecond LaserNanostructuring ofMulti-Component Glass�M. Beresna1, R. Drevinskas1,A. Lipatiev2, S. Fedotov2, S.Lotarev2, V. Sigaev2, and P.Kazansky1,2; 1OptoelectronicsResearch Centre, Southamp-ton, United Kingdom; 2DMendeleyev University ofChemical Technology ofRussia, Moscow, RussiaAn optical element is im-plemented by femtosecondlaser assisted nanostructuringof alumo-borosilicate glass.Retardance values achievedin this glass is comparableto SiO2 glass. Both glassesexhibit 1 TW/cm2 intensitythreshold for nanostructureformation process.
CK-5.2 MON 11:45AHighly E�cient NonlinearPlatformAlGaAs-On-Insulator�M. Pu, L. Ottaviano, E. Se-menova, and K. Yvind; Tech-nical University of Denmark,Lyngby, DenmarkWe propose an AlGaAs-on-insulator platform fornonlinear integrated photon-ics. We demonstrate highlye�cient four-wave mixingin a 3-mm long AlGaAs-on-insulator nano-waveguide. Arecord high conversion e�-ciency of -8.7 dB is obtainedat 145-mW pump level.
CE-6.3 MON 11:45Synthesis of Ag2Snanocrystals inchalcogenide glass andfs-laser micromachining forphotonic applications�J.M.P. Almeida1, C. Lu2, C.B.Arnold2, and C.R. Mendonça1;1University of São Paulo, SãoCarlos, Brazil; 2PrincetonUniversity, Princeton, UnitedStatesWe have used wet chemistryat room temperature to pro-duce silver sul�de nanocrys-tals in arsenic sul�de solution,which is a low-cost and fastmethod for chalcogenide glassprocessing.
CD-6.3 MON 11:45Towards supercontinuumgeneration by stimulatedRaman-Kerr scattering in anintegrated nonlinear liquidcore �ber�G. Fanjoux1, A. Sudirman2,J.-C. Beugnot1, L. Furfaro1, W.Margulis2, and T. Sylvestre1;1FEMTO-ST institute, Be-sançon, France; 2AcreoSwedish ICT, Kista, SwedenBased on a novel opto�u-idic �ber arrangement, we ex-perimentally demonstrate thegeneration by Raman cascad-ing process in Toluene ofnine Raman orders spectrallybroadened toward supercon-tinuum by stimulated Raman-Kerr scattering.
ED-2.4 MON 12:00QCL frequency stabilizationand measurement with 100Hz - level linewidth, dri�and inaccuracy, using arobust upconversiontechniqueM. Hansen, E. Magoulakis,Q.-f. Chen, I. Ernsting,and �S. Schiller; Institut fürExperimentalphysik, Heinrich-Heine-Universität Düsseldorf,Düsseldorf, GermanyWe demonstrate the �rstfrequency stabilization ofa QCL to a ULE referencecavity, achieving 100 Hzlinewidth and instability. Incombination with a frequencycomb, absolute frequencyuncertainty at the same levelis achieved.
EG-6.4 MON 12:00Coherent Oscillations inWeakly Coupled Cavity QEDby Ultrafast Cavity Switching�H. �yrrestrup1, J.-M.Gérard2,3, and W.L. Vos1;1Complex Photonics Systems(COPS), MESA+ Institutefor Nanotechnology, Univ. ofTwente, Enschede,�e Nether-lands; 2Univ. Grenoble Alpes,INAC-SP2M, Nanophysicsand Semiconductors Lab,Grenoble, France; 3CEA,INAC-SP2M, Nanophysicsand Semiconductors Lab,Grenoble, FranceWe theoretically study sponta-neous emission in weakly cou-pled cavity-QED where thecavity resonance is switchedin time. At su�ciently fastswitching rates the Marko-vian approximation becomesinvalid and Rabi-like oscilla-tions appear in the emitted in-tensity.
CM-6.4 MON 12:00STED - Lithography for Bio- Applications�R. Wollhofen1, B.Buchegger1, F. Hartmann1, C.Wolfesberger2, J. Jacak1,2, andT. Klar1; 1Institute of AppliedPhysics / Johannes KeplerUniversity Linz, Linz, Austria;2Upper Austria University ofApplied Sciences, Linz, AustriaSTED-lithography allows usto write polymeric structureswith 55 nm feature size inall three dimensions with alateral resolution of 120 nm.�e polymers allow for easilybiofunctionalization with pro-teins or covalent surface mod-i�cation.
CK-5.3 MON 12:00Second-HarmonicGeneration Engineering inLithium NiobateNanopillars�M.A. Baghban,M. Swillo, andK. Gallo; KTH Royal Instituteof Technology, Stockholm, Swe-denSingle LiNbO3 nanopillarswith diameters rangingfrom 150nm to 500nm havebeen fabricated. Experi-mental results demonstratenonlinearity enhancementand tailoring of the secondharmonic polar emissionpatterns with a control of thepillar size.
CE-6.4 MON 12:00Enhanced EmissionRadiation of GaAs/AlGaAsNanowire Laser by PurcellE�ect�W. Wei, X. Zhang, X. Yan,and X. Ren; Beijing Universityof Posts and Telecommunica-tions, Beijing, China, People’sRepublic of (PRC)We demonstrate enhancedemission radiation ofGaAs/AlGaAs nanowirelaser by Purcell e�ect, takingadvantage of the local electric�eld enhancement of theplasmonic mode to enhancethe recombination rate of theGaAs/AlGaAs nanowire.
CD-6.4 MON 12:00Intracavity up-conversion to631 nm of 1550 nm eye-safeimages in a GdVO4:Nd
3+-PPLN laserA.J. Torregrosa1, H. Maestre1,M.L. Rico2, and �J. Capmany1;1Universidad MiguelHernández, Elche, Spain;2Universidad de Alicante,Alicante, SpainWe present a wavelength up-conversion system to 631 nmof eye-safe infrared imagesat 1550 nm based on sum-frequency mixing in a pe-riodically poled lithium nio-bate crystal placed inside thecavity of a diode pumpedGdVO4:Nd
3+ laser.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 21 ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM NEWTON2 ROOM ROENTGEN NOTESEB-1.3 MON 11:45Multipartite entanglementdetection with minimale�ort�L. Knips1,2, C. Schwemmer1,2,N. Klein1,2, M. Wieśniak3,and H. Weinfurter1,2;1Department für Physik,LMU, Munich, Germany;2MPI für Quantenoptik,Garching, Germany; 3Instituteof �eoretical Physics andAstrophysics, University ofGdańsk, Gdańsk, PolandWe show how to design non-linear witnesses for genuinemultipartite entanglementwith only two correlationmeasurements independentof the number of qubits andpresent experimental dataof states like GHZ or clusterstates for illustration.
EF-5.2 MON 11:45Optical Rogue Waves inintegrable turbulence�P. Walczak, S. Randoux, andP. Suret; Université Lille 1, Vil-leneuve d’Ascq, FranceWe present an optical �berexperiment designed to studyintegrable turbulence inthe focusing regime of theone-dimensional nonlin-ear Schrödinger equation.Our experimental resultssupported by numerical sim-ulations reveal the formationof optical rogue waves.
JSII-2.2 MON 11:45Polymeric microsystemswith SERS integratedmicro�uidicsS. Uusitalo1, J. Hiltunen1,�P. Karioja1, S. Siitonen2,and V. Kontturi3; 1VTTTechnical Research Centreof Finland, Oulu, Finland;2Nanocomp Ltd., Lehmo, Fin-land; 3University of EasternFinland, Joensuu, FinlandWe have developed high-throughput manufacturingmethods for nanophotonicsensor structures using poly-mer materials and roll-to-rollprinting. Recent achieve-ments reported in this paperinclude the integration ofmicro�uidic structures withSurface-Enhanced-Raman-Spectroscopy (SERS) sensorstructures.
JSIII-1.2 MON (Invited) 11:45Laser-plasma acceleration ofelectrons to 2 GeV andbeyond�M. Downer; University ofTexas at Austin, Austin,United StatesLaser-plasma acceleratorsnow produce multi-GeVelectrons using petawattlasers. I will highlight recentresults that uniquely employ~150 fs petawatt drive pulses,and review new plasmadiagnostics that dynamicallyimage the underlying plasmastructures.
CI-5.3 MON 11:45An Optical Regenerator forLong Distance Stable FiberDelivery of Radio FrequencyStandards Based on TwoMode Injection Locked FPLasersT. Nikas1, �A. Bogris2, andD. Syvridis1; 1National andKapodistrian Universityof Athens, Athens, Greece;2Technological EducationalInstitute of Athens, Athens,GreeceWe propose and experi-mentally validate a new coste�ective optical receiver* regenerator scheme forlong distance microwavefrequency standard dis-semination, based on theproperties of dual wavelengthinjection locked Fabry * Perot(FP) lasers.
CA-6.3 MON 11:45A vortex Raman laser withsum-frequency emission at559 nm�A. Lee1, H. Pask1, and T.Omatsu2; 1Macquarie Univer-sity, Sydney, Australia; 2ChibaUniversity, Chiba, JapanWe report sum-frequencygeneration within an intracav-ity self-Raman vortex laser.We observe di�erent near-and far-�eld spatial pro�les,and time-varying topolog-ical charge, and present atheoretical model whichsupports these experimentalobservations.
EB-1.4 MON 12:00Revealing GenuineOptical-Path Entanglement�F. Monteiro1, V. CapraraVivoli1, T. Guerreiro1, A.Martin1, J.D. Bancal2, H.Zbinden1, N. Sangouard3, andR. �ew1; 1Group of AppliedPhysics, University of Geneva,Geneva, Switzerland; 2Centrefor Quantum Technologies,National University of Singa-pore, Singapore, Singapore;3Department of Physics,University of Basel, Basel,SwitzerlandWe propose a scalable methodfor detecting entanglementbetween multiple opticalpaths sharing a single photon.�e method is demonstratedexperimentally with two andthree optical paths, and isresistant to loss.
EF-5.3 MON 12:00Optical Rogue Waves inVortex Turbulence�C. Gibson, A. Yao, and G.-L. Oppo; University of Strath-clyde, Glasgow, United King-domWe introduce a novel mech-anism to generate roguewaves in nonlinear opticalsystems with a low-amplitude,detuned injected �eld. Wecharacterize this vortexturbulence and demonstrateits di�erence from stochasticsuperpositions of randomwaves.
JSII-2.3 MON 12:00Accessible Near�elds viaPlasmonic Nanoantennas onNanopedestals forUltra-Sensitive VibrationalIR-Spectroscopy�D. Etezadi1,2, A.E. Cetin1,2,and H. Altug1,2; 1ÉcolePolytechnique Federale deLausanne (EPFL), Lau-sanne, Switzerland; 2BostonUniversity, Boston, UnitedStatesWe introduce polarization-insensitive plasmonicnanoring antennas onnanopedestals to experi-mentally enable high surfaceenhanced infrared absorption(SEIRA) signals in biosensing.�ese fabricated antennasprovide larger and highlyaccessible near�elds o�eringoptimized overlap withbiomolecules.
CI-5.4 MON 12:00BER PerformanceEvaluation and HeaderRecognition UsingAll-Optical Flip-FlopOperation with AND-GateFunctionality�T. Katayama, D. Hayashi, K.Nakao, and H. Kawaguchi;Nara Institute of Science andTechnology, Ikoma, JapanWe evaluated BER perfor-mance of �ip-�op operationwith AND-gate functionalityusing 1.55-�m polarizationbistable VCSELs. �e BERwere 8.0x10^-8 and 1.6x10^-2for 500-Mb/s and 6-Gb/ssignals. We applied thisoperation to an optical packetswitching.
CA-6.4 MON 12:00High E�ciency TEM00diode end-pumpedAlexandrite laser�E. Arbabzadah1, W.Kerridge-Johns1, G. �omas1,A. Minassian2, and M.Damzen1; 1Imperial CollegeLondon, London, UnitedKingdom; 2Unilase Ltd,London, United KingdomWe present the higheste�ciency ever produced froma TEM00 diode-pumpedAlexandrite laser (Power>1W,ηs=48%) and provide anexplanation for laser slopee�ciency dependence onoutput coupling by theinclusion of pump excitedstate absorption.
101
CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 14a ROOM 14bCJ-5.4 MON 12:15Extending of FlattenedAll-Normal DispersionWavelength Range inAll-Solid So�-GlassPhotonic Crystal Fiber�B. Siwicki1,2, R.Kasztelanic1,2, M. Klimczak1,J. Cimek1,2, D. Pysz1, R.Stepień1, and R. Buczyński1,2;1Institute of ElectronicMaterials Technology, War-saw, Poland; 2University ofWarsaw, Faculty of Physics,Warsaw, PolandWe demonstrate results onextending the �attened, all-normal dispersion wavelengthrange in all-solid photoniccrystal �bers. We demonstrate�bers from various thermallymatched glasses overcomingthe limitation of dispersionengineering coming from thematerial contribution.
ED-2.5 MON 12:15Millimeter-wave synthesizerwith optically derivedinstability of 10^-15�T. Fortier1, A. Rolland1,F. Quinlan1, F. Baynes1,A. Hati1, A. Ludlow1, N.Hinkley1, N. Shimizu3, T.Ishibashi3, J. Campbell2, andS. Diddams1; 1NIST, Boul-der, Boulder, United States;2Univsersity of Virginia,Charlottsville, United States;3NTT Electronics TechnoCorporation, Atugi-shi, JapanWe demonstrate agile synthe-sis of ultra-low noise mm-wave signals with a fractionalfrequency instability of 10-15using a combination of opticalfrequency division, direct dig-ital synthesis and opto-electricmultiplication.
EG-6.5 MON 12:15A Hybrid Photonic Nanowire-Cavity Design for a Single-Indistinguishable-PhotonSource�N. Gregersen1, J. Mork1, J.Claudon2, and J.-M. Gérard2;1DTU Fotonik, Department ofTechnical Engineering, Tech-nical University of Denmark,Kongens Lyngby, Denmark;2CEA-CNRS-UJF Group*Nanophysique et Semicon-ducteurs*, CEA, INAC, SP2M,Grenoble, French PolynesiaWe propose a photonicnanowire single-photonsource design incorporatinga distributed Bragg re�ectorin the inverted taper. �eresulting weak cavity accel-erates the photon emissionrate and reduces detrimentaldecoherence e�ects from thesolid-state environment.
CM-6.5 MON 12:15Novel ImplantationTechnique for Gain Media inSilicon Photonics�M. Murray, S. Micklethwaite,A. Jha, and G. Jose; Institutefor Materials Research, Schoolof Chemical and Process En-gineering, University of Leeds,Leeds, United KingdomModi�cation of single-crystalline silicon surfacesthrough the novel photonicsplatform processing tech-nique ultrafast laser plasmaimplantation. Active andpassive regions on a singlechip with shadow masking,operational at 1.5�m areformed with this method.
CK-5.4 MON 12:15Simultaneous Super-continuum and�irdHarmonic Generation inSi3N4 waveguides�J. Epping1, T. Hellwig2, M.Hoekman3, R. Mateman3,A. Leinse3, R. Heideman3,A. van Rees4, P. van derSlot1, C. Lee1, C. Fallnich1,2,and K. Boller1; 1Universityof Twente, Enschede, �eNetherlands; 2WestfälischeWilhelms-Universität, Mün-ster, Germany; 3LioniX BV,Enschede, �e Netherlands;4XiO Photonics BV, Enschede,�e NetherlandsWe report 1550nm pumpedsimultaneous third harmonicand supercontinuum genera-tion in thick Si3N4 waveg-uides fabricated with a novelmethod. �e respective band-widths are 20nm (at -10dB)and 715nm (at -30dB).
CE-6.5 MON (Invited) 12:15Materials for MedicalImaging and Bio-Imaging�B. Viana; IRCP Chimie Paris-tech, Paris, FranceMajor improvements havebeen made in the materialsused for scintillators andoptical imaging including agood control of the defectsand the kinetics. Persistentluminescence nanosensorscan be used for di�erentmodalities in Bioimaging.
CD-6.5 MON 12:151.8 W, 80 MHz, picosecond,Yb-�ber-based ultravioletsources at 266 nm�S. Chaitanya Kumar1, J.Canals Casals1, E. SanchezBautista1, K. Devi1, and M.Ebrahim-Zadeh1,2; 1ICFO-�eInstittute of Photonic Sciences,Barcelona, Spain; 2InstitucioCatalana de Recerca i EstudisAvancats (ICREA), Barcelona,SpainWe report the �rst stable,high-average-power, MHz-repetition-rate, picosecondUV source, providing asmuch as 1.8 W at 266 nm withexcellent long-term powerstability (4% rms, 16 hours)in high beam quality withTEM00 mode-pro�le.
CJ-5.5 MON 12:30Atmospheric propagatione�ects of high-powerultrafast mid-infrared laserradiation�M. Gebhardt1, C. Gaida1,F. Stutzki1, S. Hädrich1,3,C. Jauregui1, J. Limpert1,2,3,and A. Tünnermann1,2,3;1Institute of Applied Physics,Abbe Center of Photonics,Jena, Germany; 2FraunhoferInstitute for Applied Opticsand Precision Engineering,Jena, Germany; 3Helmholtz-Institute, Jena, GermanyWe present a rigorous studyon high-power ultrashort-pulse propagation e�ectscaused by atmosphericmolecular absorption linesincluding mitigation strate-gies. �ese e�ects can be asigni�cant challenge to per-formance scaling of ultrafastmid-infrared laser sources.
ED-2.6 MON 12:30Doppler Broadening�ermometry by means ofdual-laser absorptionspectrometry at 1.39 �mE. Fasci1, H. Dinesan1, P.Amodio1, M.D. De Vizia1, A.Merlone2, G. Galzerano3, P.Laporta3, A. Castrillo1, �L.Moretti1, and L. Gianfrani1;1Dipartimento di Matematicae Fisica, Seconda Universitàdi Napoli, Caserta, Italy;2INRIM, Istituto Nazionale diRicerca Metrologica, Torino,Italy; 3Dip. di Fisica, Politec-nico di Milano, Milano, ItalyRecent advances towardsthe development of low-uncertainty Doppler broad-ening thermometry arereported. A 3rd-generationexperiment in the near-infrared region, for the aimsof the spectroscopic deter-mination of the Boltzmannconstant, will be illustrated.
EG-6.6 MON 12:30Correlated Photons FromMicrocavity Polaritons�M. Sassermann1, Z. Vörös1,G. Weihs1, and W. Langbein2;1Institut für Experimental-physik, Universität Innsbruck,Innsbruck, Austria; 2Cardi�university school of physics andastronomy, Cardi�, UnitedKingdomIn this contribution, wepresent our experimentalresults on the generation ofcorrelated photon pairs basedon high-quality microcavitystructures. We presentmeasurements on the degreeof correlations as a functionof experimental parameters.
CM-6.6 MON 12:30UV Laser-Induced PolingInhibition produces BulkDomains in MgO-dopedLithium Niobate Crystals�A. Boes1, H. Steigerwald1,D. Yudistira1, V. Sivan1, S.Wade2, S. Mailis3, E. Soergel4,and A. Mitchell1; 1ARC Centerfor Ultra-high BandwidthDevices for Optical Systems(CUDOS), RMIT Univ., Mel-bourne, Australia; 2Facultyof Science, Engineering andTechnology, Swinburne Univ.of Technology, Hawthorn,Australia; 3OptoelectronicsResearch Centre, Univ. ofSouthampton, Southampton,United Kingdom; 4Institute ofPhysics, Univ. of Bonn, Bonn,GermanyBulk domains are achieved inMgO-doped lithium niobateby using a domain invertedsurface template obtained byUV laser-induced poling inhi-bition. �e quality of the ob-tained bulk domains is veri-�ed by second harmonic gen-eration.
CK-5.5 MON 12:30Impact of Nonlinear Loss onSilicon Microwave PhotonicProcessors�B. Morrison, A. Casas-Bedoya, B. Eggleton, andD. Marpaung; CUDOS,University of Sydney, Sydney,AustraliaWe experimentally investi-gate, for the �rst time, thee�ect of nonlinear losses insilicon waveguides on theperformance of an integratedmicrowave photonic proces-sor and �nd that standardnanowires cannot achievesu�ciently high performance.
CD-6.6 MON 12:30Numerical and Experi-mental Study of Optoelec-tronic Trapping on aLithium Niobate Substratein Di�erent Conditions�G. Nava1,2, M. Gazzetto1,3,A. Zaltron4, P. Minzioni1, C.Sada4, and I. Cristiani1; 1Dip.di Ingegneria Industriale edell’Informazione, Univ. diPavia, Pavia, Italy; 2Dep.of Biomedical Science andTranslational Medicine, Univ.di Milano, Milano, Italy;3Institute of Applied Physics,Univ. of Bern, Bern, Switzer-land; 4Physics and AstronomyDep., Univ. of Padua, Padova,ItalyWe report about a set ofnumerical simulations ana-lyzing the dielectrophoreticforces induced by the pho-torefractive e�ect in a Fe:LNsubstrate, in di�erent condi-tions. �e obtained results arevalidated by comparison withexperimental data.
102
CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 21 ROOM CURIE ROOM EDISON ROOM EINSTEIN ROOM NEWTON2 ROOM ROENTGEN NOTESEB-1.5 MON (Invited) 12:15Testing quantum correla-tions of three entangledphotons generated incascaded parametricdown-conversion�T. Jennewein1, D.R. Hamel1,2,L.K. Shalm1,3, H. Hübel4,A.J. Miller3,5, F. Marsili3,V.B. Verma3, R.P. Mirin3,S.W. Nam3, and K.J. Resch1;1Institute for QuantumComputing, University ofWaterloo, Waterloo, Canada;2Département de physiqueet d*astronomie, Univer-sité de Moncton, Moncton,Canada; 3National Instituteof Standards and Technol-ogy, Boulder, United States;4Department of Physics, Stock-holm University, Stockholm,Sweden; 5Albion College,Albion, United StatesWe show the direct produc-tion of polarization-entangledphoton triplets by cascadingtwo entangled downconver-sion processes, and demon-strate heralded Bell states, aswell as tests of local realismby violating the Mermin andSvetlichny inequalities.
EF-5.4 MON 12:15Dark Soliton Statisticsduring Radiation Build-Upof Bright DissipativeSolitons in Long-CavityMode-Locked Fiber LasersR.I. Woodward and �E.J.R.Kelleher; Femtosecond OpticsGroup, Department of Physics,Imperial College London, Lon-don, United KingdomWe numerically study thestart-up dynamics of long-cavity, normal dispersionmode-locked �ber lasers,and reveal the birth andpersistence of dark soliton-like structures within theevolution of a stationarybright dissipative soliton.
JSII-2.4 MON (Invited) 12:15Opto Acoustic Toolbox forDisease Diagnostics�J.M. Cooper, J. Reboud, R.Wilson, S.N. Neale, and C.Witte; University of Glasgow,Glasgow, United KingdomHere we show how new de-velopments in the area of mi-cro�uidics open the way tocheap point-of-care diagnos-tics for infectious diseases us-ing acoustic and electromag-netic waves to perform on-chip sample processing andenrichment.
JSIII-1.3 MON 12:15Ultra-Low Emittance BeamGeneration in a Laser-Plasma Accelerator usingTwo-Color IonizationInjection�C. Schroeder1, J.-L. Vay1,E. Esarey1, S. Bulanov1, C.Benedetti1, L. Yu2, M. Chen2,C. Geddes1, and W. Leemans1;1Lawrence Berkeley NationalLaboratory, Berkeley, UnitedStates; 2Shanghai Jiao TongUniversity, Shanghai, China,People’s Republic of (PRC)Amethod of generating ultra-low emittance beams (tens ofnm) in laser-plasma accelera-tors is presented. �is methodrelies on using two lasers withdi�erent colors to ionize andtrap electrons in a laser-drivenwake.
CI-5.5 MON 12:15Monolithic dual-wavelengthDFB lasers for thegeneration ofoptically-carried RF localoscillators�M. Romanelli1, F. Van Dijk2,L. Wang1, and M. Vallet1;1Institut de Physique deRennes, Rennes, France; 2III-VLab, Palaiseau, FranceFrequency-shi�ed feedbackmonolithic DFB lasers lead toRF phase-locking at 10 GHz.�e phase noise level of thelocal oscillator is reported onthe beat-note. �e methodis extended to new OEOarchitectures.
CA-6.5 MON 12:15Birefringent Filter Tuningand Linewidth Narrowing ina Mode-Locked PumpedDeep-Ultraviolet Continu-ous-Wave Ce:LiCAF Laser�B. Wellmann, O. Kitzler, D.J.Spence, and D.W. Coutts; MQPhotonics Research Centre,Department of Physics andAstronomy, Faculty of Scienceand Engineering, MacquarieUniversity, North Ryde,AustraliaWe report spectral controlof a mode-locked-pumpedcontinuous-wave solid-stateCe:LiCAF laser, with birefrin-gent �lter tuning over a rangeof 13 nm around 290 nm, andlinewidth narrowing down to0.75 pm.
EF-5.5 MON 12:30Experimentaldemonstration ofModulation Instability indispersion oscillating �berring cavity�F. Copie1, M. Conforti1, A.Kudlinski1, S. Trillo2, and A.Mussot1; 1PhLAM, Villeneuved’Ascq, France; 2Università diFerrara, Ferrara, ItalyWe study experimentally themodulation instability processin a dispersion oscillating�berring cavity. Such a dispersionpro�le leads to the emergenceof new sidebands in the opti-cal spectra in excellent agree-ment with theory.
JSIII-1.4 MON 12:30Multi-GeV Electron Beamsat the BErkeley Lab LaserAccelerator�A. Gonsalves1, K.Nakamura1, J. Daniels1,H.-S. Mao1, C. Benedetti1, C.Schroeder1, C. Toth1, J. vanTilborg1, D. Mittelberger1,S. Bulanov1,2, J.-L. Vay1, C.Geddes1, E. Esarey1, andW. Leemans1,2; 1LawrenceBerkeley National Laboratory,Berkeley, United States;2University of California,Berkeley, United StatesLaser pulses with peak power0.3PW generated electronbeams with energy >4GeV ina 9cm-long plasma waveg-uide. Accurate alignment anda high Strehl ratio allowed forstable beams with pointing�uctuation of 0.6mrad rms.
CI-5.6 MON 12:30Wirelessmillimetre-wave-lightwavesignal conversion usingpatch-antennas on LiNbO3optical modulator�Y.N. Wijayanto1, A. Kanno1,T. Kawanishi1, H. Murata2,and Y. Okamura2; 1NationalInstitute of Information andCommunications Technology,Tokyo, Japan; 2Osaka Univer-sity, Osaka, JapanPatch-antennas on a LiNbO3optical modulator are pro-posed for direct wirelessmillimetre-wave-lightwavesignal conversion. �eproposed device was designedand fabricated successfullyfor 40GHz millimetre-wavebands. Its performance wasmeasured in a Fiber-Wirelesslink.
CA-6.6 MON 12:30First Mode-LockedOscillation of DirectlyLaser-Diode-PumpedCr4+:YAG Single-CrystalFiber Laser�S. Ishibashi; NTT DeviceTechnology Labs, NTT Corpo-ration, Atsugi-shi, KanagawaPref., JapanCr4+:YAG single-crystal �berlaser with direct laser-diodepumping is mode-locked forthe �rst time, with a pulseduration of 137 fs, by se-lecting the fundamental trans-verse mode of the multimodewaveguide using an externalcavity.
103
CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 114:30 – 15:30PL-3: CLEO/Europe 2015 Plenary TalkChair: Luc Bergé, CEA - DAM, Arpajon, France
PL-3.1 MON (Plenary) 14:30New Horizons for Combs of Light�T.W. Hänsch; Max-Planck-Institute of Quantum Optics,Garching, Germany
Mode-locked femtosecond lasers and related emerg-ing miniaturized devices can produce optical frequencycombs, which consist of a large number of preciselyevenly spaced spectral lines. Almost two decades ago,such combs were introduced as tools for optical fre-quency metrology, motivated by the challenges of pre-cision laser spectroscopy of atomic hydrogen as testsfor fundamental physics laws. Laser frequency combs
provide the long-missing clockwork for optical atomicclocks, which are now approaching relative frequencyuncertainties of 10-18. Distant clocks can be comparedvia optical �ber links at the 10-19 level, opening new op-portunities for relativistic geodesy and astronomical in-terferometry. As calibration tools for astronomical spec-trographs, frequency combs are facilitating the searchfor exoplanets, and they may lead to direct evidence
for the accelerating expansion of space in our universe.Laser combs are also becoming powerful instrumentsfor broadband molecular spectroscopy. �ey can dra-matically improve the resolution and recording speedof Fourier spectrometers, and they are creating intrigu-ing new opportunities for highly multiplexed nonlinearspectroscopy and microscopy
ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13b15:45 – 16:30CJ-6a: Waveguide LasersChair: Jacob Mackenzie, ORC, Uni-versity of Southampton, United King-dom
15:45 – 16:30ED-1b: Frequency Combs IIChair: Stephan Schiller, Heinrich-Heine-Universität Düsseldorf, Düs-seldorf, Germany
15:45 – 16:30EG-5b: Interaction of Elec-trons with Optical Near-�elds IIChair: Nahid Talebi, Max PlanckInstitute for Intelligent Systems,Stuttgart, Germany
15:45 – 16:30CM-5b: FundamentalAspects of Laser MatterInteraction IIChair: Marta Castillo, CSIC,Madrid, Spain
15:45 – 16:30CK-4b: QuantumInformation Processing IIChair: Tapio Niemi, OptoelectronicsResearch Centre Tampere Universityof Technology, Tempere, Finland
15:45 – 16:30CA-5b: Microchip Lasers IIChair: Mauro Tonelli, Universita’ diPisa, Pisa, Italy
CJ-6a.1 MON 15:45Waveguides for Active Yb:YAGBeam-Splitters Inscribed by afs-Laser�T. Calmano1,2, C. Kränkel1,2, andG. Huber1,2; 1Institut für Laser-Physik, Universität Hamburg, Ham-burg, Germany; 2�e Hamburg Cen-tre for Ultrafast Imaging, Hamburg,GermanyHere we present active Yb:YAGbeam-splitters with watt level out-put powers. �ese devices werefabricated by femtosecond-laser in-scription. Furthermore, a variablesplitting ratio resulting from an im-plemented multi-mode interferencesection was achieved.
ED-1b.1 MON 15:45Graphene modulator applied toeither fceo or frep Er comb control�N. Kuse1, C.-C. Lee2, J. Jiang1,C. Mohr1, T.R. Schibli2, and M.Fermann1; 1IMRA America, AnnArbor, United States; 2Departmentof Physics, University of Colorado,Boulder, United StatesWe demonstrate graphene modula-tor can be used to stabilize eitherfceo and frep in Er frequency combs.Locked fceo and frep are better thanlocked fceo by pump current andlocked frep by bulk EOM.
EG-5b.1 MON 15:45Waveform Controlled ElectronEmission from Isolated Nano-particles near Optical Damage�reshold�S. Zherebtsov1,2, P. Rupp1, F.Süßmann1,2, Q. Liu1, L. Sei�ert3, J.Stierle1, V. Mondes4, J. Plenge4, A.Kessel1, S. Trushin1, B.-N. Ahn5,6,D.-E. Kim5,6, C. Graf4, E. Rühl4,T. Fennel3, and M. Kling1,2; 1MPIfür Quantenoptik, Garching, Ger-many; 2Physik Department, LMUMünchen, Garching, Germany;3Institut für Physik, Univ. Rostock,Rostock, Germany; 4Physical Chem-istry, FU Berlin, Berlin, Germany;5Physics Department, POSTECH,Pohang, Korea, South; 6Max PlanckCenter for Attosecond Science,Pohang, Korea, SouthIntensity dependent waveform con-trolled electron emission from iso-lated nanospheres has been studiedin the range from low intensities inthe nonadiabatic tunnelling regimeto the near optical damage thresh-old.
CM-5b.1 MON 15:45E�ect of laser pulse duration onlaser assisted atom probe analysison metals and oxidesH. Wang2, J. Houard1, �A. Hideur2,L. Arnoldi1, B. Deconihout1, andA. Vella1; 1GPM UMR 6634, Nor-mandie Université, Saint Etiennedu Rouvray, France; 2CORIA UMR6614, Normandie Université, SaintEtienne du Rouvray, FranceUsing laser assisted atom probe to-mography, we study the in�uence ofthe laser pulse duration on the ion-ization of surface atoms frommetal-lic and oxides nanometric tip, underhigh DC �eld.
CK-4b.1 MON (Invited) 15:45Quantum Information ProcessingUsing Active Silicon PhotonicIntegrated Circuits�D. Englund1, J. Mower1, N.Harris1, G. Steinbrecher1, F. Naja�1,Y. Lahini2, T. Baehr-Jones3, M.Hochberg3, and K. Berggren1;1Research Laboratory of Elec-tronics, Massachusetts Institute ofTechnology, Cambridge, UnitedStates; 2Department of Physics,Massachusetts Institute of Tech-nology, Cambridge, United States;3Coriant Advanced TechnologyGroup, Naperville, United StatesWe discuss recent e�orts to imple-ment optical quantum informationprocessing devices in silicon pho-tonic integrated circuits. We de-scribe such PICs for quantum keydistribution, and we analyze multi-waveguide programmable PICs forquantum simulation.
CA-5b.1 MON 15:45High repetition rate 1.34 umNd:YVO4 microchip laserQ-switched with GaInNAs SESAM�J. Nikkinen, V.-M. Korpijärvi, I.Leino, A. Härkönen, and M. Guina;Optoelectronics Research Centre,Tampere University of Technology,Tampere, FinlandWe demonstrate 1.34-um Nd:YVO4microchip laser Q-switched with aGaInNAs/GaAs-based SESAM. �elaser produced 204 ps long pulseswith 24 mW average power and 2.3MHz repetition rate.
CJ-6a.2 MON 16:00Femtosecond-Laser-WrittenYb3+:CaAlGdO4 Waveguide Laser�K. Hasse1, B. Deppe1,2,3, C.Kränkel1,2, and T. Calmano1,2;1Institut für Laser-Physik, Univer-
ED-1b.2 MON 16:00Resolving the teeth of opticalfrequency comb with a multi-mode �ber spectrometerM. Cassinerio1, �N. Coluccelli1, B.Redding2, H. Cao2, P. Laporta1,
EG-5b.2 MON 16:00Strong-�eld plasmonic photo-emission in the mid-IR at 1GW/cm2 intensityP. Rácz1, S. Teichmann2, M.Ciappina3, J.A.P. Hernández4, A.
CM-5b.2 MON 16:00Dynamics of femtosecond laserenergy deposition in dielectrics�O. Uteza, M. Lebugle, M. Sentis,and N. Sanner; Aix Marseille Univ.,CNRS, LP3 UMR 7341, Marseille,
CA-5b.2 MON 16:00Automobile Engine Ignition by aPassively Q-switchedNd:YAG/Cr4+:YAG Laser�N. Pavel1, T. Dascalu1, M. Dinca2,G. Salamu1, N. Boicea3, and A.
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NOTES
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES15:45 – 16:30CE-5b: SemiconductorTechnology and Semicon-ductor Characterization IIChair: Michael Jetter, University ofStuttgart, Stuttgart, Germany
15:45 – 16:30CD-5b: Applications ofNonlinearities IIChair: Mario Bertolotti, La SapienzaUniversita’ di Roma, Roma, Italy
15:45 – 16:30EB-2a: Quantum CoherenceChair: �omas Jennewein, Univer-sity of Waterloo, Waterloo, Canada
15:45 – 16:30EF-4b: Extreme Events inOptics IIChair: Massimo Giudici, INLN, Uni-versité de Nice, Nice, France
15:45 – 16:30EE-5b: Material Dynamics onUltrafast Time Scale IIChair: Matteo Clerici, PhD Marie-Curie IOF Fellow Heriot-Watt Uni-versity, Edinburgh, United Kingdom
CE-5b.1 MON (Invited) 15:45Integration of cubic III/Vsemiconductors on silicon (001)�K. Volz; Faculty of Physics and Ma-terials Science Center, Philipps Uni-versität, Marburg, GermanyDefect-free integration of cubicIII/V semiconductors on exactSi(001) substrates allows to realizeseveral novel optoelectronic de-vices. �is contribution will reviewthe state of the art of the growthand give some examples for devices.
CD-5b.1 MON (Invited) 15:45Chirp determination of ultrashortpulses via transverse second-harmonic generation randomnonlinear crystals�B. Wang1, C. Cojocaru1, I. Sola2,A. Parra1, W. Krolikowski3,4,Y. Sheng3, R. Vilaseca1, and J.Trull1; 1Universitat Politècnicade Catalunya, Barcelona, Spain;2Universidad de Salamanca, Sala-manca, Spain; 3Australian NationalUniversity, Canberra, Australia;4Texas A&M University at Qatar,Doha, QatarWe determine the initial chirp pa-rameter and the duration of pulsesdown to 30 fs via single-shot auto-correlation method based on trans-verse second harmonic generationin crystals with random distributionof inverted nonlinear domains.
EB-2a.1 MON 15:45Measurements on the reality ofthe wavefunction�M. Ringbauer1,2, B. Du�us1,2, C.Branciard1,3, E.G. Cavalcanti4, A.G.White1,2, and A. Fedrizzi1,2; 1Centrefor Engineered Quantum Systems,School of Mathematics and Physics,�e University of Queensland, Bris-bane, Australia; 2Centre for Quan-tum Computation and Communica-tion Technology, School of Mathe-matics and Physics, �e Universityof Queensland, Brisbane, Australia;3Institut Nèel, CNRS and Univer-sité Genoble Alpes, Grenoble, France;4School of Physics, University of Syd-ney, Sydney, Australia�e nature of the wavefunction hasbeen one of the longest standingphilosophical problems in quantumfoundations. Using single pho-tons we experimentally demonstratethat epistemic interpretations of thewavefunction cannot fully explainquantum phenomena.
EF-4b.1 MON 15:45Extreme events and heavy-taileddistributions in an Yb-doped �berlaser self-pulsed by stimulatedBrillouin scatteringM. Tang, �T. Godin, and A. Hideur;CORIA, Normandie Université,Saint Etienne du Rouvray, FranceWe report the experimental obser-vation of highly-localized temporalpulses and heavy-tailed statistics ina high-power �ber laser self-pulsedby SBS. �is preliminary opens upa new �eld of investigation of rogueevents in laser physics.
EE-5b.1 MON 15:45Coherent Raman Laser - anObserver of Fast VibrationalDynamicsI. Aharonovich and �A. Pe’er; BarIlan University, Ramat Gan, IsraelWe propose an optical oscillator,where the emitted light from a co-herent vibrational wave-packet isampli�ed beyond the oscillationthreshold. �e mode-competitionin the resonator solves in real time amajor problem of coherent control.
EB-2a.2 MON 16:00Quantum information withtemporal modes�B. Brecht1, D.V. Reddy2, C.Silberhorn1, and M.G. Raymer2;1Applied Physics, University of
EF-4b.2 MON 16:00Observation of Black VectorRogue Waves in the NormalDispersion Regime of OpticalFibers�B. Frisquet1, B. Kibler1, J.
EE-5b.2 MON 16:00Non-Instantaneous PolarizationDynamics in Resonant Dielectrics�J. Hyyti1,2, M. Hofmann3, S.Birkholz1, M. Bock1, S.K. Das1,4,R. Grunwald1, M. Ho�mann5, T.Nagy5,6, A. Demircan6, M. Jupé7,D. Ristau7, U. Morgner5,7, C. Brée3,M. Woerner1, T. Elsaesser1, and G.Steinmeyer1,2; 1Max Born Institutefor Nonlinear Optics and Short PulseSpectroscopy, Berlin, Germany;2Optoelectronics Research Centre,
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ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13b
sität Hamburg, Hamburg, Germany;2�e Hamburg Centre for UltrafastImaging, Universität Hamburg,Hamburg, Germany; 3Center forFree-Electron Laser Science, DESY,Hamburg, GermanyA femtosecond-laser written waveg-uide laser in Yb3+:CaAlGdO4 hasbeen realized for the �rst time. �emaximum output power was 2.2Wat an incident pump power of 5.3W.Slope e�ciencies of up to 52% wereachieved.
and G. Galzerano1; 1Dipartimentodi Fisica - Politecnico di Milano andIstituto di Fotonica e Nanotecnologie- CNR,Milano, Italy; 2Department ofApplied Physics, YaleUniversity, NewHaven, Connecticut, United StatesWe present a new direct frequencycomb spectroscopy technique withcomb-tooth level resolution, basedon the frequency dependence of thespeckle pattern generated at the out-put of a multi-mode �ber.
�ai2, J. Fekete1, A. Elezzabi5, L.Veisz3, J. Biegert2, and �P. Dombi1;1Wigner Research Centre for Physics,Budapest, Hungary; 2ICFO �eInstitute of Photonic Sciences,Barcelona, Spain; 3Max-Planck-Institut für Quantenoptik, Garching,Germany; 4Centro de Láseres Pulsa-dos, Salamanca, Spain; 5Universityof Alberta, Department of Electricaland Computer Engineering, Alberta,CanadaStrong-�eld ultrafast photoe-mission was studied by surfaceplasmons generated at 3.1 micronswavelength. Electron accelerationand tunneling photoemission wasdemonstrated at an unprecedentlylow laser intensity (1-5 GW/cm2).
FranceWe develop a high temporal reso-lution pump-probe set-up to deter-mine the dynamics of laser energydeposition at the surface of a dielec-tric material irradiated by a singlefemtosecond pulse.
Birtas3; 1National Institute forLaser, Plasma and RadiationPhysics, Solid-State QuantumElectronics Laboratory, Bucharest077125, Romania; 2Universityof Bucharest, Faculty of Physics,Bucharest 077125, Romania;3Renault Technologie Roumanie,North Gate Business Center, B-dulPipera, Nr.2/III, Voluntari, Jud. Ilfov077190, RomaniaWe report ignition of a Re-nault automobile engine usingcompact passively Q-switchedNd:YAG/Cr4+:YAG lasers. Im-proved engine stability in terms ofpeak pressure was observed at lowengine speeds and loads in com-parison with classical-spark-plugignition.
CJ-6a.3 MON 16:15Concentration Dependence ofOptical Gain in Yb3+-dopedPotassium Double TungstateChannel Waveguides�D. Geskus1, Y.-S. Yong2,3, E.Bernhardi2, L. Agazzi2, S. M.García-Blanco2,3, S. Aravazhi2,and M. Pollnau1,2; 1Department ofMaterials and Nano Physics, KTH -Royal Institute of Technology, Kista,Sweden; 2Integrated Optical Mi-croSystems Group, MESA+ Institutefor Nanotechnology, University ofTwente, Enschede, �e Netherlands;3Optical Sciences Group, MESA+Institute for Nanotechnology, Uni-versity of Twente, Enschede, �eNetherlandsGain around 981 nm in Yb-dopedpotassium-double-tungstate chan-nel waveguides increases linearlywith dopant concentration up to∼50% Yb. A 55 nm gain bandwidthobtained in all waveguides, withat least 150 dB/cm for 47.5% Ybconcentration.
ED-1b.3 MON 16:15Frequency comb dynamicsrevealed with ultrafast pulseshaping�J. Roslund, R. Schmeissner, C. Fabre,and N. Treps; Laboratoire KastlerBrossel, Paris, FranceUltrafast pulse shaping is utilizedto diagnose spectral correlationswithin the amplitude and phasenoise of a frequency comb. �esecorrelations reveal a set of theo-retically predicted, decoupled noisemodes that govern the comb dy-namics.
EG-5b.3 MON 16:15Optically Controlling theConductance of SemiconductorNanowaveguides Using HotElectron Injection from Nanorods�C. Kumarasinghe1, M.Premaratne1, and G. Agrawal2;1Monash University, Clayton,Australia; 2University of Rochester,Rochester, United StatesWe show theoretically that opticallyinduced hot electrons injected frommetallic nanorods are ideal for con-trolling conductivity of semicon-ductor nanowaveguides. �e appli-cations include traditional transis-tor equivalent devices in nano opticscircuits.
CM-5b.3 MON 16:15Expansion dynamic of atransparent shell a�er irradiationof dielectric material withfemtosecond laser pulse�M. Garcia-Lechuga, J. Siegel, and J.Solis; Laser Processing Group, Insti-tuto de Optica, CSIC, Madrid, SpainWe report the �rst observation andquantitative analysis of transientNewton rings in dielectrics duringablation with single fs laser pulses,having important consequences forthe comprehension of the ablationmechanisms in dielectrics
CK-4b.2 MON 16:15Experimental Measurement of theGeometric Phase in PhotonicLattices�K. Wang, S. Weimann, A. Perez-Leija, and A. Szameit; Institute ofApplied Physics, Abbe Center of Pho-tonics, Friedrich-Schiller-UniversitätJena, Jena, GermanyWe design a waveguide array suit-able for measuring the geometricphase of a driven harmonic oscil-lator. For the �rst time, We ex-perimentallymeasure anAharonov-Anandan phase in photonic lattices.
CA-5b.3 MON 16:15Passive Q-switching andSelf-Raman Conversion inYb:KLu(WO4)2 Microchip Laser�P. Loiko1,2, J.M. Serres2, X.Mateos2,V. Jambunathan2,3, K. Yumashev1,V. Petrov4, U. Griebner4, M. Aguiló2,and F. Díaz2; 1Center for OpticalMaterials and Technologies, Belaru-sian National Technical University,Minsk, Belarus; 2Física i Cristallo-gra�a de Materials i Nanomaterials(FiCMA-FiCNA), Universitat Rovirai Virgili (URV), Tarragona, Spain;3HiLASE Centre, Institute of PhysicsASCR, Dolní Břežany, Czech Repub-lic; 4Max Born Institute for Non-linear Optics and Short Pulse Spec-troscopy, Berlin, GermanyDiode-pumped Yb:KLu(WO4)2microchip laser Q-switched withCr:YAG delivers an average outputpower of 1.51 W with 8 ns pulseduration. Self-Raman conversionis observed at 1151 nm with theaverage power of 119 mW.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES
Paderborn, Warburger Strasse100, 33098 Paderborn, Germany;2Oregon Centre for Optics, De-partment of Physics, University ofOregon, Eugene, Oregon 97403,United StatesTemporal modes (TMs) of single-photon states are an under-utilizedyet promising basis for high-dimensional quantum informationscience (QIS). We introduce acomplete framework for QIS basedon TMs, which can be realized withstate-of-the-art technology.
Fatome1, P. Morin1, F. Baronio2,M. Conforti3, G. Millot1, and S.Wabnitz2; 1Laboratoire Interdis-ciplinaire Carnot de Bourgogne,UMR 6303 CNRS, Dijon, France;2Dipartimento di Ingegneriadell’Informazione, Brescia, Italy;3PhLAM/IRCICA, UMR 8523/USR3380 CNRS, Villeneuve d’Ascq,FranceWe present the �rst experimentalobservation of a vector rogue wavesolution of the two component non-linear Schrödinger equation that de-scribes polarization coupling in arandomly birefringent telecom opti-cal �ber.
Tampere University of Technology,Tampere, Finland; 3WeierstrassInstitute for Applied Analysis andStochastics, Berlin, Germany; 4KIITUniversity, Bhubaneswar, India;5Institut für Quantenoptik, Leibniz-Universität Hannover, Hannover,Germany; 6Laser-LaboratoriumGöttingen, Göttingen, Germany;7Laser Zentrum Hannover, Han-nover, GermanyNon-instantaneous polarization de-cay of several femtoseconds is ob-served in a dielectric under resonantexcitation. Numerical solutions oftime-dependent Schrödinger equa-tion agree excellently with the mea-surements. Limitations to genera-tion and characterization of ultravi-olet pulses are expected.
CE-5b.2 MON 16:15Anormolous Magneto-OpticalBehavior of Rare Earth DopedGallium Nitride�A. Helbers1, B. Mitchell2, N.Woodward1, and V. Dierolf1;1Department of Physics, LehighUniversity, Bethlehem, UnitedStates; 2Department of Physics andAstronomy, University of Mt. Union,Alliance, United StatesWe report magneto-optical prop-erties of rare earth doped galliumnitride that di�er drastically fromthose seen in other materials. Amodel to explain the behavior basedon defects will be presented
CD-5b.2 MON 16:15Measuring Nonlinear RefractiveIndex of Gases with HighPrecision Using Nonlinear EllipseRotation�L.Misoguti, M.Miguez, E. Barbano,and S. Zilio; Institute of Physics ofSao Carlos - USP, Sao Carlos, BrazilA new method of determining thenonlinear refractive index of gases isdemonstrated. By using thismethodbased on the nonlinear ellipse rota-tion, the values of n2 of several gasesat 800 nm are determined.
EB-2a.3 MON 16:15Optimal Receiver for CoherentSignals�D. Sych1 and G. Leuchs1,2; 1MaxPlanck Institute for the Scienceof Light, Erlangen, Germany;2University of Erlangen-Nuremberg,Erlangen, GermanyOptimal discrimination of coherentstates is one of the long-standingfundamental problems in quantumcommunication theory. Here weshow a realistic scheme to minimizethe discrimination error down tothe Helstrom bound.
EF-4b.3 MON 16:15Rogue gap soliton�A. Degasperis1, S. Wabnitz2, andA. Aceves3; 1Università di RomaSapienza, Rome, Italy; 2Universitàdi Brescia, Brescia, Italy; 3SouthernMethodist University, Dallas, UnitedStatesWe present the rogue wave solu-tion of the classical massive�irringmodel, that applies to describe non-linear optical pulse propagation inperiodic nonlinear optical media.
EE-5b.3 MON 16:15Intensity Clamping at a FreemanResonance�M. Hofmann and C. Bree; Weier-strass Institute for Applied Analysisand Stochastics, Berlin, GermanyWe theoretically demonstrateintensity clamping at a Freemanresonance, maintaining low-densityplasma channels and subcritical�lamentation. �is sheds a sur-prising perspective on plasmaless�lamentation predicted by thehigher-order Kerr model.
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ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13b17:00 – 18:30JS SPIE/OM/EQEC:Computational Photonics forMetrology ApplicationsChair: Bernd Bodermann, PTB,Braunschweig, Germany
17:00 – 18:30ED-3: Optical ClocksChair: �omas Udem, Max PlanckInstitute of Quantum Optics, Garch-ing, Germany
17:00 – 18:30EG-7: NanospectroscopyChair: Jérôme Wenger, Institut Fres-nel, Aix-Marseille University, Mar-seille, France
17:00 – 18:30CM-7: Laser Structuring ofSurfaces and 2DMaterialsChair: Emmanuel Stratakis, IESL-FORTH, Heraklion, Greece
17:00 – 18:30CK-6: Micro/Nanostructuresand MetasurfacesChair: Peter G. R. Smith, ORC, Uni-versity of Southampton, Southamp-ton, United Kingdom
17:00 – 18:30CA-7: Advanced Concepts inSolid-state LasersChair: David Coutts, MarquarieUniversity, Sydney, Australia
JS SPIE/OM/EQEC.1 MON (Invited) 17:00Analysis of Bi-Periodic CompositeMaterials made of Stacks of TiltedOne-Dimensional Arrays of Rods�G. Granet; Clermont Universités,Université Blaise Pascal, InstitutPascal, Clermont-Ferrand, France;CNRS UMR 6602, IP, Aubière,FranceWe analyse composite materialsmade of tilted one dimensionalarrays of rods embedded insidea host medium. We use modalmethods optimized for rods withrectangular or elliptical crosssections. We thus obtain an e�cientmulti purpose code.
ED-3.1 MON (Invited) 17:00Making the best atomic clock�J. Ye; JILA, NIST and University ofColorado, Boulder, United StatesI will report new performancerecords for an atomic clock. Wehave achieved stability of 2.2 x10-16 at 1 s and uncertainty of 2.1 x10-18 for the JILA Sr clock.
EG-7.1 MON 17:00Probing the Vibrations ofIndividual Non-ResonantNanoparticles by NanoapertureOptical Tweezers�R. Gordon, S. Wheaton, R. Gelfand,T. DeWolf, A. Al Balushi, and A. Kot-nala;University of Victoria, Victoria,CanadaUsing a nanoaperture opticaltweezer with two single frequencytrapping lasers, we obtain the Ra-man spectra of individual proteinsand note their interactions withsmall molecules a�er binding fromspectral changes.
CM-7.1 MON 17:00Quantitative and QualitativeStudies of Femtosecond LaserNanopatterning of GrapheneR. Sahin1, E. Simsek2, and �S.Aktürk1; 1Istanbul Technical Univer-sity, Istanbul, Turkey; 2GeorgeWash-ington University, Washington DC,United StatesWe focus on femtosecond-lasernano-structuring of graphenewithout any damage to substrate.�en, histogram analyses of SEMimages of the fabricated structuresare used to quantify the ablationquality.
CK-6.1 MON 17:00Control of Ultrafast SurfacePlasmon Coupled on a GoldTapered Tip and Its NonlinearEmission by Shaped FemtosecondLaser Pulse�Y. Masaki, K. Toma, K. Hirosawa,and F. Kannari; Keio University,Yokohama, JapanSpatiotemporal nanofocusing ofsurface plasmon polaritons at an Autapered tip excited by femtosecondlaser pulses is deterministicallycontrolled based on the measuredplasmon response function. SHGand CARS at the apex are alsocontrolled.
CA-7.1 MON 17:00All-passive Q-switching limiterenables a high peak power 5-GHzSESAM-modelocked laser�A. Klenner and U. Keller; Depart-ment of Physics, Institute of Quan-tum Electronics, Zurich, SwitzerlandWe use a Kerr-lens inducedall-optical limiter to reduceQ-switching instabilities in ahigh-power diode-pumped 5-GHzSESAM-modelocked Yb:CALGOlaser. We can generate 4.1-Waverage output-power and 96-fspulses with a record-high peakpower of 7.5-kW.
EG-7.2 MON 17:15Förster resonance energy transfer(FRET) and local optical densityof states (LDOS) are uncorrelatednear an ideal mirror�W. Vos1 and M. Wubs2; 1COPS,University of Twente, Enschede, �eNetherlands; 2Technical Universityof Denmark (DTU), Lyngby, Den-markWe study an exact model ofNanophotonic Förster resonantenergy transfer (FRET) controlnear a mirror. �e FRET rateappears to be uncorrelated with thelocal density of states (LDOS), assupported by theoretical insights.
CM-7.2 MON 17:15Deviation from threshold modelin ultrafast laser ablation ofgraphene at sub-micron scale�A. Gil Villalba, C. Xie, R. Salut,L. Furfaro, R. Giust, J. Dudley, andF. Courvoisier; Institut FEMTO-ST,CNRS University of Franche-Comte,Besancon, FranceSingle shot ablation of graphene isinvestigated with structured hon-eycomb beams. We report a noveltechnique of ablation thresholdmeasurement and report the ap-pearance of a second condition forablation at nano-scale in graphene.
CK-6.2 MON 17:15Real-space Imaging of PlasmonicModes of Gold Tapers by EFTEMand EELS�S. Guo1, N. Talebi1, W. Sigle1,M. Esmann2, S.F. Becker2, R.Vogelgesang2, C. Lienau2, and P.van Aken1; 1Max Planck Institutefor Intelligent Systems, Stuttgart,Germany; 2Carl von OssietzkyUniversität Oldenburg, Oldenburg,GermanyMetallic tapers have been theoret-ically investigated for their amaz-ing functionalities such as adiabaticnanofocusing. Here, utilizing elec-tron energy �ltering transmissionelectron spectroscopy, we investi-gate the opticalmodes of such tapersin their energy and spatial distribu-tions.
CA-7.2 MON 17:15�in-disk Lasers with High Intra-cavity Power for the ContinuousAlignment of Molecules�B. Deppe1,2,3,4, G. Huber1,2,3, J.Küpper2,3,4, and C. Kränkel1,2;1Institut für Laser-Physik, Hamburg,Germany; 2�e Hamburg Centreof Ultrafast Imaging, Hamburg,Germany; 3Department of Physics,University of Hamburg, Hamburg,Germany; 4Center for Free-ElectronLaser Science, Hamburg, GermanyWe propose the alignment ofmolecules by the strong intracavity�eld inside a continuous-wavethin-disk laser resonator. Wedemonstrate an intracavity powerof 135 kW with Yb:YAG anddetermined intrinsic losses below0.02%.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES17:00 – 18:30CE-7: Oxide Lasers, Wave-guides and ComponentsChair: Stefan Kück, Physikalisch-Technische Bundesanstalt, Braun-schweig, Germany
17:00 – 18:30CD-7: Nonlinear Phenomena IChair: Concita Sibilia, La SapienzaUniversita’ di Roma, Roma, Italy
17:00 – 18:30EA-5: Rare Earth IonsChair: David Hunger, Ludwig-Maximilians-Universität München(LMU), Munich, Germany
17:00 – 18:30EF-6: Nonlinear BeamPropagationChair: Günter Steinmeyer, Max-Born-Institute, Berlin, Germany
17:00 – 18:30CC-5: THz Near-�eldMicroscopy andSpectroscopyChair: Jaime Gomez Rivas, AMOLF,Amsterdam,�e Netherlands
CE-7.1 MON 17:00Properties of Erbium and CeriumCo-doped TeO2 �in FilmsFabricated by Reactive Co-sput-tering for Waveguide Ampli�er�K. Vu1, J. Zhang1,2, and S.Madden1; 1Centre for UltrahighBandwidth Devices for OpticalSystems, Laser Physics Centre,Research School of Physics and En-gineering, �e Australian NationalUniversity, Canberra, Australia;2School of Microelectronics and SolidElectronics, University of ElectronicScience and Technology of China,Chengdu, China, People’s Republicof (PRC)Er and Ce co-doped TeO2 thin�lms have been achieved usingco-sputtering with three separatedmetal targets. �e achieved pho-toluminescence is very encouragingwith lifetime similar to the Er dopedonly case.
CD-7.1 MON (Invited) 17:00Expanding the Scope of OpticalNonlinearity�D. Andrews; University of East An-glia, Norwich, United Kingdom�is paper provides an overview ofseveral newly emerging directionsin the �eld of optical nonlinearity,exhibiting their connection to con-ventional nonlinear optics and high-lighting some of the new challengesthat now arise.
EA-5.1 MON (Invited) 17:00Storing light up to one minute byEIT in a doped solid�T. Halfmann; Technical Universityof Darmstadt, Darmstadt, Germany�e talk reports on electromagnet-ically induced transparency, com-bined with pulse shaping and deco-herence control to store light pulsesand images in atomic coherences ina Pr:YSO crystal, permitting storagetimes up to one minute.
EF-6.1 MON 17:00Spatiotemporal dynamics ofcounterpropagating Airy beams�N. Wiersma, N. Marsal, M. Scia-manna, and D. Wolfersberger; Cen-traleSupélec, Laboratoire MatériauxOptiques, Photonique et Systèmes(LMOPS - EA4423), Metz, FranceWe numerically study the inter-actions of two counterpropagatingAiry beams in a photorefractivecrystal under high-focusing condi-tions. By varying the interactiondistances and the photorefractivecoupling strength, soliton-like inter-actions create peculiar spatiotempo-ral dynamics.
CC-5.1 MON 17:00Near-�eld spectroscopy ofsub-wavelength (<lambda/10)anisotropic dielectric resonatorsat terahertz frequencies�O. Mitrofanov1,2, I. Khromova1,F. Dominec3, P. Kuzel3, J. Reno2,4,I. Brener2,4, U.-C. Chung5, C.Elissalde5, M. Maglione5, and P.Mounaix6; 1University CollegeLondon, London, United Kingdom;2CINT, Sandia NL, Albuquerque,United States; 3Academy of Sciencesof the Czech Republic, Prague, CzechRepublic; 4Sandia NL, Albuquerque,United States; 5ICMCB, Univ.Bordeaux, CNRS, Bordeaux, France;6LOMA, Univ. Bordeaux, CNRS,Bordeaux, FranceWe demonstrate THz near-�eldcharacterization of Mie resonances(magnetic- and electric-dipole) inindividual mono-crystalline TiO2spheres. 20-30micrometer diameterspheres show clear resonances atTHz frequencies corresponding tothe e�ective magnetic response,comparable to split-ring resonators.
CE-7.2 MON 17:15Comparative study of rare-earthdoped sesquioxides grown bypulsed laser deposition and theirperformance as planar waveguidelasers�T. Parsonage, A. Choudhary, S.Beecher, J. Grant-Jacob, P. Hua,J. Mackenzie, D. Shepherd, andR. Eason; Optoelectronics ResearchCentre, University of Southampton,Southampton, United KingdomA comparative study of rare-earthdoped sesquioxides grown by pulsedlaser deposition for use as planarwaveguide lasers; including growthrates, crystallography, spectroscopyand laser performance. Progress to-wards high laser output power willbe reported.
EF-6.2 MON 17:15Optical Parametric Ampli�cationby Coherent and IncoherentConical Beams�V. Pyragaite, V. Smilgevicius, R.Butkus, A. Narmontas, P. Stanislo-vaitis, A. Stabinis, and A. Piskarskas;Vilnius University, Vilnius, Lithua-niaOptical parametric ampli�cation ofa signal beam in the �eld of coherentas well as incoherent conical pumpbeams is investigated. It is demon-strated that in both cases the signalbeam can be e�ectively ampli�ed.
CC-5.2 MON 17:15THz-TDS based near-�eldimaging and spectroscopy at 25nm length scaleF. Huth1, D. Molter2, J. Klier2, J.Jonuscheit2, G. von Freymann2,F. Keilmann1, and �A. Huber1;1Neaspec GmbH, Munich, Ger-many; 2Fraunhofer-Institut fürPhysikalische Messtechnik IPM,Kaiserslautern, GermanyWe demonstrate THz near-�eldimaging and spectroscopy at 25nm length scale. Extreme sub-wavelength con�nement of THzlight is veri�ed and test structuresare imaged.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13bJS SPIE/OM/EQEC.2 MON (Invited) 17:30Nonlocal Light-MatterInteractions in Noble-Metal andGraphene Nanostructures�N.A. Mortensen; Department ofPhotonics Engineering, TechnicalUniversity of Denmark, KongensLyngby, DenmarkUsing nonlocal hydrodynamics wediscuss long-established and recentexperimental observations formetallic nanoparticles and dimers.We also consider graphene �akeswhere atomic-scale details andedge-state transitions are importantfor the optical properties too.
ED-3.2 MON 17:30Frequency Ratio Measurement ofHg and Sr Optical Lattice Clocks�N. Ohmae1,2,3, K. Yamanaka1,2,3, I.Ushijima1,2,4, M. Takamoto1,2,4, andH. Katori1,2,3,4; 1Quantum Metrol-ogy Laboratory, RIKEN, Saitama,Japan; 2Innovative Space-TimeProject, ERATO, Japan Science andTechnology Agency, Tokyo, Japan;3Department of Applied Physics,Graduate School of Engineering,�e University of Tokyo, Tokyo,Japan; 4RIKEN Center for AdvancedPhotonics, Saitama, JapanWe developed a Hg optical latticeclock and evaluated its systematicfrequency shi�s with total uncer-tainty smaller than 1×10−16. Andwemeasured the Hg clock frequency byreferencing Sr optical lattice clock.
EG-7.3 MON 17:30Nanoaperture enhanced�uorescence energy transfer�J. de Torres, P. Ghenuche, S.B.Moparthi, V. Grigoriev, and J.Wenger; Institut Fresnel, Marseille,FranceWe investigate the in�uence ofLDOS on the energy transferprocess between �uorescent dipolaremitters. FRET rates are quanti�edinto metal nanoapertures whichcon�ne light into attoliter volumes,enabling single-molecule FRET atmicromolar concentrations.
CM-7.3 MON 17:30Pulsed Laser Processing ofGraphene and relatedTwo-Dimensional MaterialsK. Savva1,2, G. Kakavelakis3,M. Sigletou1,2, D. Konios3, I.Paradissanos1,2, M.M. Stylianakis3,C. Petridis3, G. Kioseoglou2, C.Fotakis1,2, E. Kymakis3, and �E.Stratakis1,2; 1Foundation forResearch & Technology Hellas,Institute of Electronic Structureand Laser (IESL-FORTH), P.O. Box1527, Heraklion 711 10, Greece,Heraklion, Greece; 2University ofCrete, Dept. Of Materials Scienceand Technology, Heraklion 71409, Greece., Heraklion, Greece;3Technological Educational Institute(TEI) of Crete, Heraklion, 71003,Greece, Heraklion, Greece�is paper reviews our recent workon the pulsed laser reduction,doping and functionalizationof graphene and related two-dimensional (2D) materials.
CK-6.3 MON 17:30Active Tuning of All-DielectricMetasurfaces with Liquid CrystalsJ. Sautter1, �I. Staude1, M. Decker1,E. Rusak1, D. Neshev1, I. Brener2,and Y. Kivshar1; 1Nonlinear PhysicsCentre and Centre for UltrahighBandwidth Devices for Optical Sys-tems (CUDOS), Research School ofPhysics and Engineering, �e Aus-tralian National University, Can-berra, Australia; 2Center for In-tegrated Nanotechnologies, SandiaNational Laboratories, Albuquerque,United StatesWe demonstrate active tuning of theelectric and magnetic resonances ofa silicon-nanodisk metasurface atnear-infrared frequencies. �is isachieved by covering the metasur-face with liquid crystals and uti-lizing their temperature-dependentrefractive-index change.
CA-7.3 MON 17:30Highly e�cient grating mirrorenables high power fundamentalmode thin-disk laser emitting inthe green by SHG�M. Rumpel, S. Piehler, T. Graf,and M. Aboud Ahmed; Institutfür Strahlwerkzeuge, Stuttgart, Ger-manyWe present an intracavity frequencydoubled fundamentalmode Yb:YAGthin-disk laser, enabled by the intra-cavity use of a highly e�cient grat-ing mirror for wavelength- and po-larization stabilization as well as apumping wavelength of 969 nm.
ED-3.3 MON 17:45Two-way optical frequencycomparisons at 5x10-21 relativestability over 100-kmtelecommunication network �bers�A. Bercy1,2, F. Stefani2,1, O. Lopez1,C. Chardonnet1, P.-E. Pottie2, andA. Amy-Klein1; 1Laboratoire dePhysique des Lasers, Université Paris13, Sorbonne Paris Cité, CNRS,Villetaneuse, France; 2LaboratoireNational de Métrologie et d’EssaisSystème de Références Temps-Espace, UMR 8630 Observatoire deParis, CNRS, UPMC, Paris, FranceWe demonstrated two-way fre-quency transfer over a 100-kmtelecommunication �ber networkusing either unidirectional orbidirectional propagation. �eseresults open the way to accurateand high-resolution frequencycomparison of optical clocks overintercontinental �ber networks.
EG-7.4 MON 17:45Magnetic Response of SingleSuperparamagnetic Iron OxideNanoparticles Studied byNitrogen-Vacancy CenterMagnetometry�N. Sadzak1, J. Wolters2, A.W.Schell3, and O. Benson1; 1Humboldt-Universität zu Berlin, Berlin,Germany; 2Technische Universitätzu Berlin, Berlin, Germany; 3OsakaUniversity, Osaka, Japan�e linear and non-linear magneticresponse of single superparamag-netic nanoparticles in oscillatingmagnetic �elds is studied by meansof nitrogen-vacancy (NV) centermagnetometry. �e nanoparticle-induced magnetic �eld ampli�ca-tion enhances the NV center sensi-tivity.
CM-7.4 MON 17:45Simultaneous patterning anddeposition of thin �lms via femto-second laser-induced transferusing a digital micromirror devicefor spatial pulse shaping�M. Feinaeugle, D.J. Heath, B. Mills,J.A. Grant-Jacob, G.Z. Mashanovich,and R.W. Eason; OptoelectronicsResearch Centre, University ofSouthampton, Southampton, UnitedKingdom�e forward and backward fem-tosecond laser-induced transfer ofthin �lms in an intact state withgood adhesion, via a digital mi-cromirror array acting as a dynamicobject mask for spatial beam shap-ing is presented.
CK-6.4 MON 17:45Long-Range Energy Transfer viaHybrid Plasmonic-PhotonicStructuresK. Akulov and �T. Schwartz; Schoolof Chemistry, Raymond and BeverlySackler Faculty of Exact Sciences, TelAviv University, Tel Aviv, IsraelWe demonstrate energy transferover large distances (~100nm) in adonor-acceptor molecule pair usinga hybrid structure which resonantlycouple con�ned photons within amicrocavity to plasmons residingexternally, e�ciently funneling en-ergy between the chromophores.
CA-7.4 MON 17:45A continuous-wave frequency-doubled Nd:GdVO4 Raman laserat 586.5nm using intracavityadaptive optics�R. Li1, A. Lee2, H. Pask2, andW. Lubeigt1; 1Centre for Microsys-tems and Photonics, University ofStrathclyde, Glasgow, United King-dom; 2MQ Photonics Research Cen-tre, Macquarie University, Sydney,AustraliaAn adaptive optics-based feedbackloop featuring an intracavity de-formable mirror was integrated intoa frequency-doubled, Nd:GdVO4self-Raman laser to compensate forthe thermal lensing. �is resultedin ∼15% improvement in yellow(586.5nm) output power.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTESCE-7.3 MON 17:301050 dB/cm Gain in a 57.5at.%Yb-doped KGd(WO4)2 �in Filmat 981 nm�Y.-S. Yong1,2, S. Aravazhi1, S.Vázquez-Córdova1,2, S. García-Blanco1,2, and M. Pollnau1,3;1Integrated Optical MicroSystemsGroup, MESA+ Institute for Nan-otechnology, University of Twente,Enschede, �e Netherlands; 2OpticalSciences Group, MESA+ Institutefor Nanotechnology, University ofTwente, Enschede, �e Netherlands;3Department of Materials andNano Physics, School of Informationand Communication Technology,KTH-Royal Institute of Technology,Kista, SwedenWe present the experimentaland numerical gain results in aKGd(WO4)2 thin-�lm with >50%Yb concentration. �e record-highmeasured gain of ~1050 dB/cmshows that it is promising for real-izing short-device length high-gainwaveguide ampli�ers.
CD-7.2 MON 17:30Self-induced negative refractionin nematic liquid crystals�A. Piccardi1, A. Alberucci1,2, N.Kravets1, O. Buchnev3, and G.Assanto1,2; 1NooEL - Nonlinear Op-tics and Optoelectronics Laboratory,University of Rome ”ROMA TRE”,Rome, Italy; 2Optics Laboratory,Dept. of Physics, Tampere Universityof Technology, Tampere, Finland;3Zepler Institute, University ofSouthampton, Southampton, UnitedKingdomExploiting the large anisotropy andoptical reorientation of nematic liq-uid crystals in the highly nonlin-ear regime, we demonstrate thepower dependent transition of self-con�ned light beams from positiveto negative refraction.
EA-5.2 MON 17:30Frequency Up-Conversion ofMicrowave Photons to theTelecommunications Band in anEr:YSO Crystal�X. Fernandez Gonzalvo1, Y.-H.Chen1, C. Yin2, S. Rogge2, and J.Longdell1; 1University of Otago,Dunedin, New Zealand; 2Universityof New South Wales, Sydney,AustraliaIn a Raman heterodyne spec-troscopy study we performfrequency up-conversion frommicrowaves to telecom light, usinga cryogenically cooled Er:YSOcrystal in a microwave resonator.Adding an optical resonator willmake unity conversion e�ciencypossible.
EF-6.3 MON 17:30Temporal properties of counter-propagating twin beams close tothe threshold for MirrorlessOptical Parametric Oscillation�E. Brambilla1, T. Corti1, and A.Gatti1,2; 1University of Insubria,Como, Italy; 2Istituto di Fotonicae Nanotecnologie del CNR, Milano,ItalyWe investigate the coherence andcorrelation properties of counter-propagating twin beams generatedin a Mirrorless Optical ParametricOscillator (MOPO) with distributedfeedback in the neighborhood of thedevice emission threshold.
CC-5.3 MON 17:30Temporal Evolution of SpatialTerahertz Electric-�eld VectorImages�M. Takai and S. Watanabe; De-partment of Physics, Faculty of Sci-ence and Technology, Keio Univer-sity, Kanagawa, JapanHigh-speed spatio-temporal map-ping of the terahertz electric-�eldvector is reported. Direct mappingof a rotating electric-�eld vectorwithin a single cycle terahertz pulseenables to characterize the vectorwaveform distortion yielded by a fo-cusing mirror.
CE-7.4 MON 17:45First laser performances at 946nm on the 4F3/2 4I9/2 transitionwith Nd:Y2O3 transparentceramicsG. Aka1, A. Ikesue3, Y.L. Aung3, L.Zheng2, �P. Loiseau1, and F. Khaled1;1Institut de Recherche de ChimieParis, Paris, France; 2Shanghai In-stitute of Ceramics, Shanghai, China,People’s Republic of (PRC); 3WorldLab. Co. Ltd., Nagoya, JapanNd:Y2O3 transparent ceramics gen-erate for the �rst time 1W cw out-put laser power at 946 nm, with 11W absorbing power at 804 nm fromlaser diode and slope e�ciency of13.4 %.
CD-7.3 MON 17:45Ultrafast Kerr nonlinearities inmultimodal plasmonic meta-materials: elliptic, hyperbolic andepsilon-near zero regimes�S. Peruch, A. Neira, G. Wurtz, andA. Zayats; Department of Physics,King’s College London, London,United KingdomWemodel the ultrafast response of aplasmonic metamaterial made of anarray of gold nanorods, exploring itsrich and tunable modal response inorder to understand and control thenonlinear optical extinction modu-lation
EA-5.3 MON 17:45Spectroscopy of single rare earthions�E. Eichhammer1, T. Utikal1, S.Götzinger2,1, and V. Sandoghdar1,2;1Max Planck Institute for theScience of Light, Erlangen, Germany;2Friedrich-Alexander-UniversitätErlangen-Nürnberg, Erlangen,GermanyWe show the �rst detection of sin-gle praseodymium ions in a crystalvia the 606 nm transition, render-ing itmore accessible for existing ex-periments. We further present life-time and emission spectrum mea-surements on single ions.
EF-6.4 MON 17:45Vectorial self-accelerating beams�R. Driben1,2, V. Konotop3, andT. Meier1; 1University of Pader-born, Paderborn, Germany; 2ITMOUniversity, St. Petersburg, Russia;3University of Lisbon, Lisbon, Portu-galWe demonstrate dynamics of multi-component coupled Airy beams inlinear and nonlinear media. Inthe low-power propagation regimea complete analytic solution de-scribes a network of N-coupled self-accelerating beams, featuring peri-odically oscillating non-di�ractingbehavior.
CC-5.4 MON 17:45Towards High-intensity TerahertzGeneration: InAs/GaAs QuantumDots Based Antennae OpticallyPumped Up To 1WI. Leite1,2, A. Gorodetsky2, R.Leyman3, N. Bazieva2, and �E.Rafailov2; 1School of Engineering,Physics, and Mathematics, Uni-versity of Dundee, Dundee, UnitedKingdom; 2Optoelectronics andBiomedical Optics Group, AIPT, As-ton University, Birmingham, UnitedKingdom; 3School of Engineering,University of Glasgow, Glasgow,United KingdomWe demonstrate a quantum-dotbased THz antenna capable ofbeing optically pumped at very highintensities, 20 times higher thanthose available commercially. �isis a promising route towards thedevelopment of high-power THzsources.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 1 ROOM 3 ROOM 4a ROOM 4b ROOM 13a ROOM 13bJS SPIE/OM/EQEC.3 MON (Invited) 18:00Motion Contrast 3D Scanning�O. Cossairt1, N. Matsuda1, and M.Gupta2; 1Northwestern University,Evanston, United States; 2ColumbiaUniversity, New York, United StatesWe present a novel structured lighttechnique called Motion Contrast3D scanning (MC3D) that allowslaser scanning resolution withsingle-shot speed, even in thepresence of strong ambient illumi-nation, signi�cant inter-re�ections,and highly re�ective surfaces.
ED-3.4 MON 18:00Frequency stability performanceof crystalline silicon cryogenicoptical resonators operated at 1.5KelvinE. Wiens1, I. Ernsting1, A. Nevsky1,�S. Schiller1, and T.Müller2; 1Institutfür Experimentalphysik, Düsseldorf,Germany; 2Siltronic AG, München,GermanyWe determined an ultralow dri� of-3 mHz/s, an upper limit of the in-stability of 2*10^-15 for integrationtimes of a few 1000 s, and an e�ec-tive laser linewidth of 500 Hz, lim-ited by vibrations,
EG-7.5 MON 18:00Time-coherence properties of thetrion �uorescence in thick-shellCdSe/CdS nanocrystals byPhoton-Correlation FourierSpectroscopyL. Biadala1, H. Frederich1, L.Coolen2,3, S. Buil1, X. Quélin1,C. Javaux4, M. Nasilowski4, B.Dubertret4, and �J.-P. Hermier1,5;1Université de Versailles Saint-Quentin, Versailles, France; 2UPMCUniv Paris 06, Paris, France; 3CNRS,UMR 7588, Paris, France; 4EcoleSupérieure de Physique et ChimieIndustrielles, Paris, France; 5InstitutUniversitaire de France, Paris,France�e �uorescence of very thick shellcolloidal CdSe/CdS nanocrystals ischaracterized in detail by PhotonCorrelation Fourier Spectroscopy.Spectral di�usion of the emissionwavelength and the emissionlinewidth are analyzed.
CM-7.5 MON 18:00Phase changes of calciumphosphate ceramic biomaterialsinduced by Femtosecond lasers.�A. Jha1, A. Anastasiou1, T.Edwards2, C. �omson2, S.Hussain2, K. Metzger2,4, R.Mathieson1, T. Brown2, A. Brown1,M. Duggal3, S. Stra�ord3, and M.Malinowski3; 1Institute for MaterialsResearch, School of Chemical andProcess Engineer, University ofLeeds, Leeds, United Kingdom;2School of Physics and Astronomy,University of St. Andrews, St.Andrews, United Kingdom; 3LeedsDental School, University of Leeds,Leeds, United Kingdom; 4School ofEngineering & Physical Sciences;Photonics & Quantum Sciences,Heriot-Watt University, Edinburgh,United KingdomAn acid resistant biomaterial is ap-plied on tooth surface and is bondedwith the underlying enamel a�er ir-radiating with femtosecond lasers.Experimental results indicate melt-ing of the biomaterial and the for-mation of a homogenous surface.
CK-6.5 MON 18:00Free-electron Emission fromPhotonic Metasurfaces�J. So1, G. Adamo2, K.F.MacDonald1, and N.I. Zheludev1,2;1University of Southampton,Southampton, United Kingdom;2Nanyang Technological University,Singapore, SingaporeWe experimentally demonstratethat free-electron spontaneous lightemission can be enhanced usingphotonic meta-surfaces in a manneranalogous to the enhancement ofspontaneous emission from atomicelectrons in resonant cavities.
CA-7.5 MON 18:00Simple Technique for High-OrderRing-Mode Selection withinSolid-State Laser Resonators�A. Butler, R. Uren, D. Lin, J. Hayes,and W.A. Clarkson; Optoelectron-ics Research Centre, Southampton,United KingdomAn annular optical �bre is used totailor a �bre-coupled diode pumpbeam pro�le to directly excitehigh-order Laguerre-Gaussian ringmodes within an Nd:YAG resonator.Single azimuthal modes up to n =20 are demonstrated.
ED-3.5 MON 18:15Comb-locked cavity-ring-downspectrometer�D. Gatti1, T. Sala1, R. Gotti1, M.Prevedelli2, P. Laporta1, and M.Marangoni1; 1Istituto di Fotonica eNanotecnologie - CNR and Diparti-mento di Fisica, Politecnico di Mi-lano, Milano, Italy; 2Dipartimentodi Fisica e Astronomia, Università diBologna, Bologna, ItalyA kHz-level accuracy in a Dopplerbroadening regime and a sensitiv-ity as low as 5.7 ⋅ 10−11 cm−1 areobtained with a novel comb-lockedcavity-ring-down spectrometer op-erating in the 1.5-1.63 �m range.
EG-7.6 MON 18:15Coherent ultrafast excitondissociation in polymer:fullerenethin �lms�A. De Sio1, E. Sommer1, M.Maiuri2, J. Rehault2, C.A. Rozzi3,E. Molinari3, G. Cerullo2, andC. Lienau1; 1Institut für Physik,Carl von Ossietzky Universität,Oldenburg, Germany; 2IFN-CNR,Dipartimento di Fisica, Politecnicodi Milano, Milano, Italy; 3IstitutoNanoscienze - CNR, Centro S3,Modena, ItalyCombining high-time resolutionoptical spectroscopy and time-dependent density functionaltheory calculations, we providestrong evidence for the role ofvibronic coupling in drivingthe initial steps of the currentphotogeneration in an organicphotovoltaic system
CM-7.6 MON 18:15Investigation of surface opticalproperties of oxides under highelectric DC �eld using ultrafastlaser assisted atom probetomography�V. Angela1, S. Elena P.2, A.Laurent1, D. Bernard1, K. Markus2,and K. Juergen2; 1GPM UMR 6634,Normandie Université, Saint Etiennedu Rouvray, France; 2Departmentof Physics and Atmospheric Science,Dalhousie University, Halifax NovaScotia, CanadaUsing laser assisted atom probe,the optical properties of sub-wavelength MgO and Si tips areinvestigated under high electrical�eld. By changing the DC �eld, theabsorption coe�cient is measuredand compared to DFT predictions.
CK-6.6 MON 18:15Recon�gurable GradientMetasurfaces With RandomAccess�P. Cencillo-Abad1, J.-Y. Ou1,J. Valente1, E. Plum1, and N.I.Zheludev1,2; 1University ofSouthampton, Southampton, UnitedKingdom; 2Nanyang TechnologicalUniversity, Singapore, SingaporeWe demonstrate the �rst randomaccess recon�gurable metasurfaces,thus enabling simultaneous spatialand temporal control over meta-material optical properties. Ap-plication opportunities range fromswitchable gratings and lenses totransformation optics and videoholography.
CA-7.6 MON 18:15Widely tunable fractional vortexlaser�Y. Taximaiti1,2, A. Aizitiaili1,K. Yamane3, K. Miyamoto1, andT. Omatsu1,2; 1Chiba Univer-sity, Chiba, Japan; 2CREST, JST,Kawaguchi, Japan; 3HokkaidoUniversity, Sapporo, JapanWe demonstrate a widely tunablefractional vortex laser formed ofa 0.5-um vortex pumped LiB3O5parametric oscillator. �is systemenables us to generate a millijoulelevel fractional vortex output withinranges of 935-990nm and 1150-1234nm.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTESCE-7.5 MON 18:00Simultaneous InterferometricMeasurement of the TemperatureCoe�cient of the Refractive Indexdn/dT and the Coe�cient of�ermal Expansion of LaserCrystals�O. Kazasidis and U.Wittrock;Mün-ster University of Applied Sciences,Steinfurt, GermanyWe present an interferometricmethod to measure the temperaturecoe�cient of the refractive indexand the coe�cient of thermalexpansion of laser crystals as afunction of temperature in theinterval from 20�C to 80�C.
CD-7.4 MON 18:00Guiding Discharges AroundObstacles�M.Clerici1,2, Y. Hu2,3, P. Lassonde2,C. Milián4, A. Couairon4, D.Christodoulides5, Z. Chen6, L.Razzari2, F. Vidal2, F. Légaré2,D. Faccio1, and R. Morandotti2;1School of Engineering and Phys-ical Sciences, Heriot-Watt Univ.,Edinburgh, United Kingdom; 2INRS-EMT, Varennes, Canada; 3�e MOEKey Lab. of Weak Light NonlinearPhotonics, School of Physics andTEDA Applied Physics School,Nankai Univ., Tianjin, China,People’s Republic of (PRC); 4Centrede Physique �eorique, CNRS, EcolePolytechnique, Palaiseau, France;5College of Optics - CREOL, Univ.of Central Florida, Orlando, UnitedStates; 6Department of Physics andAstronomy, San Francisco StateUniv., San Francisco, United StatesWe show that beam shaping allowsguiding electric discharges alongcurved trajectories avoiding obsta-cles in the line of sight of the elec-trodes. Furthermore we demon-strate that beam self-healing can as-sist the charge transfer on target.
EA-5.4 MON 18:00Experimental demonstration ofstopped light in a spectral hole�K. Kutluer1, M.F. Pascual-Winter2, J. Dajczgewand3, M.Mazzera1, T. Chanelière3, and H.de Riedmatten1,4; 1ICFO-Institutde Ciencies Fotoniques, Barcelona,Spain; 2Centro Atomico Barilochee Instituto Balseiro, Río Negro,Argentina; 3Laboratoire AiméCotton, CNRS-UPR, Paris, France;4ICREA-Institució Catalana de Re-cerca i Estudis Avançats, Barcelona,SpainWe report the �rst experimentaldemonstration of an optical mem-ory based on stopped light in a spec-tral hole, using a Pr3+:Y2SiO5 crys-tal. Slow light pulses are convertedreversibly to long-lived spin-wavesusing short control pulses.
EF-6.5 MON 18:00Generation of intense purehigher-order modes inhollow-core PCF�J.-M. Ménard, B.M. Trabold, A.Abdolvand, and P.S.J. Russell; MaxPlanck Institute for the Science ofLight, Erlangen, GermanyE�cient Raman ampli�cation ofside-seeded higher-order opticalmodes inside hydrogen-�lledhollow-core kagomé-PCF enablesthe generation of complex and well-de�ned multi-lobed transverse �eldpro�les at output pulse energiesreaching 8 �J.
CC-5.5 MON 18:00Optical Pump - Terahertz ProbeCarrier Lifetime Measurement inInAs/GaAs Quantum Dots BasedPhotoconductive Antennae�A. Gorodetsky1, I.T. Leite1,2, N.Bazieva1, and E.U. Rafailov1; 1AstonUniversity, Birmingham, UnitedKingdom; 2University of Dundee,Dundee, United KingdomWe demonstrate optical pump - ter-ahertz probe QD wafer lifetime re-sults, showing lifetime shorteningwith pump power increase. �ise�ect is responsible for spectrumbroadening of a THz radiation fromQD PCA under higher pump pow-ers.
CE-7.6 MON 18:15Terbium Scandium AluminiumGarnet - Unique Magneto-ActiveMaterial for Faraday Isolators andRotators for Multikilowatt LaserApplication�I. Snetkov1, R. Yasuhara2, A.Starobor1, E. Mironov1, and O.Palashov1; 1Institute of AppliedPhysics of the Russian Academy ofSciences, Nizhny Novgorod, Russia;2National Institutes of NaturalSciences, National Institute forFusion Science, Toki, Japan�ermooptical and magnetoopticalproperties of TSAG were measured.�is material has demonstrated aunique set of properties, whichmake it the best to our knowledgemagneto-activematerial for Faradaydevices operating at high-average-power laser radiation.
CD-7.5 MON 18:15Non-paraxial non-di�ractingbeams in scale-free optics�F. Di Mei1,2, D. Pierangeli1, J.Parravicini1, C. Conti3, A. Agranat4,and E. DelRe1; 1University of Rome*La Sapienza*,, Rome,, Italy; 2Centerfor Life Nano Science@Sapienza, Is-tituto Italiano di Tecnologia, Rome,Italy; 3ISC-CNR, University of Rome*La Sapienza*, Rome, Italy; 4AppliedPhysics Department, HebrewUniver-sity of Jerusalem,, Jerusalem, IsraelUsing scale-free optics in nanodis-ordered KLTN we demonstrate thebreaking of the distinction betweenthe paraxial and the non-paraxialoptical regimes, from beam widthsthat allow geometrical optics downto the single wavelength scale.
EA-5.5 MON 18:15A Solid State Spin-Wave QuantumMemory for Photonic Time-BinQubitsM. Gündogan1, P.M. Ledingham1,K. Kutluer1, �M. Mazzera1, and H.de Riedmatten1,2; 1ICFO-Institut deCiences Fotoniques, MediterraneanTechnology Park, Castelldefels(Barcelona), Spain; 2ICREA-Institució Catalana de Recerca iEstudis Avançats, Barcelona, SpainIn this contribution, we report the�rst solid state spin-wave opticalquantum memory with on-demandread-out. We also demonstratethe �rst spin-wave storage of time-bin qubits with conditional �delitieshigher than for classical memories.
EF-6.6 MON 18:15Harmonics Generation by GuidedSurface Plasmon Polaritons onSingle Plasmonic Nanowires�A. de Hoogh, A. Opheij, N. Roten-berg, and K. Kuipers; FOM InstituteAMOLF, Amsterdam, �e Nether-landsWe experimentally observeharmonic generation at visiblewavelengths, scattering from aplasmonic nanowire. By studyingthe propagation lengths of thesecond harmonic signal, we identifythe fundamental nanowire surfaceplasmon polaritons as the source.
CC-5.6 MON 18:15THz pulse generation by chargedensity gradients investigated bynear-�eld microscopyR. Mueckstein1, M. Natrella1, O.Hatem2, J. Freeman2, C. Graham1,C. Renaud1, A. Seeds1, E. Lin�eld2,G. Davies2, P. Cannard3, M.Robertson3, D. Moodie3, and �O.Mitrofanov1; 1University CollegeLondon, London, United Kingdom;2University of Leeds, Leeds, UnitedKingdom; 3CIP Technologies,Ipswich, United KingdomUsing THz near-�eld microscopy,we investigate the process of THzpulse generation from semiconduc-tor surfaces. We demonstrate thatdynamics of the charge carriers inthe surface plane can be the domi-nant source of THz emission.
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HALL B013:30 – 14:30CB-P: CB Poster SessionCB-P.1 MONHigh power GaInNAs VECSEL emitting at 1230/615nm�J.-P. Penttinen, T. Leinonen, V.-M. Korpijärvi, E. Kan-tola, and M. Guina; Optoelectronics Research Centre,Tampere University of Technology, Tampere, FinlandWe report a frequency-doubled VECSEL operating at1230/615 nm. �e gain chip was grown by plasma-assisted MBE and comprised 10 GaInNAs quantumwells. Preliminary experiments show an output powerof >8 W at 615 nm.
CB-P.2 MONHigh-power optically in-well-pumped semiconductordisk lasers with reduced quantum defect�A. Hein1, U. Brauch2, S. Menzel1, M. Abdou Ahmed2,T. Graf2, and P. Unger1; 1Universität Ulm, Institut fürOptoelektronik, Ulm, Germany; 2Institut für Strahlw-erkzeuge, Universität Stuttgart, Stuttgart, GermanyDesign and characterization of high-power in-well-pumped InGaAs semiconductor disk lasers emitting at986 nm are presented. �e devices are designed toeliminate major loss mechanisms attributed to heat gen-eration in conventional barrier-pumped semiconductordisk lasers.
CB-P.3 MONBeam Shaping in Spatially Modulated Broad AreaEdge-Emitting Semiconductor Lasers�M. Radziunas1, R. Herrero2, M. Botey3, and K.Staliunas2,4; 1Weierstrass Institute, Berlin, Germany;2Departament de Física i Enginyeria Nuclear, UniversitatPolitècnica de Catalunya, Terrassa, Spain; 3Departamentde Física i Enginyeria Nuclear, Universitat Politècnica deCatalunya, Barcelona, Spain; 4Institució Catalana de Re-cerca i Estudis Avançats (ICREA), Barcelona, SpainWe consider theoretically lateral (angular) shaping ofthe radiation of broad area edge-emitting semiconduc-tor lasers. �e angular �ltering is realized by an appro-priate periodic structuring of the semiconductor mediain both lateral and longitudinal directions.
CB-P.4 MONBeam quality improvement by suppression ofModulation Instability in broad area semiconductorlaser ampli�er�S. Kumar1, R. Herrero1, M. Botey1, and K. Staliunas1,2;1Universitat Politècnica de Catalunya, Terrassa, Spain;2Institució Catalana de Recerca i Estudis Avançats,Barcelona, SpainA signi�cant improvement in the spatial beam qualityof broad area semiconductor laser ampli�er is numeri-
cally demonstrated. �e mechanism is based on using2D-spatial gain modulation to suppress modulation in-stability at high pump powers.
CB-P.5 MONIncreased slow-axis beam quality in 9xx nm highpower broad area diode lasers by modifying thelateral current pro�le at the device edges�M. Winterfeldt, P. Crump, S. Knigge, A. Maaßdorf, andG. Erbert; Ferdinand-Braun-Institut, Berlin, GermanyImproved radiance is achieved in 9xx-nm broad arealasers by suppressing lateral current spreading usingdeep proton-bombardment. Beam parameter product at7W output was reduced by 20% to 2.1mm-mrad. How-ever, e�ciency is also 7% reduced.
CB-P.6 MONNarrowband GaN external cavity diode laser with 400mW output power at 445 nm for deep ultravioletfrequency doubling�N. Ruhnke, A. Müller, B. Eppich, R. Güther, M. Mai-wald, B. Sumpf, G. Erbert, and G. Tränkle; Ferdinand-Braun-Institut, Leibniz-Institut für Höchstfrequenztech-nik Berlin, Berlin, GermanyWepresent aGaN external cavity diode laser systemwith400 mW optical power and an emission width of 20 pmat 445 nm suitable for frequency conversion into the UVspectral range.
CB-P.7 MONGaSb-based 2 �m Semiconductor Disk Laser: Powerscaling for optical pumping of Ho:YAG�P. Holl1, M. Rattunde1, S. Adler1, S. Kaspar1,3, W.Bronner1, A. Bächle1, R. Aidam1, J. Wagner1, K. Scholle2,S. Lamrini2, and P. Fuhrberg2; 1Fraunhofer Institutefor Applied Solid State Physics, Freiburg, Germany;2LISA laser products OHG, Katlenburg-Lindau, Ger-many; 3AIM Infrarot-Module GmbH, Heilbronn, Ger-manyBy improving the heat sinking and reducing the quan-tum de�cit we achieved 10W cw output power at 20�Cwith a GaSb-based, 2 �m-emitting VECSEL. Tailored se-tups for Holmium-pumping and �rst measurements areshown.
CB-P.8 MONLifetime of High Power Laser Diodes with Feedbackfrom Optical Systems�D. Bonsendorf; LIMO Lissotschenko MikrooptikGmbH, Dortmund, Germany; Ruhr-Universität Bochum,Bochum, Germany�e destroy threshold of AlGaAs and InGaAs laserdiodes due to back re�ected light is evaluated, includ-ing time depending e�ects. �eoretical and experimen-
tal data show the in�uence of optical elements to the laserdiode reliability.
CB-P.9 MONQuantitative analysis of the output power andlinewidth of blue light laser sources for future displayapplications�J. Hofmann, A. Sahm, D. Jedrzejczyk, G. Blume, D. Feise,and K. Paschke; Ferdinand Braun Institut Leibniz Institutfür Höchstfrequenztechnik, Berlin, GermanyWe present detailed experimental analysis of di�erentimplementations of blue light laser sources for futureholographic display applications. �is includes an anal-ysis of the optical output power, the linewidth and thecomplexity of a micro-integration.
CB-P.10 MONComparison of AlGaInP red-emitting taperedampli�ers with and without ridge waveguide section�G. Blume, J. Pohl, D. Feise, M. Jendrzejewski, M. Greiner,B. Eppich, B. Sumpf, and K. Paschke; Ferdinand Braun In-stitut, Berlin, GermanyWe compared tapered ampli�er with (TPA) and without(TTA) ridge wavguide sections emitting near 647 nm,and achieve about 470mW and 700mWwith a TPA anda TTA, respectively.
CB-P.11 MONDual-polarization VCSEL-based optical frequencycomb generation�E. Prior1, C. de Dios1, M. Ortsiefer2, P. Meissner3, andP. Acedo1; 1Electronics Technology Department, Univer-sidad Carlos III de Madrid, Leganés, Spain; 2VertilasGmbH, Garching, Germany; 3Technische UniversitätDarmstadt, Darmstadt, GermanyWe present results suggesting that VCSEL-based combsunder Gain-Switching are formed by two orthogonallypolarized combs with a strong phase relation. Broadercoherent combs could be obtained balancing the powerof these orthogonal components
CB-P.12 MONMicro-Integrated, Narrow Linewidth MasterOscillator Power Ampli�er Designed for QuantumSensors in Space�A. Kohfeldt1, M. Schiemangk1,2, A. Wicht1, G. Erbert1,A. Peters1,2, and G. Tränkle1; 1Ferdinand-Braun-Institut,Berlin, Germany; 2Institut für Physik, Humboldt-Universität, Berlin, GermanyWe developed a narrow linewidth DFB-Master Oscilla-tor Power Ampli�er module for the deployment of coldatom based quantum sensors in space. �e micro opti-cal benches not larger than 80 x 25mm2 passed randomvibration and shock tests.
CB-P.13 MONSpectro-temporally resolved Stokes polarizationparameters of transverse multi-mode oxide-con�nedVertical-Cavity Surface-Emitting Lasers�A.Molitor1, T. Mohr1, S. Hartmann1, andW. Elsäßer1,2;1Institute of Applied Physics, TU Darmstadt, Darmstadt,Germany; 2Center of Smart Interfraces, TU Darmstadt,Darmstadt, GermanyWe present experimentally obtained time-resolved andspectro-temporally resolved Stokes polarization param-eters of a transverse multi-mode VCSEL on a microsec-ond timescale. �ese results uncover the complex polar-ization dynamic of each particular transverse mode.
CB-P.14 MONEpitaxy-Based Electro-�ermal Simulation Approachfor Vertical-Cavity Surface-Emitting Laser Structures�M. Daubenschüz1, P. Gerlach2, and R. Michalzik1; 1UlmUniversity, Institute of Optoelectronics, Ulm, Germany;2Philips Technologie GmbH, U-L-M Photonics, Ulm, Ger-manyWe present a novel quasi-3D electro-thermal VCSELsimulation approach based on epitaxial growth designsas data input. Without any adjustable parameter thecomputation results show excellent agreement withmea-sured current-voltage characteristics and thermal wave-length shi�s.
CB-P.15 MONSpontaneous Formation of InhomogeneouslyPolarized Vortex Soliton States in Vertical-CavitySurface-Emitting Lasers with Feedback�J. Jimenez1, T. Ackemann1, W. Firth1, G.-L. Oppo1, andP. Rodriguez2; 1University of Strathclyde, Glasgow, UnitedKingdom; 2Dpto de Fisica, Universidad de Cordoba, Cor-doba, SpainWe observe inhomogeneously polarized vortex solitonstates in a vertical-cavity surface-emitting laser withfrequency-selective feedback, and demonstrate the evo-lution of vortex solitons with homogeneous polarizationto azimuthally polarized states as the current injection isdecreased
CB-P.16 MONEnhanced E�ciency of Quantum well pumpedAlGaInP VECSEL�C.M. Mateo1, U. Brauch1, T. Schwarzbäck2,3, H. Kahle2,M. Jetter2, M. Abdou Ahmed1, P. Michler2, and T.Graf1; 1Institut für Strahlwerkzeuge, Stuttgart, Ger-many; 2Institut für Halbleiteroptik und FunktionelleGrenz�ächen, Stuttgart, Germany; 3TRUMPF Lasersys-tems for SemiconductorManufacturingGmbH,Ditzingen,Germany�e e�ciency with respect to the absorbed power of the
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HALL B0665-nm AlGaInP VECSEL, was enhanced by 3.5 timeswhen using a 640-nm pump (quantum well pumping)instead of a 532-nm pump (barrier pumping).
CB-P.17 MONTunable external cavity laser with graded CRIGFs�lters�O. Gauthier-Lafaye1,2, A. Monmayrant1,2, S. Augé1,2,S. Calvez1,2, and E. Daran1,2; 1CNRS, LAAS, Toulouse,France; 2Université de Toulouse, Toulouse, FranceTunable CRIGF �lters made of spatially graded gratingsare reported for the �rst time. Once inserted into a cat’seye external cavity setup, they enable wide wavelengthtuning of a laser diode.
CB-P.18 MONFrequency doubling of a mode-lockedAlGaInP-VECSEL�R. Bek1, G. Kersteen1, S. Baumgärtner1, F. Sauter1, H.Kahle1, T. Schwarzbäck1,2, M. Jetter1, and P. Michler1;1Institut für Halbleiteroptik und Funktionelle Gren-z�ächen and Research Center SCoPE, Stuttgart, Ger-many; 2Optics Development, TRUMPF Lasersystems forSemiconductor Manufacturing GmbH, Ditzingen, Ger-manyWe present intra-cavity frequency doubling of a SESAMmode-locked AlGaInP-VECSEL using InP quantumdots as active material. Our measurements show laserpulses at 324 nm with a repetition frequency of around850 MHz.
CB-P.19 MONNanosecond high-current pulsed operation ofridge-waveguide lasers�A. Klehr, T. Prziwarka, A. Liero, T. Ho�mann, H.-J. Wünsche, H. Wenzel, and G. Erbert; Ferdinand-Braun-Institut, Leibniz Institut für Höchstfrequenztech-nik, Berlin, GermanyExtremely strong ns-pulses are generated with 808nmridge-waveguide lasers. Unusual post-pulse reverse cur-rents are revealed under excitation beyond 10A.�ey areattributed to the re�ow of excess carriers leaked beforefrom the active layer.
CB-P.20 MONIncreased nonlinear-imaging signal-intensity byamplitude-modulated mode-locking�C. Weber, L. Drzewietzki, and S. Breuer; Institute of Ap-plied Physics, Technische Universität Darmstadt, Darm-stadt, GermanyWe experimentally show a gain in signal amplitude fornonlinear imaging applications by intensity autocorre-lation measurements of an amplitude-modulated pulse-
train from a passively mode-locked quantum-dot laseras compared to an amplitude-constant pulse-train.
CB-P.21 MONOptimization of a mode-locked diode laser bymanipulation of intracavity dispersion andabsorption with an evolutionary algorithm�R.H. Pilny, B. Döpke, C. Brenner, J.C. Balzer, and M.R.Hofmann; Ruhr-Universität Bochum, Bochum, GermanyIntracavity dispersion management increases the spec-tral bandwidth inmodelocked semiconductor lasers. Weoptimize second- and third order dispersion, as well asfurther relevant system parameters using an evolution-ary algorithm, increasing the bandwidth by over 50%.
CB-P.22 MONTwo state QD laser turn on: slow passage e�ects�E.A. Viktorov1,2,3, T. Erneux2, M. Abu Saa3,4,J. Danckaert3, V.V. Dudelev5, E.D. Kolykhalova6,K.K. Soboleva7, A.G. Deryagin5, I.I. Novikov5,M.V. Maximov5, A.E. Zhukov8, V.M. Ustinov5, V.I.Kuchinskii5, W. Sibbett9, E.U. Rafailov10, and G.S.Sokolovskii5; 1ITMO University, St. Petersburg, Rus-sia; 2Optique Nonlinéaire �éorique, Bruxelles, Belgium;3Vrije Universiteit Brussel, Applied Physics research group(APHY), Brussels, Belgium; 4Arab American University,Jenin, Palestinian territories; 5Io�e Physical-TechnicalInstitute, Saint Petersburg, Russia; 6St. Petersburg StateElectrotechnical University (LETI), St. Petersburg, Rus-sia; 7St. Petersburg State Polytechnical University, St.Petersburg, Russia; 8Academic University, St. Petersburg,Russia; 9University of St. Andrews, St. Andrews, UnitedKingdom; 10Aston Institute of Photonic Technologies,Aston University, Birmingham, United KingdomWe investigate the turn-on dynamics of quantum dotlaser operating simultaneously at the ground and excitedstates. �e time interval between their respective turn-on is determined experimentally and analytically and ex-hibits precise scaling laws.
CB-P.23 MONAll Optical Dual-Wavelength Switching andInjection-Locking of InAs/InGaAs Passively ModeLocked Quantum Dot Fabry-Perot Lasers�C. Mesaritakis1, A. Bogris2, and D. Syvridis1; 1Nationaland Kapodistrian University of Athens, Athens, Greece;2Department of Informatics, Technological EducationalInstitute of Athens, Egaleo, GreeceAll-optical dual and ground-excited state switchingalongside clock recovery is achieved through regulatedunidirectional injection locking of two InAs/InGaAsquantum dot based Fabry-Perot passively mode-lockedlasers without repetition frequency tuning.
CB-P.24 MONFeedback induced dark solitons in a quantum dotlaser�B. Kelleher1,2, B. Tykalewicz1,2, D. Goulding1,2, S.P.Hegarty1,2, G. Huyet1,2,3, and E.A. Viktorov3,4; 1CAPPA,Cork Institute of Technology, Cork, Republic of Ireland;2Tyndall National Institute, University College Cork,Cork, Republic of Ireland; 3National Research Universityof Information Technologies, Mechanics and Optics, St.Petersburg, Russia; 4Université Libre de Bruxelles, Brus-sels, BelgiumWe report, experimentally and numerically on darkpulse generation in a quantum dot laser with opticalfeedback. �ese dark pulses form various bound statesdepending on the feedback strength and delay.
CB-P.25 MONChaos generation and communications usingquantum dots laser sources with an integrated air gapA. Sanduta, S. Rusu, and �V. Tronciu; Technical Univer-sity of Moldova, Chisinau, Moldova, Republic ofWe study the dynamical behavior of integrated devicecomposed by quantum dots semiconductor laser anddouble cavity that provides optical feedback. �e op-timal conditions for chaos generation, synchronizationand examples of message encoding are presented.
CB-P.26 MONDual-Mode Behavior in Multi-Section DFBSemiconductor Lasers with Laterally-CoupledRidge-Waveguide Surface Gratings�T. Uusitalo, H. Virtanen, J. Viheriälä, J. Salmi, A. Aho,and M. Dumitrescu; Tampere University of Technology,Tampere, FinlandExperimental studies of dual-mode multi-section DFBlasers fabricated using cost-e�ective UV-NIL are pre-sented alongside time-domain-travelling-wave simula-tions. �e reported results advance the understanding ofdual-mode behavior inmulti-section quantum-well DFBlasers based on a rigorous model.
CB-P.27 MONExternal-cavity semiconductor laser withstate-dependent delay�X. Porte, J. Martinez-Llinas, M.C. Soriano, P. Colet, andI. Fischer; IFISC, Instituto de Fisica Interdisciplinar y Sis-temas Compejos (CSIC-UIB), Palma de Mallorca, SpainWe introduce and implement a semiconductor laser sys-temwith two external cavities of di�erent length and dis-junct spectral re�ection. We demonstrate self-organizeddynamical switching between states dominated by theindividual cavities, inspiring novel applications.
CB-P.28 MONCoexistence of Multiple Stable Continuous-WaveStates in Micro-Integrated External-Cavity DiodeLasers�M. Radziunas1, V.Z. Tronciu2, E. Luvsandamdin3, C.Kuerbis3, A. Wicht3, and H. Wenzel3; 1Weierstrass In-stitute, Berlin, Germany; 2Dept. of Physics, TechnicalUniversity of Moldova, Chisinau, Moldova, Republic of ;3Ferdinand-Braun-Institut, Leibniz-Institut für Höchst-frequenztechnik, Berlin, GermanyWe investigate dynamics of external cavity diode lasers.We present a theoretical and experimental evidence ofthe coexisting stable stationary states and discuss the rec-ommendations for manufacturing single-state deviceswith a suppressed mode-beating dynamics.
CB-P.29 MONMicroscopic model for gain from electrically pumpedquantum dots: Connection between quantum dotdensity and current density�S. Michael1, W.W. Chow2, and H.C. Schneider1;1University of Kaiserslautern, Kaiserslautern, Germany;2Sandia National Laboratories, Albuquerque, UnitedStatesWe investigate a microscopic model for electrically-pumped quantum dots as active material for a quantumcascade laser. We study the dependence on dot den-sity and predict reduced current densities as comparedto quantum wells.
CB-P.30 MONInP-based Tunable Single Longitudinal Mode 1x2Multimode-Interference-Fabry-Perot SemiconductorLaser Diode�H. Yang1, M. Yang1, P. Morrissey1, B. Corbett1, andF. Peters1,2; 1Tyndall National Institute, University Col-lege Cork, Cork, Republic of Ireland; 2Department ofPhysics,University College Cork, Cork, Republic of IrelandA tunable single mode 1x2 Multimode-interference-Fabry-Perot composite cavity laser is presented. �e de-vices were fabricated using standard FP laser processingtechniques without regrowth and gratings and demon-strated 39dBm SMSR, 14nm tuning range and coherentoutputs.
CB-P.31 MONSignal properties and correlated emission ofexperimentally built coupled semiconductor lasernetworks�A. Argyris, A. Fragkos, M. Bourmpos, and D. Syvridis;National and Kaposidtrian University of Athens, Athens,GreeceIn the present work, a large-scale network of coupledsemiconductor lasers is built experimentally and inves-
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HALL B0tigated, including a large number of laser devices in amulti-directionally mesh-type coupling topology.
CB-P.32 MONLaser generation of coherent photon state carryingSpin-Angular-Momentum with handedness controlusing electronic spin transfer�S. Mohamed. Seghir1, M. Mikhaël1, S. Isabelle2, B.Grégoire2, and G. Arnaud1; 1Institut d’Electronique dusud,CNRS-UMR 5214, Université Montpellier, Montpel-lier, France; 2Laboratoire de Photonique et de Nanostruc-tures, CNRS-UPR 20, Marcoussis, FranceWe show a spin laser with spin transfer from pump-injected electrons to emitted photons. Our design is
based on (100)-oriented quantum-well GaAs-based Ver-tical External Cavity Surface Emitting laser (VECSEL) ina V-shaped cavity
CB-P.33 MONOriginal Screening Methodology Based onCorrelation between Low-Frequency NoiseMeasurement and Reverse Bias Behavior ofGaAs-based Laser Diodes�P. Del Vecchio1, A. Curutchet1, Y. Deshayes1, S. Joly1,M. Bettiati2, F. Laruelle2, and L. Béchou1; 1IMS Labo-ratory, University of Bordeaux, Bordeaux, France; 23SPTechnologies SAS, Nozay, FranceWe demonstrate that correlation between reverse I-
V and low-frequency noise measurements appears asa complementary tool for improvement of screeningmethodology in order to precisely discriminate GaAs-based Laser diodes and guarantee outstanding level ofperformance.
CB-P.34 MONDi�ractively coupled networks of semiconductorlasers�D. Brunner and I. Fischer; Instituto de Física Interdis-ciplinar y Sistemas Complejos (IFISC), Universitat de lesIlles Balears,, Palma de Mallorca, SpainSemiconductor laser networks are of high relevance forthe photonics community. We report a new scheme
based on di�ractive coupling and demonstrate interac-tion for 24 lasers. Our scheme is scalable, allowing forlarge network sizes.
CB-P.35 MONA New Compact Broadband Re�ector: �e HybridGrating�A. Taghizadeh, J. Mørk, and I.-S. Chung; Technical Uni-versity of Denmark, Kgs. Lyngby, DenmarkA new type of grating re�ector denoted hybrid gratingis introduced which shows large re�ectivity in a broadwavelength range. It has a structure suitable for realizinga vertical cavity laser with ultra-small modal volume.
13:30 – 14:30CK-P: CK Poster Session
CK-P.1 MONPlasmon Induced Enhancement of the Photoresponseof Heterostructures with Composite Layers of Si andAu NanoparticlesO.S. Ken, D.A. Yavsin, S.A. Gurevich, and �O.M. Sreseli;Io�e Physicotechnical Institute, St. Petersburg, RussiaPhotoresponse enhancement in rectifying heterostruc-tures based on composite layers of Si and Au nanoparti-cles was observed in the blue and UV spectral regions.�e e�ect is connected with surface plasmon resonancein metal particles.
CK-P.2 MONUltra-high E�ciency and Broadband SubwavelengthGrating CouplerS. Nambiar and �S.K. Selvaraja; Center for Nano Scienceand Engineering, Indian Institute of Science, Bangalore,IndiaWe present subwavelength based grating �bre-chip cou-pler in SOI with coupling e�ciency in excess of 90%and an operational 3dB bandwidth of >85 nm. �is isachieved by mode matching and directionality improve-ment.
CK-P.3 MONControlling Laser-induced Self-organized Patternsvia Engineered Defects�E. Ergecen1, Ö. Yavuz2, O. Tokel2, I. Pavlov3, A.Rizaoglu2, and F.Ö. Ilday2,3; 1Department of Electri-cal and Electronics Engineering, Middle East Techni-cal University, Ankara, Turkey; 2Department of Elec-trical and Electronics Engineering, Bilkent University,Ankara, Turkey; 3Department of Physics, Bilkent Univer-sity, Ankara, Turkey
Nonlinear laser lithography allows creating nanostruc-tures with remarkable order. Emergence of patterns isa stochastic process due to the intrinsic surface rough-ness. We demonstrate engineered substrates enable �necontrol of the evolution of surface patterns.
CK-P.4 MONUltimate Propulsion of Wavelength-Size andLow-Index-Contrast Dielectric Particles insideHollowWaveguides�A. Maslov; University of Nizhny Novgorod, Nizhny Nov-gorod, Russia�ree-dimensional full-wave modeling shows that par-ticles form resonant states with the below-cuto� modesof circular waveguides for various modes, particle sizes,and refractive indices. �e propelling force reachesalmost twice the incident electromagnetic momentum�ow.
CK-P.5 MONSuper-Resolution Mapping of Purcell EnhancementVariations within the Unit Cell of a Si PhotonicCrystal�F. Hackl, E. Lausecker, R. Jannesari, M. Glaser, F. Schäf-�er, and T. Fromherz; Institute of Semiconductor Physics,Johannes Kepler University, Linz, AustriaUtilizing the Moiré e�ect we systematically positionedSiGe islands within the unit cell of a Si Photonic Crys-tal and investigated the Purcell enhancement in depen-dence of the island positions by mapping the photolumi-nescence emission pro�le.
CK-P.6 MONModal method for second harmonic generation innanostructures�S. Héron1, F. Pardo2, P. Bouchon1, J.-L. Pelouard2, and R.Haïdar1; 1Onera - �e French Aerospace Lab, Palaiseau,
France; 2Laboratoire de Photonique et de Nanostructures(LPN-CNRS), Marcoussis, France�e contribution has been withdrawn by the authors.
CK-P.7 MONA High-Performance Polarization Converter Basedon Modulated Silicon Taper Waveguide forPolarization Multiplexing Designed by WavefrontMatching Method�S. Makino, T. Fujisawa, and K. Saitoh; Hokkaido Uni-vercity, Sapporo, JapanWe propose a polarization converter based on modu-lated silicon taper waveguide. �e loss of the proposedstructure is drastically improved by 1.24 dB in entireC-band compared with polarization converter based onconventional taper waveguide.
CK-P.8 MONSlow-Light Enhanced Second-Harmonic Generationin Periodic NanobeamWaveguides�R. Quintero-Bermudez, S. Saravi, F. Setzpfandt, and T.Pertsch; Institute of Applied Physics, Abbe Center of Pho-tonics, Friedrich-Schiller-Universität Jena, Jena, GermanyWe numerically analyze second-harmonic generation inperiodically structured nanobeamwaveguides. We iden-tify slow-light enhanced phase-matching points where,dependent on the geometry parameters, the second-harmonic can be generated in either forward or back-ward direction.
CK-P.9 MONDetermining the Parity of Fano Resonance fromField Distribution in a Photonic CrystalWaveguide-Cavity Structure�A.D. Østerkryger, J.R. de Lasson, Y. Yu, J. Mørk, and N.Gregersen; Department of Photonics Engineering, Techni-cal University of Denmark, Kongens Lyngby, DenmarkWe investigate the relation between the parity of Fano
resonances and �eld distribution in a photonic crystalstructure using Fourier modal method, establishing acorrelation between Fano parity and �eld pro�le.
CK-P.10 MONAxisymmetric Photonic Crystals for Beam SpatialShaping�V. Purlys1, L. Maigyte2, D. Gailevicius1, M. Peckus1, M.Malinauskas1, R. Gadonas1, and K. Staliunas2,3; 1LaserResearch Center, Department of Quantum Electronics,Vilnius University, Vilnius, Lithuania; 2Departament deFisica i Enginyeria Nuclear, Universitat Politecnica deCatalunya, Terrassa, Spain; 3Institucio Catalana de Re-cerca i Estudis Avancats (ICREA), Barcelona, SpainWe investigate axisymmetric photonic crystals for spatialbeam �ltering/shaping applications and report a far �eldsuper-collimation e�ect, caused by axisymmetric geom-etry. We use direct laser writing inside soda-lime glassand support the results numerically.
CK-P.11 MONFirst-Principle Constraints on the Performance ofOptical Actuators�S. Zanotto, F. Morichetti, and A. Melloni; Politecnico diMilano, Milano, ItalyRelying on the sole Maxwell equations for linear di-electrics, we introduce an inequality which sets a lowerlimit to spurious losses of phase and amplitude opticalactuators.
CK-P.12 MONCoupling Quantum Dots to a Nano�ber Bragg Cavity�Y. Oe1,2, A. Schell1,2,3,4, H. Takashima1,2,3, S.Kamioka1,2, M. Fujiwara1,2,4, O. Benson4, and S.Takeuchi1,2,3; 1Research Institute for Electronic Sci-ence, Sapporo, Japan; 2�e Institute of Scienti�c andIndustrial Research, Osaka, Japan; 3Graduate School ofEngineering, Kyoto University, Kyoto, Japan; 4Institute of
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
HALL B0Physics, AG Nano-Optik, Humboldt-Universitt zu Berlin,Newtonstr, Berlin, GermanyFor highly-e�cient �ber-integrated single photonsources, we report the enhanced photon-emissionfrom CdSe/ZnS quantum dots coupled to a nano�berBragg cavity with a mode volume below 1 �m3 andrepeatable tuning capability over 20 nm.
CK-P.13 MONFast magneto-optical modulation in opto�uidicdevices based on ferro�uid- �lled microstructuredoptical �bers�P. Agruzov1, I. Pleshakov1,4, E. Bibik2, S. Stepanov3, andA. Shamray1,4,5; 1Io�e Institute, Saint-Petersburg, Russia;2Saint Petersburg State Institute of Technology (Techni-cal University), Saint-Petersburg, Russia; 3CICESE, En-senada, Mexico; 4St. Petersburg Polytechnic Univer-sity, Saint-Petersburg, Russia; 5ITMO University, Saint-Petersburg, RussiaDetailed investigations of magneto-optical modulationin a silica-core microstructured �ber with a ferro�uidiccladding are reported. �e mechanism and conditionsof a fast modulation are discussed. A submicrosecondresponse time is demonstrated.
CK-P.14 MONHigh Q Cavities and Low-loss Waveguides inHyperuniform Photonic Slabs�T. Amoah and M. Florescu; University of Surrey, Guild-ford, United KingdomWe introduce novel planar hyperuniform-disordered(HUD) architectures as potential general-purpose plat-form for optical microcircuits. E�cient con�nementof TE-polarized radiation and high-Q optical-cavitiesand low-loss waveguides is demonstrated using �-nite di�erence-time-domain and band-structure simu-lations.
CK-P.15 MONPolarized emission from single CdSe/CdSnanocrystals coupled to a 1D gold grating and adisordered structureF. Eloi1, H. Frederich1, D. Canneson1, B. Bérini1,X. Quélin1, J.-P. Hermier1, �S. Buil1, A. Kumar2, A.Bouhelier2, J.-C. Weeber2, G. Colas Des Francs2, M.Nasilowski3, C. Javaux3, B. Bubertret3, and T.P.L. Ung1;1GEMAC, Université de Versailles, Versailles, France;2UCB, Université de Bourgogne, Dijon, France; 3ESPCI,Paris, France�ick shell colloidal CdSe/CdS nanocrystals are coupledto 1D gold gratings and disordered structures. �eiremission can be polarized in a single direction for thegrating and in any direction on the disordered structure.
CK-P.16 MONTunable plasmonic structures containing liquidcrystals�H. Kitzerow1,3, B. Atorf1,3, H. Mühlenbernd2,3, M.Muldarisnur2,3, and T. Zentgraf2,3; 1Department ofChemistry, University of Paderborn, Paderborn, Ger-many; 2Department of Physics, University of Paderborn,Paderborn, Germany; 3Center for Optoelectronics andPhotonics Paderborn, University of Paderborn, Pader-born, GermanyConcepts for tunable metamaterials with liquid crys-tals and resonance frequency measurements of split ringresonators embedded in nematic and ferroelectric liq-uid crystals owing to electric�eld-induced reorientation,Kerr-like optical nonlinearities or temperature changesare presented.
CK-P.17 MONFabrication of IR Polarization Device by DirectImprinting Process onto Sb-Ge-Sn-S systemChalcogenide Glass�I. Yamada1, N. Yamashita2, M. Saito3, K. Fukumi4, andJ. Nishii5; 1University of Shiga Prefecture, Hikone, Japan;2Isuzu Glass Co., Ltd., Osaka, Japan; 3Ryukoku Univer-sity, Otsu, Japan; 4AIST, Ikeda, Japan; 5Hokkaido Uni-versity, Sapporo, Japan�e contribution has been withdrawn by the authors.
CK-P.18 MONTowards microfabricated actuators controlled andpowered by light�A. Forrester, T. Freegarde, and J. Bateman; University ofSouthampton, Southampton, United KingdomWe discuss theoretical and experimental progress to-ward using two-photon lithography to fabricate micro-scopic actuators that change shape in ways that we cancontrol by tuning the wavelength of light incident on thestructure.
CK-P.19 MONNarrow peaks in a random laser at localizationtransition regime�E. Jimenez Villar1, V. Mestre2, and G. F. de Sá1;1Universidade Federal de Pernambuco, Departamento deQuímica Fundamental, Recife, Brazil; 2Universidade Fed-eral da Paraíba, Departamento de Física, Joao Pessoa,BrazilRandom lasing is reported at localization transition.Narrow peaks overlapped to a super-�uorescence bandare observed in the random laser emission spectrum.Localization transition was demonstrated by transportexperiments. �e sample residual absorption was neg-ligible.
CK-P.20 MONAnalysis of Surface Plasmons by Scanning Near-FieldOptical Microscopes: Modeling by GeometricalOptics and Rigorous Di�raction�eory�G. Bose1, H.J. Hyvärinen2, J. Tervo1, and J. Turunen1;1Institute of Photonics, University of Eastern Finland,Joensuu, Finland; 2Nanocomp Oy Ltd, Lehmo, FinlandWe present a geometry for scanning near-�eld micro-scopes using a local plane-interface approach. Using ge-ometrical optics and rigorous di�raction calculations wemodel near-�eld interaction of inhomogeneous waveswith a dielectric wedge.
CK-P.21 MONGeometry-Induced Inhomogeneous Broadening ofthe Stimulated Brillouin Resonance and its Relationto Radiation Pressure�C.Wol�1, M.J. Steel2, and C.G. Poulton1; 1Centre for Ul-trahigh bandwidth Devices for Optical Systems (CUDOS),School ofMathematical Sciences, University of TechnologySydney, Sydney, Australia; 2CUDOS, School of Physics,Macquarie University, Sydney, AustraliaWe theoretically demonstrate how the sensitivity of theoptical wave equation regarding geometry perturbationspractically limits the experimentally observable Stimu-lated Brillouin gain of silicon nanowires in the regime ofstrong radiation pressure.
CK-P.22 MONOn the stability of direct femtosecond laser writtenwaveguides in poly(methyl methacrylate)�W. Pätzold1, C. Reinhardt2, B. Chichkov2, andU. Morgner1,2; 1Institut für Quantenoptik, LeibnizUniversität Hannover, 30167 Hannover, Germany;2Laserzentrum Hannover e.V., 30419 Hannover, Ger-manyWe present investigations into the relation between thelong-term stability of femtosecond-written embeddedwaveguides in PMMA and the corresponding writingparameters, such as repetition rate, wavelength andbeam polarization.
CK-P.23 MONAnalysis on Minimizing Complex Spatial LightModulator Systems by Using Metamaterial Prism�H. Kwon1, J. Kim1, H. Kim2, and B. Lee1; 1National Cre-ative Research Center for Active Plasmonics ApplicationSystems, Inter-University Semiconductor Research Cen-ter and School of Electrical Engineering, Seoul NationalUniversity, Seoul, Korea, South; 2Department of Elec-tronics and Information Engineering, College of Scienceand Technology, Korea University, Sejong Campus, Se-jong, Korea, South
To overcome scale-down limit of a complex spatial lightmodulator (CSLM) system, we propose a CSLM modelonmicro-scale by usingmetamaterial prism, and investi-gate the scale-down limit of the model and related phys-ical issues.
CK-P.24 MONFine Tuning of the Emission Properties ofNano-Emitters in Multilayered Structures byDeterministic Control of their Local PhotonicEnvironment�J.F. Galisteo-López, A. Jiménez-Solano, and H. Míguez;Instituto de Ciencia de Materiales de Sevilla (ICMSe-CSIC), Seville, Spain�e local photonic environment of photonic systemscomprisingmultilayered nanoporous structures formingan optical microcavity is studied by deterministic posi-tioning nano-scale probes with nanometer precision andmonitoring the evolution of their emission dynamics.
CK-P.25 MONDetermination of the orientation of a single emitterby polarimetryC. Lethiec1, J. Laverdant2, C. Javaux3, B. Dubertret3,F. Pisanello4, L. Carbone4, A. Bramati5, L. Coolen1,and �A. Maitre1; 1Institut des Nanosciences de Paris,Paris, France; 2Institut Lumière Matière, Lyon, France;3Laboratoire de Physique et d*Etude desMatériaux, Paris,France; 4Università del Salento, Lecce, Italy; 5laboratoireKastler Brossel, Paris, FranceE�cient coupling of nanoemitters to photonic structuresrequires the control of their orientation which remainsan experimental challenge. We propose here to deter-mine the orientation of nanoemitters by a polarimetricanalysis of their emission
CK-P.26 MONFiberized Plasmonic Fresnel Zone Plate forGenerating a Wavelength-Dependent Focal Point ofRadially Polarized Light�H. Kim, L. Vazquez-Zuniga, J. Kim, K. Park, D. Lee, S.Hong, and Y. Jeong; Seoul National University, Seoul, Ko-rea, SouthWe propose and numerically investigate a �berized plas-monic Fresnel zone plate scheme capable of readily pro-ducing radially polarized focused light, based on whichthe wavelength-dependent focal-point tuning range canextend to 10.79 �m.
CK-P.27 MONOptical parametric oscillation based on nonlinearphotonic crystals (2D-PPLT)M. Lazoul1, �A. Boudrioua2, L.M. Simohamed1, and L.H.Peng3; 1Laboratoire des Systèmes Electroniques et Op-
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
HALL B0troniques, École Militaire Polytechnique, Algiers, Alge-ria; 2Laboratoire de Physique des Lasers, Université deParis 13, Paris, France; 3Graduate Institute of Photonicsand Optoelectronics, National Taiwan University, Taipei,China, Republic of (ROC)Two-dimensional quadratic nonlinear photonic crys-tals are characterized by multiple quasi-phase matchingschemes that are in the origin of multiple wavelengthparametric generation. �ese properties are exploited todesign a multi-resonant optical parametric oscillator.
CK-P.28 MONGuiding performance and spectroscopy studies infemtosecond written Cr3+: LiSAF optical waveguidesD. Biasetti, M. Tejerina, and �G. Torchia; Centro de Inves-tigaciones Opticas CONICET La Plata - CICBA, La Plata,ArgentinaIn this work, optical waveguides obtained by ultrashortlaser writing support TE and TMpropagation. Lumines-cence studies have con�rmed that the Cr3+ optical prop-erties in the waveguides are similar that those measuredin the bulk.
CK-P.29 MONMetallic meta�lms as broadband antire�ectivecoatings and transparent electrodes forsemiconductor devices�F. Afshinmanesh, M. Esfandyarpour, and M.L.Brongersma; Stanford University, Stanford, United StatesWe propose a metallic meta�lm as both a broadband an-tire�ective coating and a transparent electrode for lowand high index semiconductor materials. We numeri-cally and experimentally demonstrate our devices in thevisible and near IR.
CK-P.30 MONBasic Features of Multi-Splitting FilteringTechnology�A. Tsarev; Rzhanov Institute of Semiconductor PhysicsSB RAS, Novosibirsk, Russia;Novosibirsk State University,Novosibirsk, RussiaPaper presents the original results describing the multi-splitting �ltering technology. It provides the general de-scription and simulations by FDTD and MEIM of noveloptical �lter/multiplexer constructed by multiply cou-pled silicon wires in SOI technology.
CK-P.31 MONMesoscopic Self-Collimation: beyond the highsymmetry constraint�G. Magno1,2, A. Monmayrant2,3, M. Grande1, F. Lozes-Dupuy2,3, O. Gauthier-Lafaye2,3, G. Calò1, and V.Petruzzelli1; 1Politecnico di Bari, Bari, Italy; 2LAAS-CNRS, Toulouse, France; 3Université de Toulouse,Toulouse, FranceMesoscopic Photonic Crystals are exploited to achieveMesoscopic Self-Collimation in arbitrary directions (notof high symmetry). �is is possible even below the lightline, eluding the out-of-plane losses usually associatedwith the long mesoscopic period.
CK-P.32 MONPhoton-pair generation in a nonlinearone-dimesional metallo-dielectric photonic crystal�D. Javůrek1, J. Peřina2, and J. Svozilík1; 1RCPTM, JointLaboratory of Optics of Palacký University and Instituteof Physics of AS CR, Olomouc, Czech Republic; 2Instituteof Physics, Joint Laboratory of Optics of Palacký Univer-sity and Institute of Physics of AS CR, Olomouc, CzechRepublicMetallo-dielectric nonlinear one-dimensional crystalshave been analyzed as e�cient sources of entangled pho-ton pairs generated by spontaneous parametric down-conversion. Spatial, spectral and temporal characteris-tics of the emitted photon pairs have been discussed.
CK-P.33 MONContactless Light Monitoring in InP-basedWaveguidesD. Melati, M. Carminati, �F. Morichetti, and A. Melloni;Dipartimento di Elettronica, Informazione e Bioingegne-ria, Politecnico di Milano, Milano, Italy�e realization of the non-invasive light monitorContactLess Integrated Photonic Probe on Indium-Phosphide-based waveguides is demonstrated. An inno-vative vertical scheme exploiting a shared common elec-trode is also presented and characterized.
CK-P.34 MONLaser Writing Deep inside Silicon for 3D InformationProcessing�O. Tokel1, A. Turnali2, I. Pavlov1, and F.Ö. Ilday1,2;1Department of Physics, Bilkent University, Ankara,Turkey; 2Department of Electrical and Electronics Engi-neering, Bilkent University, Ankara, TurkeyFabricating subsurface structures in silicon is highly de-sired. We report a laser writing method enabling buried
structures inside Si, with one micrometer widths, overlong ranges. We demonstrate 3D information encodingin multilayer Si barcodes.
CK-P.35 MONTopology-Dependent Light Transport in PlanarPlasmonic-Photonic Architectures�R. Tuzakli1,2, N. Vogel3, A. Romanova2, S. Romanov2,and U. Peschel2,4; 1Master Programme in Advanced Op-tical Technologies, Erlangen, Germany; 2Institute of Op-tics, Information and Photonics, Erlangen, Germany;3Institute of Particle Technology, Erlangen, Germany;4Institute of Solid State�eory and Optics, Erlangen, Ger-manyMerging plasmonic and photonic structures with di�er-ent topologieswas used to demonstratemixing of surfaceplasmon polaritons, cavity modes and Fabry Perot reso-nances in the complex optical response and to achievedi�erent regimes of waveguiding.
CK-P.36 MONTopological Edge Modes in Arrays of PhotonicCrystal Cavities�M. Minkov and V. Savona; Institute of �eoreticalPhysics, Ecole Polytechnique Fédérale de Lausanne, Lau-sanne, SwitzerlandWe demonstrate that a chain of optical cavities can betuned to be topologically equivalent to the Kitaev chain,and propose an implementation in a photonic crystal set-ting that shows Majorana-like edge modes.
CK-P.37 MONMulti-purpose, Automated Optimization of PhotonicCrystal Cavities�M. Minkov and V. Savona; Institute of �eoreticalPhysics, Ecole Polytechnique Fédérale de Lausanne, Lau-sanne, SwitzerlandUsing a fast simulation tool and a genetic algorithm, weoptimize in a fabrication-friendly way the quality factorand other parameters of various photonic crystal cavi-ties, and show the improvements both in theory and ex-periment.
CK-P.38 MONDiameter characterization of silica microwires usingforward Brillouin scattering�O. Florez, P. Jarschel, and P. Dainese; Instituto de FísicaGleb Wataghin, Universidade Estadual de Campinas,Campinas, BrazilDiameter uniformity in silica microwires is critical forvarious applications. We use forward Brillouin scatter-
ing to precisely measure the diameter and gain insightinto its uniformity along length. Non-uniformities of 1%and 3% were observed.
CK-P.39 MONStrain and Temperature Sensitivity of Beatlength in aDual-Core Microstructured Polymer Optical Fiber�G. Town1, S. Ghatrehsamani1, C. Markos2, and O.Bang2; 1Dept. Engineering, Macquarie University, NorthRyde, Australia; 2Dept. Photonics Engineering, DanishTechnical University, Kgs. Lyngby, DenmarkWe present results concerning the strain and tem-perature sensitivity of coupling in a dual-core micro-structured polymer optical �ber.
CK-P.40 MONIs E�ective Medium Approximation Always Valid forUltrathin Multilayer All-dielectric Metamaterials?�A. Andryieuski, A.V. Lavrinenko, and S.V. Zhukovsky;Technical University of Denmark, Kongens Lyngby, Den-markWe demonstrate anomalous e�ective medium approxi-mation breakdown for ultra-subwavelength all-dielectricmultilayer stacks. Re�ectance strongly depends on pe-riod, layers ordering and ambient material propertiesand that can be used for all-dielectric sensors.
CK-P.41 MONFabrication of Tailored Surface Relief Gratings forSolar Cell Applications�T. Schemme, M. Boguslawski, and C. Denz; Instituteof Applied Physics, University of Münster, Münster, Ger-manyWe employ a spatial light modulator (SLM)-based ap-proach to generate complex-structured surface reliefgratings (SRGs) in azopolymer layers. �ese SRGs aresubsequently transferred into PDMS. Again, these re-sulting light-harvesting �lms are applied onto solar cells.
CK-P.42 MONTransverse Mode Coupling and Di�raction Loss inFibre-Based Optical Microcavities�J. Benedikter1,2, T. Hümmer1,2, M. Mader1,2, T.W.Hänsch1,2, and D. Hunger1,2; 1Ludwig-Maximilians-Universität, München, Germany; 2Max-Planck-Institutfür Quantenoptik, Garching, Germany�e non-spherical mirrors of �bre-based microcavitiesinduce transverse mode coupling leading to mode dis-tortions and losses for certain mirror separations. Wemeasure those e�ects and successfully model them us-ing resonant state expansion.
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
HALL B013:30 – 14:30ED-P: ED Poster Session
ED-P.1 MONNoise Fluctuations in Kerr Frequency CombsD. Gomila1, �P. Colet1, A. Coillet2,3, and Y.K. Chembo3;1Insituto de Física Interdisciplinar y Sistemas Comple-jos, IFISC (CSIC-UIB), Palma de Mallorca, Spain; 2NIST,Boulder, United States; 3FEMTO-ST Institute [CNRSUMR6174], Optics Department, Besançon, FranceWe study analytically and numerically the broadening offrequency comb peaks due to noise using the Lugiato-Lefever model. �e neutral mode does not contribute tointensity �uctuations which are mainly determined byso�modes.
ED-P.2 MONStabilization of frequency combs using third orderdispersion�P. Parra-Rivas1,2, D. Gomila2, F. Leo3, S. Coen4, and L.Gelens1,5; 1Applied Physics Research Group, Vrije Univer-siteit Brussel, Brussels, Belgium; 2IFISC institute (CSIC-UIB), Campus Universitat de les Illes Balears, Palmade Mallorca, Spain; 3Photonics Research Group, De-partment of Information Technology, Ghent University,Ghent, Belgium; 4Dodd-Walls Centre and Physics Depart-ment,University of Auckland, Auckland, New Zealand;5Department of Chemical and Systems Biology, StanfordUniversity School of Medicine, Stanford, United StatesUsing the Lugiato-Lefever model we show that third-order chromatic dispersion stabilizes dynamical regimessuch as oscillations and chaos. �is stabilization couldbe of great interest for the frequency combs community.
ED-P.3 MONProgress of Aluminum Ion Optical Clock ProjectZ. Xu, H. Che, W. Yuan, X. Shi, X. Zeng, W.Wu, Y. Liu, S.Zhou, K. Deng, J. Zhang, and �Z. Lu; MOE Key Labora-tory of Fundamental Quantities Measurement, School ofPhysics, Huazhong University of Science and Technology,Wuhan, China, People’s Republic of (PRC)We report progress of Al ion optical clock at HuazhongUniversity of Science and Technology. An Al ion istrapped with a single Mg ion. Clock laser performancesbased on di�erent cavities are reported.
ED-P.4 MONAbsolute, Interferometric Calibration ofSubwavelength Displacement�V.�iel, J. Roslund, P. Jian, C. Fabre, and N. Treps; Lab-oratoire Kastler Brossel, Paris, FranceWepresent amethodology that results in an absolute cal-ibration of an interferometer, thus allowing high sensi-tivity measurement. �is relies on the determination ofa sub-wavelength displacement induced by a piezo ele-ment in the interferometer.
ED-P.5 MONUltra sensitive detection of HD lines by means ofNICE-OHMSH. Dinesan, �E. Fasci, S. Gravina, A. Castrillo, and L. Gi-anfrani; Dipartimento di Matematica e Fisica, SecondaUniversità di Napoli, Caserta, ItalyWe report on a new implementation of NICE-OHMS byusing an extended-cavity diode laser at 1.39 micron tomonitor weak vibration-rotation transitions of the HDmolecule and perform highly-precise measurements.
ED-P.6 MONMid-infrared 333-MHz frequency comb continuouslytunable from 1.95 �m to 4.0 �m�K. Balskus, Z. Zhang, R.A. McCracken, and D.T. Reid;Scottish Universities Physics Alliance (SUPA), Institute ofPhotonics and Quantum Sciences, School of Engineeringand Physical Sciences, Heriot-Watt University, Riccarton,Edinburgh EH14 4AS, UK, Edinburgh, United KingdomIdler pulses from a 333-MHz femtosecond optical para-metric oscillator were carrier-envelope-o�set stabilizedusing a versatile locking technique which allowed the re-sulting comb to be tuned continuously over a range from1.95um to 4.0um.
ED-P.7 MONCharacterization and Active Linewidth Narrowing ofa Passively Phase-Locked Er:Fiber Frequency Comb�D. Fehrenbacher, P. Sulzer, D.V. Seletskiy, and A. Leit-enstorfer; Department of Physics and Center for AppliedPhotonics, Konstanz, GermanyWe demonstrate an o�set-free Er:�ber frequency combestablished by di�erence frequency mixing. Linewidthnarrowing with an extra-cavity EOM and direct mHz-level stabilization of the repetition rate to a two-photon-transition in Rb are achieved.
ED-P.8 MONPhotonic Chip Based Optical Frequency Comb UsingSoliton Induced Cherenkov Radiation�V. Brasch1, M. Geiselmann1, T. Herr2, G. Lihachev3,M.H.P. Pfei�er1, M.L. Gorodetsky3, and T.J. Kippenberg1;1École Polytechnique Fédérale de Lausanne (EPFL), Lau-sanne, Switzerland; 2Centre Suisse d’ Electronique et
Microtechnique SA (CSEM), Neuchatel, Switzerland;3Faculty of Physics, M.V. Lomonosov Moscow State Uni-versity, Moscow, RussiaWe show for the �rst time a fully coherent frequencycomb generated in a SiN photonic chip which spans2/3 of an octave using solitons and soliton inducedCherenkov radiation. Additionally we stabilize the spec-trum.
ED-P.9 MONDevelopment of a strontium optical lattice clock forspace applications�Y. Singh1, L. Smith1, S. Origlia2, W. He1, D. Śweirad1,J. Hughes1, O. Kock1, S. Alighanbari2, S. Schiller2, K.Bongs1, S. Vogt3, U. Sterr3, C. Lisdat3, R. Le Targat4,J. Lodewyck4, D. Holleville4, B. Venon4, S. Bize4, G. PBarwood5, P. Gill5, I. R Hill5, Y. B Ovchinnikov6, N. Poli6,G. M Tino6, J. Stuhler7, W. Kaenders7, E. M. Rasel8,and S. team9; 1University of Birmingham, Birmingham,United Kingdom; 2Heinrich- Heine-Universität Düssel-dorf, Düsseldorf, Germany; 3Physikalisch-Technische-Bundesanstalt, Brounsweig, Germany; 4Observatoire deParis, Paris, France; 5National Physical Laboratory, Ted-dington, United Kingdom; 6Universita di Firenze, Flo-rence, Italy; 7TOPTICA Photonics AG, Munich, Ger-many; 8Leibniz Universität Hannover, Hannover, Ger-many; 9Menlo Systems GmbH, Munich, GermanyDevelopment of a strontium optical lattice clock forspace applications
13:30 – 14:30EG-P: EG Poster Session
EG-P.1 MONMeasurement of Belinfante’s spin momentum densityin tightly focused �elds�M. Neugebauer1,2, T. Bauer1,2, A. Aiello1,2, and P.Banzer1,2,3; 1Max Planck Institute for the Science of Light,Erlangen, Germany; 2Institute of Optics, Informationand Photonics, University Erlangen-Nuremberg, Erlan-gen, Germany; 3Department of Physics, University of Ot-tawa, Ottawa, CanadaWe reconstruct the longitudinal component of Belin-fante’s spin momentum density in tightly focused lightbeams by measuring the transverse spin density of theelectric �eld. �e experimental approach is based on anano-probe scanning technique.
EG-P.2 MONTowards nanoscale light-matter interfaces withsilicon-vacancy centers coupled to integrateddielectric nanostructures�M. Zeitlmair1, L. Liebermeister1, F. Böhm1, N.Heinrichs1, P. Fischer1, L. Worthmann1, P. Altpeter1,C. Nebel3, H. Weinfurter1,2, and M. Weber1,2; 1Facultyof Physics, Ludwig-Maximilian University of Munich,Munich, Germany; 2Max-Planck-Institute of QuantumOptics, Garching, Germany; 3Fraunhofer Institute forApplied Solid State Physics, Freiburg, GermanyWe present �rst steps towards a nanoscale light-matterinterface based on fabricated dielectric slot waveguidesand single SiV centers. By realizing coupling e�cienciesnear unity, optical nonlinear e�ects and single photonsensitivity are feasible.
EG-P.3 MONMulti-atom stimulated Raman adiabatic passagemediated by plasmons�G. Colas des Francs, B. Rousseaux, D. Dszotjan, H.Jauslin, and S. Guérin; ICB, Dijon, FranceWe develop an e�ective hamiltonian that fully trans-poses cQED concepts to quantum plasmonics and applyit to plasmonmediated adiabatic population transfer be-tween two atoms. We anticipate applications to quantumcontrol of at the nanoscale.
EG-P.4 MONBloch Surface Wave Polaritons at room temperatureS. Pirotta1, M. Patrini1, M. Liscidini1, M. Galli1, G.Dacarro1, G. Guizzetti1, D. Comoretto2, and �D. Bajoni3;1Dipartimento di Fisica, Universita degli Studi di diPavia, Pavia, Italy; 2Dipartimento di Chimica e Chim-ica Industriale, Universita degli Studi di Genova, Gen-
ova, Italy; 3Dipartimento di Ingegneria Industriale e In-formazione, Universita degli Studi di Pavia, Pavia, ItalyWe demonstrate strong coupling between Bloch SurfaceWaves (BSW) and excitons in a J-agg layer in both re-�ectance and photoluminescence. �e Rabi splitting is290 meV, sign of the good spatial overlap.
EG-P.5 MONLower-Upper Polariton Interactions Proved withTwo-Dimensional Fourier Transform (2DFT)Spectroscopy in Semiconductor Microcavity�N. Takemura1, S. Trebaol2, V. Kohnle1, Y. Léger3,M.D. Anderson1, M. Portella-Oberli1, and B. Deveaud1;1Laboratory of Quantum Optoelectronics, École Poly-technique Fédérale de Lausanne, Lausanne, Switzerland;2UMR FOTON, CNRS, Université de Rennes 1, Enssat,Lannion, France; 3FOTON Laboratory, Université Eu-ropéenne de Bretagne, CNRS-INSA-UR1, Rennes, France
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CLEO®/Europe-EQEC 2015 ⋅ Monday 22 June 2015
HALL B0Two-dimensional Fourier transform (2DFT) spec-troscopy of semiconductor microcavity has been per-formed. Comparing the experiments with Gross-Pitaevskii simulations, we demonstrate that, in additionto the known self-interaction, there exists a cross-interaction between lower and upper-polaritons.
EG-P.6 MONGap Plasmon Formation in Metallic, NanofocusingSNOM Tapers for Broadband Nanospectroscopy�S.F. Becker1, M. Esmann1, K. Yoo1,2, H. Kollmann1, P.Groß1, R. Vogelgesang1, N. Park2, and C. Lienau1; 1Carlvon Ossietzky Universität, Oldenburg, Germany; 2SeoulNational University, Seoul, Korea, SouthNanofocusing of surface plasmon polaritons enablesbroadband elastic scattering spectroscopy on individualnanoantennas without any signal demodulation. Clearexperimental signatures of tip-sample gap plasmon for-mation suggest a potential increase in lateral resolutionto single nanometers.
EG-P.7 MONCasimir-Polder interactions of atoms trapped in alattice close to a surface�A. Maury1, M. Donaire1, M.-P. Gorza1,2, R. Guerout1,and A. Lambrecht1; 1Laboratoire Kastler Brossel, UPMC-Sorbonne Universités, CNRS, ENS-PSL-Research Univer-sity, Collège de France, Paris, France; 2on leave from Lab-oratoire de Physique des Lasers, Université Paris 13, Sor-bonne Paris Cité, CNRS, Villetaneuse, FranceWe study the Casimir-Polder interaction of an atomtrapped in an optical lattice with a surface by perturba-tive and non-perturbative methods. We also discuss indetail the atomic eigenergies in the full atom-surface po-tential.
EG-P.8 MONEnhanced and polarized emission from singleCdSe/CdS nanocrystals coupled to a gold gratingdecoupler at low temperature�F. Eloi1, S. Buil1, X. Quélin1, A. Kumar2, A. Bouhelier2,J.-C. Weeber2, G. Colas des Francs2, M. Nasilowski3,P. Spinicelli3, B. Dubertret3, and J.-P. Hermier1,4;1Université de Versailles Saint Quentin, Versailles,
France; 2Université de Bourgogne, Dijon, France; 3EcoleSupérieure de Physique et Chimie Industrielles, Paris,France; 4Institut Universitaire de France, Paris, France�ick shell colloidal CdSe/CdS nanocrystals coupled tostraight 1D or circular gold gratings are studied at lowtemperature. �e emission of a single NC is enhancedand can be nearly completely polarized.
EG-P.9 MONNanolevitation phenomena in real plane-parallelsystems mediated by Casimir forces�V. Esteso, S. Carretero-Palacios, and H. Míguez; Insti-tuto de Ciencia deMateriales de Sevilla. CSIC-US, Seville,SpainWe report on the theoretical prediction of nanolevita-tion phenomena due to the balance betweenCasimir andgravity forces at thermal equilibrium, by modifying theoptical properties of the materials involved in a control-lable way.
EG-P.10 MONPlasmonic Nanoprobes For High ResolutionMapping�F. Tantussi, A. Jacassi, M. Malerba, P. Zilio, and F. DeAngelis; Istituto Italiano di Tecnologia, Genova, ItalyWe are going to present an AFM cantilever witha nanofabricated gold-nanocone surface plasmonicwaveguide. With a speci�c radially polarized light, theplasmonic tip acts as nanophotonic source for opticalmapping.
EG-P.11 MONTunable nonlinear e�ects through focused spatiallyphase-shaped beams�L. Turquet1, G. Bautista1, L. Karvonen2, V. Dhaka2,Y. Chen2, H. Jiang3, T. Huhtio2, H. Lipsanen2, and M.Kauranen1; 1Department of Physics, Tampere Universityof Technology, Tampere, Finland; 2Department of Mi-cro and Nanosciences, Aalto University, Espoo, Finland;3Department of Applied Physics and NanomicroscopyCenter, Aalto University, Espoo, FinlandWe demonstrate controllable second-harmonic genera-tion from a single vertically aligned GaAs nanowire us-ing a phase-shaped HG10 beam. �e results open new
opportunities for controlling nonlinear interactions inindividual nanostructures through polarization encodedincident beams.
EG-P.12 MONStabilization, bistability and suppression of nuclearspin �uctuations around semiconductor electrons�D. O’Shea1, J. de Jong1, A. Onur1, U. Gupta1, S.Volker1, D. Reuter2, A. Wieck3, and C. van der Wal1;1Zernike Institute for Advanced Materials, University ofGroningen, Groningen, �e Netherlands; 2Fakultaet fuerNaturwissenscha�en, Universitaet Paderborn, Pader-born, Germany; 3Angewandte Festkoerperphysik, Ruhr-Universitaet Bochum, Bochum, GermanyWe demonstrate experimentally and theoretically howoptical coherent population trapping of the spin oflocalized semiconductor electrons stabilizes and sup-presses noise from the surrounding nuclear spins via au-tonomous feedback control.
EG-P.13 MONSubwavelength Nanopatch SiN/Au NanocavitiesS. Bisschop1,2,3, J. Ciers2, A. Guille1,3, P. Geiregat1,3,�E. Brainis1,3, Z. Hens1,3, and D. Van �ourhout2,3;1Physics and Chemistry of Nanostructures, Ghent Uni-versity, Ghent, Belgium; 2Photonics Research Group, IN-TEC Department, Ghent University-IMEC, Ghent, Bel-gium; 3Center for Nano and Biophotonics (NB Photonics),Ghent University, Ghent, BelgiumWe present the fabrication and optical characterisationof light emission fromnanopatch cavities containing col-loidal quantum dots in a silicon-nitride matrix sand-wiched between two layers of gold. Purcell speed-up ofthe spontaneous emission in demonstrated.
EG-P.14 MONFine-Structure Relaxation Mechanisms and DiscreteExciton-Phonon Coupling in Single ColloidalCdSe/CdS/PMMAQuantum Dots�F. Werschler1, C. Hinz1, T. de Roo2, S. Mecking2, A.Leitenstorfer1, and D.V. Seletskiy1; 1Universität Kon-stanz, Department of Physics, Konstanz, Germany;2Universität Konstanz, Department of Chemistry, Kon-stanz, Germany
Temporal decay and spectral characteristics of pho-toluminescence of single colloidal CdSe/CdS/PMMAnanoparticles are analyzed. Together with temperature-dependent relaxation rates, these results reveal strongexciton-phonon coupling mediated by con�ned acousticphonons, in agreement with model calculations.
EG-P.15 MONChaos and Random-Number Generation Based onNanoscale Optical Energy Transfer�M. Naruse1, S.-J. Kim2, M. Aono3,4, H. Hori5, and M.Ohtsu6; 1National Institute of Information and Commu-nications Technology, Tokyo, Japan; 2National Institutefor Materials Science, Tsukuba, Japan; 3Tokyo Institute ofTechnology, Tokyo, Japan; 4Japan Science and TechnologyAgency, Saitama, Japan; 5University of Yamanashi, Ya-manashi, Japan; 6�e University of Tokyo, Tokyo, JapanWe theoretically demonstrate that chaotic oscillationand random-number generation (RNG) occur based oninter-quantum-dot energy transfer by optical near-�eldinteractions, showing that complex oscillatory dynamicsand ultrasmall RNGs should be available by near-�eldoptics.
EG-P.16 MONSimulation study of the stability of polarisationstructure in disordered PHC waveguides�B. Lang, D. Beggs, A. Young, J. Rarity, and R. Oulton;University of Bristol, Bristol, United Kingdom�e e�ects of short range disorder on the polarizationcharacteristics of light in W1 photonic crystal waveg-uides were simulated. It was found that points of localcircular polarization (C-points) were robust in quantityand location.
13:30 – 14:30JSV-P: JSV Poster Session
JSV-P.1 MONQuantum information interface between telecom-munication wavelengths and Yb+-dipole transition�H. Rütz, K.-H. Luo, H. Suche, and C. Silberhorn; Inte-
grated Quantum Optics, University of Paderborn, Pader-born, GermanyWe present a quantum information interface betweentelecommunication wavelengths (1310 nm) and an Yb+-dipole transition (369,5 nm) based on a second-ordersum-frequency process in a PPKTP waveguide, showinga conversion e�ciency above 5% and signal-to-noise ra-tio above 2.
JSV-P.2 MONCoherent Spectral Manipulation of Non-ClassicalOptical Wave Packets�M. Karpinski, L. Wright, and B. Smith; University of Ox-ford, Oxford, United Kingdom�e contribution has been withdrawn by the authors.
JSV-P.3 MONEmission of time-energy entangled photons from asilicon microring resonator.D. Grassani1, S. Azzini1, M. Liscidini1, M. Galli1,M. Strain2, M. Sorel3, J. Sipe4, and �D. Bajoni5;1Dipartimento di Fisica, Universita‘ di Pavia, Pavia, Italy;2Institute of Photonics, University of Strathclyde, Glas-gow, United Kingdom; 3School of Engineering, University
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HALL B0of Glasgow,, Glasgow, United Kingdom; 4Department ofPhysics and Institute for Optical Sciences, University ofToronto, Toronto, Canada; 5Dipartimento di IngegneriaIndustriale e Informazione, Universita di Pavia, Pavia,ItalyWe show emission of time-energy entangled photonsfrom a silicon microring resonator. �e footprint of thesource is hundreds of square microns, yet the spectralintensity is much larger than previous silicon sources.
JSV-P.4 MONA two-channel, degenerate polarizationentanglement source on chip�L. Sansoni, K.H. Luo, R. Ricken, S. Krapick, H. Her-rmann, and C. Silberhorn; Integrated Quantum Optics,University of Paderborn, Paderborn, GermanyWe report on the realization of an integrated, post-selection free source of polarization entangled statesemitted on two channels at degenerate wavelength. �isdevice represents a step forward to exploit polarizationencoding in integrated setups.
JSV-P.5 MONNonlocal Parametric Down-Conversion inMulti-Mode Nonlinear Waveguide Arrays�F. Setzpfandt1,2, A.S. Solntsev1, T. Pertsch2, and A.A.Sukhorukov1; 1Nonlinear Physics Centre, Research School
of Physics and Engineering, Australian National Univer-sity, Canberra, Australia; 2Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-UniversitätJena, Jena, GermanyWe identify an e�ectively nonlocal regime of photon-pair generation outside of the pumped region throughspontaneous parametric down-conversion in coupledmulti-mode waveguides, creating new possibilities forquantum state control including dipole-like biphotonemission.
JSV-P.6 MONGenerating Telecom-Band Pure Heralded SinglePhotons On A Silica Chip�T. Hiemstra1, A. Eckstein1, U. Ho�2, J. Spring1, B.Metcalf1, P. Humphreys1, T. Bartley3,1, P.L. Mennea4,J.C. Gates4, P.G.R. Smith4, S. Kolthammer1, and I.A.Walmsley1; 1Clarendon Laboratory, University of Ox-ford, Oxford, United Kingdom; 2Department of Physics,Technical University of Denmark, Copenhagen, Denmark;3Applied Physics, University of Paderborn, Paderborn,Germany; 4Optoelectronics Research Centre, University ofSouthampton, Southampton, United KingdomWe present a source of pure heralded telecom-band sin-gle photons from spontaneous four wavemixing on a sil-ica chip capable of achieving high heralding e�ciency.We showmeasurements of photon correlations and two-photon joint spectra.
JSV-P.7 MONUV-written Silica Waveguide devices for IntegratedQuantum Optics�P.L. Mennea1, B.J. Metcalf2, J.B. Spring2, A.E. Lita3, B.Calkins3, P.C. Humphries2, T.J. Bartley3, T. Gerrits3, M.T.Posner1, J.C. Gates1, W.S. Kolthammer2, S.W. Nam3, I.A.Walmsley2, and P.G.R. Smith1; 1University of Southamp-ton, Southampton, United Kingdom; 2University of Ox-ford, Oxford, United Kingdom; 3National Institute ofStandards and Technology, Boulder, United StatesWe present details of the UV-written silica-on-siliconplatform for integrated quantum optics with referenceto recent results, and discuss the fabrication challengesinvolved in scaling to larger experiments.
JSV-P.8 MONBirefringent Optical Fibres and Laser WrittenWaveguides for Generation of Photon Pairs�W. McCutcheon1, A. McMillan1, B. Bell1, J. Rarity1, G.Corrielle2, and R. Osellame2; 1University of Bristol, Bris-tol, United Kingdom; 2Politecnio di Milano, Milan, ItalyPolarisation entangled photons based on four-wavemix-ing in birefringent �bre and birefringent laser-writtenwaveguides on chip.
JSV-P.9 MONIntegrating optics and alkali vapours on amicroscopic scale�R. Löw, H. Kübler, and T. Pfau; Universität Stuttgart,Stuttgart, GermanyWewill demonstrate three di�erent schemes to integrateAlkali vapours with various optical systems as a) SiN-waveguides, b) hollow core crystal �bres and c) electri-cally contacted vapour cells.
JSV-P.10 MONElectrically Injected Source of Photon Pairs at RoomTemperature: Device Performances andEntanglement Generation�C. Autebert1, F. Boitier1, Y. Halioua1, A. Lemaître2,I. Favero1, G. Leo1, and S. Ducci1; 1LaboratoireMatériaux et Phénomènes Quantiques Université ParisDiderot/CNRS, Paris, France; 2Laboratoire de Photoniqueet Nanostructures CNRS, Marcoussis, FranceWe present the performances of an electrically injectedAlGaAs source of photon pairs, as a function of tempera-ture and of the duty cycle of the injected current. We dis-cuss preliminary results on the generated entanglement.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b8:30 – 10:00CD-8: Nonlinear Phenomena IIChair: Concita Sibilia, La Sapienza Univer-sita’ di Roma, Roma, Italy
8:30 – 10:00EC-1: Quantum Gases ManipulationCorrelation and EntanglementChair: Ulrich Schneider, LMU München,Munich, Germany
8:30 – 10:00EB/EG: Polaritons and QuantumMemoriesChair: Elisabeth Giacobino, LaboratoireKastler-Brossel, Paris, France
8:30 – 10:00CM/LIM: Diagnostics and ControlChair: Marc Sentis, University of Aix Mar-seille, Marseille, France
8:30 – 10:00CF-1: Ultrafast FemtosecondAmpli�ersChair: Kjeld Eikema, University of Vrije, Am-sterdam,�e Netherlands
CD-8.1 TUE 8:30Phase-matched Second HarmonicGeneration in Lithium Niobate SlowLight Photonic Crystal Slab Waveguides�S. Saravi, S. Diziain, M. Zilk, F. Setzpfandt,and T. Pertsch; Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, GermanyWe theoretically investigate second har-monic generation with slow light and leakymodes in a lithium niobate photonic crystalwaveguide and identifymechanisms to engi-neer the phase-matching wavelength. Goodagreement between simulation and analyticsis achieved.
EC-1.1 TUE (Invited) 8:30Ultracold Fermions in PeriodicPotentials: a Bottom-Up Approach�S. Jochim; Universität Heidelberg, Heidel-berg, GermanyWe will present our technique to prepare �-nite samples of ultracold fermions in tightlyfocused optical potentials with very low en-tropy.
EB/EG.1 TUE (Tutorial) 8:30Cavity polaritons: from fundamentalphysics to non-linear and quantumdevices�J. Bloch; LPN/CNRS, Marcoussis, FranceSemiconductor microcavities operating inthe exciton-photon strong coupling regimeprovide a new platform to manipulate quan-tum �uid of lights in non-linear devices, andemulate complexHamiltonians using lithog-raphy and etching.
CM/LIM.1 TUE (Invited) 8:30Laser Process Monitoring and Control ofReal Process Features�S. Kaierle; Laser Zentrum Hannover e.V.,Hannve, GermanyLaser materials processing has already beenestablished for many years in industrial ap-plication, however processmonitoring is stillon its way. �is contribution describes thecurrent state-of-art and new developmentsin research of process monitoring.
CF-1.1 TUE 8:30Ultrastable and High-Power Yb:FiberAmpli�er Driving Optical ParametricAmpli�cation at High Repetition Rate�P. Storz, M. Wunram, D. Brida, and A. Leit-enstorfer; University of Konstanz, Konstanz,GermanyAn ultrastable Yb:�ber ampli�er, delivering145 fs pulses with 6 �J energy at 10MHz rep-etition rate, drives optical parametric ampli-�cation of broadband spectra provided bythe Er:�ber seed laser via highly nonlinear�bers.
CD-8.2 TUE 8:45Frequency Comb Generation inQuadratic Nonlinear MediaI. Ricciardi1, S. Mosca1, M. Parisi1, P.Maddaloni1, L. Santamaria1, P. De Natale2,and �M. De Rosa1; 1CNR-INO, IstitutoNazionale di Ottica, Pozzuoli (NA), Italy;2CNR-INO, Istituto Nazionale di Ottica,Firenze, ItalyWe experimentally demonstrate the onsetof optical frequency combs in a cw-pumpedcavity-enhanced second-harmonic-generation system. �e observed results arediscussed in view of a specially developeddynamical model.
CF-1.2 TUE 8:45Millijoule Picosecond Pulses at kHz repe-tition rates from a Ho:YLF RegenerativeAmpli�er Operating at 2.06 �m�L. von Grafenstein, M. Bock, U. Griebner,and T. Elsaesser; Max Born Institute, Berlin,GermanyWe report a cw-pumped picosecondHo:YLFregenerative ampli�er delivering 2 mJ pulsesat 1 kHz. �e laser source emitting at 2060nm is broadband seeded and implementedin a chirped pulse ampli�cation system.
CD-8.3 TUE 9:00Optimal conversion in the depleted stageof modulation instability�A. Bendahmane1, A. Mussot1, A.Kudlinski1, P. Szri�giser1, M. Conforti1, S.Wabnitz2, and S. Trillo3; 1Université Lille 1,Villeneuve d’ascq, France; 2Universita deglistudi di Brescia, and INO-CNR, Brescia,Italy; 3Universita di Ferrara, Ferrara, ItalyWe report the �rst experimental measure-ment of pump depletion in the nonlinearregime of modulation instability process. Amaximum conversion of 95 % is obtainedvery close to the theoretically predicated fre-quency.
EC-1.2 TUE 9:00Local Probing of a Fermionic MottInsulator�M. Koschorreck1, L. Miller1,2, E. Cocchi1,2,J. Drewes1, D. Pertot1, F. Brennecke1, and M.Köhl1,2; 1Physikalisches Institut, Universityof Bonn, Bonn, Germany; 2Cavendish Labo-ratory, University of Cambridge, Cambridge,United KingdomWe produce and characterize two-dimensional Fermionic Mott-insulatingstates by performing in-situ imaging com-bined with radio-frequency spectroscopy.We measure density distributions for single-and double-occupancies, make detailed
CM/LIM.2 TUE (Invited) 9:00Control of Femtosecond Pulsed LaserDeposition by Temporal Pulse Shaping�F. Garrelie1,2, F. Bourquard1,2, A.-S. Loir1,2,and C. Donnet1,2; 1Université de Lyon, Lyon,France; 2Université de Saint-Étienne, Labora-toire Hubert Curien, Saint-Etienne, France�e temporal laser pulse shaping is shownto strongly modify the laser-induced plasmacomposition and kinetics, giving the possi-bility to an adaptive control of Pulsed Laserdeposition of thin �lms.
CF-1.3 TUE 9:00�ird-generation femtosecond technology�H. Fattahi1,2, N. Karpowicz1, T. Metzger3,and F. Krausz1,2; 1MPI für Quantenoptik,Garching, Germany; 2Department für Physik,Ludwig-Maximilians-Universität München,Muenchen, Germany; 3TRUMPF Scienti�cLasers GmbH + Co. KG, Muenchen, Ger-manyWe demonstrate a design study and prelimi-nary results of a 3-channel OPCPA system,generating ultrashort pulses with terawattpeak and sub-kilowatt average powers. Co-herent synthesis of the channels is predictedto produce intense, sub-cycle transients.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN8:30 – 10:00CK-7: Photonics IntegrationChair: Stefano Pelli, Istituto di Fisica Appli-cata Nello Carrara, Firenze, Italy
8:30 – 10:00CA-8: Visible Solid-state LasersChair: Christian Kränkel, Institut für Laser-Physik, Universität Hamburg, Hamburg, Ger-many
8:30 – 10:00CB-1: New Frontiers inSemiconductor LasersChair: Erwin Bente, Technische UniversiteitEindhoven, Eindhoven,�e Netherlands
8:30 – 10:00EF-7: Nonlinear Behaviour of Lightin Waveguides and PhotonicLatticesChair: Rachel Grange, ETH, Zürich, Switzer-land
8:30 – 10:00CC-6: Ultrafast THz Generationand DetectionChair: Christoph Peter Hauri, Paul-ScherrerInstitut, Villigen, Switzerland
CK-7.1 TUE (Invited) 8:30InP-Based Generic Photonic Integration -Capabilities and Limitations�F. Soares1, M. Baier1, T. Gaertner1, W.Passenberg1, J. Decobert2, J.-L. Gentner2,M. Achouche2, M. Möhrle1, and N. Grote1;1Fraunhofer Heinrich-Hertz Institute, Berlin,Germany; 2III-V Lab, Marcoussis, FranceA generic PIC foundry process based on InPtechnology is described that can integrate alarge variety of photonic devices and opticalfunctionalities for various applications usinga single fabrication process and layerstack.
CA-8.1 TUE 8:30Power Scaling of InGaN-Blue-LD pumpedPr3+:YLF Laser and Passive Q-switching�K. Iijima, R. Kariyama, H. Tanaka, K. Hiro-sawa, and F. Kannari; Keio University, Yoko-hama, JapanA 2.9 W cw 640 nm Pr3+:YLF laser consist-ing of two laser crystals pumped by two 3.5W InGaN-LDs for each was demonstrated.Laser output powers with passive and activeQ-switching were also scaled up.
CB-1.1 TUE (Invited) 8:30Electrically driven exciton-polaritonlasers�S. Hö�ing1,2, C. Schneider1, A. Rahimi-Iman1, N.Y. Kim3,4, J. Fischer1, I.Savenko5,6, M. Amthor1, M. Lermer1,A. Wolf1, L. Worschech1, V. Kulakovskii7, I.Shelykh5,6, M. Kamp1, S. Reitzenstein1,8, Y.Yamamoto3,9, and A. Forchel1; 1UniversitätWürzburg, Würzburg, Germany; 2Universityof St Andrews, St Andrews, United Kingdom;3Stanford University, Stanford, UnitedStates; 4University of Tokyo, Tokyo, Japan;5University of Iceland, Reykjavik, Ice-land; 6Nanyang Technological University,Singapore, Singapore; 7Russian Academyof Science, Chenrnogolovka, Russia;8Technische Universität Berlin, Berlin,Germany; 9National Institute of Informatics,Tokyo, JapanWe report exciton-polariton laser opera-tion under electrical pumping. �e hybridlight-matter nature of this lasing system isprobed by measuring the exciton-polaritonZeeman-splitting, which clearly reveals thatthis laser remains in the strong couplingregime.
EF-7.1 TUE (Invited) 8:30Nonlinear Interactions in HighlyDispersive Nanostructured LithiumNiobate�T. Pertsch; Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, GermanyCombined with new nanofabrication meth-ods lithium niobate proves to be a versatileplatform for highly integrated e�cient non-linear optics. We demonstrate several ge-ometries and application example rangingfrom simple nanowires to sophisticated pho-tonic crystal cavities.
CC-6.1 TUE 8:30Cherenkov-Type Electro-Optic Samplingof Terahertz Waves in a GaAs Crystal�E. Mashkovich1, A. Shugurov1, M. Tani2,and M. Bakunov1; 1University of NizhnyNovgorod, Nizhny Novgorod, Russia;2Research Center for Development of Far-Infrared Region, University of Fukui, Fukui,JapanWe report on a theoretical analysis andexperimental study of the Cherenkov-type(non-collinear) scheme for e�cient electro-optic sampling detection of terahertz pulseswith a thick GaAs crystal and practicallyconvenient �ber laser.
CA-8.2 TUE 8:45Rare Earth Doped Oxides for Visible LaerOperation�D.-T. Marzahl1, P.W. Metz1, T. Calmano1,2,F. Reichert3, C. Kränkel1,2, and G. Huber1,2;1Institut für Laser-Physik, Universität Ham-burg, Hamburg, Germany; 2�e HamburgCentre for Ultrafast Imaging, UniversitätHamburg, Hamburg, Germany; 3Centre forFree-Electron Laser Science, Hamburg, Ger-manyWe report on our latest results on rare earthdoped oxide crystals for visible laser opera-tion and present to the best of our knowledgethe �rst Sm3+-based waveguide laser.
CC-6.2 TUE 8:45Asymmetric Cherenkov Radiation forImproving Terahertz Emission from theSi-prism-coupled LiNbO3 layer�M. Bakunov, E. Mashkovich, and E. Svink-ina; University of Nizhny Novgorod, NizhnyNovgorod, RussiaAsymmetric Cherenkov emission of tera-hertz waves from a femtosecond opticalpulse propagating in LiNbO3 is demon-strated. �is e�ect is proposed for improv-ing the spectral characteristics of the e�-cient optical-to-terahertz converter: the Si-prism-coupled LiNbO3 layer.
CK-7.2 TUE 9:00Angled MMI CWDM structure onGermanium on Silicon�J. Soler Penades1, Y. Hu1, M. Nedeljkovic1,C.G. Littlejohns1, A.Z. Khokhar1, C.J.Mitchell1, S. Stankovic1, G. Roelkens2,F.Y. Gardes1, and G.Z. Mashanovich1;1Optoelectronics Research Centre, Universityof Southampton, Southampton, UnitedKingdom; 2Department of InformationTechnology, Universiteit Gent,, Gent,BelgiumWe present the �rst mid-infrared an-gled multimode interferometer in thegermanium-on-silicon platform at the
CA-8.3 TUE (Invited) 9:00Wavelength Tuning of Diode-PumpedPr3+-Lasers�P.W. Metz1, D.-T. Marzahl1, C. Kränkel1,2,and G. Huber1,2; 1Institut für Laser-Physik,Universität Hamburg, Hamburg, Germany;2�e Hamburg Centre for Ultrafast Imaging,Universität Hamburg, Hamburg, GermanyWe review the state-of-the-art of Pr3+-dopedlasers at di�erent transitions in the visi-ble and in wavelength tuning experiments.Slope e�ciencies around 60% and a to-tal tuning range exceeding 100 nm wereachieved.
CB-1.2 TUE 9:00Emission dynamics in supersymmetriclaser arrays�R. El-Ganainy1, D. Christodoulides2, andL. Ge3; 1Department of Physics, MichiganTechnological University, Houghton, UnitedStates; 2College of Optics and Photonics(CREOL), University of Central Florida, Or-lando, United States; 3College of Staten Is-land, CUNY, Staten Island, New York, UnitedStatesDespite their potential applications, con-trolling the emission characteristics of highpower laser arrays remains a hurdle. Herewe present the concept of supersymmetric
EF-7.2 TUE 9:00Continuous solitons in a latticenonlinearity�D. Pierangeli1, M. Flammini1, F. Di Mei1,J. Parravicini1, C.E.M. de Oliveira2, A.J.Agranat2, and E.DelRe1; 1University of RomeLa Sapienza, Rome, Italy; 2Applied PhysicsDepartment, HebrewUniversity of Jerusalem,Jerusalem, IsraelWe study the optical solitons in a lattice non-linearity, a periodic pattern that both a�ectsand is strongly a�ected by the wave. Re-sults demonstrate continuous solitons form-ing out of the compensation of di�ractionand of the underlying periodic pattern.
CC-6.3 TUE 9:00Highly precise and accurate terahertzpolarization measurement by usingphotoelastic modulation�N. Nemoto1, T. Higuchi2, N. Kanda3,4, K.Konishi5, K. Yoshioka1, and M. Kuwata-Gonokami1,4,5; 1Dep. of Physics, �eUniversity of Tokyo, Tokyo, Japan; 2Dep.of Physics, Friedrich-Alexander UniversityErlangen-Nuremberg, Erlangen, Germany;3Laser Technology Laboratory, RIKEN,Saitama, Japan; 4Photon Science Center, �eUniversity of Tokyo, Tokyo, Japan; 5Institutefor Photon Science and Technology, �eUniversity of Tokyo, Tokyo, Japan
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b
comparison to HTSE and extract theequation of state.
CD-8.4 TUE 9:15Double-Stage Spectral Broadening inBulk Crystals of 50W, 1.3 �J, 250-fs pulsesto a Fourier transform limit of 15 fs�M. Seidel1, J. Brons1, V. Pervak2, A.Apolonski1,2, O. Pronin1, and F. Krausz1,2;1Max-Planck-Institut für Quantenoptik,Garching, Germany; 2Ludwig-Maximilians-Universität München, Garching, GermanySpectral broadening of 1.3-�J, 250-fs pulsesin a quartz crystal is presented. A transformlimit of 30-fs and pulse compression to 53-fswas achieved. A second bulk stage broaden-ing reduced the transform limit to 15-fs.
EC-1.3 TUE 9:15First realization of a chromium dipolarFermi seaB. Naylor1,2, A. Reigue1,2, E. Maréchal2,1,B. Laburthe-Tolra2,1, L. Vernac1,2, and �O.Gorceix1,2; 1Laboratoire de Physique desLasers, Université Paris 13, Sorbonne ParisCité, Villetaneuse, France; 2Laboratoire dePhysique des Lasers, CNRS, UMR7538, Vil-letaneuse, FranceWe report on the �rst creation of a degener-ate dipolar Fermi gas made of strongly mag-netic chromium atoms. �is system fea-turing long-range interactions constitutes apromising platform to tackle various quan-tum many-body phenomena.
CF-1.4 TUE 9:15Coherent synthesis from independentfemtosecond Yb-�ber lasers�H. Tian, Y. Song, P. Qin, M. Hu, andC. Wang; Ultrafast Laser Laboratory, KeyLaboratory of Opto-electronic InformationTechnical Science of Ministry of Education,School of Precision Instruments and Opto-electronics Engineering, Tianjin University,Tianjin, China, People’s Republic of (PRC)We phase-coherently stabilize two indepen-dent femtosecond Yb-doped �ber lasers to arecord-breaking residual relative timing andcarrier envelope phase jitter of 380 as and450 mrad, respectively.
CD-8.5 TUE 9:30Optically Switchable GalliumMetasurfaces�R.F. Waters1, K.F. MacDonald1, P.A.Hobson2, and N.I. Zheludev1,3; 1Universityof Southampton, Southampton, UnitedKingdom; 2QinetiQ Ltd., Farnborough,United Kingdom; 3Nanyang TechnologicalUniversity, Singapore, SingaporeReversible, optically-driven nanoscale sur-facemetallisation of elemental gallium in thebackplane of a photonic metamaterial ab-sorber provides a mechanism for a strong,resonantly enhanced re�ective optical non-linearity at �W/�m2 intensities.
EC-1.4 TUE 9:30Generation of long-range entanglementin a macroscopic spin singlet�R.J. Sewell1, N. Behbood1, G. Colangelo1,F. Martin Ciurana1, G. Tóth2,3,4, andM.W. Mitchell1,5; 1ICFO-Institut deCiencies Fotoniques, Castelldefels, Spain;2Department of �eoretical Physics, Univer-sity of the Basque Country, Bilbao, Spain;3IKERBASQUE, Basque Foundation forScience, Bilbao, Spain; 4Wigner ResearchCentre for Physics, Hungarian Academyof Sciences, Budapest, Hungary; 5ICREA- Institució Catalana de Recerca i EstudisAvançats, Bilbao, SpainWe report the generation and detection oflong-range entanglement macroscopic spinsinglet (MSS) via quantum non-demolition(QND) measurement of cold atomic spinsusing a novel spin noise spectroscopy tech-nique.
EB/EG.2 TUE 9:30Controlled rephasing of single collectivespin excitations in a cold atomic ensemblefor temporally multiplexed quantummemories�G. Heinze1, B. Albrecht1, P. Farrera1, M.Cristiani1, and H. de Riedmatten1,2; 1ICFO-�e Institute of Photonic Sciences, Castellde-fels (Barcelona), Spain; 2ICREA-InstitucióCatalana de Recerca i Estudis Avançats,Barcelona, SpainWe demonstrate active control of single col-lective spin excitations in a cold atomicquantum memory via externally inducedinhomogeneous broadening of spin transi-tions. �e creation of time-separated spin-waves with selective readout is shown.
CM/LIM.3 TUE (Invited) 9:30Ship-in-a-bottle Fabrication of FunctionalBiochips by Hybrid Femtosecond LaserProcessing�K. Sugioka, J. Xu, F. Sima, D.Wu, andK.Mi-dorikawa; RIKEN Center for Advanced Pho-tonics, Wako, JapanWe propose a new method termed hybridfemtosecond laser processing which com-bines subtractive 3D glass micromachin-ing with additive two-photon polymeriza-tion for realizing 3D functional biochips. Bi-ological applications of fabricated biochipsare demonstrated.
CF-1.5 TUE 9:30A broadband tunable dual-wavelengthmid-infrared optical parametric oscillatorand its applications�Y. Jin, S. Cristescu, F. Harren, and J.Mandon; Life Science Trace Gas Facility,Molecular and Laser Physics, Institute forMolecules and Materials, Radboud Univer-sity, Nijmegen,�e NetherlandsWe present a broadband tunable dual-wavelength mid-infrared optical parametricoscillator. �e single cavity is capable of gen-erating two idlers that are separated up to 30THz, o�ering an opportunity for a variety ofapplications.
CD-8.6 TUE 9:45Enhanced two-photon-absorption usingsub-wavelength antennasB. Vest1, �B. Portier2, F. Pardo2, N. Péré-Laperne2, E. Steveler2, J. Jaeck1, C. Dupuis2,N. Bardou2, A. Lemaître2, E. Rosencher1, R.Haïdar1, and J.-L. Pelouard2; 1ONERA -�eFrench Aerospace lab, PALAISEAU, France;
EC-1.5 TUE 9:45E�cient Collisional Blockade Loading ofSingle Atoms in Tight Optical Microtraps�Y.H. Fung andM.Andersen; JackDoddCen-ter for Quantum Technology, Department ofPhysics, University of Otago, Dunedin, NewZealandWe experimentally observe ∼ 80% e�-
EB/EG.3 TUE 9:45A Nano�ber-based Memory for Light�B. Gouraud, D. Maxein, A. Nicolas, O.Morin, and J. Laurat; Laboratoire KastlerBrossel, UPMC-Sorbonne Universités, CNRS,ENS-PSL Research University, Collège deFrance, Paris, FranceWe report the single-photon-level storage of
CF-1.6 TUE 9:45CEO Frequency of Sychronously PumpedDoubly Resonant OPOs�C. Wan1,2, P. Li1, A. Chong1,2, A. Ruehl1,and I. Hartl1; 1DESY, Hamburg, Germany;2Univ. Dayton, Dayton, United StatesWe present a detailed study of the CEO fre-quencies of a doubly resonant synchronously
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN
wavelength of 3.8�m. �e �ve-channeldevices had 3dB insertion loss, -10dBcrosstalk and 20nm channel spacing.
(SUSY) laser arrays that can provide solutionto this problem.
We developed a method for highly preciseand accurate terahertz polarization mea-surement by using photoelastic modulationin electro-optic sampling. We achieved aprecision of 0.1 mrad which realizes sensi-tive detection of chiral molecules.
CK-7.3 TUE 9:15Photonic crystal SOI-PIC for integratedmicrowave photonics �lters�J. Bourderionnet1, S. Combrié1, Z. Han2,X. Chécoury2, and A. De Rossi1; 1�alesResearch & Technology, Palaiseau, France;2Institut d’Electronique Fondamentale (IEF),Orsay, FranceSilicon on Insulator 2-tap unit-cell is pro-posed for implementation in �lter architec-tures. �e structure includes electricallytunable photonic crystal directional couplerand delay line. Simultaneous control of am-plitude, optical phase, and group delay isdemonstrated.
CB-1.3 TUE 9:15Laser generation of coherent photon statecarrying orbital angular momentum withcharge and handedness control using�at-photonics�S. Mohamed. Seghir1, S. Mohamed1,M. Mikhaël1, L. Luc2, S. Isabelle2, B.Grégoire2, L. Philippe3, and G. Arnaud1;1Institut d’Electronique du sud,CNRS-UMR5214, Université Montpellier, Montpellier,France; 2Laboratoire de Photonique et deNanostructures, CNRS-UPR 20, Marcoussis,France; 3Laboratoire Photonique, Numériqueet Nanoscience, CNRS-UMR5298, Institutd’Optique d’Aquitaine, Talence, FranceIn this work we show direct laser genera-tion of highly coherent laser beam carryingOrbital angular momentum with controlledcharge |m| and handedness, using compactvertical external cavity surface emitting laserwith integrated �at-photonics element
EF-7.3 TUE 9:15Demonstration of an Optical EventHorizon in a Silicon NanophotonicWaveguide�C. Ciret1, F. Leo1,2,3, B. Kuykens2,3, G.Roelkens2,3, and S.-P. Gorza1; 1OPERA-Photonique, Université libre de Bruxelles(ULB), Bruxelles, Belgium; 2Photonics Re-search Group, Department of InformationTechnology, Ghent University-IMEC, Ghent,Belgium; 3Center for Nano- and Biophoton-ics (NB-photonics), Ghent, BelgiumWe experimentally demonstrate the �rst op-tical analog of an event horizon in integratedphotonic nonlinear structures, through there�exion of a continuous wave around 1550nm on an intense pulse at 1940 nm.
CC-6.4 TUE 9:15Contact grating device with Fabry-Perotresonator for e�ective THz lightgeneration�M. Tsubouchi, K. Nagashima, F. Yoshida, Y.Ochi, and M. Maruyama; Japan Atomic En-ergy Agency, Kyoto, JapanTo realize a contact grating device for high-power THz light generation, we proposedand demonstrated a novel design in whichwe deposited multilayers on a LiNbO3 sub-strate and fabricated a grating on the outer-most layer.
CK-7.4 TUE 9:30Segmentation of waveguide arrays fordiscrete photonics: Di�ractionmanagement in coupled waveguides or ina photonic crystal ?�N. Belabas Plougonven1, A. Pénillard1,R. Negru1, S. Guilet1, L. Legratiet1, E.Cambril1, C. Minot1,2, and J.-M. Moison1;1C.N.R.S, Laboratory of Photonic andNanostructures, Marcoussis, France;2Institut Mines-Telecom/Telecom ParisTech,Paris, FranceWe derive an analytical di�raction relationand a numerical angular signature in seg-mented waveguide arrays. Our 2D e�ectiveindex model matches our experiments andconnects the photonic crystal picture withthe di�raction management approach.
CA-8.4 TUE 9:30Yellow-Orange Emission from aPlane-Plane Monolithic Diamond RamanLaser�V. Savitski, S. Reilly, and A. Kemp; Instituteof Photonics, Department of Physics, Univer-sity of Strathclyde, Glasgow, United KingdomA compact and alignment free plane-planemonolithic diamond Raman laser for greento yellow-orange wavelength conversionwith 59% e�ciency is demonstrated. Ramangain-guiding is suggested as the main mech-anism responsible for laser mode stabilisa-tion.
CB-1.4 TUE (Invited) 9:30GeSn as gain material for infrared groupIV laser devices�S. Wirths1, R. Geiger2,3, N. von denDriesch1, G. Mussler1, Z. Ikonic4, J.-M. Hartmann5, J. Faist3, S. Mantl1, D.Grützmacher1, H. Sigg2, and D. Buca1;1Peter Grünberg Inst. 9 and JARA-Funda-mentals of Future Information Technology,Forschungszentrum Jülich, Jülich, Germany;2Laboratory for Micro- and Nanotechnology,Paul Scherrer Institute, Villigen, Switzerland;3Inst. for Quantum Electronics, ETH Zürich,Zürich, Switzerland; 4Inst. of Microwavesand Photonics, School of Electronic andElectrical Engineering, University of Leeds,Leeds, United Kingdom; 5Univ. of GrenobleAlpes & CEA, Leti, MINATEC Campus,Grenoble, FranceWe present photoluminescence, gain andlasing results on direct bandgap groupIV GeSn alloys. An optically pumpedGe0.875Sn0.125 laser on Si(001) is realizedat 90 K with an emission wavelength around2250 nm.
EF-7.4 TUE 9:30Optical analogue of neutrino oscillationsin binary waveguide arrays�A. Marini1, S. Longhi2, and F.Biancalana3,4; 1ICFO-Institut de Cien-cies Fotoniques, Castelldefels, Spain;2Dipartimento di Fisica, Politecnico diMilano, and IFN-CNR, Milano, Italy; 3MaxPlanck Institute for the Science of Light,Erlangen, Germany; 4School of Engineering& Physical Sciences, Heriot-Watt University,Edinburgh, United KingdomWe theoretically investigate the optical ana-logue of neutrino oscillation in a pair ofvertically displaced binary waveguide arrayswith longitudinally modulated e�ective in-dex. We demonstrate that neutrino oscilla-tions can be quenched by nonlinear e�ects.
CC-6.5 TUE 9:30Micro-Slit Assisted Coherent BroadbandTerahertz Detection�M.Clerici1,2, S.-P. Ho1,3, A.Mazhorova1, M.Peccianti4, A. Pasquazi4, L. Razzari1, J. Ali3,and R. Morandotti1; 1INRS-EMT, Varennes,Canada; 2School of Engineering and PhysicalSciences, Heriot-Watt University, Edinburgh,United Kingdom; 3Nanophotonics ResearchAlliance, Universiti Teknologi Malaysia, Jo-hor, Malaysia; 4Department of Physics andAstronomy, University of Sussex, Brighton,United KingdomWe show a way to miniaturize ultra-broadband Terahertz detection relying onfour-wave mixing in a chip where the non-linear interaction occurs in a few micronthick glass, biased through deposited goldelectrodes.
CK-7.5 TUE 9:45All integrated Lithium Niobate StandingWave Fourier Transform Spectrometer toimprove sampling resolutionF. �omas1, S. Heidmann1, M. de Mengin1,N. Courjal2, G. Ulliac2, A. Morand3, P.Benech3, P. Kern1, E. Le Coarer1, and�G. Martin1; 1IPAG, Grenoble, France;
CA-8.5 TUE 9:45Spectroscopic Study and Laser Operationof Eu:KY(WO4)2 Monoclinic Crystal at703 nm�P. Loiko1, V. Dashkevich2, V. Orlovich2,A. Bui2, S. Bagaev3, K. Yumashev1, A.Yasukevich1, N. Kuleshov1, S. Vatnik3, andA.Pavlyuk4; 1Center for Optical Materials and
EF-7.5 TUE 9:45Fast light self-trapping in isolatedLiNbO3 slab waveguide by pyroelectrice�ect�M. Chauvet, F. Bassignot, F. Henrot, F. De-vaux, and L. Gauthier-manuel; FEMTO-ST,Besançon, FranceBeam self-trapping by pyroelectric e�ect is
CC-6.6 TUE 9:45Terahertz homodyne self-mixing and itsapplication to two-dimensionaltomographic terahertz imaging�T. Mohr1, S. Breuer1, D. Blömer1, M.Simonetta2, S. Patel1, M. Schlosser1, A.Deninger3, G. Birkl1, G. Giuliani4, and W.Elsäßer1,5; 1Institute for Applied Physics,
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b2Laboratoire de Photonique et de Nanostruc-tures (LPN-CNRS), Marcoussis, FranceWe investigate the performances of a metal-lic nanostructure enhancing two-photon ab-sorption in a thin GaAs p-i-n junction. Atwo orders of magnitude gain due to �eldcon�nement at 1.47 um has been observed.
ciency of collisional blockade loading of sin-gle atoms in a tight optical microtrap by in-ducing controlled inelastic light-assisted col-lisions during loading.
light tightly guided in an optical nano�ber.Our setup is based on electromagneticallyinduced transparency for atoms interactingwith the evanescent �eld surrounding thenano�ber.
pumped OPO over oscillating cavity res-onances transitioning from degenerate tonon-degenerate regime.
ROOM 110:30 – 12:30PL-4: EQEC 2015 Plenary Talk and AwardsCeremonyChair: Jürgen Eschner, Universität des Saarlandes, Saar-brücken, Germany
�is session will feature a plenary talk presented bySerge Haroche, Collège de France, Laboratoire KastlerBrossel, & Ecole Normale Supérieure, Paris, France to-gether with a series of Prize and Award Ceremonies asdescribed hereunder:
PL-4.1 TUE (Plenary)Real and Arti�cial Atoms Interacting with Photons:From Fundamental Physics to Quantum Information�S. Haroche; Collège de France, Laboratoire KastlerBrossel, Paris, FranceFundamental tests of quantum physics have been real-izedwith Rydberg atoms or arti�cial two-level Josephsoncircuits coupled to microwave or radiofrequency pho-tons stored in a high Q cavity, opening promising per-spectives for quantum information processing.
Prize and Award CeremoniesEPS-QEOD and EPS Young Minds 2015Travel Grant Student Awards:For the International Year of Light, the Quantum Elec-tronics and Optics Division and Young Minds ActionCommittee of the European Physical Society o�eredten travel grants for PhD Students wishing to attendCLEO®/Europe-EQEC 2015.�e Selection Committee of the EPS-QEOD TravelGrant Student Awards composed by EPS-QEOD Boardmembers and EPS Young Minds members are happy toannounce the names of the laureates and the title of theircontribution to the conference:Jonas Nils Becker, All-Optical Formation of CoherentDark States in Single Silicon-Vacancy Color Centers in Di-amondFrancesco Cappelli,Quantum limited frequency noise ofa quantum cascade laser frequency combMamoru Endo, 15-GHz, Kerr-Lens Mode-Locked Laserand Fourier Synthesis of Each Comb ToothDordaneh Etezadi, Accessible Near�elds via PlasmonicNanoantennas on Nanopedestals for Ultra-Sensitive Vi-brational IR-SpectroscopyXavier Fernandez Gonzalvo, Frequency Up-ConversionofMicrowave Photons to the Telecommunications Band inan Er:YSO CrystalMatin Hallaji, How a Single Photon Can Act Like ManyPhotonsChih-Hsuan Lu, Generation of Intense Supercontinuumin Condensed Media
Martin Ringbauer, Measurements on the reality of thewavefunctionAntoine F. J Runge, Soliton explosions in a passivelymode-locked �ber laser
2015 Awards of the European Physical Society– Quantum Electronics and Optics Division:
(2) Quantum Electronics Prizes�e 2015 Prize for fundamental aspects of QuantumElectronics and Optics is awarded to Sir John Pendry,Professor of theoretical solid-state physics at Imperial Col-lege London, United Kingdom. �e Prize is awarded toProfessor Pendry for helping formulate rules on how toincorporate di�erent kinds of materials with nanoscalestructures to form larger scale metamaterials with excit-ing new optical properties not seen in nature.�e 2015 Prize for applied aspects of Quantum Electron-ics and Optics is awarded to Professor Bahram Javidi,Professor at the University of Connecticut, USA.�e Prizeis awarded to Professor Javidi for pioneering contribu-tions to information optics, including 3D imaging, 3Ddisplays, and 3D imaging of photon starved scenes.
(2) Fresnel Prizes�e 2015 Fresnel Prize for fundamental aspects isawarded to Tim Hugo Taminiau, Del� University ofTechnology, Del�, �e Netherlands, for his fundamentalcontributions to nano-optics and quantum informationscience through the control of solid-state quantum emit-ters and spins.
�e 2015 Fresnel Prize for applied aspects is awardedto Daniele Brida, University of Konstanz, Konstanz,Germany, for the development of broadly tunable few-optical-cycle laser sources and their application in the in-vestigation of primary photo-induced processes in con-densed matter systems.
(4) PhD Thesis Prizes�e 2015 �esis Prize for fundamental aspects isawarded to Tim Langen, JILA, University of Coloradoand NIST, Boulder, CO, USA, for his work on non-equilibrium dynamics of one-dimensional Bose gases.�e 2015 �esis Prize for fundamental aspects isawarded to Søren Raza, Centre for Nano Optics at theUniversity of Southern Denmark (SDU), Lyngby, Den-mark, for his work on probing plasmonic nanostructureswith electron energy-loss spectroscopy (EELS).�e 2015 �esis Prize for applied aspects is awarded toTobias Herr, Swiss Center for Electronics and Microtech-nology (CSEM), Time and Frequency Division, Neuchâtel,Switzerland, for his work on solitons and dynamics offrequency comb formation in optical microresonators.�e 2015 �esis Prize for applied aspects is awarded toPete Shadbolt, Quantum Optics & Laser Science Group,Faculty of Natural Sciences, Imperial College, London,United Kingdom, for his work on complexity and controlin quantum photonics.See EPS-QEOD Prize Ceremony brochure.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN2FEMTO-ST, Besancon, France; 3IMEP-LAHC, Grenoble, FranceWe present an all integrated electro-opticFourier transform spectrometer, allowinghigh resolution spectroscopy in the near andmid-IR, using a Y-junction together with aLippmann interferometer, all realized in thesame lithium niobate channel waveguide.
Technologies, Belarusian National TechnicalUniversity, Minsk, Belarus; 2B.I. Stepanov In-stitute of Physics, National Academy of Sci-ences of Belarus, Minsk, Belarus; 3Instituteof Laser Physics, Siberian Branch of RAS,Novosibirsk, Russia; 4A.V. Nikolaev Institutefor Inorganic Chemistry, Siberian Branch ofRAS, Novosibirsk, RussiaAbsorption and stimulated-emissioncross-section spectra are evaluated forEu:KY(WO4)2 crystal; together with aJudd-Ofelt analysis. Quasi-CW and trueCW deep-red (703 nm) lasers are realizedbased on this monoclinic crystal.
reported in a LiNbO3 �lm. �e underly-ing physics speci�c to this arrangement isespecially characterized by a response timeorders of magnitude faster than in bulkLiNbO3
Technische Universität Darmstadt, Darm-stadt, Germany; 2Istituto Nazionale di FisicaNucleare, Sezione di Pavia, Pavia, Italy;3Toptica Photonics AG, Gräfeling, Germany;4Dipartimento di Ingegneria Civile e Ar-chitettura, Università di Pavia, Pavia, Italy;5Center of Smart Interfaces, Technische Uni-versität Darmstadt, Darmstadt, GermanyA novel homodyne self-mixing terahertzconcept is experimentally demonstrated, inwhich a single photoconductive antennaserves simultaneously as transmitter and re-ceiver for cw-terahertz radiation. As a proof-of-principle application, 2D tomographicterahertz imaging is realized.
ROOM 1
IUPAP Commission 17 - Laser Physics andPhotonics biennial Young Scientists Prizes2015:Two prizes are being awarded. One prize is for outstand-ing contributions of a fundamental nature. �e other isfor outstanding contributions of an applied nature. �ewinners have demonstrated signi�cant achievement, andexceptional promise for future achievement in the areasof laser physics and/or photonics in which they research.�e current Chair of the Commission, Professor DebKane, Dept. of Physics and Astronomy, MacquarieUniversity, Sydney, Australia, will award the Prizes atCLEO®/Europe-EQEC 2015.�e IUPAP C17 Laser Physics and Photonics “Funda-mental Aspects” Young Scientist Prize is awarded to DrRobert Fickler, Institute for Quantum Optics and Quan-tum Information, University of Vienna, Austria. Dr. Fick-ler is awarded the prize “for his ground breaking con-tributions to the entanglement of complex structures ofphotons, which have opened up new avenues for quan-tum communication”.�e IUPAP C17 Laser Physics and Photonics “AppliedAspects” Young Scientist Prize, has been awarded to DrMark �ompson, Centre for Quantum Photonics, Uni-versity of Bristol, United Kingdom. DrMark�ompson isawarded the prize “for his contributions to the new andemerging �eld of quantum photonics, and particularlyfor his pioneering work in integrated quantum photoniccircuits”.
Announcement of the LIGHT2015 Awards:�e European Optical Society and the LIGHT2015project will announce the winners for the LIGHT2015Young Photonics Entrepreneur Award and the LIGHT2015Young Women in Photonics Awards. �e Award Cer-emony will take place on Wednesday 24 June, 16:00 –16:20, Room 2.
OSA Robert E. Hopkins Leadership Award:�e Robert E. Hopkins Leadership Award of �e Opti-cal Society recognizes an individual or group who hashad a signi�cant impact on the global optics and photon-ics community or an individual or group from the opticsand photonics community who has had a signi�cant im-pact on society as a whole stemming from non-researchoriented activities. With perfect timing, OSA PresidentPhilip Russell will present the 2015 Award to John M.Dudley, University of Franche-Comté, Besançon, France,for his tireless support over many years of internationalcollaboration in science, in particular his remarkablesuccess in almost single-handedly creating the 2015 UN-ESCO International Year of Light.John Dudley’s research covers various topics in ultrafastand nonlinear optics and he has worked in New Zealandand Scotland and is currently Distinguished Professor atthe University of Franche-Comté in France where he di-rects a research group in optoelectronics and photonicswithin the CNRS Institute FEMTO-ST. He is a Fellow ofOSA, the IEEE, and the European Optical Society, andhas served as President of the European Physical Societyfrom April 2013-2015. He is Chair of the InternationalYear of Light 2015 Steering Committee.
OSA Fellow Member Recognition:OSA Fellows will be recognized during the Awards Cer-emony of CLEO®/Europe-EQEC 2015.
OSA Fellow Members to be recognized:
Alberto Bramati, Université Pierre et Marie Curie,France, for outstanding contributions to the �eld ofquantumoptics and quantum �uid properties of exciton-polaritons in microcavity semiconductors, with thedemonstration of squeezing, super�uid �ow, solitonsand quantized vortices.Jean-Jacques Gre�et, Institut d’Optique, France, for the-oretical and experimental work on the role of surfacewaves in radiative heat transfer at nanoscale and emis-sion of radiation, including achievements of large spatialcoherence in thermal radiation leading to a new class ofradiation emitters.R. J. Dwayne Miller,Max Planck Institute for the Struc-ture and Dynamics of Matter, Germany, for ground-breaking development of ultrabright femtosecond elec-tron sources for probing atomic motions on the primarytimescales governing chemistry.�omas Pertsch, Friedrich-Schiller-Universität Jena,Germany, for groundbreaking contributions to spatio-temporal nonlinear dynamics in discrete optics, for theobservation of light bullets, and for seminal contribu-tions to metamaterial science and nanophotonics.
OSA/DPGHerbert Walther Award:�e Optical Society (OSA) and the Deutsche Physikalis-che Gesellscha� (DPG) will present the 2015 HerbertWalther Award to Peter E. Toschek, Institut für Laser-Physik, Universität Hamburg, Germany. �e Award hon-ours Herbert Walther for the seminal in�uence of hisground-breaking innovations in quantum optics andatomic physics, and for his wide-ranging contributionsto the international scienti�c community. �is year, Pe-ter Toschek will be honoured for his pioneering exper-iments to laser cooling and trapping of single ions, hiscontributions to the understanding of principles of laserspectroscopy as well as of atomic physics.Among his many discoveries, Toschek and associates aremost widely known for the elimination of quantumnoisein the beat signal of two laser waves and the developmentof absorption spectroscopy of gases in the resonator of amulti-mode laser, both of which may substantially im-prove the precision and enhance the sensitivity of inter-ferometric measurements. He founded research teamsat the Heidelberg University in 1963 and the HamburgUniversity in 1981. Toschek received the Wichard PohlPrize from DPG in 1990 and has been a Member of theAkademie derWissenscha�en in Hamburg since 1994, aFellow of JILA since 1986/87, and a Fellow of OSA since2002.Established in 2007, the Award recognizes distinguishedcontributions in quantum optics and atomic physics aswell as leadership in the international scienti�c commu-nity.�e winner will join the list of esteemed past recipi-ents including Alain Aspect, Marlan O. Scully, SergeHaroche, David J. Wineland and H. Je� Kimble.�e Award is jointly sponsored by DPG and OSA andpresented by each society in alternate years.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b14:00 – 15:30CD-9: Information and QuantumComputingChair: Mario Bertocotti, La SapienzaUniver-sita’ di Roma, Roma, Italy
14:00 – 15:30EC-2: Control of Ultracold Atomsand Molecules with LightChair: Elisabeth Giacobino, LaboratoireKastler-Brossel ENS, Paris, France
14:00 – 15:30EA-6: Single Photons andSingle-photon DetectorsChair: OlivierMorin, Max Planck Institute ofQuantum Optics, Garching, Germany
14:00 – 15:30TF-1: Ultrafast Solid-state and FibreLasersChair: Anatoly Grudinin, Fianium Ltd,Southampton, United Kingdom
14:00 – 15:30CF-2: Ultrafast ParametricAmpli�ersChair: Daniele Brida, University of Konstanz,Konstanz, Germany
CD-9.1 TUE 14:00Tunable source of ultrafast bright twinbeams�M. Finger1, T. Iskhakov1, N. Joly2,1, M.Chekhova1,2, and P. Russell1,2; 1Max PlanckInstitute for the Science of Light, Erlan-gen, Germany; 2University of Erlangen-Nuremberg, Erlangen, GermanyWepresent a hollow-core kagomé-style pho-tonic crystal �bre source for pressure tun-able, ultrafast photon number correlatedtwin beams. �e Raman-free, spatiallysingle-mode system shows ∼40% twin-beamsqueezing below the shot-noise level.
EC-2.1 TUE (Invited) 14:00Why Do Single Cold Atoms Matter?�P.E. Toschek; Universität Hamburg, Institutfür Laser-Physik, Hamburg, GermanyTrapped and laser-cooled atomic particles,when individually addressed by coherentradiation, allow non-destructive reiteratedquantum measurements in real time. �econtrolled quantum state and the dynamicsrecordable in real time reveal intricate as-pects of quantum measurement.
EA-6.1 TUE 14:00A Time and Space MultiplexedSingle-Photon Source�G.J. Mendoza, J. Munns, R. Santagati, E.Hemsley, M. Piekarek, E. Martín-López, G.D.Marshall, D. Bonneau, M.G. �ompson, andJ.L. O’Brien; Centre for Quantum Photonics,University of Bristol, Bristol, United KingdomWe demonstrate an actively multiplexedsingle-photon source using eight spatio-temporal photon bins. �e multiplexedsource exhibits enhanced heralded photonstatistics compared to the non-multiplexedsources.
TF-1.1 TUE (Tech Focus) 14:00Micromachining and MaterialsProcessing with High Energy UltrafastFiber Lasers�T. Gerke; Fianium, Southampton, UnitedKingdom�e short pulsewidth and high peak powerprovided with ultrafast lasers allow for newprocessing regimes andmaterials. For exam-ple, processing transparent materials and in-side the bulk of materials is newly enabled.
CF-2.1 TUE (Invited) 14:00Scaling mid-IR driver sources to terawattpeak powers�A. Baltuska1,2, A. Pugzlys1,2, S. Alisauskas1,V. Shumakova1, G. Andriuskaitis1, T.Balciunas1, G. Fan1, T. Floery1, P. Malevich1,and T. Kanai1; 1Photonics Institute ViennaUniversity of Technology, Vienna, Austria;2Center for Physical Sciences & Technology,Vilnius, LithuaniaWe review several architectures of high-intensity mid-IR few-cycle laser systems andsummarize proof-of-concept applications ofour longwave sources related to the genera-tion of Xray and terahertz pulses and fem-tosecond �laments in gases.
CD-9.2 TUE 14:15How a Single Photon Can Act Like ManyPhotons�M. Hallaji, A. Feizpour, G. Dmochowski, J.Sinclair, and A. Steinberg; Centre for Quan-tum Information and Quantum Control andInstitute for Optical Sciences, Departmentof Physics, University of Toronto, Toronto,Canada�e e�ect of a single photon on a probeis ampli�ed using weak value ampli�ca-tion. �e ampli�cation is achieved by post-selecting on a rare �nal state. We observe apost-selected single photon acting like �ve.
EA-6.2 TUE 14:15Reversing�e Temporal Envelope Of AHeralded Single Photon Using A CavityB. Srivathsan1, G. Kaur Gulati1, �A. Cere1,B. Chng1, and C. Kurtsiefer1,2; 1Centrefor Quantum Technologies, National Uni-versity of Singapore, Singapore, Singapore;2Department of Physics, National Universityof Singapore, Singapore, Singapore�e resonant interaction of the biphotonsfrom a cascade atomic decay with an asym-metrical cavity results in heralded singlephotons with an exponentially rising tempo-ral envelope suitable for e�cient interactionwith a two-level system.
CD-9.3 TUE (Invited) 14:30E�cient Photonic Quantum Computing�F.A. Bovino; Quantum Technologies LabFinmeccanica-Selex, Genova, Italy; Dip.Scienze di Base Applicate all’Ingegneria, LaSapienza, Roma, ItalyWe propose a novel architecture to imple-ment a scalable quantum processor based onsilicon-photonics overcoming the overheaddue to multiple single photon sources anddetectors.
EC-2.2 TUE 14:30Hong-Ou-Mandel Interference BetweenTriggered And Heralded Single PhotonsFrom Separate Atomic Systems�A. Cere1, V. Leong1, G. Kaur Gulati1, B.Srivathsan1, S. Kosen1, and C. Kurtsiefer1,2;1Centre for Quantum Technologies, NationalUniversity of Singapore, Singapore, Singa-pore; 2Department of Physics, National Uni-versity of Singapore, Singapore, SingaporeWe experimentally demonstrate the Hong-Ou-Mandel interference of single photonsoriginating from spatially separated sourcesbased on di�erent pysical processes in cold
EA-6.3 TUE 14:30Tomography of photon-number resolvingcontinuous-output detectors�P.C. Humphreys1, B.J. Metcalf1, T. Gerrits2,T. Hiemstra1, A.E. Lita2, J. Nunn1, S.W.Nam2, A. Datta1, W.S. Kolthammer1, andI.A. Walmsley1; 1Clarendon Laboratory, De-partment of Physics, Univ. of Oxford, Oxford,United Kingdom; 2National Institute of Stan-dards and Technology, Boulder, United StatesWe analyse the output of photon-numberresolving detectors by employing principle-component analysis and a novel noise-tolerant method for detector tomography.
TF-1.2 TUE (Tech Focus) 14:30Mid IR Fiber Frequency Combs andApplications�M. Fermann, K. Lee, C. Mohr, J. Jiang, andN. Kuse; IMRA America Inc, Ann Arbor,United StatesWe review recent developments in �berbased mid IR combs based on supercontin-uum generation, DFG, OPOs and OPAs anddiscuss their applications in spectroscopy.
CF-2.2 TUE 14:30Development of a Millijoule Few-Cycle IRLight Source and its Application to High-Flux High Harmonics in the WaterWindow�N. Ishii1, K. Kaneshima1, T. Kanai1, S.Watanabe2, and J. Itatani1; 1Institute forSolid State Physics, Kashiwa, Japan; 2TokyoUniversity of Science, Noda, JapanWe developed a BIBO optical para-metric chirped-pulse ampli�er thatdelivers 1.5-mJ, 10.1-fs optical pulsesat 1 kHz with carrier-envelope phasestabilization. �is light source is applied
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN14:00 – 15:30CK-8: Plasmonic Micro/Nano-structuresChair: Stefano Pelli, Istituto di Fisica Appli-cata Nello Carrara, Firenze, Italy
14:00 – 15:30CE-8: Organic Materials for LasersWaveguides and Nonlinear OpticsChair: Kenichi Goushi, Kyushi University,Fukuoka, Japan
14:00 – 15:30CB-2: Vertical Cavity Lasers(VCSELs) IChair: Martin Kamp, Technische Physik,Universität Würzburg, Würzburg, Germany
14:00 – 15:30EF-8: Spatio-Temporal Dynamics inNonlinear Optical SystemsChair: Sergei Turitsyn, Aston University, As-ton, United Kingdom
14:00 – 15:30CG-1: Novel Attosecond LightSourcesChair: Giulio Cerullo, Politecnico di Milano,Milano, Italy
CK-8.1 TUE 14:00Nano-plasmonic chiral S.H.G. emittersR. Kolkowski1,2, L. Petti3, �C. Lafargue1, andJ. Zyss1; 1Ecole normale supérieure de cachan,Cachan, France; 2Advanced Materials En-gineering and Modelling Group, Faculty ofChemistry, Wroclaw University of Technol-ogy, Wroclaw, Poland; 3Institute of Cybernet-ics of CNR, Pozzuoli, ItalyWe present chiral plasmonic nanoparticlesshowing giant chiroptical Second Harmonicresponse. Speci�cally patterned with sym-metry considerations by e-beam lithogra-phy, and studied under polarization resolvedtwo-photon microscope, their strong non-linear circular dichroism allows e.g. water-marking applications.
CE-8.1 TUE (Invited) 14:00Overcoming Losses in Organic Lasers�T. Riedl; University of Wuppertal, Wupper-tal, GermanyOrganic semiconductor lasers are subject tovarious loss mechanisms related to chargesand/or triplet excitons. We will discuss theirphoto-physics and present avenues to over-come them on the way to cw operation orinjection lasing.
CB-2.1 TUE 14:00Tuning the Frequency of PolarizationOscillations in Spin-VCSELs byMechanical Strain Induction�M. Lindemann1, T. Pusch2, N.C. Gerhardt1,M.R. Hofmann1, and R. Michalzik2; 1Ruhr-University Bochum, Photonics and TerahertzTechnology, Bochum, Germany; 2Ulm Uni-versity, Inst. of Optoelectronics, Ulm, Ger-manySwitchable polarization oscillations in Spin-VCSELs are highly interesting for ultrafastoptical data communication. We demon-strate frequency tunability to a maximum of38 GHz by manipulating the birefringencewithmechanical strain in simulation and ex-periment.
EF-8.1 TUE 14:00Neuromimetic Dynamics in a MicropillarLaser with Saturable Absorber�F. Selmi, R. Braive, G. Beaudoin, I. Sagnes,R. Kuszelewicz, and S. Barbay; Laboratoirede Photonique et de Nanostructures (LPN-CNRS), Marcoussis, FranceFast excitable, neuromimetic dynamics is ex-perimentally evidenced with response timesin the 200ps range in a micropillar laser withsaturable absorber. Relative and absolute re-fractory periods and temporal synaptic sum-mation are demonstrated and analysed.
CG-1.1 TUE (Invited) 14:00Laser-Induced Electron Wave Packets as aSub-nanometer and Sub-femtosecondProbe�L. Di Mauro; �e Ohio State University,Columbus, OH, United StatesAn approach is discussed for producingmolecular images with sub-Angstromatomic precision with few femtosecondexposures. �e laser-induced electrondi�raction procedure extracts a di�ractionpattern from the photoelectron momentumdistribution produced by strong-�eldmid-infrared ionization.
CK-8.2 TUE 14:15AModel for Spasers and DielectricNanolasers: Strategies for Lower�resholds�G. Kewes1, R. Rodriguez-Oliveros1, K.Höfner1, A. Kuhlicke1, O. Benson1, and K.Busch1,2; 1Humboldt-Universität zu Berlin,Berlin, Germany; 2Max-Born Institut, Berlin,GermanyAn analytic model for spasers and dielectricnanolasers is presented. Mie theory allowscalculating realistic gain relaxation rates (sofar underestimated). We derive strategies forthreshold reduction and explore silicon forpurely dielectric nanolasers.
CB-2.2 TUE 14:15Increasing the Birefringence of VCSELsBeyond 250 GHz�T. Pusch1, M. Lindemann2, N.C. Gerhardt2,M.R. Hofmann2, and R. Michalzik1; 1UlmUniversity, Institute of Optoelectronics, Ulm,Germany; 2Ruhr-University Bochum, Pho-tonics and Terahertz Technology, Bochum,GermanyBy applying anisotropic mechanical stresswe have induced a record-high birefrin-gence of 251 GHz in an 850 nm oxide-con�ned single-mode GaAs-based vertical-cavity surface-emitting laser. Such devicescan be used to generate ultrafast polarizationoscillations.
EF-8.2 TUE 14:15Burst-mode operation of a 655GHz modelocked laser based on an 11th ordermicroring resonator�J. Li1, A. Pasquazi2, K. Tsang3, V. Ho1,M. Peccianti2, A. Cooper2, L. Caspani4,5,M. Ferrera5, B. Little6, D.J. Moss7, R.Morandotti4, and S.T. Chu1; 1City Uni-versity of Hong Kong, Hong Kong, HongKong; 2University of Sussex, Brighton, UnitedKingdom; 3Polytechnic University of HongKong, Hong Kong, Hong Kong; 4INRS-EMT,Varennes, Canada; 5Herriot-Watt University,Edinburg, United Kingdom; 6Xi’an Instituteof Optics, Xi’an, China, People’s Republic of(PRC); 7RMIT, Melbourne, AustraliaWe report burst operation of a mode-lockedlaser based on an 11th order microring res-onator.
CK-8.3 TUE 14:30Integrated Localized Surface PlasmonNanotweezer�B. Dagens1,2, V. Yam1,2, R. Megy1,2,C. Pin3, E. Picard4, E. Hadji4, and B.Cluzel3; 1Université Paris-Sud, Institutd*Electronique Fondamentale, Orsay,France; 2CNRS, UMR 8622, Orsay, France;3Laboratoire ICB, Université de Bour-gogne, Dijon, France; 4Laboratoire SiNaPS,INAC/SP2M/SiNaPS, CEA MINATEC,Grenoble, FranceWe show a �rst demonstration of guidedoptical nanotweezer behavior using a short
CE-8.2 TUE 14:30Prospects for thermal limitations in thecontext of future CW organicsemiconductor solid-state lasersZ. Zhao1,2, O. Mhibik1,2, S. Forget1,2, and�S. Chénais1,2; 1Université Paris 13, Sor-bonne Paris Cité, Laboratoire de Physique desLasers, Villetaneuse, France; 2CNRS, UMR7538, LPL, Villetaneuse, France�ermal e�ects are investigated in thin-�lm organic semiconductor solid-statelasers, both experimentally and numer-ically. �ey are shown to be negligiblein low repetition rate pulsed lasers,
CB-2.3 TUE 14:307-GHz Small-signal Modulation Responseof a Surface Micromachined BCBMEMSVCSEL with > 50-nm Continuous Tuning�S. Paul1, C. Gierl1, J. Cesar1, F. Küppers1,B. Kögel2, J. Rosskopf2, M. Görblich2, Y. Xu2,C. Neumeyr2, and M. Ortsiefer2; 1TU Darm-stadt, Darmstadt, Germany; 2VERTILASGmbH, Garching, GermanyWe demonstrate a small-signal modulationresponse (S21) of an electro-thermally ac-tuated MEMS tunable VCSEL. More than4 GHz of S21 3-dB bandwidth is achievedacross a 54 nm continuous tuning range.
EF-8.3 TUE 14:30Harmonic pulse pattern generation in a�ber laser by an adaptative feedback loop�U. Andral, R. Si Fodil, F. Amrani, F. Bil-lard, E. Hertz, and P. Grelu; Lab. ICB UMR6303 CNRS, Université de Bourgogne, Dijon,FranceWe test a new adaptative feedback loop toobtain through optimization and computercontrol the harmonicmode locking of a �berring laser. �e peculiar self-generated har-monic pulse patterns are interpreted.
CG-1.2 TUE 14:30Synchronised attosecond XUV and VUVpulses for pump-probe experiments�D. Fabris1, T. Witting1, W. Okell1, D.Walke1, P. Matia-Hernando1, J. Henkel2, T.Barillot1, M. Lein2, J. Marangos1, and J.Tisch1; 1Imperial College London, London,United Kingdom; 2Leibniz Universität Han-nover, Hannover, GermanyWe present the generation of a syn-chronised pair of attosecond pulsesin the XUV (90eV) and VUV (15 or20eV) for attosecond pump attosec-ond probe experiments. �e pulses
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atoms: scattering from a single trapped atomand photon-pair generation in a parametricprocess.
We further propose a quantitative measureof photon-number-resolution. We applythese techniques to transition-edge-sensordetectors.
to generate high-�ux so� x-ray highharmonics.
EC-2.3 TUE 14:45Spatially dependent electromagneticallyinduced transparency�N. Radwell1, T.W. Clark1, B. Piccirillo2,S.M. Barnett1, and S. Franke-Arnold1;1University of Glasgow, Glasgow, UnitedKingdom; 2Universita di Napoli Federico II,Napoli, ItalyElectromagnetically induced transparency isa coherent e�ect which does not tradition-ally rely on phase. We show that we can pro-duce spatially varying transparency by in-troducing a phase dependence and applyingbeams with spatially varying phase.
EA-6.4 TUE 14:45Quantum Tomography ofSuperconducting Single Photon DetectorsJ.J. Renema1, R. Gaudio2, Q. Wang1, Z.Zhou2, A. Gaggero3, F. Mattioli3, R. Leoni3,D. Sahin2, M.J.A. DeDood1, A. Fiore2, and�M.P. Van Exter1; 1Huygens-KamerlinghOnnes Laboratory, Leiden, �e Netherlands;2Eindhoven Technical University, Eindhoven,�e Netherlands; 3Istituto di Fotonica e Nan-otecnologie, Roma, ItalySuperconducting single-photon detectorsare studied with detector tomography. Byperforming this analysis under variousconditions, we can distinguish betweenvarious detector models, demonstrateenhanced sensitivity at the detector*s edgesand determine the characteristic detectionarea.
CF-2.3 TUE 14:45Monolithic 2D-QPM Frequency DomainOPA�B.W.Mayer1, C.R. Phillips1, L. Gallmann1,2,and U. Keller1; 1Department of Physics, In-stitute for Quantum Electronics, ETH Zurich,Zurich, Switzerland; 2Institute of AppliedPhysics, University of Bern, Bern, SwitzerlandWe demonstrate broadband mid-IRfrequency-domain OPA (FOPA) in theFourier-plane of a 4f pulse shaper via two-dimensional (2D) quasi-phasematching(QPM) device adapted to the pump intensitypro�le and spatial chirp of the mid-infraredbeam.
CD-9.4 TUE 15:00Polychromatic selective lasing of con�nedpolaritons�G. Grosso1,2, S. Trebaol3, M. Wouters4, F.Morier-Genoud1, M. Portella-Oberli1, andB. Deveaud1; 1ICMP, Ecole PolytechniqueFédérale de Lausanne (EPFL), Lausanne,Switzerland; 2EECS, Massachusetts Instituteof Technology, Cambridge, United States;3UMR Foton, CNRS, Université de Rennes,Lannion, France; 4TQC, University ofAntwerp, Anterwerpen, BelgiumWe present an innovative laser device basedon a new relaxationmechanism for con�nedexciton-polaritons which preserves nonlin-earity. We demonstrate the selective acti-vation of polariton lasers at di�erent wave-lengths allowing for all-optical spin logic op-erations.
EC-2.4 TUE 15:00Stimulated Raman Adiabatic passagebetween hyper�ne ground states of a87Rb Bose-Einstein condensate�M. Dupont-Nivet1,2, C. Westbrook2, and S.Schwartz1; 1�ales Research and TechnologyFrance, Palaiseau, France; 2LaboratoireCharles Fabry de l’Institut d’Optique,Palaiseau, FranceWe describe microwave stimulated Ramanadiabatic passage between hyper�ne groundstates of an 87 rubidium Bose-Einstein con-densate. Shi�s in the resonance conditionsare reported, and quantitatively explained asan e�ect of collisions and losses.
EA-6.5 TUE 15:00Wavelength-Multiplexed Heralded SinglePhoton Source on a Chip�L. Caspani1,2, C. Reimer1, M. Clerici1,2,M. Ferrera1,2, M. Kues1, M. Peccianti1,3,A. Pasquazi1,3, L. Razzari1, B.E. Little4,S.T. Chu5, D.J. Moss6, and R. Morandotti1;1INRS-EMT, Varennes, Canada; 2School ofEngineering and Physical Sciences, Heriot-Watt University,, Edinburgh, United King-dom; 3Department of Physics and Astron-omy, University of Sussex, Brighton, UnitedKingdom; 4Xi’an Institute of Optics and Preci-sion Mechanics of CAS, Xi’an, China, People’sRepublic of (PRC); 5Department of PhysicsandMaterial Science, City University of HongKong, Hong Kong, China, People’s Republicof (PRC); 6School of Electrical and ComputerEngineering, RMIT University, Melbourne,AustraliaWe report an integrated, wavelength-multiplexed source of photon pairscompatible with standard �ber communi-cation channels and quantum memories.It is a based on a CMOS-compatible mi-croring resonator operating in a self-lockedpumping mode.
TF-1.3 TUE (Tech Focus) 15:00Industrial Ultrafast Lasers for AdvancedManufacturing Applications�E. Mottay; Amplitude Systèmes, Pessac,FranceUltrafast lasers play a key role in many in-dustrial processes. We review the currentstatus of high power ultrafast laser technol-ogy, and present selected manufacturing ap-plications in the pharmaceutical, mobile dis-play and medical device industries.
CF-2.4 TUE 15:00Broadband 6-�m ParametricAmpli�cation Driven by a Sub-psHo:YAG Chirped Pulse Ampli�er�T. Kanai1, P. Malevich1, G. Gitzinger2, R.Maksimenka2, N. Forget2, A. Baltuška1,3,and A. Pugžlys1,3; 1Photonics Institute, Vi-enna University of Technology, Vienna, Aus-tria; 2FASTLITE, Valbonne, France; 3Centerfor Physical Sciences & Technology, Vilnius,LithuaniaWe demonstrate a broadband OPA at 6 �mdriven by a femtosecond 2.1-�m Ho:YAGCPA, which o�ers an all-in-one solution forseeding, pumping, and CEP stabilization offew-cycle pulses in ZnGeP2 and similarmid-IR crystals.
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metal nanorod chain supporting localizedsurface plasmons and coupled to a SiliconOn Insulator (SOI) waveguide.
but are signi�cant under CW pump-ing
have been characterised by attosecondstreaking.
CK-8.4 TUE 14:45Nonlinear Plasmonics in Nanographenes�J. Cox1 and F.J. García de Abajo1,2; 1ICFO-Institut de Ciencies Fotoniques, Castelldefels,Spain; 2ICREA-Institucío Catalana de Re-cerca i Estudis Avançats, Barcelona, SpainWe show that graphene nanostructures canbe electrically tuned to provide an unprece-dentedly strong plasmon-enhanced nonlin-ear response, leading to e�cient harmonicgeneration, sum/di�erence frequency gen-eration, and four-wave mixing at subwave-length scales.
CE-8.3 TUE 14:45Production processes andcharacterization of all-polymer basedoptical waveguides and interconnects�A. Günther, A.B. Petermann, M. Rezem,M. Rahlves, M. Wollweber, and B. Roth;Hannover Centre for Optical Technologies,Hanover, GermanyWe present various novel production meth-ods for creating optical waveguides andinterconnects integrated in large area all-polymer based foils. �e waveguides andcoupling structures are characterized withrespect to attenuation and coupling e�-ciency.
CB-2.4 TUE 14:45High-Speed 850 nm VCSEL with 30 GHzModulation Bandwidth�E. Haglund1, P. Westbergh1, J.S.Gustavsson1, E.P. Haglund1, A. Larsson1,M. Geen2, and A. Joel2; 1Department ofMicrotechnology and Nanoscience (MC2),Chalmers University of Technology, Göteborg,Sweden; 2IQE Europe Ltd., Cardi�, UnitedKingdomWe present the results from our new genera-tion of high-speed 850 nmVCSELs. By engi-neering the oxide layers, low threshold cur-rents, reduced di�erential resistance and arecord-high small-signal modulation band-width of 30 GHz was achieved.
EF-8.4 TUE 14:45Nematicons routing through disclinationlines in chiral nematic liquid crystals�M. Kwaśny, U. Laudyn, F. Sala, K.Rutkowska, and M. Karpierz; Faculty ofPhysics, Warsaw University of Technology,Warsaw, PolandIn this work we demonstrate nematiconsrouting at disclination lines in chiral nematicliquid crystals. In proposed con�gurationlogic switching is realized through interac-tion between nematicons and line defects inperiodic liquid crystals layered structure.
CG-1.3 TUE 14:45Generation of high-energy isolatedattosecond pulses forXUV-pump/XUV-probe experiments at100 eV�D. Rivas1,2, M. Weidman1, B. Bergues1,A. Muschet1,2, L. Hofmann1,2, O.Razskazovskaya2, H. Schröder1, W. Helml1,G. Marcus1, V. Pervak2, P. Tzallas3, D.Charalambidis3, F. Krausz1,2, and L. Veisz1;1Max-Planck-Institut fuer Quantenoptik,Garching, Germany; 2Ludwig-Maximilians-Universitaet Muenchen, Garching, Germany;3Foundation for Research and Technology-Hellas, Heraklion, GermanyWe report on the generation of high or-der harmonics in gas media using a sub-5 fs multi-ten-terawatt laser system. �esehigh-harmonics exhibit record energies witha continuous spectrum at photon energiesup to 130 eV.
CK-8.5 TUE 15:00Dual-colour Nano-Pixels for imageswitching beyond the di�raction limit�Z. Li, J. Cooper, and A. Clark; BiomedicalEngineering Division, School of Engineering,University of Glasgow, Glasgow, United King-domDual-colour plasmonic nano-pixels whichallow polarisation controlled image andcolour switching are demonstrated. Fab-ricated as cross-shaped plasmonic nano-apertures in an aluminium thin-�lm, theseswitchable sub-wavelength pixels are used todisplay complex images with nano-scale res-olution.
CE-8.4 TUE 15:00Molecular orientations of nonelectricallypoled guest-host NLO polymers�A. Sugita, Y. Sato, T. Matsui, and Y. Kawata;Shizuoka University, Hamamatsu, JapanMolecular orientation orders of nonelectri-cally poled guest-host NLO polymers wereexamined with polarization-resolved SHG,dichroic linear absorption and heterodyneSHG spectroscopies. �e orientation dis-tribution and the polar directions of theguest chromophores were speci�ed unam-biguously.
CB-2.5 TUE 15:00Passive Mode-Locking and Tilted Wavesin Electrically Biased Broad-Area VCSELsM. Marconi1, �J. Javaloyes2, S. Balle3, andM. Giudici1; 1Institut Non Linéaire de Nice,Valbonne, France; 2Universitat de les IllesBaleares, Palma de Mallorca, Spain; 3InstitutMediterrani d’Estudis Avançats, Esporles,SpainA broad-area VCSEL with optical feedbackfrom a distant saturable absorber mirror isoperated in passive mode locking regime,leading to pulses of approximately 1 W peakpower and 10 ps width.
EF-8.5 TUE 15:00Asymmetric counter propagating frontswithout �owI. Andrade-Silva1, M.G. Clerc1, and �V.Odent1,2; 1Departamento de Fisica, Facultadde Ciencias Fisicas y Matematicas, Universi-dad de Chile, Santiago, Chile; 2Laboratoirede Physique des Lasers, Atomes et Molécules,CNRS UMR8523, Université Lille 1, Vil-leneuve d’Ascq, FranceWe investigate the asymmetrical counterpropagation of fronts in an in-plane-switching cell �lled with a nematic liquidcrystal connecting di�erent molecularorientations. �eoretically, we propose asimple bistable model, which qualitativelydescribes the observed dynamics.
CG-1.4 TUE 15:00Bright attosecond pulse generation undertransient phase-matching in two-colourhigh-order harmonic generationB. Schütte1, P. Weber1, K. Kovács2,3,4,�E. Balogh2,4, B. Major2, V. Tosa2,4, S.Han1, M. Vrakking1, K. Varjú2,4, and A.Rouzée1; 1Max-Born-Institut, Berlin, Ger-many; 2Department of Optics and Quan-tum Electronics, University of Szeged, Szeged,Hungary; 3National Institute for R&D ofIsotopic and Molecular Technologies, Cluj-Napoca, Romania; 4ELI-HU Nonpro�t K�.,Szeged, HungaryExperimental and theoretical study of two-colour HHG is presented. We show e�cientcontinuum generation up to 160 eV, and cal-culations suggest the generation of single at-tosecond pulse isolated by hybrid optical andtransient phase-matching gating.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCD-9.5 TUE 15:15Time-Multiplexed Guided-Wave OpticalParametric Oscillator at Degeneracy forLarge-Scale Ising Machines�A. Marandi1,2, C. Langrock1, M. Fejer1, R.Byer1, and Y. Yamamoto1,2; 1Stanford Uni-versity, Stanford, United States; 2National In-stitute of Informatics, Tokyo, JapanWe report stable operation of an N=160time-multiplexed optical parametric oscilla-tor at degeneracy comprising a periodicallypoled lithium niobate waveguide and PM�ber ring resonator as the building block ofa large-scale optical Ising machine.
EC-2.5 TUE 15:15Rotational state cooling of trappedpolyatomic molecules via opticalpumping�R. Glöckner, A. Prehn, M. Ibrügger, M. Zep-penfeld, and G. Rempe; Max-Planck-Institutfür Quantenoptik, Garching, GermanyControlling molecules at the quantum levelrequires motional cooling and internal statecontrol. We present rotational cooling ofpolyatomic molecules achieving a cold en-semble (∼30mK) with at least 70% populat-ing a single rotational state.
EA-6.6 TUE 15:15A Highly E�cient Heralded SinglePhoton Source for TelecomWavelengthsbased on a PPLN Ridge Waveguide�M. Bock, A. Lenhard, and C. Becher; Saar-land University, Saarbrücken, GermanyWe realize a highly e�cient photon pairsource for telecom wavelengths in the O–and C–band. �e photon pair emissionrate is up to 10MHz with large signal–to–background ratio resulting in a low �(2)(0) =0.04
CF-2.5 TUE 15:15Passively CEP-stabilized OPCPAFront-End Based on Yb:KGW Laser�R. Budriunas1,2, T. Stanislauskas1,2, Š.Straigis1, and A. Varanavičius1; 1VilniusUniversity, Vilnius, Lithuania; 2Light Con-version Ltd., Vilnius, LithuaniaAn OPCPA front-end operating in thevisible-NIR range is demonstrated. �efront-end delivers 40 �J pulses with octavespanning spectra and short-termCEP stabil-ity better than 70 mrad.
16:00 – 17:30CD-10: Whispering GalleryMode-applicationsChair: Crina Cojocaru, Polytechnic Univer-sity of Catalonia, Barcelona, Spain
16:00 – 17:30EC-3: Cavity Mediated Control ofQuantumMattersChair: Selim Jochim, University of Heidel-berg, Heidelberg, Germany
16:00 – 17:30EA-7: Quantum Light SourcesChair: Ana Predojevic, Universität Insbruck,Innsbruck, Austria
16:00 – 17:30TF-2: Materials Structuring UsingShort Laser PulsesChair: Ludger Overmeyer, Institut für Trans-port und Automatisierungstechnik, Garbsen,Germany
16:00 – 17:30CF-3: Spectral Broadening ofUltrashort PulsesChair: Giulio Cerullo, Politecnico di Milano,Milano, Italy
CD-10.1 TUE 16:00Brillouin lasing in barium �uoridewhispering-gallery-mode resonators�G. Lin, S. Diallo, K. Saleh, R. Martinenghi,J.-C. Beugnot, T. Sylvestre, and Y.K. Chembo;FEMTO-ST, Besançon, FranceWe report the observation of cascaded Bril-louin lasing at 1550 nm in barium �uoride(BaF2) whispering gallery mode resonators.Brillouin lasing in BaF2 can �nd potentialapplications for high-coherence lasers andmicrowave photonics.
EC-3.1 TUE (Keynote) 16:00Microcavity polaritons: from quantumoptics to quantum �uids�E. Giacobino; Laboratoire Kastler Brossel,UPMC, CNRS, ENS, Paris, FranceWe show how photons in an optical micro-cavity containing a nonlinear medium canboth exhibit quantum squeezing and super-�uid properties similar to those of low tem-perature Helium, together with solitons andquantized vortices.
EA-7.1 TUE 16:00Photonic gears for ultra-sensitive angularmeasurementsV. D’Ambrosio1, �N. Spagnolo1, L. Del Re1,S. Slussarenko2, Y. Li3, L.C. Kwek3, L.Marrucci2, S.P. Walborn4, L. Aolita5, and F.Sciarrino1; 1Dip. di Fisica, Sapienza Univ.di Roma, Rome, Italy; 2Dip. di Fisica, Univ.di Napoli Federico II, Napoli, Italy; 3Centerfor Quantum Technologies, National Univ. ofSingapore, Singapore; 4Inst. de Fisica, Univ.Federal do Rio de Janeiro, Rio de Janeiro,Brazil; 5Dahlem Center for Complex Quan-tum Systems, FU Berlin, Berlin, GermanyWe report the experimental implementationof a method, based on high-m quanta of or-bital angular momentum, leading to robustsingle-photon angular measurements withenhanced sensitivity. �is method can bealso be combined with entanglement-basedstrategies.
TF-2.1 TUE (Tech Focus) 16:00Functional Surfaces Generated withFemtosecond Lasers�R. Kling, M. Faucon, and G. Mincuzzi; AL-PhANOV, Talence, FranceIn this presentation the creation mecha-nisms of LIPSS are introduced with the feed-back on laser speci�cations and handlingsystems. Applications of the laser inducedsurface functions covering decoration, tri-bology and antire�ection are discussed.
CF-3.1 TUE 16:00Generation of Intense Supercontinuum inCondensed Media�C.-H. Lu1, Y.-J. Tsou1, H.-Y. Chen1, B.-H.Chen1, Y.-C. Cheng2, P.-C. Huang1,2, S.-D.Yang1, M.-C. Chen1, C.-C. Hsu3, and A.H.Kung1,2; 1Institute of Photonics Technolo-gies, National Tsing Hua University, Hsinchu,China, Republic of (ROC); 2Institute ofAtomic and Molecular Sciences, AcademiaSinica, Taipei, China, Republic of (ROC);3Dep. of Physics, National Chung Cheng Uni-versity, Chiayi, China, Republic of (ROC)An octave-spanning supercontinuum spec-trum with high pulse energy and excellentbeam quality is generated by strategicallyplacing several thin fused silica plates.
CD-10.2 TUE 16:15Coupling of Whispering Gallery Modes inOptical Fiber Resonators Based onRe�ectionless Potentials�S. Suchkov1, M. Sumetsky2, and A.Sukhorukov1; 1Australian National Univer-sity, Canberra, Australia; 2Aston University,Birmingham, United Kingdom
EA-7.2 TUE 16:15High Intensity Broadband Source ofEnergy-Time Entangled Photons forSpectroscopy
CF-3.2 TUE 16:15Direct Generation of 7 fs WhitelightPulses�E. Wittmann, M. Bradler, and E. Riedle;LS für BioMolekulare Optik, LMU,München,GermanyWe demonstrate for the �rst time sub-10fs supercontinuum pulses from a bulk ma-
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCK-8.6 TUE 15:15Impact of Nonlocal Free-Electron OpticalResponse on�ird-Harmonic Generationin Plasmonic Nanostructures�C. Ciracì1, M. Scalora2, and D.R. Smith3;1Istituto Italiano di Tecnologia (IIT), Cen-ter for Biomolecular Nanotechnologies, Arne-sano, Italy; 2C.M. Bowden Research Facil-ity, US Army, RDECOM, Huntsville, UnitedStates; 3DukeUniversit, Durham, NC, UnitedStatesA study of third-harmonic generation inmetal �lm-coupled nanowires reveals thatfor sub-nanometer gaps classical nonlocalitymay strongly enhance e�ective nonlineari-ties as the �eld penetrates deeper inside themetal than assuming a local electronic re-sponse.
CE-8.5 TUE 15:15Fabrication and Nonlinear OpticalCharacterization of Highly CdSeQuantum Dot Dispersed PolymerNanocomposites�Y. Tomita, R.-i. Yamagami, andT.-a. Jinzenji; University of Electro-Communications, Tokyo, JapanPolymer nanocomposites dispersed withCdSe quantum dots as high as 6.8 vol.%wereprepared and the nonlinear optical proper-ties were characterized. It was found that theobserved ��h-order optical nonlinearity hasthe cascading third-order contribution.
CB-2.6 TUE 15:15Novel Oxide-Free VCSELWith OpticallyControlled Current Con�nement�S. Bader1, P. Gerlach2, and R. Michalzik1;1Ulm University, Institute of Optoelectronics,Ulm, Germany; 2Philips Technologie GmbH,U-L-M Photonics, Ulm, GermanyWe present the �rst vertical-cavity surface-emitting laser with optically controlled cur-rent con�nement via an epitaxially inte-grated phototransistor, improving manufac-turability and avoiding built-in strain ofpresent VCSELs. Continuous-wave opera-tion characteristics are shown and hysteresisfeatures explained.
EF-8.6 TUE 15:15Experimental manipulation of phasesymmetries in photorefractive oscillatorsvia rocking: bistability and dissipativestructures�R. Martínez-Lorente1, J. Ruiz-Rivas1,A. Esteban-Martín1,2, K. Staliunas3, E.Roldán1, G.J. De Valcárcel1, and F. Silva1;1Departament d’Òptica, Universitat deValència, Valencia, Spain; 2ICFO-Institutde Ciències Fotòniques, Barcelona, Spain;3ICREA and Departament de Física iEnginyeria Nuclear, Universitat Politècnicade Catalunya, Barcelona, SpainWe convert a phase invariant optical systeminto a phase bistable optical system througha modulation technique known as Rocking.A photorefractive oscillator is used to sup-port it in a non-degenerate four wavemixingcon�guration.
CG-1.5 TUE 15:15Noncollinear Optical Gating - A methodfor intra-cavity single attosecond pulsegeneration?�C.M. Heyl1, M. Louisy1, M. Miranda1,E.W. Larssen1, S.N. Bengtsson1, D. Kroon1,M. Kotur1, D. Guérnot1, L. Rading1, P.Rudawski1, F. Brizuela1, F. Campi1, B. Kim1,A. Jarnac2, A. Houard2, J. Mauritsson1, P.Johnsson1, A. L’Huillier1, and C.L. Arnold1;1Department of Physics, Lund University,Lund, Sweden; 2Laboratoire d’Optique Ap-pliquée, ENSTA Paristech, École Polytech-nique, CNRS, Palaiseau, FranceWepresent the concept and experimental re-sults of NoncollinearOptical Gating, a singleattosecond pulse gating scheme that com-bines angular streaking and noncollinearhigh-order harmonic generation, providingangularly separated but perfectly synchro-nized isolated attosecond pulses.
16:00 – 17:30CK-9: Photonic Micro- andNanocavitiesChair: Tapio Niemi, Tampere University ofTechnology, Tampere, Finland
16:00 – 17:30CE-9: Fabrication andCharacterization of Organic andInorganic Nonlinear MaterialsChair: �omas Riedl, University of Wupper-tal, Wuppertal, Germany
16:00 – 17:30CB-3: Vertical Cavity Lasers(VECSELs) IIChair: Mircea Guina, Optoelectronics Re-search Centre Tampere University, Tampere,Finland
16:00 – 17:30CH-5: Photonic Crystals andMicrostructured Fibres for SensingChair: Trevor Benson, University of Notting-ham, Nottingham, United Kingdom
16:00 – 17:30CG-2: High Average/Peak PowerSources and ApplicationsChair: LukasGallmann, ETHZürich, Zürich,Switzerland
CK-9.1 TUE 16:00Topology Optimization of CoupledPhotonic Crystal Cavities for Flat-topDrop Filter Functionality�L. Hagedorn Frandsen1, Y. Elesin2,3, O.Sigmund2, and K. Yvind1; 1DTU Fotonik,Department of Photonics Engineering, Lyn-gby, Denmark; 2DTU Mekanik, Departmentof Mechanics Engineering, Lyngby, Denmark;3Haldor Topsoe, Lyngby, DenmarkOutperforming conventional design con-cepts, a low-loss �at-top drop �lter has beendesigned by applying 3D topology optimiza-tion to coupled photonic crystal cavities.Measurements on the design fabricated insilicon-on-insulator material veri�es the op-timized drop �lter.
CE-9.1 TUE 16:00Photonic Damascence Process for high-QSiN Microresonator Fabrication forNonlinear Photonics�M. Pfei�er, A. Kordts, V. Brasch, C.Lecaplain, J. Jost, M. Geiselmann, and T.Kippenberg; Ecole Polytechnique Federale deLausanne, Lausanne, SwitzerlandIntegrated microresonators based on SiNwaveguides are an attractive platform fornonlinear optics. Here we present a newphotonic Damascene fabrication processthat solves common problems in SiN waveg-uide fabrication and demonstrate frequencycomb formation.
CB-3.1 TUE 16:0050 W VECSEL emitting at 1180 nm�E. Kantola, T. Leinonen, J.-P. Penttinen, M.Tavast, S. Ranta, and M. Guina; Optoelec-tronic research Centre, Tampere University ofTechnology, Tampere, FinlandWe report a 50 W VECSEL emitting at 1180nm. �e gain chip was grown by MBEand TEC-cooled. �e maximum power wasmeasured for a mount temperature of -15�C.
CH-5.1 TUE 16:00Kagome Hollow-Core Photonic CrystalFiber Resonator for Rotation Sensing�I. Fsaifes1, G. Feugnet2, S. Schwartz2, B.Debord3, F. Gérôme3, G. Humbert3, F.Benabid3, and F. Bretenaker1; 1LaboratoireAimé Cotton, CNRS-Université Paris Sud 11-ENS Cachan, Orsay, France; 2�ales Re-search and Technology, Palaiseau, France;3GPPMM group, Xlim Research Institute,Limoges, FranceResults on using Kagome hollow-core �berbased resonator for rotation sensing appli-cations are presented. Finesse up to 33 isdemonstrated leading to a shot-noise sensi-tivity limit in the high performance rangegyroscopes.
CG-2.1 TUE 16:00Few-Cycle, CEP-Stable, 300 kHz-OPCPASystem with Multi-GW Peak Powers�M. Schultze1, S. Prinz1,2, C. Teisset1, K.Michel1, M. Haefner1, R. Bessing1, R.Kienberger2,3, and T. Metzger1; 1TRUMPFScienti�c Lasers GmbH & Co.KG, Unter-foehring, Germany; 2Department of Physics,TU Muenchen, Garching, Germany; 3Max-Planck-Institut für Quantenoptik, Garching,GermanyWe demonstrate a 300 kHz-OPCPA systemgenerating CEP-stabilized 50�J pulses witha duration of 5.74 fs, a peak power of 4.4GW and long-term power �uctuations ofless than 1.4% rms.
CK-9.2 TUE 16:15A Photolithographic High-Q PhotonicCrystal Nanocavity Fabricated on aSilicon-on-insulator Structure�Y. Ooka, T. Tetsumoto, A. Fushimi, W.Yoshiki, and T. Tanabe; Keio University,Yokohama, JapanIn order to integrate photonic-crystal
CE-9.2 TUE 16:15Blue Light Induced Infrared Absorptionand Color-Center Fluorescence in KTPIsomorphs�S. Tjörnhammar1, V. Maestroni1,2, T.K.Uždavinys3, A. Zukauskas1, C. Canalias1,V. Pasiskevicius1, and F. Laurell1; 1RoyalInstitute of Technology (KTH), Department
CB-3.2 TUE 16:15High-Power Operation of InfraredQuantum-Dot BasedVertical-External-CavitySurface-Emitting Lasers�D. Al Nakdali1, M.K. Shakfa1, M. Gaafar1,K. Fedorova2, M. Wichmann1, F. Zhang1, A.Rahimi-Iman1, E. Rafailov2, and M. Koch1;
CH-5.2 TUE 16:15Compact highly sensitive photonic crystal�bre bending sensor�J. Villatoro1,2, V. Minkovich3, and J.Zubia1; 1ETSI Communications EngineeringDept., University of the Basque Country(UPV/EHU), Bilbao, Spain; 2IKERBASQUE,Basque Foundation for Science, Bilbao,
CG-2.2 TUE 16:15Passive coherent combining of CEP-stablefew-cycles pulses from a temporallydivided hollow �ber compressor�H. Jacqmin1,2, A. Jullien1, B. Mercier1, M.Hanna3, F. Druon3, D. Papadopoulos4, andR. Lopez-Martens1; 1Laboratoire d’OptiqueAppliquée, Palaiseau, France; 2�ales Op-
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We reveal that optical �ber resonators sup-port close packing of elements based on re-�ectionless potentials which locally a�ectlight coupling to whispering gallery modes,and formulate coupled-mode equations gov-erning mode interactions in dispersive non-linear media
�S. Lerch and A. Stefanov; University of Bern,Institute of Applied Physics, Bern, Switzer-landWe present a shaper setup, inspired by ultra-fast optics, which is a very promising toolto experimentally implement entangled-photon spectroscopy. Moreover, this setupcan be used to implement quantum informa-tion processing in high dimensions.
terial. In our approach no external com-pression is needed. �e setup bases on athin sapphire crystal and an astigmatism-free, achromatic telescope.
CD-10.3 TUE 16:30Lithium tetraborate whispering galleryresonator for second-harmonicgeneration into the ultraviolet�J.U. Fürst1, I. Breunig1, K. Buse1,2,P. Becker3, J. Liebertz3, and L. Bohatý3;1Laboratory for Optical Systems, Departmentof Microsystems Engineering, University ofFreiburg, Freiburg, Germany; 2FraunhoferInstitute for Physical Measurement Tech-niques, Freiburg, Germany; 3Institute ofCrystallography, University of Cologne,Cologne, GermanyWe demonstrate the generation of ultravio-let light at 245 nm wavelength by frequencydoubling in a millimeter-sized monolithicresonator made of lithium tetraborate. 2.2% conversion e�ciency is reached at 6 mWCW input power.
EA-7.3 TUE 16:30Direct Generation of Cross-PolarizedPhotons on a Chip�L. Caspani1,2, C. Reimer1, M. Kues1, B.Wetzel1, P. Roztocki1, M. Clerici1,2, Y.Jestin1, M. Ferrera1,2, M. Peccianti1,3, A.Pasquazi1,3, B.E. Little4, S.T. Chu5, D.J.Moss6, and R. Morandotti1; 1INRS-EMT,Varennes, Canada; 2Heriot-Watt University,Edinburgh, United Kingdom; 3University ofSussex, Brighton, United Kingdom; 4Xi’an In-stitute of Optics and Precision Mechanics ofCAS, Xi’an, China, People’s Republic of (PRC);5City University of Hong Kong, Hong Kong,China, People’s Republic of (PRC); 6RMITUniversity, Melbourne, AustraliaWe report the �rst bi-chromatically pumpedcross-polarized optical parametric oscillatorvia type II spontaneous four-wavemixing ona chip, featuring the direct generation of or-thogonally polarized signal and idler �elds.
TF-2.2 TUE (Tech Focus) 16:30Ultrafast Burst-Mode Fiber Lasers:Source Development and MaterialProcessing�F.O. Ilday; Department of Electrical andElectronics Engineering, Bilkent University,Ankara, Turkey; Department of Physics,Bilkent University, Ankara, TurkeyUltrafast burst-mode micromachining al-lows enhanced control against thermal ef-fects and increases processing speed. De-velopments in burst-mode �ber lasers andtheir applications to processing ofmetals, di-electrics, so� and hard tissue will be pre-sented.
CF-3.3 TUE 16:30Coherent Near-Mid-IR SupercontinuumGeneration in Highly NonlinearMulti-Cladding Liquid-Core FiberDesigned for Flat Normal Dispersion�C. Wang1,2,3 and M. Bache1; 1TechnicalUniversity of Denmark, Department of Pho-tonics Engineering, Kgs.Lyngby, Denmark;2Key Lab of All Optical Network & AdvancedTelecommunication Network of EMC, BeijingJiaotong University, Beijing, China, People’sRepublic of (PRC); 3Institute of LightwaveTechnology, Beijing Jiaotong University, Bei-jing, China, People’s Republic of (PRC)�e CS2-�lled liquid core �ber (LCOF) witha three-layer cladding based on the heavilyGe-doped silica is proposed to obtain the�attened normal dispersion pro�le and highnonlinearity in the �ber.
CD-10.4 TUE 16:45Stabilization of a whispering-galleryoptical-parametric oscillator:mode-hop-free tuning and truecontinuous-wave operation�C.S. Werner1, K. Buse1,2, and I. Breunig1;1Department of Microsystems Engineering- IMTEK, University of Freiburg, Freiburg,Germany; 2Fraunhofer Institute for Physi-cal Measurement Techniques, Freiburg, Ger-manyBy locking a tunable pump laser to awhispering-gallery resonator, we achievetrue continuous-wave operation of anoptical-parametric oscillator. Mode-hop-free tuning over 480 MHz is possible by atemperature sweep of the resonator.
EC-3.2 TUE 16:45Enhanced zero phonon line emissionfrom a nitrogen-vacancy centre indiamond coupled to an opticalmicrocavityS. Johnson, P. Dolan, A. Trichet, and �J. Smith;University of Oxford, Oxford, United King-domWe report the enhancement of zero phononline emission froma single nitrogen-vacancycentre in diamond coupled to an open mi-crocavity at cryogenic temperature. �ework is of importance in developing solidstate spin-photon interfaces.
EA-7.4 TUE 16:45Giant Twin-Beam Generation along thePump Energy Propagation�K. Spasibko1,2,3, A. Perez1,2, P. Sharapova3,O. Tikhonova3, M. Chekhova1,2,3, andG. Leuchs1,2; 1Max Planck Institute forthe Science of Light, Erlangen, Germany;2Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany; 3Departmentof Physics, M. V. Lomonosov Moscow StateUniversity, Moscow, RussiaExtremely bright narrowband twin beamscan be generated via high-gain parametricdown conversion if one of the twin beams isemitted along the pump Poynting vector orits group velocity matches that of the pump.
CF-3.4 TUE 16:45Generation of Sub-two-cycleMid-infrared Pulses in the SpectralRegion from 6 to 8 mkm�A.A. Lanin1,2, A.A. Voronin1,2, E.A.Stepanov1,2, A.B. Fedotov1,2, and A.M.Zheltikov1,2,3; 1Physics Dep., InternationalLaser Center, M. V. LomonosovMoscow StateUniv., Moscow, Russia; 2Russian QuantumCenter, Skolkovo, Moscow Region, Russia;3Dep. of Physics and Astronomy, Texas A&MUniv., College Station TX, United StatesWe achieved few-cycle pulses in a spectralregion from 4 to 8 mkm due to supercon-tinuum generation in a GaAs crystal. �eshortest pulses (1.2-cycles at 7.9 mkm) wereobtained through self-compression in thecrystal.
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nanocavities with other silicon-photonicdevices, we designed and demonstrated aphotonic-crystal nanocavity that exhibitan ultrahigh-Q of 2.2×105 even when itis fabricated by photolithography and iscladded with SiO2.
of Applied Physics, Stockholm, Sweden;2Politecnico di Milano, Milano, Italy; 3RoyalInstitute of Technology (KTH), Departmentof Materials and Nano Physics, Kista, SwedenWe compared blue induced infrared absorp-tion in KTP and the isomorphs RKTP, RTP,KTA and RTA using thermal lens spec-troscopy. Ti3+ color-center induced �uores-cence was investigated during illuminationby high-intensity radiation at 400 nm.
1Department of Physics and Material Sci-ences Center, Philipps-University of Marburg,Marburg, Germany; 2Optoelectronics andBiomedical Photonics Group, School of Engi-neering and Applied Science, Aston Univer-sity, Birmingham, United KingdomWe present latest achievements regard-ing quantum-dot based semiconductor disklasers designed for emission in the infrared.Device optimization and power scaling leadto record-high output powers exceedingmultiple Watts for 1040- and 1180-nm de-vices, respectively.
Spain; 3Centro de Investigaciones en OpticaA. C., Leon, MexicoA simple and highly sensitive bending sen-sor based on a photonic crystal �bre inter-ferometer is presented. �e device is suitablefor monitoring low tilt angles with high res-olution along the angle orientation.
tronique SA, Elancourt, France; 3LaboratoireCharles Fabry, Palaiseau, France; 4LULI,Palaiseau, FranceWe demonstrate a robust passive coherentcombining technique for post-compressionof mJ energy CEP-stable laser pulses downto few-cycle duration in a gas-�lled hollow-�ber. High combining e�ciency is achievedusing carefully oriented calcite plates.
CK-9.3 TUE 16:30High order transversal modes incorrugated DFB micro-cavities�E. Marin1, C. Bonzon2, R. Geiger1, T.Zabel1, H. Sigg1, and J. Faist2; 1Laboratoryfor Micro- and Nanotechnology, Paul Scher-rer Institute, 5232 Villigen PSI, Switzerland;2Institute for Quantum Electronics, ETHZürich, 8093 Zürich, SwitzerlandWe present an investigation of high-Q lat-erally corrugated DFB cavity modes. Basedon �nite element method calculations highintrinsic Q-factors of more than 40000have been observed using ��h order cavitymodes.
CE-9.3 TUE 16:30Domain wall kinetics near the hexagonalcorner of MgO doped stoichiometriclithium niobate�J.W. Choi1, S.-J. Son2, D.-K. Ko3, N.E. Yu4,and J.H. Ro5; 1Gwangju Institute of Sci-ence and Technology, Gwangju, Korea, South;2Gwangju Institute of Science and Technol-ogy, Gwangju, Korea, South; 3Gwangju Insti-tute of Science and Technology, Gwangju, Ko-rea, South; 4Gwangju Institute of Science andTechnology, Gwangju, Korea, South; 5PusanNational University, Busan, Korea, SouthA mesospheric approach based on a sim-ple microscopic 2-dimensional Ising modelis newly suggested to explain themacroscop-ically observed asymmetric in-out domainwall motion in (0001) plane of MgO dopedstoichiometric lithium niobate.
CB-3.3 TUE 16:30E�ciency of Solar Pumping of VECSELs�A. Quarterman and K.Wilcox; University ofDundee, Dundee, United KingdomMeasurements of the internal quantum e�-ciency of a VECSEL gain sample are madeby both lasing and solar-pumped photo-luminescence methods in order to assessthe prospects of VECSELs as solar-pumpedsemiconductor lasers.
CH-5.3 TUE 16:30Cavity Optomechanics With PhotonicCrystal Nanomembrane�K. Makles1, T. Jacqmin1, S. Deléglise1, T.Biant1, P.-F. Cohadon1, A. Heidmann1, R.Braive2, and I. Robert-Philip2; 1LaboratoireKastler Brossel, Paris, France; 2Laboratoire dePhotonique et deNanostructures, Marcoussis,FranceWe presente a new optomechanical de-vice, based on photonic cristal suspendednanomembrane. It combines high re�ec-tivity, low mechanical losses, and an inte-grated capacitive actuationwhichwill enableits coupling to a radio-frequency circuit.
CG-2.3 TUE 16:30A compact single cycle driver for strong�eld applications based on aself-compression in a Kagome �ber�T. Balciunas1, G. Fan1, S. Haessler1, C.Fourcade-Dutin2, T. Witting3, A. Voronin4,A. Zheltikov4,5, F. Gerome2, G. Paulus6, A.Baltuska2, and F. Benabid2; 1Photonics In-stitute Vienna Univ. of Technology, Vienna,Austria; 2GPPMM group, Xlim Research In-stitute, UMR 7252 CNRS, Univ. de Limoges,Limoges, France; 3Blackett Laboratory, Impe-rial College London, London, United King-dom; 4Physics Dep., International Laser Cen-ter, M.V. Lomonosov Moscow State Univ.,Moscow, Russia; 5Department of Physics andAstronomy, Texas A & M Univ., College Sta-tion Texas, United States; 6Institut fuer Optikund Quantenelektronik, Jena, GermanyWe report on Kagome �ber based self-compression of 100 uJ IR pulses to singlecycle duration and demonstrate HHG inan integrated scheme which allows isolated-attosecond-pulse generation above 50 eVrange in a compact setup.
CK-9.4 TUE 16:45Nanocavity Formation with aQ of aHalf-million using Photonic CrystalWaveguide and Nano�ber�T. Tetsumoto, Y. Ooka, A. Fushimi, and T.Tanabe; Keio University, Yokohama, JapanWe experimentally demonstrated high Qcavity formation on silicon photonic crystalwaveguide with nano�ber. �e obtained Qwas of 5.1 × 105. We also demonstrated theresonant wavelength tuning of the cavity.
CE-9.4 TUE 16:45Impurity limitations of the quality factorof whispering gallery resonators made oflithium niobate�M. Leidinger1, K. Buse1,2, and I. Breunig1;1Laboratory for Optical Systems, Depart-ment of Microsystems Engineering - IMTEK,University of Freiburg, Freiburg, Germany;2Fraunhofer Institute for Physical Measure-ment Techniques, Freiburg, GermanyA whispering gallery resonator made of un-doped, congruently grown lithium niobateis characterized regarding its quality factorQ in the wavelength range from 390 to 2700nm. Q-factor values up to 109 are obtained.
CB-3.4 TUE 16:45High-power (> 400 mW) laser emission at332 nm of frequency-doubled, opticallypumped AlGaInP disk laser with anoptimized quantum well structure�H. Kahle1, S. Baumgärtner1, F. Sauter1,R. Bek1, T. Schwarzbäck1,2, M. Jetter1, andP. Michler1; 1Institut für Halbleiteroptikund Funktionelle Grenzächen and ResearchCenter SCoPE, University of Stuttgart,Allmandring 3, 70569, Stuttgart, Germany;2Optics Development, TRUMPF Lasersys-tems for Semiconductor ManufacturingGmbH, Johann-Maus-Straße 2, 71245,Ditzingen, GermanyWe show a new AlGaInP-VECSEL designwith inhomogeneous distributed quantumwells optimized for the absorption pro�le ofthe pump laser which leads to high outputpowers of 1.6 W in the red and 429 mW inthe UV spectral range.
CH-5.4 TUE 16:45High order modes in�uence in laserfrequency stabilization using gas-�lledhollow-core �bers�M. Triches1,2, J. Hald1, M. Michieletto2,3,J.K. Lyngsø3, J. Laegsgaard2, and O. Bang2;1Danish Fundamental Metrology, Kgs. Lyn-gby, Denmark; 2DTU Fotonik, Kgs. Lyngby,Denmark; 3NKT Photonics, Birker\o d, Den-mark�is work aims to demonstrate that hollow-core �bers with small core diameter arepreferable to the detriment of large coreones in laser frequency stabilization, be-cause high-order-modes contribution de-grades the accuracy performance, despitestate-of-the-art suggestions.
CG-2.4 TUE 16:45Limitation of laser wake�eld accelerationof electrons�D. Cardenas1,2, S.-w. Chou1,2, L.Hofmann1,2, J. Xu1,3, A. Buck1,2, K.Schmid1,2, C. Sears1, B. Shen3, F. Krausz1,2,and L. Veisz1; 1Max Planck Institutefor Quantum Optics, Garching, Ger-many; 2Ludwig-Maximilian-UniversitaetMuenchen, Munich, Germany; 3ShangaiInstitute of Optics and Fine Mechanics,Shangai, China, People’s Republic of (PRC)�e electron dephasing e�ect limits themaximum obtainable energy in laser-drivenelectron accelerators. Direct measurementof dephasing lengths is now possible inwake�elds excited by sub-5-fs and 8-fs laserpulses, yielding below 100 micrometers.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCD-10.5 TUE 17:00Continuous-Wave, Multi-Milliwatt,Tunable Mid-Infrared Generation Across6.4-7.5 um In Orientation-PatternedGaAs�K.Devi1, P. Schunemann2, andM. Ebrahim-Zadeh1,3; 1ICFO-Institut de Ciencies Fo-toniques, Castelldefels, Barcelona, Spain;2BAE Systems, New Hampshire, UnitedStates; 3Institucio Catalana de Recerca i Es-tudis Avancats (ICREA), Barcelona, SpainWe report a mid-infrared, tunable,continuous-wave source based on OP-GaAs, across 6460-7517nm, providing51.1mW at 6790nm, with passive powerstability of ~2.3% rms (>1 hour) andfrequency stability of 1.8GHz (>1 minute),in high-beam quality.
EC-3.3 TUE 17:00Spin pattern formation in cold atoms viathe single-mirror feedback scheme�I. Kresic1, P. Gomes1, A. Camara2, G.Labeyrie2, G.-L. Oppo1, W. Firth1, G. Robb1,E. Tesio1, P. Gri�n1, A. Arnold1, R. Kaiser2,and T. Ackemann1; 1University of Strath-clyde, Glasgow, United Kingdom; 2InstitutNon Lineaire de Nice, Valbonne, France�e spontaneous formation of hexagonalpatterns in cold atomic samples with light-mediated coupling is investigated. We ob-serve a spin instability and study the in�u-ence of optical molasses on dynamics for ared detuned pump beam.
EA-7.5 TUE 17:00How a Classical Radio-FrequencyExperiment can Inspire Measurement ofQuantum Two-Mode Quantum SqueezingY. Shaked, H. Sanhedrai, G. Bashan, T. Geller,and �A. Pe’er; Bar Ilan University, RamatGan, IsraelFrom analogy to RF theory and applications,we devise general measurement schemes fortwo-mode squeezing using nonlinear opticalmixing as the physical detector. We providecomplete quantum and classical theory, withRF and optical demonstrations.
TF-2.3 TUE (Tech Focus) 17:00Additive and Subtractive3D-Microfabrication ofMicro/Nanostructures�Y. Lu; University of Nebraska - Lincoln, Lin-coln, United StatesIn this study, we developed a complementary3D micro/nanofabrication process by inte-grating both additive two-photon polymer-ization (TPP) and subtractive multi-photonablation (MPA) into a single platform offemtosecond-laser direct writing process.
CF-3.5 TUE 17:00Self-Compressed to Sub-�ree OpticalCycles Multi-millijoule mid-IR Pulses:Balancing between SolitonicSelf-Compression and Spatial Collapse�V. Shumakova1, P. Malevich1, S.Ališauskas1, A. Voronin2, A. Zheltikov2,3,D. Faccio4, D. Kartashov5, G. Gitzinger6, R.Maksimenka6, N. Forget6, A. Baltuška1,7,and A. Pugžlys1,7; 1Photonics InstituteVienna Univ. of Technology, Vienna, Austria;2Physics Dep., International Laser Center,M.V. Lomonosov Moscow State Univ.,Moscow, Russia; 3Dep. of Physics and As-tronomy, Texas A&M Univ., College StationTX, United States; 4Institute of Photonicsand Quantum Sciences, Edinburgh, UnitedKingdom; 5Institute for Optics and QuantumElectronics, Friedrich-Schiller Univ. Jena,Jena, Germany; 6FASTLITE, Valbonne,France; 7Center for Physical Sciences &Technology, Vilnius, LithuaniaWe demonstrate self-compression to sub-three �eld cycles of mid-IR ultrashort pulseswith peak powers of hundreds of gigawattsthru decoupling of nonlinear phase neededfor soliton self-compression from spatialmodulation instability, leading to multiple�lamentation.
CD-10.6 TUE 17:15Frequency conversion in AlGaAsmicrodisks at 1.55 micron�N. Morais1, S. Mariani1, A. Lemaître2, S.Ducci1, I. Favero1, and G. Leo1; 1UniversitéParis Diderot, Laboratoire MPQ, Paris,France; 2CNRS Laboratoire de Photonique etNanostructures, Marcoussis, FranceWe report on the demonstration of CWSHG in AlGaAs suspended microdisks onGaAs pedestal, with FF wavelength around1.55 micron and an e�ciency comparable tostate-of-the-art monolithic telecom devices.
EC-3.4 TUE 17:15Cavity Optomechanics with FreeElectronsA. Niguès1, A. Siria1, and �P. Verlot2;1Ecole Normal Supérieure, Paris, France;2Université Claude Bernard Lyon 1, Villeur-banne, FranceWe demonstrate that the coupling betweena focused electron beam and a suspendednanowire enables massive cooling of thenanomechanical motion. Our result extendsthe phenomenology of cavity optomechan-ics to any topologically con�ned interaction.
EA-7.6 TUE 17:15Joint Spectral Density measurement ofenergy correlations of photon pairsgenerated by a silicon microringresonator.D. Grassani1, A. Simbula1, M. Galli1, S.Pirotta1, T. Baehr-Jones2, M. Hochberg2,N. Harris3, C. Galland4, M. Liscidini1,and �D. Bajoni5; 1Dipartimento di Fisica,Universita degli Studi di di Pavia, Pavia,Italy; 2Coriant Advanced Technology Group,Naperville, United States; 3Department ofElectrical Engineering and Computer Science,Massachusetts Institute of Technology, Cam-bridge, United States; 4Stuttgart University,Stuttgart, United States; 5Dipartimento di In-gegneria Industriale e Informazione, Univer-sita degli Studi di Pavia,, Pavia, ItalyWe use stimulated four wave mixing to mea-sure the Joint Spectral Density of photonpairs emitted by a microring resonator with2pmx4pm spectral resolution. �e pairs canbe emitted uncorrelated or strongly corre-lated.
CF-3.6 TUE 17:15High-Energy Compression of Mid-IRPulses in a Bulk Nonlinear Crystal�M. Bache and B. Zhou; DTU Fotonik, Tech-nical University of Denmark, Kgs. Lyngby,DenmarkA mid-IR high-energy external compres-sor is proposed using self-defocusing spec-tral broadening in bulk quadratic nonlinearcrystals pumped in the anomalous disper-sion regime, followed by a dispersion com-pensation stage. Simulations show e�cient,high-quality few-cycle compressed pulses.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCK-9.5 TUE 17:00Optically Controlled Elastic Microcavities�S. Nocentini1, A. Flatae2, M. Burresi1, H.Zeng1, S. Wiegele2, C. Parmeggiani1, H.Kalt2, and D. Wiersma1; 1European Labo-ratory for non Linear Spectroscopy (LENS),University of Florence, Sesto Fiorentino, Italy;2Institute of Applied Physics, Karlsruhe In-stitute of Technology (KIT), Karlsruhe, Ger-manyReversible and stable tuning of resonantwavelengths is an important aim for opticalstructures in integrated chips. We presentthe photo-induced tuning of a whisperinggallery mode microlaser using the photo-response of liquid crystal elastomers.
CE-9.5 TUE 17:00Nonlinear optical properties of chalconesL. Abegão1, F. Santos1, M. Alencar1, �J.Rodrigues1, R. Fonseca2, E. Barbano2, C.Mendonça2, L. Misoguti2, and L. De Boni2;1Departamento de Física - UniversidadeFederal de Sergipe, São Cristóvão, Brazil;2Instituto de Física de São Carlos - USP, SãoCarlos, Brazil�ree types of Chalcones in solutions thatwere characterized with two techniques:Hyper-Rayleigh Scattering and Z-scan,which allowed us to determine the �rsthyperpolaribilities and spectral two-photonabsortion cross-sections.
CB-3.5 TUE 17:00Low-Repetition-Rate (112 MHz)High-Peak-Power ModelockedSemiconductor Disk Laser in a MultipassCavity Geometry�L. McKnight, P. Schlosser, A. Lagatsky, M.Dawson, and J.-M. Hopkins; Fraunhofer Cen-tre for Applied Photonics, Glasgow, UnitedKingdomWe demonstrate a modelocked semiconduc-tor disk laser with a low repetition rate of 112MHz, 120 mW of power and a pulse dura-tion of 2.3 ps in a novel eight-gain-pass cav-ity geometry.
CH-5.5 TUE 17:00Simple Technique to Determine theDiameter of Etched Optical Fibres In-situwith Sub-micron Precision Accuracy�M.Namiq andM. Ibsen;Optoelectronics Re-search Centre, Southampton, United King-domBy monitoring the wavelength-shi�s, inreal-time, of higher-order mode Bragg-resonances in a �bre grating duringcladding-etching, we show that it is possibleto determine the diameter of the �brewith ~0.5micron accuracy, for diameters<25micron.
CG-2.5 TUE 17:00Direct and e�cient high harmonicgeneration at 10 MHz repetition rate�S. Hädrich1,2, M. Krebs1, A. Ho�mann1,A. Klenke1,2, J. Rothhadt1,2, J. Limpert1,2,and A. Tünnermann1,2,3; 1Friedrich-Schiller-Universität Jena, Abbe Center of Photonics,Institute of Applied Physics, Jena, Germany;2Helmholtz-Institute Jena, Jena, Germany;3Fraunhofer Institut for Applied Optics andPrecision Engineering, Jena, GermanyNonlinear compression in a Kagome PCFyields 7 �J, 31 fs pulses at 10.7 MHz repe-tition rate (76 W average power), which areused for e�cient HHG. Up to 50 �Ware ob-tained per harmonic.
CK-9.6 TUE 17:15Fabrication of Crystalline WGMMicrocavity using Ultra-precisionMachining to Reveal the Size Dependenceof�ermo-opto-mechanical Oscillation�H. Itobe, Y. Nakagawa, S. Azami, Y. Kak-inuma, and T. Tanabe; Keio University, Yoko-hama, JapanWe have demonstrated that a high Q crys-talline WGM microcavity can be obtainedby employing ultra-precision machining. Itallowed us to design the diameter of cavi-ties, whichmade it possible to study thermo-opto-mechanical oscillation.
CE-9.6 TUE 17:15Giant Hyper-Rayleigh ScatteringObserved in a Class of Chiral PolymersM.G. Vivas’1, G. Koeckelberghs2, C.R.Mendonça3, and �L. De Boni3; 1Institutode Ciência e Tecnologia, UniversidadeFederal de Alfenas, Poços de Caldas,Brazil; 2Laboratory of Polymer Synthesis,Katholieke Universiteit Leuven, Heverlee,Belgium; 3Instituto de Física de São Carlos,Universidade de São Paulo, São Carlos,BrazilIn this work, we report the giant �rst-orderhyperpolarizability of four chiral donorem-bedded polybinaphthalenes polymersin which the increment on the nonlin-ear optical e�ect is related to the chiralconformation adopted by the samples.
CB-3.6 TUE 17:15Carrier-Dependent Nonlinear Lens in aVECSEL Gain MediumA. Quarterman1, E. Shaw2, and �K. Wilcox1;1University of Dundee, Dundee, UnitedKingdom; 2University of Southampton,Southampton, United Kingdom�e carrier-density-dependent nonlinearlens in a 1050 nm VECSEL gain mediumwas measured using a re�ection-type z-scansystem. �e magnitude of the lensing islarge enough to perturb a VECSEL cavityunder typical operating conditions.
CH-5.6 TUE 17:15A Comparison Between Multimode TipAnd Suspended Core FluorescenceOptical Fibre SensorsE. Schartner1,2, �G. Tsiminis1,2, M.Henderson1, M. Hutchinson1,2, and T.Monro1,2; 1ARC Centre of Excellence forNanoscale BioPhotonics, �e University ofAdelaide, Adelaide, Australia; 2Institute forPhotonics and Advanced Sensing, School ofPhysical Sciences,�e University of Adelaide,Adelaide, AustraliaWe examine the potential sensitivity im-provements by employing suspended-coremicrostructured �bres rather than conven-tional multi-mode �bres for �uorescencesensing applications, demonstrating experi-mentally that they show a larger �uorescencesignal for a given excitation power.
CG-2.6 TUE 17:15Ptychographic measurements ofhigh-order harmonics generated on solidtarget�a. leblanc, s. monchoce, s. kahaly, and f.quere; CEA, Saclay, FranceWe present the �rst experimental measure-ments of the amplitude and phase spatialproperties of high-order harmonic sourcesgenerated by ultraintense laser pulses onsolid targets, using a ptychographic lenslessimaging.
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HALL B013:00 – 14:00CD-P: CD Poster Session
CD-P.1 TUEOptical nonlinear barium titanate thin �lmsintegrated in silicon photonic devices�S. Abel1, T. Stöferle1, C. Marchiori1, D. Caimi1, L.Czornomaz1, M.D. Rossell2, R. Erni2, M. Sousa1, B.J.O�rein1, and J. Fompeyrine1; 1IBM Research - Zurich,Rüschlikon, Switzerland; 2Electron Microscopy Center,Empa, Swiss Federal Laboratories for Materials Scienceand Technology, Dübendorf, SwitzerlandWe demonstrate the integration of optical nonlinearbarium titanate thin �lms into silicon photonic struc-tures. �erefore, we designed, fabricated, and success-fully characterized passive and active slot waveguidestructures such as couplers, interferometers, and ringresonators.
CD-P.2 TUEA Photonic Saturable Absorber in ChalcogenideGlass�S. Minardi1, G. Cheng2,3, C. D’Amico2, and R.Stoian2; 1Institute of Applied Physics, Jena, Germany;2Laboratoire Hubert Curien, S. Etienne, France; 3Xi’anInstitute of Optics and Precision Mechanics, Shaanxi,China, People’s Republic of (PRC)We present the �rst experimental and numerical char-acterization of a photonic saturable absorber manufac-tured by laser writing in a highly nonlinear chalcogenideglass. We observed the saturation threshold at 2 kW forpicosecond pulse excitation.
CD-P.3 TUEAcoustic sources in water designed and triggered byoptical �lamentation�C. Milian1, V. Jukna1,2, A. Couairon1, A. Houard2, andA. Mysyrowicz2; 1Ecole Polytechnique, Palaiseau, France;2Ecole Polytechnique, Palaiseau, FranceIn this work we study bymeans of numerical simulationsthe in�uence of the input pulse chirp on the acousticwaves generated in water. We �nd that the shape of theexcited electron plasma strongly in�uence sound propa-gation.
CD-P.4 TUEHighy Nonlinear AlGaAs Waveguides for BroadbandSignal Generation�C. Lacava1,2, M. Strain3, V. Pusino4, R. Marchetti1, P.Minzioni1, M. Sorel4, and I. Cristiani1; 1Dipartimento diIngegneria Industriale e dell’Informazione, Università diPavia, Pavia, Italy; 2Optoelectronic Research Centre, Uni-versity of Southampton, Southampton, United Kingdom;3Institute of Photonics, Department of Physics, University
of Strathclyde, Glasgow, United Kingdom; 4School of Engi-neering, University of Glasgow, Glasgow, United KingdomHere we describe the nonlinear characterization of Al-GaAs waveguides. We show the continuos wave Fourwave mixing characterization together with the supercontinuum generation obtained by using a femtosecondoptical source beam.
CD-P.5 TUEExtreme localization of rare events on photonic chips�C. Liu1, R. van der Wel2, N. Rotenberg2, K. Kuipers2,T. Krauss3, A. Di Falco4, and A. Fratalocchi1;1PRIMALIGHT, Faculty of Electrical Engineering; Ap-plied Mathematics and Computational Science, KingAbdullah University of Science and Technology., �uwal,Saudi Arabia; 2Center for Nanophotonics, FOM InstituteAMOLF, Amsterdam, �e Netherlands; 3Departmentof Physics, University of York, York, United Kingdom;4School of Physics and Astronomy, University of St.Andrews, St. Andrews, United KingdomBy using theory and experiments, we investigate a newmechanism based on spontaneous synchronization ofrandom waves which generates ultrafast subwavelengthrare events in integrated photonic chips.
CD-P.6 TUESecond Harmonic Generation from ZnONanostructured Surface by Femtosecond Laser Pulsesat Near Damage�reshold Intensities�Z. Samsonova1,2, R. Hollinger1, D. Kartashov1, M.Zürch1, R. Röder3, L. Tre�ich3, C. Ronning3, and C.Spielmann1; 1Institute for Optics and Quantum Electron-ics, Abbe Center of Photonics, Friedrich-Schiller Univer-sity Jena, Jena, Germany; 2Helmholtz Institute Jena, Jena,Germany; 3Institute for Solid State Physics, Friedrich-Schiller University Jena, Jena, GermanyWereport experimental results on second harmonic gen-eration from nanostructured ZnO samples by high in-tensity femtosecond laser pulses. Abrupt dependencebeyond quadratic law of the second harmonic yield onthe pump energy is demonstrated.
CD-P.7 TUENonlinear imaging of vertically aligned semi-conductor nanowires using focused vector beams�G. Bautista1, J. Mäkitalo1, Y. Chen2, V. Dhaka2, M.Grasso1, L. Karvonen2, H. Jiang3, M.J. Huttunen4, T.Huhtio2, H. Lipsanen2, and M. Kauranen1; 1Departmentof Physics, Tampere University of Technology, Tam-pere, Finland; 2Department of Micro and Nanosciences,Aalto University, Aalto, Finland; 3Department of Ap-plied Physics and Nanomicroscopy Center, Aalto Univer-sity, Aalto, Finland; 4COMPCentre of Excellence, Depart-ment of Applied Physics, Aalto University, Aalto, Finland
We show that vertically-aligned GaAs nanowires arepreferentially excited by the longitudinal �elds of fo-cused vector beams. Strong second-harmonic signalsprovided by focused radial polarization allow such wiresto be addressed in their native environment.
CD-P.8 TUEAnderson Localization In Optical Mesh LatticesRealized In Time Domain�I. Vatnik1,2, A. Tikan2, D. Churkin1,2,3, and A.Sukhorukov4; 1Institute of Automation and Electrome-try SB RAS, Novosibirsk, Russia; 2Novosibirsk State Uni-versity, Novosibirsk, Russia; 3Aston Institute of PhotonicTechnologies, Birmingham, United Kingdom; 4NonlinearPhysics Centre, Research School of Physics and Engineer-ing, Australian National University, Canberra, AustraliaWe experimentally demonstrate Anderson localizationfor optical pulses in time domain in a synthetic pho-tonics lattice implemented with coupled �ber loops. Wediscuss interplay of photonic band-gaps and disorder insuch lattices.
CD-P.9 TUEPhase-sensitive resonant four-wave mixing in siliconnitride microresonators�A. Fülöp1, C. Krückel1, D. Castelló-Lurbe2, E. Silvestre2,and V. Torres-Company1; 1Chalmers University of Tech-nology, Göteborg, Sweden; 2Universitat de València, Bur-jassot, SpainWe have investigated the phase sensitive nature of res-onant four-wave mixing in silicon nitride microres-onators. �e generated idlers show a clear periodic be-havior as a function of the input signal’s phase matchingour simulations.
CD-P.10 TUETransverse optical probing of axial distribution oflight-driven optomechanical resonances indual-nanoweb �bre�J.R. Koehler, A. Butsch, R.E. Noskov, and P.S.J. Russell;Max Planck Institute for the Science of Light, Erlangen,GermanyGiant resonant optomechanical nonlinearities in dual-nanoweb �bres result in frequency comb generation foronly a few mW of CW pump light. Optical side-probingcon�rms the existence of 2-cm-localized acoustic reso-nances caused by structural nonuniformities.
CD-P.11 TUEBroadband all-optical �ber transistors�B. Gholipour1,2, J.Y. Ong1, P. Bastock2, C. Craig2, K.Khan2, D. Hewak2, and C. Soci1; 1Centre for disruptivePhotonic Technologies, Nanyang Technology University,Singapore, Singapore; 2Optoelectronics Research Centre,
University of Southampton, Southampton, United King-domBroadband photoinduced e�ects in chalcogenide �bersare utlised for realising an all-optical room temperaturetransistor. We show single and multi-wavelength opera-tion across the visible and near infrared parts of the spec-trum in a mass-manufacturable platform.
CD-P.12 TUEOptical simulation of photon-pair generation innonlinear lossy waveguidesM. Gräfe1, D. Antonosyan2, A. Solntsev2, A. Szameit1,and �A. Sukhorukov2; 1Institute of Applied Physics, AbbeCenter of Photonics, Friedrich-Schiller-Universitat, Jena,Germany; 2Nonlinear Physics Centre, Research School ofPhysics and Engineering, Australian National University,Canberra, AustraliaWe demonstrate a coupled-waveguide platform whichrealizes classical optical simulation of quantum photon-pair generation through spontaneous parametric down-conversion in a nonlinear lossy waveguide. We experi-mentally map the biphoton creation vs. the phase mis-match and loss.
CD-P.13 TUEFour Wave Mixing in CMOS Compatible High OrderRing Resonators�J. Li1, A. Pasquazi2, L. Di Lauro2, B. Little3, D.J. Moss4,R. Morandotti5, and S.T. Chu1; 1City University of HongKong, Hong Kong, Hong Kong; 2University of Sussex,Brighton, United Kingdom; 3Xi’an institute of Optics,Xi’an, China, People’s Republic of (PRC); 4RMIT, Mel-bourne, Australia; 5INRS-EMT, Varennes, CanadaWe report wavelength conversion via four wave mixingin showed in a CMOS compatible 5th order microringresonator at mW powers.
CD-P.14 TUEChemical composition of laser induced atmosphericaerosols�D. Mongin1, J.G. Slowik3, E. Schubert1, J.-G.Brisset1,4, N. Berti1, A. Prévôt3, U. Baltensperger3, J.Kasparian2, and J.-P. Wolf1; 1University of Geneva,GAP-Biophotonics, Geneva, Switzerland; 2University ofGeneva, GAP-Nonlinear, Geneva, Switzerland; 3PaulScherrer Institut, Laboratory of Atmospheric Chem-istry, Villigen, Switzerland; 4Max-Born Institut, Berlin,Germany�e contribution has been withdrawn by the authors.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
HALL B0CD-P.15 TUEMeasuring the Contribution of theNon-instantaneous Nonlinear Refraction in CarbonDisul�de and Acetone by Nonlinear PolarizationRotation�M. Miguez, E. Barbano, S. Zilio, and L. Misoguti; Insti-tute of Physics of Sao Carlos - USP, Sao Carlos, BrazilContributions of non-instantaneous refractive nonlin-earities in carbon disul�de and acetone are investi-gated by single-beam nonlinear ellipse-rotation mea-surements. Pulse duration was used to discriminate theinstantaneous and the non-instantaneous signals. Silicawas used as reference sample.
CD-P.16 TUEAll-optical control of form birefringence�S. Bej, J. Tervo, Y. Svirko, and J. Turunen; Institute ofPhotonics, University of Eastern Finland, Joensuu, Fin-landNumerical experiments reveal that subwavelengthdi�raction gratings with isotropic Kerr nonlinear me-dia can be exploited to construct birefringent deviceswhere the degree of birefringence can be �ne tuned withvariation in the incident light intensity.
CD-P.17 TUEHigh-energy, high-power, near- and mid-IRpicosecond pulses generated by a�ber-MOPA-pumped optical parametric generatorand ampli�er�L. Xu, H.-Y. Chan, S.-u. Alam, D. Richardson, and D.Shepherd; Optoelectronics Research Centre, Southamp-ton, United KingdomWe present an e�cient picosecond optical parametricgenerator based on MgO:PPLN, producing 3.8 �J and1.7 �J signal and idler pulse energies when pumped by again-switched-diode-seeded Yb-doped �ber MOPA sys-tem employing direct ampli�cation
CD-P.18 TUESpectral Broadening and Peak Power Limitations ofNormally Dispersive Photonic Crystal Fibres forHigh-Power fs Light Sources�M. Seidel1, X. Xiao1, A. Hartung2, L. Lötscher1, A.Apolonski1,3, and F. Krausz1,3; 1Max-Planck-Institut fürQuantenoptik, Garching, Germany; 2Leibniz-Institute ofPhotonic Technology (IPHT), Jena, Germany; 3Ludwig-Maximilians-Universität München, Garching, GermanyPeak power and peak irradiance limitations of photoniccrystal �bres with various mode-�eld-diameters are in-vestigated with 250-fs input pulses. Maximal spectralbroadening factors increase with decreasing core sizefrom 18 to 50.
CD-P.19 TUEFiber Master Oscillator Power Ampli�er withIntegrated Raman-Shi�er for Nonlinear,Multiphoton Microscopy�S. Karpf1, M. Eibl1,2, W. Wieser1, T. Klein1, andR. Huber1,2; 1Ludwig-Maximilians-Universität, Munich,Germany; 2Universität zu Lübeck, Lübeck, GermanyA �ber based laser is presented based on a master os-cillator power ampli�er (MOPA). �is multi-color laserenables time-encoded (TICO) detection of stimulatedRaman scattering (SRS) spectroscopy, SRS microscopy,and Two-Photon Excitation Fluorescence (TPEF) mi-croscopy.
CD-P.20 TUETowards telecom frequency comb generation inAlGaAs microrings�N. Morais1, O. Stepanenko1, A. Lemaître2, C. Gomez2,T. Hansson3,4, G. Leo1, and S. Wabnitz3; 1UniversitéParis Diderot, Laboratoire MPQ, Paris, France; 2CNRSLaboratoire de Photonique et Nanostructures, Marcoussis,France; 3Dipartimento di Ingegneria dell’Informazione,Università di Brescia, Brescia, Italy; 4Department of Ap-plied Physics, Chalmers University of Technology, Gote-borg, SwedenWe report on the fabrication and characterization ofbandgap engineered AlGaAs microrings designed togenerate frequency combs in the near infrared via fourwave mixing.
CD-P.21 TUESecond Harmonic Generation from ZnWO4 SingleCrystal�A. Belardini1, P. Osewski2, E. Petronijevic1, D.A.Pawlak2, M. Centini1, and C. Sibilia1; 1Sapienza Univer-sità di Roma - SBAI Dept., Roma, Italy; 2Institute of Elec-tronic Materials Technology, Warsaw, ItalyWe measure nonlinear optical response from ZnWO4obtained by means of micro-pulling-down technique,annealed and not annealed. We found good second har-monic generation, especially from the annealed sample,and we modelled the conversion e�ciency
CD-P.22 TUEorthogonally polarized bright-dark pulse pair �berlaser with a large-angle tilted �ber grating�Z. Zhang;Nanjing University of Posts and Telecommuni-cations, Nanjing, China, People’s Republic of (PRC);AstonInstitute of Photonic Technologies, Birmingham, UnitedKingdomWe report on the generation of orthogonally polarizedbright-dark pulse pair in a mode-locked �ber laser withlarge-angle tilted �ber grating (LA-TFG). �e unique
polarization properties of the LA-TFG enable dual-wavelength orthogonally polarized mode-locking oper-ation.
CD-P.23 TUE�eory of the strong phonon-photon coupling in anoptical �ber taper�K. Phan Huy, J.-C. Beugnot, J.-C. Tchahame, and T.Sylvestre; FEMTO-ST, BESANCON, FranceWe theoretically investigate the conditions to observe thestrong phonon-photon coupling regime using Brillouinscattering in a submicron silica-based �ber taper. Rabioscillations can be observed for 700nm diameter �bertaper under high optical power.
CD-P.24 TUESingle Mode, Multimode Infrared Optical Switchingbased on Phase Change Materials Cored OpticalFibers�D.-M. Nguyen1,2, B. Gholipour1, L. Cui1, and C. Soci1;1Centre for disruptive photonic technologies, Nanyangtechnological University, Singapore, Singapore; 2CINTRACNRS/NTU/THALES,UMI 3288, Research Techno Plaza,Singapore, SingaporeWe present a new concept of an optical mode switchusing phase change materials cored optical �bers thatcan be triggered thermally by optical pulses to switchbetween single-mode and multimode operation attelecommunication wavelength.
CD-P.25 TUEMultimode Brillouin scattering in a long taperedphotonic crystal �ber�J.C. Tchahame Nougnihi1, J.-C. Beugnot1, H. Maillotte1,A. Kudlinski2, and T. Sylvestre1; 1FEMTO-ST institute,Besançon, France; 2IRCICA institute, Villeneuve d’Ascq,FranceWe investigate the stimulated Brillouin scattering in along tapered birefringent photonic crystal�ber and showthat the taper induces a broadband and multimode Bril-louin spectrum and a strong increase of the Brillouinthreshold power.
CD-P.26 TUEInvestigation of the grade of polarization of solitonsgenerated by soliton �ssion process in a twisted �ber�G. Beltán-Pérez1, I. Armas Rivera1, Y.-E. BracamontesRodriguez1, B. Ibarra-Escamilla2, M. Durán-Sánchez2,and E. Kuzin2; 1Benemérita Universidad Autonoma dePuebla, Facultad de Ciencias Fisico Matemáticas, Puebla,Mexico; 2Instituto Nacional de Astro�sica Optica y Elec-trónica, Puebla, MexicoWe found that a 0.7 ps pump pulse with high elliptic-ity introduced to a twisted �ber produces solitons with
a high grade of circular polarization while linear inputpolarization results in �uctuation of output polarization.
CD-P.27 TUEHigh-Sensitivity Measurement of NonlinearRefractive Indices of Noble GasesA. Blumenstein1, M. Kovacev2, U. Morgner2, P. Simon1,and �T. Nagy1,2; 1Laser-Laboratorium Göttingen e.V.,Göttingen, Germany; 2Institut für Quantenoptik, LeibnizUniversität Hannover, Hannover, Germany�e nonlinear refractive indices of noble gases were de-termined by measuring and simulating spectral broad-ening in a long hollow �ber. Reliable n2 values are gainedfor all noble gases including helium and neon.
CD-P.28 TUETunable visible dual-wavelength SHG from adiode-pumped PPKTP waveguide�K.A. Fedorova1, S.N. Turtaev1,2, I.O. Bakshaev3, D.A.Livshits3, and E.U. Rafailov1; 1Aston University, Birming-ham, United Kingdom; 2University of Dundee, Dundee,United Kingdom; 3Innolume GmbH, Dortmund, Ger-manyWe demonstrate a compact CW laser source in the vis-ible spectral region generating tunable dual-wavelengthSHG output from a PPKTP waveguided crystal using asingle laser diode. �e generation of sum-frequency ra-diation was also observed.
CD-P.29 TUEFi�h-order intensity autocorrelations of femtosecondlaser pulses by noncollinear six-wave mixing�K. Steponkevičius and V. Vaičaitis; Vilnius UniversityLaser Research Center, Vilnius, LithuaniaFi�h order autocorrelations obtained from six wavemix-ing in air have been registered for a wide range of laserintensity. �e in�uence of the instantaneous and delayedcontributions of ��h order optical nonlinearity is dis-cussed.
CD-P.30 TUESimultaneous second harmonic generation andconical refraction using a biaxial crystal�S. Grant1, S. Zolotovskaya1, T. Kalkandjiev2, W.Gillespie1, and A. Abdolvand1; 1University of Dundee,Dundee, United Kingdom; 2Conerefringent Optics SL,Barcelona, SpainSecond harmonic generation (SHG) and conical refrac-tion patterns from a single KTP crystal upon ps pulsedlaser pumping at 1064nm were simultaneously regis-tered. Types 0, I and II SHG are observed in non-phase-matched conditions.
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HALL B0CD-P.31 TUESecond Harmonic Generation and Pendulum E�ectunder Dynamical Di�raction at the Laue Scheme inDi�raction-�ick 1D PCsD. Kopylov1, V. Novikov1, S. Svyakhovskiy1, L. Frolova1,S. Chekalin2, V. Kompanets2, T. Murzina1, and �B.Mantsyzov1; 1Department of Physics, M. V. LomonosovMoscow State University, Moscow, Russia; 2Institute ofSpectroscopy RAS, Troitsk, Russia�e second harmonic generation in porous-silicon 1DPC at Laue geometry of di�raction are studied exper-imentally and theoretically. We have observed phase-matching and noncollinear quasi-phase-matching gen-eration caused by the interaction of Borrmann and anti-Borrmann modes.
CD-P.32 TUEIdentifying the role of the local density of opticalstates in frequency conversion of light in amicrocavity�E. Yüce1, H. �yrrestrup1, E. Peinke2, G. Ctistis1, J.Claudon2, J.-M. Gérard2, andW. L. Vos1; 1Complex Pho-tonic Systems (COPS), MESA+ Institute for Nanotechnol-ogy, University of Twente, 7500AE, Enschede,�e Nether-lands; 2CEA/INAC/SP2M, Nanophysics and Semiconduc-tor Laboratory, 38054, Grenoble, FranceWe study frequency conversion of light in a GaAs/AlAsmicrocavity that is switched within 300 fs. We iden-tify the role of the local density of optical states (LDOS)available to the newly generated light frequencies.
CD-P.33 TUEOptimal Femtosecond Pulse Energy Partitioning forAir Ionization�E. Schubert1, J.-G. Brisset1,2, M. Matthews1, A.Courjaud3, J. Kasparian4, and J.-P. Wolf1; 1GAP-Biophotonics, Université de Genève, Geneva, Switzerland;
2Max-Born Institut, Berlin, Germany; 3Amplitude Sys-tèmes, Pessac, France; 4GAP-Nonlinear, Université deGenève, Geneva, Switzerland�e contribution has been withdrawn by the authors.
CD-P.34 TUENonlinear Enhancement in a Coherently ExcitedMicrocavityS. Serna1,2, J. Oden1, M. Hanna1, C. Caer2, X.Le Roux2, C. Sauvan1, P. Delaye1, E. Cassan2, and�N. Dubreuil1; 1Laboratoire Charles Fabry, Institutd’Optique, CNRS, Univ Paris Sud, Palaiseau, France;2Institut d’Electronique Fondamentale, Université Paris-Sud 11, CNRS UMR 8622, Orsay, FranceEnhancement of nonlinear interactions in a coherentlyexcited silicon microcavity is demonstrated. Tailoredchirped pulses enable to maintain the cavity light local-ization e�ect, despite the resonance nonlinear frequencydri� driven by the free-carrier refractive e�ect.
CD-P.35 TUEGeneration of 0.7 W second harmonic picosecondpulses near 560 nm using a DBR diode laser and aridge-waveguide PPLN crystal�A. Kaltenbach, R. Bege, K. Paschke, and G. Tränkle;Ferdinand-Braun-Institut, Leibniz Institut für Höchstfre-quenztechnik, Berlin, GermanyPicosecond laser pulses near 1120nm from a DBR diodelaser are frequency doubled in a ridge-waveguide crys-tal. �e 558nm pulses reach a pulse power of 0.7W andshow very good pulse and beam characteristics.
CD-P.36 TUEPurity, Linewidth, and Real-Time Spectral Analysisof an Ampli�ed Pulsed Nested Cavity OpticalParametric Oscillator�D. Mammez1,2, J.-B. Dherbecourt1, M. Raybaut1, A.
Bresson1, N. Zahzam1, J.-M. Melkonian1, and A.Godard1; 1ONERA, Palaiseau, France; 2CNES, Toulouse,FranceWe study an optical heterodyne analysis of the spectralcontent of an ampli�ed nanosecond nested cavity OPO.�e beat waveform is recorded with broadband electron-ics (>12 GHz), enabling linewidth, purity, and real-timefrequency shi�s measurements.
CD-P.37 TUEComplex inhibition of picosecond pulsed highfrequency second harmonic generation by aperiodically poled stoichiometric LiTaO3�L. Oleg1, H. Hideki2,3, T. Tomohiro1, W. Satoshi1, T.Shunji2,3, and K. Kenji2,3; 1RIKEN,Wako, Japan; 2NIMS,Tsukuba, Japan; 3SWING Ltd., Tsukuba, JapanWe report experimental, temperature-controlled, pshigh-frequency second harmonic generation by a peri-odically poled LiTaO3 crystal for 1030 nm input radia-tion, and theoretical analysis revealing a complex mech-anism of observed conversion e�ciency inhibition, sat-uration and stabilization.
CD-P.38 TUEPhase transition in Laser multiple �lamentation�W. Ettoumi1, J. Kasparian2, and J.-P. Wolf1; 1GAP-Biophotonics, University of Geneva, Geneva, Switzerland;2GAP-Nonlinear, University of Geneva, Geneva, Switzer-land�e contribution has been withdrawn by the authors.
CD-P.39 TUEPlasma-Induced Emission of Tunable Few-CycleMid-IR Light in Gas-Filled Hollow-CorePCF:�eoretical Study�M. Cassataro, D. Novoa, J.C. Travers, and P.S.J. Russell;MPI for the Science of Light, Erlangen, Germany
Plasma-induced phase-matching, in gas-�lled kagomé-style hollow-core PCF, is shown theoretically to allowtunable dispersive wave emission of few-cycle pulses inthe mid-infrared. �e mechanism operates even in theabsence of a zero dispersion wavelength.
CD-P.40 TUEGaAs-based Phase Modulator for Laser Radiation at1070 nm�B. Arar, H. Wenzel, O. Brox, A. Maaßdorf, A. Wicht,M. Weyers, G. Erbert, and G. Tränkle; Ferdinand-Braun-Institut, Leibniz-Institut für Höchstfrequenztech-nik, Berlin, GermanyWe report the design and fabrication of a double het-erostructure GaAs/AlGaAs ridge waveguide electro-optic phase modulator for frequency stabilization of a1070 nm laser. �e measured modulation e�ciency us-ing the Fabry-Perot technique is 13 deg/(V.mm).
CD-P.41 TUEE�ciency-optimized, 30 W continuous-wave OPOemploying a variable re�ectivity volume Bragggrating�P. Zeil, N.�ilmann, V. Pasiskevicius, and F. Laurell;De-partment of Applied Physics, Royal Institute of Technol-ogy, Stockholm, SwedenWe propose a functional method to control the output-coupling of high-power cw OPOs, by employing a VBGwith continuously chirped di�raction e�ciency as out-put coupler. �e output optimized OPO delivers 30W at75% extraction e�ciency.
13:00 – 14:00CE-P: CE Poster Session
CE-P.1 TUENovel metal-glass-nanocomposite based substratesfor Surface-Enhanced Raman Spectroscopy�S. Zolotovskaya,W. Gillespie, and A. Abdolvand;Univer-sity of Dundee, Dundee, United KingdomNovel SERS substrates based on metal-glass nanocom-posites are proposed. Laser-assisted formation of regularmonolayers of high-density, narrow-size distribution sil-ver nanoparticles is reported. �e e�ect of size & particledensity on SERS signal is examined.
CE-P.2 TUEMeasuring the Optical Absorption of Spider SilksD. Little and �D. Kane; MQ Photonics Research Centre,Department of Physics and Astronomy, Macquarie Uni-versity, Sydney, AustraliaSpider silks have potential uses in photonics, howevertheir optical absorption is largely unknown. Here, amethod for measuring spider silk absorption is pre-sented and preliminary results on Plebs eburnus draglinesilks are discussed.
CE-P.3 TUETowards Fabrication of 10 W Class Planar WaveguideLasers: Analysis of Crystalline Sesquioxide LayersFabricated via Pulsed Laser Deposition�J. Grant-Jacob, T. Parsonage, S. Beecher, A. Choudhary,P. Hua, J. Mackenzie, D. Shepherd, and R. Eason; Opto-electronics Research Centre, Southampton, United King-dom�in �lm sesquioxide waveguide layers fabricated viapulsed laser deposition are characterised by XRD. Weshow that the crystal growth orientation a�ects the crys-talline structure and the optical propagation perfor-mance of the waveguides.
CE-P.4 TUEPreparation of Er, Eu, and Ce Co-doped Ta2O5 �inFilms Using a Simple Co-sputtering Method�K. Miura, T. Osawa, T. Suzuki, Y. Yokota, and O.Hanaizumi; Gunma University, Kiryu, JapanEr, Eu, and Ce co-doped Ta2O5 thin �lms were preparedusing a simple co-sputtering method for the �rst time,and yellow-light emission was observed from a sampleannealed at 900 �C for 20 min.
CE-P.5 TUEGlass-Ceramics with γ-Ga2O3:Co Nanocrystals:Novel Saturable Absorber for 1.6 �m Er LasersP. Loiko1, �N. Skoptsov1, O. Dymshits2, V. Vitkin3, A.
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HALL B0Kharitonov3, A. Zhilin2, I. Alekseeva2, S. Zapalova2, A.Malyarevich1, I. Glazunov1, and K. Yumashev1; 1Centerfor Optical Materials and Technologies, Belarusian Na-tional Technical University, Minsk, Belarus; 2NITIOMS.I. Vavilov State Optical Institute, St.Petersburg, Russia;3University ITMO, St.Petersburg, RussiaSpectroscopic and nonlinear properties are studied forglass-ceramics containing γ-Ga2O3:Co nanocrystals. Itsfeature is a red-shi� of the absorption band related with4A2�-
4T1�(4F) transition which makes it promising for
Q-switching of long-wavelength erbium lasers.
CE-P.6 TUECharacteristics of a Monolayer Graphene Q-switchedChannel Waveguide Laser with and without OutputCoupler near 1 �m�M.H. Kim1, S.Y. Choi1, T. Calmano2,3, D.-I. Yeom1, K.J.Ahn1, C. Kränkel2,3, G. Huber2,3, and F. Rotermund1;1Ajou University, Suwon, Korea, South; 2UniversitätHamburg, Hamburg, Germany; 3�e Hamburg Centre forUltrafast Imaging, Hamburg, GermanyCharacteristics of a Q-switched channel waveguide laseroperating near 1 �m are studied in two di�erent con-�gurations. Monolayer graphene deposited onto outputcoupler and end facet of waveguide is used as saturableabsorber for Q-switching.
CE-P.7 TUEElectrically tuneable group velocity dispersion inphotonic liquid crystal �bers measured byinterference of supercontinuum pulses�M. Wahle and H.-S. Kitzerow; University of Paderborn,Paderborn, Germany�e in�ltration of solid-core photonic crystal �bers withliquid crystals leads to a photonic band gap waveguidewhose waveguiding properties such as group delay anddispersion can be electrically controlled.
CE-P.8 TUEFusion splicing of silicon optical �bres�L. Xiao1, N. Healy1, U. Gibson2, T. Hawkins3, M. Jones3,J. Ballato3, and A. Peacock1; 1Optoelectronics ResearchCentre, University of Southampton, Southampton, UnitedKingdom; 2Department of Physics, Norwegian Univer-sity of Science and Technology, Trondheim, Norway; 3�eCenter for Optical Materials Science and Engineering,Technologies (COMSET), Department ofMaterial Scienceand Engineering, Clemson, United States�e �rst splicing experiments between silicon optical �-bres (SOFs) and conventional �bres are investigated. Anoptimized fusion splicing approach for a polycrystallineSOF is demonstrated and the material properties a�ersplicing are characterized.
CE-P.9 TUEE�cient Organic-Inorganic Hybrid WhiteLight-Emitting Diodes with High Color RenderingIndex�K.-J. Chen1,2, Y.-C. Lai1, B.-C. Lin1, C.-C. Lin3, S.-H.Chiu1, Z.-Y. Tu1, M.-H. Shih4, P. Yu1, P.-T. Lee1, X. Li2,H.-F. Meng5, G.-C. Chi1, T.-M. Chen6, and H.-C. Kuo1;1Department of Photonics & Institute of Electro-OpticalEngineering, National Chiao Tung University, Hsinchu,China, Republic of (ROC); 2Department of Electrical andComputer Engineering, University of Illinois at Urbana-Champaign Urbana, Illinois, China, Republic of (ROC);3Institute of Photonic System, National Chiao Tung Uni-versity, Tainan, China, Republic of (ROC); 4ResearchCenter for Applied Sciences, Academia Sinica, Taipei,China, Republic of (ROC); 5Institute of Physics, Na-tional Chiao Tung University, Hsinchu, China, Republicof (ROC); 6Phosphors Research Laboratory, Departmentof Applied Chemistry, National Chiao Tung University,Hsinchu, China, Republic of (ROC)�is study demonstrates high quality hybrid white LEDwith poly�uoren (PFO) polymer and quantum dot (QD)materials by dispensing method at the di�erent corre-lated color temperature (CCT) for cool and warm colortemperature.
CE-P.10 TUEHigh Quality Liquid-type Quantum Dots WhiteLight-Emitting Diode�T.-L. Shen1, K.-J. Chen1, C.-W. Sher2, H.-V. Han1, K.-Y. Wang3, J.-R. Li1, C.-C. Lin3, M.-H. Shih4, C.-C. Fu2,and H.-C. Kuo1; 1Department of Photonics & Instituteof Electro-Optical Engineering, National Chiao Tung Uni-versity, Hsinchu, China, Republic of (ROC); 2Departmentof Power Mechanical Engineering, National Tsing HuaUniversity, Hsinchu, China, Republic of (ROC); 3Instituteof Photonic System, National Chiao Tung University,Hsinchu, China, Republic of (ROC); 4Research Center forApplied Sciences, Academia Sinica, Taipei, China, Repub-lic of (ROC)High quality quantum dots white LED is investigated byliquid-type Quantum Dots package. �is novel packag-ing scheme could produce pure white LED and the CRIvaluse could acheive 90.
CE-P.11 TUEAn Indium Tin Oxide Metamaterial Filter for theTerahertz regime: Design, Fabrication andCharacterization�T. Takan1, M.A. Nebioglu1, M. Kurt2, Y. Demirhan2, L.Ozyuzer2, C. Sabah3, and H. Altan1; 1Middle East Tech-nical University, Physics Department, Ankara, Turkey;2Izmir Institute of Technology, Physics Department, Izmir,Turkey; 3Middle East Technical University - Northern
Cyprus Campus, Department of Electrical and Electron-ics Engineering, Güzelyurt, Northern Cyprus, Turkish Re-public ofFishnet structures with sub-micron thick, indium tin ox-ide thin�lm, patterned on quartz substrates are inves-tigated by both our home-built terahertz time domainspectroscopy and CW tunable THz systems and com-pared to FDTD and FDFD simulations.
CE-P.12 TUELaser Power Density Dependent Emission in Tb3+,Tm3+, Yb3+ Co-doped NaYF4 UpconversionPhosphors�X. Xue, T. Cheng, D. Deng, L. Zhang, L. Liu, T.Suzuki, and Y. Ohishi; Research Center for Advanced Pho-ton Technology, Toyota Technological Institute, Nagoya,JapanLaser power density dependent energy transfer fromTm3+ to Tb3+ was investigated in Tm3+, Tb3+, Yb3+co-doped NaYF4 upconversion phosphors. �e energytransfer occurs e�ectively in the case of low power den-sity.
CE-P.13 TUERotation of the Dielectric Frame and Optical Axes inMonoclinic KRE(WO4)2 (RE = Gd, Y or Lu) Crystals�P. Loiko1, P.L. Inácio2, P. Segonds2, A. Peña2, J. Debray2,S. Douillet2, C. Félix2, B. Boulanger2, D. Rytz3, K.Yumashev1, V. Filippov4, S. Guretsky4, X. Mateos5, andM.C. Pujol5; 1Center for Optical Materials and Tech-nologies, BNTU, Minsk, Belarus; 2CNRS, Institute NEEL,Grenoble, France; 3FEE, GmbH, Idar-Oberstein, Ger-many; 4National Academy of Sciences of Belarus, Minsk,Belarus; 5FiCMA-FiCNA, Universitat Rovira i Virgili,Tarragona, Spain�e dielectric frame rotation as a function of the wave-length is measured in monoclinic double tungstates,KRE(WO4)2, where RE = Gd, Y, Lu. Consequence onthe optical axes orientation and conical refraction angleis reported.
CE-P.14 TUEMagnetic circular polarization of luminescence inGa/Bi and Al/Bi co-doped silica glasses�O. Laguta1, H. El Hamzaoui1, M. Bouazaoui1, V.Arion2, and I. Razdobreev1; 1University Lille-1, Vil-leneuve d’Ascq, France; 2Institute of Inorganic Chemistry,University of Vienna, Vienna, AustriaMagnetic circular polarization of luminescence inGa(Al)/Bi doped silica was studied. �e results of ourexperiments rule out the assumptions of the isolated Bis-muth ions as a possible origin of the NIR PL.
CE-P.15 TUEAnti-Stokes photoluminescence in Ga/Bi co-dopedsol-gel silica glass�O. Laguta1, H. El Hamzaoui1, M. Bouazaoui1, V.Arion2, and I. Razdobreev1; 1University Lille-1, Vil-leneuve d’Ascq, France; 2Institute of Inorganic Chemistry,University of Vienna, Vienna, AustriaUnusual temperature dependence of anti-Stokes photo-luminescence in Ga/Bi co-doped silica was discoveredand investigated. �e proposed model satisfactorily ex-plains all the experimental features.
CE-P.16 TUERevealing the Dynamic of Excited State ProtonTransfer of a Novel π- conjugated SalicylideneChromophoreM. Vivas1,2, J. Germino3, C. Barbosa3, L. De Boni1,T. Atvarz3, and �C. Mendonca1; 1Universidade de SãoPaulo, São Carlos, Brazil; 2Universidade Federal de Alfe-nas, Poços de Caldas, Brazil; 3Universidade Estadual deCampinas, Campinas, BrazilWe have carefully studied the excited state intramolec-ular proton transfer of a novel pi-conjugated salicyli-dene chromophore. For that, we employed the white-light femtosecond pump-probe technique and the Den-sity Functional�eory.
CE-P.17 TUEDistributed Feedback Lasers based on DopedPhotochromic Liquid-Crystalline PolymerL. Goldenberg1, V. Lisinetskii2, �A. Ryabchun3,4, A.Bobrovsky4, and S. Schrader2; 1Plasmachem GmbH,Berlin, Germany; 2Technical University of Applied Sci-ences Wildau, Wildau, Germany; 3Fraunhofer Institutefor Applied Polymer Research, Potsdam-Golm, Germany;4Faculty of Chemistry, Moscow State University, Moscow,RussiaLiquid crystalline azobenzene-containing side-chaincopolymer was employed as matrix material for DFBlasers based on orientation gratings. Laser wavelengthtunning by changing the angle between the liquid crys-tal director and the grating vector was demonstrated.
CE-P.18 TUEEpitaxial lateral overgrowth of GaAs on (001) Sinano-trenches�Y. He, J. Wang, H. Hu, Q. Wang, Y. Huang, and X. Ren;Beijing University of Posts and Telecommunications, Bei-jing, China, People’s Republic of (PRC)High-quality widespread GaAs thin �lms with RMSroughness value of 6.29 nm (10um * 10um) have beenobtained on Si nano-trenches using epitaxial lateralovergrowth by MOCVD. Pre-epi cleaning process andgrowth procedures are optimized.
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HALL B0CE-P.19 TUEDefect Compatible Defect Engineering of Eu-dopedgallium nitride for red LED applicationsB. Mitchell1, D. Timmerman2, W. Zhu2, Y. Fujiwara2,and �V. Dierolf3; 1Department of Physics and Astron-omy, University of Mt. Union, Alliance, United States;2Division of Materials andManufacturing Science, Grad-uate School of Engineering, Osaka University, Osaka,Japan; 3Department of Physics, Lehigh University,, Beth-lehem, United StatesWe report about the challenges related to the presenceof oxygen in europium doped gallium nitride that hasthe potential as active layer for red nitride-based LEDs.Ways to overcome them will be discussed.
CE-P.20 TUEDispersion in THz waveguides with scaledmicrostructure�G. Town1, S. Ghatrehsamani1, S. Alessio2, O. Bang2,and P. Jepsen2; 1Dept. Engineering, Macquarie Univer-sity, North Ryde, Australia; 2Dept. Photonics Engineering,Danish Technical University, Lyngby, Denmark�eoretical and experimental results are presented con-cerning the dispersion properties of microstructuredpolymer THz waveguides in which the microstructurescales with distance from the waveguide axis.
CE-P.21 TUEPrecise Optical Absorption Measurement ofNonlinear-Optical CrystalsO. Ryabushkin1,2, �A. Konyashkin1,2, andO. Vershinin1,2;1Moscow Institute of Physics and Technology, Dolgoprud-nyy, Russia; 2NTO ’IRE-Polus’, Fryazino, RussiaMethod of piezoelectric laser calorimetry is proposedfor determination of nonlinear-optical crystal opticalabsorption coe�cients by measuring kinetics of crys-tal temperature-dependent piezoelectric resonance fre-quency during interaction with laser radiation
CE-P.22 TUERare-earth doped sesquioxides for lasers in themid-infrared spectral range�P. von Brunn1, A. Heuer1,2, and C. Kränkel1,2; 1Instituteof Laser-Physics, Hamburg, Germany; 2�e HamburgCentre of Ultrafast Imaging, Hamburg, GermanyWe explore the suitability of sesquioxides doped with therare-earth ions Ho3+, Er3+, Tm3+, Pr3+ and Dy3+ forlasing transitions in the near- and mid-infrared spectralrange.
CE-P.23 TUETemperature Gradient of Nonlinear-Optical Crystalsin Process of Second Harmonic Generation�A. Baranov1,2, A. Konyashkin1,2, and O. Ryabushkin1,2;
1Moscow Institute of Physics and Technology (StateUniversity), Dolgoprudnyy, Russia; 2NTO ”IRE-Polus”,Fryazino, Russia�ermal e�ects, especially longitudinal temperature gra-dient in nonlinear-optical crystals in process of SHGwere studied. Coupled equations of SHG and crystalheating have been solved. Temperature tuning curves areobtained using equivalent temperature concept.
CE-P.24 TUEHighly Er3+-doped phosphate glass for short lengthoptical �bre ampli�er�N.G. Boetti1, D. Pugliese1, E. Ceci Ginestrelli1, E.Bertone1, S. Abrate2, and D. Milanese1; 1Politecnico diTorino, Torino, Italy; 2Istituto Superiore Mario Boella,Torino, ItalyA new phosphate glass stable, robust, able to incorporatehigh amount of RE ions and suitable for �bre drawingwas developed. �e e�ect of Er3+ doping level (up to 10mol%) on properties was investigated.
CE-P.25 TUEBroadband Near-IR Luminescence of Univalent Bi+in CsCdBr3 Crystal�D.N. Vtyurina1, A.N. Romanov1, A.A. Veber2, Z.T.Fattakhova1, K.S. Zaramenskikh3, P.A. Loiko4, M.S.Kouznetsov3, E.V. Haula1, I.S. Lisitsky3, V.B. Tsvetkov5,K.V. Yumashev4, and V.N. Korchak1; 1N.N. SemenovInstitute of Chemical Physics, Russian Academy of Sci-ences, Moscow, Russia; 2Universität Erlangen-Nürnberg,Lehrstuhl für Glas und Keramik, Erlangen, Germany;3State Scienti�c-Research and Design Institute of Rare-Metal Industry Giredmet JSC, Moscow, Russia; 4CenterforOpticalMaterials andTechnologies, BNTU,Minsk, Be-larus; 5A.M. Prokhorov General Physics Institute, RussianAcademy of Sciences, Moscow, Russia�e single crystals of the ternary bromide CsCdBr3doped with univalent bismuth was prepared by theBridgman method. �e material demonstrated thebroadband long lived near-IR luminescence, speci�c forBi+ in halide crystal matrices.
CE-P.26 TUERenewable forsterite production by a solar furnace�C. R. Vistas, D. Liang, and J. Almeida; UniversidadeNova de Lisboa, Lisboa, PortugalForsterite, an ideal material for tunable laser, was renew-able produced from thermal decomposition of serpen-tineminerals using a heliostat-parabolicmirror solar en-ergy collection and concentration system.
CE-P.27 TUEVolume phase gratings inside borosilicate glass in theRaman-Nath regime with high visibility patterns inthe near �eld di�raction�A. Dias Ponte1, M. Martínez Calderón1, M. GomezAranzadi1, T. Morlanes2, J.L. de la Peña2, A. Rodriguez3,and S.M. Olaizola1; 1CEIT-IK4 and Tecnun (Universityof Navarra), San Sebastián, Spain; 2FAGOR AOTEK, S.COOP, Arrasate-Mondragón, Spain; 3CIC microGUNE,Arrasate-Mondragón, SpainVolume phase gratings were fabricated by femtoseconddirect laser writing inside borosilicate. Gratings workin the Raman-Nath regime and they produce near �elddi�raction patterns with high values of visibility.
CE-P.28 TUESilica optical �ber with a multilayer metal protectivecoating for applications in extremely hightemperatures�T. Stańczyk1, K. Wysokiński1, T. Tenderenda1, A.Ziołowicz2, M. Broczkowska2, S. Lipiński1, Ł. Ostrowski1,and T. Nasiłowski1; 1InPhoTech Ltd., Warsaw, Poland;2Polish Centre for Photonics and Fibre Optics, Rogoźnica,PolandIn this paper we present a method of depositing addi-tional protective layers on the copper surface of the cop-per coated optical �bers. Such multilayer structure al-lows to enchant �bers’ high temperature parameters.
CE-P.29 TUEHigh-e�ciency Uni-Traveling-Carrier PhotodetectorIncorporating InP/InGaAsP Bragg Re�ectors�Q. Chen, Y. Huang, X. Duan, W. Fang, J. Fei, and X. Ren;Beijing University of Posts and Telecommunications, Bei-jing, China, People’s Republic of (PRC)A re�ection-enhanced UTC-PD with InP/InGaAsPDBRs was fabricated. �e quantum e�ciency of58.56% and 3dB bandwidth of 18.5GHz were obtainedat 1550nm wavelength. �e dark current is 7.29nA at areverse bias of 3.3V.
CE-P.30 TUETransient response of optically excited Al-doped zincoxide�N. Kinsey1, C. De Vault2, J. Kim1, M. Ferrera1,3, A.Kildishev1, V. Shalaev1, and A. Boltasseva1; 1School ofElectrical and Computer Engineering and Birck Nan-otechnology Center, Purdue University, West Lafayette,United States; 2Dep. of Physics and Birck NanotechnologyCenter, Purdue University, West Lafayette, United States;3School of Engineering and Physical Sciences, Heriot-WattUniversity, Edinburgh, United KingdomUsing a pump-probe technique, the transient re�ectionand transmission of aluminum doped zinc oxide �lms
are studied. A large (~80%) modulation with ultrafastresponse (~1 ps) was observed for a 1.4 �m thick �lm.
CE-P.31 TUEPhoto-darkening In�ulium-DopedAlumino-Silicate Fibres Pumped At 1.07 �m: E�ectof Co-Doping with Lanthanum or Cerium�J.-F. Lupi, M. Vermillac, W. Blanc, and B. Dussardier;Université Nice Sophia Antipolis, CNRS, Laboratoire dePhysique de la Matière Condensée, Nice, France�e photo-darkening process in thulium-dopedalumino-silicate optical �bres under 1.07 um up-conversion pumping is strongly reduced by co-dopingwith lanthanum or cerium. �is would allow for laserand ampli�er operation at new wavelengths.
CE-P.32 TUEOn the stability of periodically poled stoichiometriclithium tantalate�H. Kianirad, A. Zukauskas, G. Lindgren, C. Canalias,and F. Laurell; Applied Physics Department, Royal Insti-tute of Technology, Stockholm, Sweden�e domain stability of �ne pitch periodically poled sto-ichiometric LiTaO3 was investigated. A shallow pinninglayer at the surface was found necessary to avoid backswitching and loss of the nonlinear optical features.
CE-P.33 TUEZ-Scan Measurements of Nonlinear RefractiveIndices of Selected Oxide So� Glasses for PhotonicCrystal Fiber Drawing�J. Cimek1,2, N. Liaros3,4, S. Couris3,4, R. Stepień1, and R.Buczyński1,2; 1Institute of Electronic Materials Technol-ogy, Warsaw, Poland; 2University of Warsaw, Faculty ofPhysics, Warsaw, Poland; 3University of Patras, Depart-ment of Physics, Patras, Greece; 4Institute of ChemicalEngineering Sciences (ICE-HT), Foundation for Researchand Technology-Hellas (FORTH), Patras, GreeceNonlinear refractive index of various highly nonlin-ear oxide so� glasses has been measured. �e highestvalue is reported for lead-bismuth-gallium silicate glass1.14x10-17 W/m2 along with high thermal stability al-lowing to fabricate microstructured �bers.
CE-P.34 TUETemperature dependent Nd:KGW spectroscopy study�S.J. Yoon, S. Beecher, and J. Mackenzie; OptoelectronicsResearch Centre, Southampton, United KingdomWe report a high resolution spectroscopic characterisa-tion of Nd:KGW over the range 80 K - 450 K, providingcritical values to enables accurate prediction of laser per-formance, particularly for cryogenic picosecond lasers.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
HALL B0CE-P.35 TUEFabrication of Single Wall Carbon NanotubeSaturable Absorber in the Micro-grooved SingleMode Fiber
�K. Viskontas1,2, M. Mikutis3, J. Pilipavicius4, R.Gumenyuk5, O. Okhotnikov5, andN. Rusteika1,2; 1Centerfor Physical Sciences and Technology, Vilnius, Lithuania;2Ekspla Uab, Vilnius, Lithuania; 3Altechna uab, Vilnius,
Lithuania; 4Vilnius University, Faculty of Chemistry, Vil-nius, Lithuania; 5Tampere University of Technology, Tam-pere, FinlandWedescribe technological solution for fabrication of sin-
gle wall carbon nanotube (SWCNT) based saturable ab-sorber. �e mode-locking of Tm/Ho �ber laser withthe �ber-integrated SWCNT saturable absorberwas con-�rmed.
13:00 – 14:00CI-P: CI Poster Session
CI-P.1 TUEP3HT-coated coreless silica �ber for in-linephotodetection�D.-M. Nguyen1,2, Z. Wang1, L. Cui1, and C. Soci1;1Centre for disruptive photonic technologies, Nanyangtechnological University, Singapore, Singapore; 2CINTRACNRS/NTU/THALES,UMI 3288, Research Techno Plaza,Singapore, SingaporeWe demonstrate a �ber embedded photodetector usingP3HT coated coreless silica �bers that can simultane-ously transmit optical signal and track its power. Photo-conductivity induced by optical modes leaking into theactive layer is studied.
CI-P.2 TUEPhotons as Ants: a Stigmergic Photonic Network�W. Hu1,2, K. Wu1, P. Shum1,2, N. Zheludev1,3, and C.Soci1,2; 1Centre for Disruptive Photonic Technologies,,Singapore, Singapore; 2School of Electrical and ElectronicEngineering, Singapore, Singapore; 3Optoelectronics Re-search Centre, Southampton, United KingdomWe implement an all-optical stigmergic �ber network torealize the famous ant colony optimization algorithm.�is demonstrates the potential of *cognitive photonicnetworks* to mimic learning and plasticity of the brain.
CI-P.3 TUESimultaneous Dual-Channel Reception Scheme forIncoherently Multiplexed Dual-Carrier Signals�T. Sakamoto; National Institute of Information andCommunications Technology, Tokyo, JapanWe prove that incoherently multiplexed dual-carrier sig-nals, assuming WDM channels, can be simultaneouslydemutiplexed by using coherent matched detector with-out relying on optical �ltering.
CI-P.4 TUEOriginal Ampli�er For Mode Division MultiplexingBased On Dual Core Erbium-Doped Fibre AndAsymmetric Long-Period-Grating ConvertersV. Rastogi1, A. Gaur1, P. Aschieri2, and �B. Dussardier2;1Department of Physics, Indian Institute of Technology,Roorkee, India; 2Université Nice Sophia Antipolis, CNRS,LPMC, UMR 7336, Nice, France
An original concept of integrated few-mode erbiumdoped �bre ampli�er for mode division multiplexing(MDM) reaches nearly zero di�erential modal gain be-tween two mode groups (8 MDM channels) with morethan 20 dB of gain.
CI-P.5 TUEFibre Optical Parametric Ampli�er incorporating aRaman-Pump for Reduced Four-Wave MixingCrosstalk�M. Stephens, I. Phillips, P. Harper, and N. Doran; AstonInstitute of Photonic Technologies, Birmingham, UnitedKingdomWe report 20dB-gain optical ampli�cation of ten 58Gb/ssignals using a �bre optical parametric ampli�er incor-porating a counter-propagating Raman pump. Inter-channel crosstalk is reduced by 6dB over a conventionalFOPA using this technique.
CI-P.6 TUEAdaptive Doublet Pulse Generation for UWBTransmission in Hybrid Wireless-Optical AccessNetworks�M. Malekizandi, Q.T. Le, H. Nessling, D. Briggmann, A.Emsia, and F. Kueppers; TU Darmstadt, Darmstadt, Ger-manyAn UWB signal generation method based on directlymodulated semiconductor laser, optical �ltering andaccumulative �ber dispersion is proposed to generateGaussian derivatives. Transmitter is adapted to accumu-lated chromatic dispersion variations in optical �ber net-works.
CI-P.7 TUEFlat-top interleavers: a novel approach based on MMIsplitters�M. Cherchi, S. Ylinen, M. Kapulainen, M. Harjanne, T.Vehmas, and T. Aalto; VTT technical Research Centre ofFinland, Espoo, FinlandA novel design of �at-top �lters based on MMI splitteris presented. Six di�erent example implementations havebeen fabricated on amicron-scale silicon photonics plat-form, and their characterization led to very promisingresults.
CI-P.8 TUEImpact of waveguide cross section on nonlinearimpairments in integrated optical �lters for WDMcommunication systemsC. Lacava1,2, �R. Marchetti1, G. Giuliani3, M.Fournier4, S. Menezo4, S. Messaoudene4, and P.Minzioni1; 1Dipartimento di Ingegneria Industriale edell’Informazione, Università di Pavia, Pavia, Italy;2Optoelectronic Research Centre, University of Southamp-ton, Southampton, United Kingdom; 3Dipartimento diIngegneria Edile ed Architettura, Università di Pavia,Pavia, Italy; 4Univ. Grenoble Alpes CEA, LETI, MI-NATEC, DOPT, Grenoble, FranceHere we present the nonlinear characterization ofWave-length DivisionMultiplexing (WDM) silicon �lters. Dif-ferent cross-sections waveguide were analyzed and re-sults on low-height silicon multiple ring resonator (twoand three rings) are presented.
CI-P.9 TUEAdaptive control of modes in a two-mode-�ber inall-�berized format�L. Huang, J. Leng, P. Zhou, S. Guo, H. Lü, and X.Cheng; College of Optoelectronic Science and Engineer-ing, National University of Defense Technology, Chang-sha, China, People’s Republic of (PRC)We demonstrate the real-time all-�berized selective ex-citation of linear-polarized modes in a two-mode-�berbased on adaptive-control. �e �ber is adaptivelysqueezed, while the feedback signal is the target-modeweight resulted from the mode decomposition tech-nique.
CI-P.10 TUEFlexible Space Division MultiplexedWDM-PON with16-QAM Point-to-Point and PolSK ModulatedMulticast Overlay Services�R. Asif1, M. Imran2, F. Ye3, L. Poti4, and T. Morioka5;1DTU Fotonik, Technical University of Denmark, Kgs.Lyngby, Denmark; 2Scoula Superiore Sant’Anna, Pisa,Italy; 3DTU Fotonik, Technical University of Denmark,Kgs. Lyngby, Denmark; 4CNIT, Photonics Network Na-tional Lab, Pisa, Italy; 5DTU Fotonik, Technical Univer-sity of Denmark, Kgs. Lyngby, DenmarkWe numerically propose SDM-WDM-PON architecturefor downstream signaling of 10Gbit/s 16-quadratureamplitude modulation (16-QAM) point-to-point sig-
nals and 2.5Gbit/s polarization shi� keying (PolSK)multicast-overlay signals over 20 km 19-core �ber link.
CI-P.11 TUEPump-Phase-Noise-Free Multichannel WavelengthMulticasting for QAM Signals using CoherentMulti-Carrier Pump�G.-W. Lu1,2, T. Sakamoto1, and T. Kawanishi1;1National Institute of Information and Communica-tions Technology (NICT), Tokyo, Japan; 2Institute ofInnovative Science and Technology, Tokai University,Kanagawa, JapanWe propose and experimentally demonstrate a pump-phase-noise-free multi-channel wavelength multicast(MWM) scheme using coherent multi-carrier pumps. Itenables the use of low-cost DFB laser as pump source,providing low-cost MWM solution for phase-sensitivehigh-order QAM.
CI-P.12 TUEMulti-level Approach to the Optimization ofUnrepeatered WDM Systems with DistributedAmpli�cation�G. Rizzelli, M. Camarasa-Gómez, D. Hernangómez-Pérez, and J.D. Ania-Castañón; Instituto de Óptica, IO-CSIC, Madrid, SpainWe present a new general approach to the numerical op-timization of unrepeatered systems with distributed am-pli�cation, based on nonlinearity management theory.Our method generalises and updates tried-and-testedmulti-level optimization techniques previously appliedto long-haul transmission.
CI-P.13 TUEOptical phase processor with enhanced phasequantization properties for higher order modulationformats relying on phase sensitive ampli�cation andlimiting ampli�ers�A. Bogris; Technological Educational Institute of Athens,Athens, GreeceA new phase sensitive ampli�er that attains almost idealphase quantization for multi-level phase modulated sig-nals is proposed. �e e�cient quantization is achievedwith the use of a limiting ampli�er prior the �nal coher-ent summation.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
HALL B0CI-P.14 TUEHigh-Photocurrent and Large-BandwidthUni-Traveling-Carrier Photodiodes: Suppresion ofCurrent Blocking Using Dipole-Doped Interface�H. Wang; Nanyang Technological University, Singapore,Singapore
In this paper, Uni-Traveling-Carrier photodiodes (UTC-PDs) using a dipole-doped interface to e�ectively sup-press the current blocking and improve the devicebandwidth and power/current handling capability aredemonstrated.
CI-P.15 TUEAll-Optical Silicon-Photonic ConstellationConversion�T. Yeminy1, D. Sadot1, and Z. Zalevsky2; 1Department ofElectrical and Computer Engineering, Ben Gurion Uni-versity, Beer Sheva, Israel; 2Faculty of Engineering, Bar
Ilan University, Ramat Gan, IsraelA silicon-photonic constellation conversion method forgeneric amplitude-phase modulation formats is pro-posed. A neural network mathematical model is devel-oped and full optical simulation of a four symbol constel-lation conversion yields output EVM lower than 3.5%.
13:00 – 14:00CN-P: CN Poster session
CN-P.1 TUEEmissivity switch during semiconductor-metal phasetransition of vanadium dioxide �lms on silicon�G. Leahu, R. Li Voti, M. Bertolotti, and C. Sibilia; Dipar-timento di Scienze di Base ed Applicate per l’Ingegneria -Sapienza Università di Roma, Rome, ItalyWe measured the infrared properties of vanadium diox-ide layered structures during the semiconductor-to-metal phase transition. We show a large emissivityswitch as a function of the temperature
CN-P.2 TUEImprovement of range accuracy of streak tubeimaging lidar at kilometre-range distances�G. Ye, R. Fan, D. Chen, Z. Chen, and W. Yuan; HarbinInstitute of Technology, Harbin, China, People’s Republicof (PRC)An improved method based on the relation betweenrange accuracy and static blurring width is proposed toimprove the range accuracy of streak tube imaging lidarsystem at kilometre-scale distances.
CN-P.3 TUEInjection Seeding a Q-Switched Ho:YAG Laser basedon a Self-Organizing Technique for Doppler WindLIDAR�G. Renz and D. Oberbeckmann;German Aerospace Cen-ter, Stuttgart, GermanyWe report on a Q-switched 2.1 micrometer Ho:YAGinjection-seeded laser system based on a self-organizingtechnique for Doppler wind LIDAR of up to 10 W av-erage power with a minimal amount of control compo-nents.
CN-P.4 TUEEnergy reservoir of femtosecond �lament and plasmachannel formation in focused beamsA.A. Dergachev1, A.A. Ionin2, V.P. Kandidov1, D.V.Mokrousova2,3, L.V. Seleznev2, D.V. Sinitsyn2, �E.S.Sunchugasheva2,3, and S.A. Shlenov1; 1LomonosovMoscow State University, Moscow, Russia; 2Lebedev Phys-ical Institute of the Russian Academy of Sciences, Moscow,Russia; 3Moscow Institute of Physics and Technology, Dol-goprudny, RussiaWe experimentally and numerically investigated en-ergy reservoir role in plasma channel formation duringtightly focused beam �lamentation. �e reservoir diam-eter was found to be much smaller than for collimatedbeam and decreasing approaching focal plane.
13:00 – 14:00EC-P: EC Poster Session
EC-P.1 TUEPhase-engineered Light Patterns for Ultracold AtomExperimentsG.D. Bruce, T. Harte, D. Bowman, P. Ireland, J. Keeling,and �D. Cassettari; University of St Andrews, St Andrews,United KingdomWe present advances in the use of Spatial Light Modu-lators for the manipulation of ultracold neutral atoms,by increasing the control over hologram calculation andthe accuracy of experimental light patterns, and demon-strate multi-wavelength holograms.
EC-P.2 TUEMaximum Contrast Interferometry and Coherence inBose-Einstein Condensates�V. Henderson, Y. Zhai, C. Carson, P. Gri�n, E. Riis,and A. Arnold; University of Strathclyde, Glasgow, UnitedKingdomMagnetic levitation is used to obtain interference pat-terns between two spatially separated BECs and to probethe phase �uctuations of highly elongated BECs. With160ms levitation, Talbot enhanced fringe contrast of >95% is observed.
EC-P.3 TUEChiral optical force�R. Cameron1, S. Barnett1, and A. Yao2; 1Universityof Glasgow, Glasgow, United Kingdom; 2University ofStrathclyde, Glasgow, United KingdomLight carrying helicity in unusual ways can accelerate theopposite enantiomers of a chiral molecule in opposite di-rections; a remarkable new phenomenon that may �nduse in a wealth of contexts.
EC-P.4 TUEGeneration and re�ection of travelling breathers inBose-Einstein condensates in optical latticesR. Campbell and �G.-L. Oppo; University of Strathclyde,Glasgow, United KingdomGaussian wavepackets evolve into travelling breathers inthe presence of localised dissipations for BEC in opticallattices in ring traps. In linear traps with con�ning po-tentials, travelling breathers are shown to re�ect at theboundaries.
EC-P.5 TUEStrong atom-light interaction in near-concentricoptical resonators�H. Nguyen1, K. Durak1, N. Lewty1, and C. Kurtsiefer1,2;1Center forQuantumTechnologies, NationalUniversity ofSingapore, Singapore, Singapore; 2Department of Physics,
National University of Singapore, Singapore, SingaporeWe report on experimental progress demonstratingstrong single atom-photon coupling in a near concen-tric cavity. We expect a large vacuum Rabi frequency(350MHz) and cooperativity (160) for a single Rb87atom.
EC-P.6 TUEOptomechanical Self-Structuring in a Bose-EinsteinCondensate�G. Robb1, E. Tesio1, G.-L. Oppo1, W. Firth1, T.Ackemann1, and R. Bonifacio2,3; 1University of Strath-clyde, Glasgow, United Kingdom; 2INFN-LaboratorioNazionale di Frascati, Rome, Italy; 3Universidade Federalda Paraiba, Paraiba, BrazilWe present analysis of an optomechanical instability in aBose-Einstein Condensate, producing a supersolid statewith a self-selected length scale by spontaneous breakingof two continuous symmetries in the plane orthogonal tothe pump axis.
EC-P.7 TUEQuantum Zeno Dynamics induced by LightScattering from Ultracold Atoms in Optical Lattices�G. Mazzucchi, S.F. Caballero Benitez, and I. Mekhov;University of Oxford, Oxford, United Kingdom
We demonstrate the quantum measurement-inducedgeneration of many-body entangled spatial modes andtheir Quantum Zeno dynamics for bosons and fermionsin optical lattices. Single quantum trajectories show gi-ant oscillations, beyond solutions averaged over manyruns.
EC-P.8 TUEAmesoscopic blue-detuned light ring forBose-Einstein Condensates based on conicalrefraction�A. Turpin1, J. Polo1, Y. Loiko1,2, J. Küber3, F.Schmaltz3, T. Kalkandjiev1,4, V. Ahu�nger1, G. Birkl3,and J. Mompart1; 1Departament de Física, UniversitatAutònoma de Barcelona, Bellaterra, Spain; 2Aston Insti-tute of Photonic Technologies, School of Engineering&Ap-plied Science AstonUniversity, Birmingham, United King-dom; 3Institut für Angewandte Physik, TechnischeUniver-sität Darmstadt, Darmstadt, Germany; 4ConerefringentOptics S.L., Vilanova i la Geltrú, SpainWe present a novel blue-detuned optical ring trap basedin conical refraction. We provide the trapping frequen-cies and depths of the optical potential and demonstrateits applicability in the trapping of a 87Rb Bose-Einsteincondensate.
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CLEO®/Europe-EQEC 2015 ⋅ Tuesday 23 June 2015
HALL B013:00 – 14:00EI-P: EI Poster Session
EI-P.1 TUEElectron dynamics in dielectric materials induced bytwo-color femtosecond laser pulses�L. Barilleau, G. Duchateau, B. Chimier, N. Fedorov, G.Geo�roy, and V. Tikhonchuk; Université de Bordeaux-CNRS-CEA, CELIA, UMR 5107, TALENCE, FranceExperimental and theoretical photoemission spec-troscopy induced by two color intense femtosecondlaser pulses (800 nm and 266 nm) in α-quartz, havebeen investigated. A strong cooperation of laser pulsestakes place.
EI-P.2 TUESpectral Delay Algebraic Equation Approach for theModeling of Broad Area Laser Diodes�J. Javaloyes1, A. Perez-Serrano2, and S. Balle3;1Departament de Fisica, Universitat de les Illes Baleares,Palma de Mallorca, Spain; 2Universidad Politecnica deMadrid, Madrid, Spain; 3Institut Mediterrani d’EstudisAvançats, Esporles, Spain
We discuss an e�cient modeling approach for the simu-lation of broad area laser diodes based on the combina-tion of spectral transforms and delay equation mapping.We obtain speedups between one and two orders ofmag-nitudes.
EI-P.3 TUEE�cient semi-analytical modeling of passivelymode-locked lasers�M. Alsaleh, C.B.L. Mback, E. Tchomgo-Felenou, P.Tchofo-Dinda, and P. Grelu; Laboratoire InterdisciplinaireCarnot de Bourgogne, Dijon, FranceWe merged the modeling of the propagation and char-acterization of light pulses in a �ber laser, into a singlemethod having the advantage of being versatile, accu-rate, and very thri�y in calculation time.
EI-P.4 TUEDi�raction of Optical Weierstrass Waves by SimpleApertures: Circular Symmetry and FractalDimension�J.M. Christian, E.P. Woodroofe, and G.S. McDonald;University of Salford, Greater Manchester, United King-dom
We consider the di�raction of an incident fractal wave,modelled with aWeierstrass function, by a circular aper-ture. Fresnel di�raction theory is used to calculate near-�eld patterns, whose fractal characteristics are quanti�edusing specialist so�ware.
EI-P.5 TUEGeneration of light pulses with speci�cally carvedpro�les in a �ber laser using a NOLM and a spectral�lterC.B.L. Mback, �P. Tchofo-Dinda, P. Grelu, and A.B.Moubissi; Laboratoire Interdisciplinaire Carnot de Bour-gogne, Dijon, FranceA model of �ber laser incorporating a NOLM and aGaussian �lter allows to ensure both a high stability ofthe light pulses and a custom sculpture of the pulse pro-�le within the cavity.
EI-P.6 TUESpontaneous emission dynamics in strongly modi�edvacuaM. Teimourpour and �R. El-Ganainy; Department ofPhysics, Michigan Technological University, Houghton,Michigan, United States
We present an e�cient computational scheme for study-ing spontaneous emission dynamics in both weak andstrong coupling regimes.
EI-P.7 TUEEigenmodes of Next-Generation Unstable CavityLasers: Kaleidoscopes, Snow�akes, Penta�akes, andFractal Dimension�J.M. Christian1, I. Begleris2, S.J. Wickham1, G.S.McDonald1, and J. Huang3; 1University of Salford,Greater Manchester, United Kingdom; 2University ofSouthampton, High�eld, United Kingdom; 3University ofSouth Wales, Pontypridd, United KingdomTwo new classes of unstable-cavity laser are proposed,involving transverse boundary conditions that are frac-tal in nature. �e virtual-source modelling of these res-onator systems is discussed, and we analyse the detailedcharacteristics of their eigenmodes.
13:00 – 14:00JSI-P: JSI Poster Session
JSI-P.1 TUENonlinear Laser Lithography for Photonic Design ofSi Solar Cells�I. Pavlov1, T. Colakoglu2, F. Es2, A. Bek2, R. Turan2, I.Gnilitskyi3, and O. Ilday1; 1Bilkent University, Ankara,
Turkey; 2Middle East Technical University, Ankara,Turkey; 3University of Modena and Reggio Emilia, Reg-gio Emilia, ItalyWe propose and experimentally demonstrate NonlineaLaser Lithography technique for photonic design of Si-
based solar cells. For high-resistive single-crystalline Si,relative increase of conversion e�ciency of solar cell isfound to be 45%.
13:00 – 14:00JSII-P: JSII Poster Session
JSII-P.1 TUENumerical Study of a High Sensitive Polymer Bio-sensor Using a Trimodal Waveguide Interferometer�J. C. Ramirez1, L. M. Lechuga1,2, L. H. Gabrielli1, andH. E. Hernandez-Figueroa1; 1School of Electrical and
Computer Engineering (FEEC), UNICAMP, Campinas,Brazil; 2Nanobiosensors and Bioanalytical Group, Insti-tut Català de Nanociència i Nanotecnologia (ICN2), CSICand CIBER-BBN, Barcelona, SpainA novel, highly sensitive and compact optical interfero-
metric biosensor based on the interaction between thefundamental mode and the second order mode is pre-sented.
13:00 – 14:00JSIV-P: JSIV Poster Session
JSIV-P.1 TUEPhotonic Topological Anderson Insulator�S. Stützer1, M. Rechtsman2, Y. Plotnik2, Y. Lumer2, J.Zeuner1, S. Nolte1, M. Segev2, and A. Szameit1; 1Instituteof Applied Physics, Abbe Center of Photonics, Friedrich-
Schiller-University, Jena, Germany; 2Department ofPhysics, Technion - Israel Institute of Technology, Haifa,IsraelWe report the realization of the Topological AndersonInsulator: a system transformed into being topological
due to the presence of disorder. �is constitutes the �rstexperiment on topological Anderson insulator in anysystem in nature.
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CLEO®/Europe-EQEC 2015 ⋅ Wednesday 24 June 2015
ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a8:30 – 10:00EH-1: Chirality in Plasmonics andMetamaterialsChair: Kevin F. MacDonald, University ofSouthampton, Southampton, United King-dom
8:30 – 10:00EB-3: Sources of Quantum LightChair: Andreas Popper, Austrian Institute ofTechnology, Vienna, Austria
8:30 – 10:00CJ-7: Mid-IR Fibre Laser Systems IIChair: Real Vallee, Université Laval, Québec,Canada
8:30 – 10:00CLEO/ECBO-1: BioimagingChair: Monika Ritsch-Marte, BiomedicalPhysics, Innsbruck, Austria
8:30 – 10:00CK-10: Optomechanics and MemsChair: Peter Horak, ORC, University ofSouthampton, United Kingdom
EH-1.1 WED (Invited) 8:30Spinning and orbiting surface plasmons:twisted light and near- �eld chiral forces�C. Genet; University of Strasbourg & CNRS,Strasbourg, FranceStructured light beams with phase or po-larization singularities have revealed uniqueoptical properties that can be enhanced atthe level of chiral nanostructures. �is drawspromissing routes in the context of opticalforces.
EB-3.1 WED 8:30Addressing Rb and Cs transitions with atunable source of photon pairs�G. Schunk1,2,3, U. Vogl1,2, M. Förtsch1,2,3,D. Strekalov1,2, F. Sedlmeir1,2,3, H.G.L.Schwefel1,2, G. Leuchs1,2, and C.Marquardt1,2,4; 1Max Planck Institutefor the Science of Light, Erlangen, Germany;2Institut für Optik, Information und Pho-tonik, University of Erlangen-Nuremberg,Erlangen, Germany; 3SAOT, School inAdvanced Optical Technologies, Erlangen,Germany; 4Department of Physics, TechnicalUniversity of Denmark, Erlangen, GermanyWe experimentally show that our source ofphoton pairs based on spontaneous para-metric down-conversion in a triply reso-nant whispering-gallery resonator can ad-dress the atomic transitions of both rubid-ium and cesium.
CJ-7.1 WED 8:30Watt-Level In-Band Pumped Ho:ZBLANWaveguide Chip Laser at 2.1 �mV. Michaud-Belleau1, S. Gross2, J. Genest1,and �D. Lancaster3,4; 1Centre d’optique, pho-tonique et laser, Université Laval, Québec,Canada; 2Centre for Ultrahigh Bandwidth forOptical Systems, Macquarie University, Syd-ney, Australia; 3Institute for Photonics andAdvanced Sensing, University of Adelaide,Adelaide, Australia; 4Division of Informa-tion Technology, Engineering and the Envi-ronment, University of South Australia, Ade-laide, AustraliaWe report 2.1�m laser emission from anin-band pumped Ho:ZBLAN depressedcladding waveguide chip laser. Outputpower of 1.1W at 69% slope e�ciencyis obtained in a large area lowest ordertransverse mode.
CLEO/ECBO-1.1 WED (Tutorial) 8:30Optical Coherence Tomography - A noveldiagnostic standard ?�W. Drexler; Center for Medical Physics andBiomedical Engineering, Medical University,Vienna, AustriaIn the last 25 years optical coherence tomog-raphy has advanced to be one of the mostinnovative and most successful translationaloptical imaging techniques, achieving sub-stantial economic impact as well as clinicalacceptance.
CK-10.1 WED 8:30Heterogeneously integrated 2D photoniccrystal system for cavity optomechanics�V. Tsvirkun1, A. Surrente1, G. Beaudoin1,F. Raineri1,2, R. Raj1, I. Robert-Philip1, andR. Braive1,2; 1Laboratoire de Photoniqueet de Nanostructures, Marcoussis, France;2Université Paris Diderot, Paris, France2D photonic crystal defect cavity InP mem-brane coupled via an integrated siliconwaveguide shows optomechanical couplingphenomena. Among them, optical spring ef-fects are observed, revealing the nature ofthe optical forces involved.
EB-3.2 WED 8:45High heralding e�ciency single photonsource at telecom wavelength�S. Wollmann1,2, M. Weston1,2, H.Chrzanowski1,2, S. Slussarenko1,2, and G.Pryde1,2; 1Centre for Quantum Dynamics,Brisbane, Australia; 2Centre for Quan-tum Computation and CommunicationTechnology, Brisbane, AustraliaWe demonstrate the generation and mea-surement of frequency factorable pairs ofsingle photons using spontaneous paramet-ric downconversion in a high-heralding-e�ciency source engineered for group ve-locity matching at telecom wavelength.
CJ-7.2 WED 8:45High-Energy Q-switched Er:ZBLAN FibreLaser at 2.79 �m�S. Lamrini1, K. Scholle1, M. Schäfer1, P.Fuhrberg1, J. Ward2, M. Francis2, S. Sujecki3,A. Oladeji3, B. Napier4, A. Seddon3, M.Farries2, and T. Benson3; 1LISA laser prod-ucts OHG, Katlenburg-Lindau, Germany;2Gooch & Housego Ltd., Ilminster, UnitedKingdom; 3Division of Electrical Systems andOptics, Nottingham, United Kingdom; 4VividComponents Ltd., Paderborn, GermanyWe demonstrate a Q-switched Er:ZBLAN �-bre laser at 2790 nm with unprecedentedperformance. At room-temperature morethan 0.5 mJ of pulse energy were achievedand the pulse peak power exceeded the 10kW level.
CK-10.2 WED 8:45AMEMS Device for ContinuouslyTunable Optical Bu�ering�N. Podoliak1, W. Ng2, J. Wu2, H. Liu2,W. Stewart1, A. Kenyon2, and P. Horak1;1Optoelectronics Research Centre, Universityof Southampton, Southampton, United King-dom; 2Department of Electronic and Electri-cal Engineering, University College London,London, United KingdomWe present design and fabrication of free-standing InP optical waveguides for MEMS-actuated optical bu�ering. A continuouslytunable delay time of 10ps is predicted in a1mm long device with the operation voltageof 3V.
EH-1.2 WED 9:00Rigorous Numerical Analysis ofPlasmonically Enhanced ChiropticalSpectroscopy�M.Nesterov, X. Yin, M. Schäferling, T.Weiss,and H. Giessen; 4th Physics Insitute and Re-search Centre SCoPE, University of Stuttgart,Stuttgart, Germany
EB-3.3 WED 9:00Ultra precise characterization of a novelintegrated high-order W-state generationdevice�R. Heilmann, M. Gräfe, S. Nolte, andA. Szameit; Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, Germany
CJ-7.3 WED (Invited) 9:00Improving the prospects for �uoride-glass-based mid-infrared �bre lasers�S. Jackson1, D. Hudson2, T. Hu2, and S.Crawford2; 1MQ Photonics, Department ofEngineering, Macquarie University, NorthRyde 2109, Sydney, Australia; 2Centre for Ul-trahigh bandwidth Devices for Optical Sys-
CK-10.3 WED 9:00Optomechanics with GrapheneMechanical Resonators�P. Weber, J. Güttinger, A. Noury, I. Tsiout-sios, D.E. Chang, and A. Bachtold; ICFO -�e Institute of Photonic Sciences, Barcelona,SpainGraphene is an attractive material for nano-
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ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES8:30 – 10:00CE-10: Optical Devices Based onDiamond and SilicaChair: Stefan Kück, Physikalisch-TechnischeBundesanstalt, Braunschweig, Germany
8:30 – 10:00CB-4: Semiconductor Micro- andNano-LasersChair: Pallab Bhattacharya, University ofMichigan, Ann Arbor, USA
8:30 – 10:00CH-6: Fibre andWaveguide BasedSensorsChair: Marian Marciniak, National Instituteof Telecommunications, Warsaw, Poland
8:30 – 10:00CG-3: Attosecond Applications ofMid-IR SourcesChair: Markus Kitzler, University of Technol-ogy, Vienna, Austria
CE-10.1 WED (Invited) 8:30Diamond - an engineer’s best friend�A. Bennett andD. Twitchen; Element Six, USCorp., Santa Clara, United StatesDiamond possesses remarkable physical andchemical properties, and inmany ways is theultimate optical engineering material. Wewill summarize key progress in fabricationtechniques utilizing chemical vapour depo-sition (CVD), processing and solutions forintegration.
CB-4.1 WED (Invited) 8:30Semiconductor Alloy Nanowires andNanobelts with Widely Tunable Bandgapsfor Full-Spectrum Emission andMulti-Color LasingF. Fan1, S. Turkdogan1, Z. Liu1, and �C.-Z. Ning1,2; 1Arizona State University, Tempe,AZ, United States; 2Tsinghua University, Bei-jing, China, People’s Republic of (PRC)�is talk focuses on semiconductor alloynanowires and nanobelts with controlledvariation of composition in a wide rangeover a single substrate or across a singlenanostructure, as well as their applicationsin multi-color lasing.
CH-6.1 WED 8:30Experimental demonstration of chiralspiral waveguides without waveguidecrossings�T. Aalto, M. Cherchi, S. Ylinen, M. Kapu-lainen, M. Harjanne, and T. Vehmas; VTTtechnical Research Centre of Finland, Espoo,FinlandWe propose a novel design of chiral spi-rals based on nested loops coupled by MMIcouplers. Spirals 6.6 cm, 12.5 cm and 47.9cm long have been fabricated with e�ectivepropagation losses of 0.3 dB/cm.
CG-3.1 WED 8:30High power coherent so� X-ray source forelement- and state-selective imaging inthe water window�J. Rothhardt1,2, S. Hädrich1,2, A. Klenke1,2,S. Demmler1, J. Limpert1,2, and A.Tünnermann1,2; 1Institute of AppliedPhysics, Friedrich Schiller University Jena,Jena, Germany; 2Helmholtz-Institute-Jena,Jena, GermanyWe demonstrate a high-photon �ux so� X-ray source based on a few-cycle �ber lasersystem. It deliversmore than 10^6 photons/swithin the water window and will be em-ployed for coherent di�ractive imaging andspectroscopy.
CH-6.2 WED 8:45Highly functional interferometer builtwith tapered optical �bre tips�C. Moreno-Hernández1, D. Monzón-Hernández1, and J. Villatoro2,3; 1Centrode Investigaciones en Óptica, A.C., León,Mexico; 2ETSI, Communications Engineer-ing Dept. University of the Basque Country(UPV/EHU), Alda. Urquijo s/n, Bilbao,Spain; 3IKERBASQUE Basque Foundationfor Science, Bilbao, SpainA simple and highly functional Fabry-Perotinterferometer built with tapered optical �-bre tips capable of simultaneously measur-ing distance, thickness (with error of *1%),and group refractive index (with *0.5% de-viation) of samples is presented.
CG-3.2 WED 8:45Table-Top Attosecond Transients Isolatedat 500 eV at 1 kHz repetition rateS.M. Teichmann1, F. Silva1, �S.L. Cousin1, N.Suárez1, M. Hemmer3, D.R. Austin4, M.G.Pullen1, and J. Biegert1,2; 1ICFO, Mediter-ranean Technology Park, Castelldefels, Spain;2Institució Catalana de Recerca i EstudisAvancats, Barcelona, Spain; 3Center for Free-Electron Laser Science, DESY, Hamburg, Ger-many; 4Blackett Laboratory, Imperial CollegeLondon, London, United KingdomWe generate CEP-controlled high harmoniccuto�s up to 550 eV in helium. Full numer-ical simulations match the measurementsvery well and suggest the generation of iso-lated, 130 attosecond pulses at 500 eV.
CE-10.2 WED 9:00Diamond optical windows withsub-wavelength surface structures�E. Anoikin and A. Muhr; Element Six Tech-nologies US Corporation, Santa Clara, CA,United StatesDiamond windows with sub-wavelengthsurface structures were designed, fabricated
CB-4.2 WED 9:00Sub- and Superradiance in Quantum-DotMicrolasers�H.A.M. Leymann1, A. Foerster1, J. Wiersig1,F. Jahnke2, and C. Gies2; 1Institut für�eoretische Physik, Otto-von-Guericke-Universität, Magdeburg, Germany; 2Institutfür�eoretische Physik, Universitüt, Bremen,
CH-6.3 WED 9:00Photonic integrated interrogator for�ber-optic sensor networks�S. Stopiński1, M. Lelit1, A. Jusza1, K.Anders1, T. Osuch1, P. Szczepański1, K.Rózanowski2, J. Lewandowski2, and R.Piramidowicz1; 1Faculty of Electronics andInformation Technology, Warsaw University
CG-3.3 WED 9:00Compression and Ampli�cation of SWIRSingle-Cycle Pulses for Water WindowAttosecond Pulse Generation�A.S. Wyatt1, P. Matía-Hernando2, A.S.Johnson2, O. Alexander1, R. Chapman1, C.Cacho1, D.R. Austin2, J.W.G. Tisch2, J.P.Marangos2, and E. Springate1; 1STFC Cen-
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ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a
We present a thorough numerical investi-gation of the electrodynamical interactionbetween chiral media and chiral plasmonicstructures.We show that plasmonic nanoan-tennas can give numerically up to two ordersof magnitude of CD enhancement.
We present a universal three dimensional in-tegrated quantum circuit to generate multi-partite entangled W-states. Additionally, weshow a novel scheme to determine the cir-cuits unitary employing classical light only.
tems (CUDOS), Institute of Photonics andOptical Science, School of Physics, �e Uni-versity of Sydney, NSW 2006, Sydney, Aus-traliaWe present our recent results from work di-rected towards the creation of highly func-tional 3micron output from a �bre laser. �eprimary challenges and directions for fur-ther research in this �eld will be discussed.
electromechanical systems because of its lowmass and exceptionalmechanical properties.We report on results, in which we couplea graphene resonator to a superconductingmicrowave cavity.
EH-1.3 WED 9:15Optical Activity of Chiral PlasmonicNanohelices�A. de Hoogh, D. Kosters, N. Rotenberg, H.Acar, H. Zeijlemaker, and K. Kuipers; FOMInstitute AMOLF, Amsterdam, �e Nether-landsWe show that electron beam induced depo-sition can be used to successfully fabricatecore-shell (silica-gold) plasmonic nanohe-lices. We investigate their optical activityand �nd that the maximum optical activityincreases with increasing helix height.
EB-3.4 WED 9:15On-Demand Single Photon EmissionBased on Dynamic Photon Storage on aPhotonic Integrated Circuit�M. Heuck, M. Pant, and D. Englund;Massachusetts Institute of Technology, Cam-bridge, United StatesWe propose a microring-resonator basedintegrated structure that uses spontaneousfour wavemixing to generate single photons,which can be released on-demand via dy-namic tuning of the ring resonances.
CK-10.4 WED 9:15Tunable GHz optomechanical crystals�H. Pfeifer1, T. Paraiso1,2, L. Zang1, and O.Painter2; 1Max Planck Institute for the Sci-ence of Light, Erlangen, Germany; 2Institutefor Quantum Information and Matter and�omas J. Watson, Sr., Laboratory of Ap-plied Physics, California Institute of Technol-ogy, Pasadena, United StatesWe describe the design of an optomechan-ical nanobeam cavity with an electrostat-ically tunable acoustic mode in the GHzregime. Such tunable cavity elements areexpected to be critical in realizing coupledopto-mechanical cavity arrays.
EH-1.4 WED 9:30Chiral Mirrors�E. Plum1 and N.I. Zheludev1,2; 1Universityof Southampton, Southampton, United King-dom; 2Nanyang Technological University,Singapore, SingaporeWe demonstrate a novel mirror whichuniquely re�ects one circular polarizationwithout polarization change, while acting asperfect absorber for the other. �is ultimateplanar chiral e�ect enables circularly polar-ized cavities, lasers and spectroscopic tech-niques.
EB-3.5 WED (Invited) 9:30Quantum-dot-based Quantum-opticalCircuits�M. Skolnick; University of She�eld,She�eld, United KingdomA review will be given of recent progress inthe achievement of quantum-optical func-tionality in prototype circuits based on III-V suspended waveguides containing embed-ded self-assembled quantum dots.
CJ-7.4 WED 9:30Graphene-mode-locked Holmium FiberLaser Operating Beyond 2.1 um�V. Dvoyrin1,2,3, N. Tolstik1,2, E. Sorokin2,I. Sorokina1, and A. Kurkov4; 1NorwegianUniversity of Science and Technology, Trond-heim, Norway; 2Technical University of Vi-enna, Vienna, Austria; 3Fiber Optics Re-search Center, Russian Academy of Sciences,Moscow, Russia; 4A.M. Prokhorov GeneralPhysics Institute, Moscow, RussiaA graphene-modelocked Ho-�ber laser gen-erates 0.22 nJ linearly polarized picosecondpulses beyond 2.1 um for the �rst time. 1.8-ps pulses were observed. �e 7 nm-widesech-shaped spectra correspond to 0.68 pstransform-limited pulse duration.
CLEO/ECBO-1.2 WED 9:30In vivo single cell labeling in zebra�shusing three-photon activationI. Tekeli1, I. Aujard2,3,4, X. Trepat1,5, L.Jullien2,3,4, A. Raya1,5,6,7, and �D. Zalvidea1;1IBEC, Barcelona, Spain; 2Ecole Normale Su-perieure, Paris, France; 3Sorbonne Univer-sites, UPCM, Paris, France; 4CNRS, Paris,France; 5ICREA, Barcelona, Spain; 6CIBER-BBN, Barcelona, Spain; 7CMRB, Barcelona,Spain�ree-photon activation with 4D resolutionfor permanent labeling internal tissues invivo at the single cell level. �e resultingmodi�cation (GFP-labeled cardiomyocytes)is permanent and transmitted to daughtercells upon division.
CK-10.5 WED 9:30Strong Optomechanical Interactions in aSliced Photonic Crystal Nanobeam�R. Leijssen and E. Verhagen; FOM-InstituteAMOLF, Amsterdam,�e NetherlandsWe create a novel optomechanical systembased on a slot waveguide mode, demon-strating sensitive free-space readout of ther-mal motion. Comparison to radiation-pressure e�ects attributes the sensitive trans-duction to a large photon-phonon couplingrate of ∼9MHz.
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and tested. Less than 1% re�ection per sur-face is achieved at 10.6 micron wavelength.Laser damage threshold has increased atleast tenfold over thin-�lm coated windows.
GermanyWe study the in�uence of radiative couplingin a semiconductor quantum dot based mi-crocavity laser. Our results show that for suf-�ciently small systems a laser transition isonly observable when superradiant couplinge�ects are present.
of Technology, Warsaw, Poland; 2MilitaryInstitute of Aviation Medicine, Warsaw,PolandIn this work a new concept of a photonic in-tegrated interrogator for application in FBG-based sensor networks is discussed. �e op-tical chip was designed in a generic approachand fabricated in a multi-project wafer run.
tral Laser Facility, Didcot, United Kingdom;2Blackett Laboratory, Imperial College, Lon-don, United KingdomWe simulate 12.5mJ single-cycle ampli�ca-tion and compression of SWIR pulses ina Ti:Sapph pumped OPA and outline aproof-of-principle experiment on the STFCArtemis laser facility for the generation ofisolated attosecond water window pulses.
CE-10.3 WED 9:15Fused-silica mirror substrates withlaser-microstructured openings withreduced chipping�D. Esser, J.-H. Staasmeyer, J. Weitenberg, P.Rußbüldt, T. Sartorius, and H.-D. Ho�mann;Fraunhofer Institut f. Lasertechnik, Aachen,GermanyMirrors with small openings for geometricseparation of laser beams manufactured byInverse Laser Drilling su�er from chippingat the opening’s edges. A simple method toeliminate the chipping is presented.
CB-4.3 WED 9:15A nitride-on-Silicon microdisk laseremitting at 275 nm androom-temperature�T. Guillet1, J. Sellés1, C. Brimont1,G. Cassabois1, B. Gayral2,3, M. Mexis4, F.Semond4, I. Roland5, Y. Zeng5, X. Checoury5,and P. Boucaud5; 1Laboratoire CharlesCoulomb, Université Montpellier 2-CNRS,Montpeller, France; 2Université GrenobleAlpes, Grenoble, France; 3CEA-INAC-SP2M,Grenoble, France; 4CNRS-CRHEA, Val-bonne, France; 5Institut d’ElectroniqueFondamentale, Université Paris Sud-CNRS,Orsay, FranceA microlaser emitting at 275nm is demon-strated at room temperature under opticalpumping by combining ultrathin GaN/AlNquantum wells grown on silicon in highquality factor (Q=6000) microdisk res-onators.
CH-6.4 WED 9:15Low-cost monitoring of the wavelengthdi�erence of two transmitters for two-waytime transfer over optical �breR. Slavik1, �J. Vojtech2, and V. Smotlacha2;1University of Southampton, Southampton,United Kingdom; 2CESNET z.s.p.o., Praha,Czech RepublicUse of the leading and trailing edge of astandard telecom 200-GHz low-cost �lter isdemonstrated to provide enough bandwidthto be used to monitor relative frequencyof two low-cost wavelength-�xed telecomtransmitters.
CG-3.4 WED 9:15Extraction of the Bond Lengths ofAligned Acetylene Using Laser-InducedElectron Di�raction�M. Pullen1, B. Wolter1, A.T. Le2, M.Baudisch1, M. Hemmer1, A. Sen�leben3,C.D. Schröter4, J. Ullrich4,5, R. Moshammer4,C.D. Lin2, and J. Biegert1,6; 1ICFO-Institut deCiencies Fotoniques, Barcelona, Spain; 2J. R.Macdonald Laboratory, Physics Department,Kansas State University, Manhattan, Kansas,United States; 3Universität Kassel, Institutfür Physik und CINSaT, Kassel, Germany;4Max-Planck-Institut für Kernphysik, Hei-delberg, Germany; 5Physikalisch-TechnischeBundesanstalt (PTB), Braunschweig, Ger-many; 6ICREA-Institució Catalana de Re-cerca i Estudis Avançats, Barcelona, SpainLaser-induced electron di�raction (LIED) isable to image molecular dynamics at un-precedented temporal resolutions. We applyLIED to polyatomic molecules for the �rsttime and therefore open the door to creatinga ’molecular movie’.
CE-10.4 WED 9:30Micromilled Silica Refractometer withNanoscale Surface Roughness�L.G. Carpenter, P.A. Cooper, C. Holmes,C.B.E. Gawith, J.C. Gates, and P.G.R. Smith;Optoelectronics Research Centre, Universityof Southampton,, Southampton, United King-domWe demonstrate mircromilling of precisionslots in �ame hydrolysis deposition silicawith nanoscale surface roughness (3.0nm)and a tens of micron feature size, these slotsare integrated with waveguides and Bragggratings to produce refractometers.
CB-4.4 WED 9:30PT-symmetric microring lasers�M. Heinrich1,2, H. Hodaei1, M.-A.Miri1, D.N. Christodoulides1, and M.Khajavikhan1; 1CREOL �e College ofOptics and Photonics, University of CentralFlorida, Orlando, United States; 2Institute ofApplied Physics, Abbe Center of Photonics,Friedrich-Schiller-University, Jena, GermanyWe show that parity-time-symmetric no-tions can be harnessed to enforce stablesingle-mode lasing in highly multi-modedresonators. Undesirable modes are reliablysuppressed over a broad bandwidth, withoutthe need for additional �lters or frequency-selective components.
CH-6.5 WED 9:30High-performance Low-loss FibrePolarizer Based on Graphene and PVB�H. Zhang, N. Healy, L. Shen, C.C. Huang,D. Hewak, and A. Peacock; University ofSouthampton, Southampton, United King-domA broadband �bre polarizer based onGraphene and PVB is presented. Itstransmission loss is much less than anyprevious graphene based �bre polarizer andit has high extinction ratio across a widewavelength range.
CG-3.5 WED (Invited) 9:30New Opportunities in Ultrafast Sciencewith the European Light Infrastructure(ELI)�G. Sansone; Dipartimento di Fisica, Politec-nico di Milano, Milano, Italy; ELI-AttosecondLight Pulse Source, ELI-Hu K�, Szeged, Hun-garyI will review recent experiments performedat the FEL FERMI@Elettra, in connectionto the new opportunities o�ered by the up-coming facility Extreme Light Infrastructurefor investigations at an unprecedented com-bined intensity level and temporal resolu-tion.
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ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14aEH-1.5 WED 9:45topological photonic phase in chiralhyperbolic metamaterials�W. Gao1,2, M. Lawrence1, B. Yang1, F. Liu3,F. Fang2, B. Béri1, J. Li1, and S. Zhang1;1School of Physics &Astronomy, University ofBirmingham, Birmingham, United Kingdom;2State Key Laboratory of PrecisionMeasuringTechnology and Instruments, Tianjin, China,People’s Republic of (PRC); 3Department ofPhysics and Materials Science, City Univer-sity of Hong Kong, Hong Kong, China, Peo-ple’s Republic of (PRC)We propose a novel e�ective medium ap-proach towards achieving topologically pro-tected photonic surface states on chirohy-perbolic metamaterials. �is approach willpave the way for highly compact one-waytransportation of electromagnetic waves inintegrated photonic circuits.
CJ-7.5 WED 9:451 mJ, 10 kW, nanosecond all-�berthulium-doped �ber laser at 2050 nmL. Li, B. Zhang, �K. Yin, A. Jin, Z. Chen, andJ. Hou; College of Optoelectronic Science andEngineering, National University of DefenseTechnology, Changsha 410073, China, Peo-ple’s Republic of (PRC)We present an all-�ber high pulse energythulium-doped �ber laser at 2050 nm, withpulsewidth of 100 ns, output pulse energy upto 1 mJ and pulse peak power over 10 kW.
CLEO/ECBO-1.3 WED 9:45Digital Holographic Microscopy inMorphometric Analysis of�ree-dimensional Cell Cultures�T. Pitkäaho1,2, A. Manninen3, and T.Naughton1; 1Department of Computer Sci-ence, Maynooth University, Maynooth, Re-public of Ireland; 2RFMedia-Laboratory,Oulu Southern institute, University of Oulu,Ylivieska, Finland; 3Biocenter Oulu, Univer-sity of Oulu, Oulu, FinlandDigital holographic microscopy is used forimaging three-dimensional cysts of epithe-lial cells. Several segmentation techniquesare compared. We �nd statistical di�erencesin the reconstructed phase from normal andgenetically transformed cysts.
CK-10.6 WED 9:45Side-pumpedWGMMilled-MicrostubLaser�S. Bakhtiari Gorajoobi, G. Senthil Muru-gan, and M. Zervas; Optoelectronics Re-search Centre, University of Southampton,Southampton, United KingdomA new Yb-doped silica high Q WGM mi-crostub laser fabricated by CO2 laser millingis demonstrated. Fabrication time is short,and unique structure of the resonator allowsrealization of robust lasers and sensors.
10:30 – 12:00EH-2: Plasmons in LowDimensional MaterialsChair: Cyriaque Genet, University of Stras-bourg, Strasbourg, France
10:30 – 12:00EB-4: Quantum Key DistributionChair: Nicolo Spagnolo, La Sapienza Univer-sita’ di Roma, Roma, Italy
10:30 – 12:00CJ-8: Ultrafast Fibre Laser SystemsChair: Yoann Zaouter, Amplitude Systems,Pessac, France
10:30 – 12:00CLEO/ECBO-2: OpticalManipulation of BiomatterChair: �omas Huser, Bielefeld University,Bielefeld, Germany
10:30 – 12:00CK-11: Interactions and PhotonicControlChair: Alfredo De Rossi,�ales Research andTechnology, Palaiseau, France
EH-2.1 WED 10:30Near-�eld detection of plasmonic modesin topological insulator nanostructures inthe visible part of the spectrum�A. Dubrovkin1, G. Adamo1, A. Sulaev2,Q.J. Wang1,3, L. Wang4, and N. Zheludev1,5;1Centre for Disruptive Photonic Technolo-gies, Nanyang Technological University, Sin-gapore; 2School of Physical andMathematicalSciences, Nanyang Technological University,Singapore; 3OPTIMUS, Photonics Centre ofExcellence, School of Electrical and ElectronicEngineering, Nanyang Technological Univer-sity, Singapore; 4RMIT University, Physics,School of Applied Sciences, Melbourne, Aus-tralia; 5Optoelectronics Research Centre andCentre for Photonic Metamaterials, Univer-sity of Southampton, Southampton, UnitedKingdomDirect near-�eld imaging of topologicalinsulator nanostructures resolves localizedsurface plasmons in the visible range. Am-plitude and phase distributions of the plas-mons �eld are found to be dependent on par-ticles shape and size.
EB-4.1 WED 10:30Quantum Key Distribution sender add-onfor handheld devices�G. Mélen1, M. Rau1, L. Fuchs1, T. Vogl1,G. Corrielli2, A. Crespi2, R. Osellame2,and H. Weinfurter1,3; 1Faculty of Physics,Ludwig-Maximilian-Universität, München,Germany; 2Istituto di Fotonica e Nanotec-nologie, Consiglio Nazionale delle Ricerche(IFN-CNR) and Dipartimento di Fisica, Po-litecnico di Milano, Milano, Italy; 3Max-Planck-Institut für Quantenoptik, Garchingbei München, GermanyWe developed a miniaturized Quantum KeyDistribution sender unit for asymmetricserver-client scenarios. �is module canbe integrated in mobile devices to guaran-tee secure short-range communications withshared dedicated receivers such as an ATM.
CJ-8.1 WED 10:30Carrier-Envelope-Phase-Stable Ti:Sa-Master-Oscillator-Yb-Power-Ampli�erSystem�T. Saule1,2, O. deVries3, S. Holzberger1,2,M. Plötner3, F. Lücking4, J. Limpert3,5, A.Tünnermann6, F. Krausz1,2, and I. Pupeza1,2;1Max-Planck-Institut für Quantenoptik,85748 Garching, Germany; 2Ludwig-Maximilians-Universität München, 85748Garching, Germany; 3Fraunhofer Institutefor Applied Optics and Precision Engineer-ing, 07745 Jena, Germany; 4FemtolasersProduktions GmbH, 1100 Vienna, Austria;5Active Fiber Systems GmbH, 07745 Jena,Germany; 6Friedrich-Schiller-UniversitätJena, Institut für Angewandte Physik, 07745Jena, GermanyWe demonstrate that Yb:�ber-based ampli-�er systems seeded by Ti:Sa oscillators aresuitable for highly phase-stable pump-probeexperiments, as the 1000-fold ampli�cationincreases the integrated phase noise by only38 mrad.
CLEO/ECBO-2.1 WED (Invited) 10:30Twice around is more: �e bene�ts ofspatial phase modulation larger than 2 pifor imaging and trapping�M. Ritsch-Marte; Biomedical Physics, Inns-bruck, AustriaHigh resolution liquid crystal SLMs canachieve a phase modulation pitch of morethan 2 pi. We show how this may be ex-ploited to hugely expand the range of appli-cations for LC-SLMs in imaging and trap-ping.
CK-11.1 WED 10:30Heavy Photons for Light Localization atVanishingly Small Disorder-Levels�A. Baron1, R. Faggiani2, X. Zang2, L.Lalouat3, S. Schulz4,5, K. Vynck2, B.O’Regan4,6, B. Cluzel3, F. de Fornel3, T.Krauss4,6, and P. Lalanne2; 1Center forMetamaterials and Integrated Plasmonics,Duke University, Durham, United States;2LP2N, Université de Bordeaux, Talence,France; 3ICB, Université de Bourgogne,Dijon, France; 4SUPA, University of StAndrews, St Andrews, United Kingdom;5Department of Physics, University ofOttawa, Ottawa, Canada; 6Department ofPhysics, University of York, York, UnitedKingdomWe show that the key parameter drivingthe spatial extent of localized modes formedin randomly-perturbed periodic media nearthe band edge is the e�ective photon massrather than the group index.
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ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTESCE-10.5 WED 9:4545� tilted gratings for silica-basedintegrated polarizers�M.T. Posner, P.L. Mennea, N. Podoliak, P.Horak, J.C. Gates, and P.G.R. Smith; Univer-sity of Southampton, Southampton, UnitedKingdomWe report a novel study and demonstra-tion of a broadband tilted grating-based in-tegrated polarizer on a silica platform anddemonstrate a polarisation extinction ratioof 4.9±0.4dB and operation in the C-band.
CB-4.5 WED 9:45Ultrasmall Microdisk and MicroringLasers�N. Kryzhanovskaya1,3, A. Zhukov1,3, M.Maximov2,1, E. Moiseev1, I. Shostak1, Y.Kudashova1, M. Kulagina2, A. Lipovskii1,3,V.-M. Korpijärvi4, H. Karjalainen4, T.Niemi4, and M. Guina4; 1St PetersburgAcademic University, St Petersburg, Rus-sia; 2Io�e Physical-Technical Institute, StPetersburg, Russia; 3St Petersburg StatePolitechnical University, St Petersburg,Russia; 4Optoelectronic Research Centre,Tampere University of Technology, Tampere,FinlandLasing characteristics of 1.3 �m quan-tum dot and 1.55 �m quantum well mi-crodisks and microrings of ultra-small di-ameter (down to 1 �m) are presented atroom and high (up to 100�C) temperatures.
CH-6.6 WED 9:45Enhancing the sensitivity of temperaturesensing with Fiber Bragg Gratings with aweak value ampli�cation scheme�L.J. Salazar-Serrano1,2, D. Barrera3,W. Amaya1, S. Sales3, V. Pruneri1,4, J.Capmany3, and J.P. Torres1,5; 1ICFO -Institut de Ciencies Fotoniques, Barcelona,Spain; 2Quantum Optics Laboratory, Uni-versidad de los Andes, Bogota, Colombia;3iTEAM Institute, Universidad Politecnicade Valencia, Valencia, Spain; 4ICREA -Institucio Catalana de Recerca i EstudisAvançats, Barcelona, Spain; 5Dep. Signal�eory and Communications, UniversitatPolitecnica de Catalunya, Barcelona, SpainWe present a proof-of-concept experimentthat substantially improves the sensitivity oftemperaturemeasurements with Fiber BraggGratings. �e scheme, based on the conceptof weak ampli�cation, requires only linearoptics for its implementation.
10:30 – 12:00CE-11: Novel Lasers and LightEmitters Based on SemiconductorsChair: Stefan Kück, Physikalisch TechnischeBundesanstalt, Braunschweig, Germany
10:30 – 12:00CB-5: High-power SemiconductorLasersChair: Katrin Paschke, Ferdinand Braun-Institut, Berlin, Germany
10:30 – 12:00CH-7: SpectroscopyChair: Walter Lubeigt, M Squared LasersLtd., Glasgow, United Kingdom
10:30 – 12:00CG-4: Attosecond PhotoemissionDelaysChair: Peter Dombi, Wigner Research Centrefor Physics, Budapest, Hungary
CE-11.1 WED 10:30High-Power GaAs-based Superlumin-escent Diodes Employing Window-likeFacets for Low Spectral Modulation�O.M.S. Ghazal1, K.M. Groom1, B.J.Stevens2, N. Babazadeh1, D.T.D. Childs1,and R.A. Hogg1; 1Department of Electronicand Electrical Engineering, �e Universityof She�eld., She�eld, United Kingdom;2EPSRC National Centre for III-V Tech-nologies, Dept. of Electronic & ElectricalEngineering, �e University of She�eld.,She�eld, United KingdomWe present a window structure technologyfor realisation of high-power (~45mW), lowspectral modulation (~2%) superlumines-cent diodes on GaAs, without need for ap-plication of anti-re�ective coatings.
CB-5.1 WED 10:30High-power 1550 nm tapered DBR lasersfabricated using so� UV-nanoimprintlithography�J. Viheriälä1, J. Mäkelä1,2, A. Aho1, H.Virtanen1, T. Leinonen1, M. Dumitrescu1,andM. Guina1; 1Tampere University of Tech-nology, Tampere, Finland; 2University ofTurku, Turku, FinlandWe report 1550nm DBR-RWG grating de-sign, the fabrication process, and the outputcharacteristics of tapered DBR lasers pat-terned using novel so� UV-NIL. DBR lasersexhibited CW output power of 400mW andside-mode-suppression-ratio of 45dB.
CH-7.1 WED 10:30Dual-Comb Spectroscopy by SpectralBroadening of an Intensity-ModulatedContinuous-wave Laser in the C- andL-Telecom Bands�G. Millot1, S. Pitois1, and N. Picqué2;1Université de Bourgogne, Dijon, France;2Max-Planck-Institute für Quantenoptik,Garching, GermanyWe generate two mutually coherent fre-quency combs by wave-breaking in a non-linear �ber. We harness them for multi-heterodyne spectroscopy in the near in-frared, where the absorbing sample is con-tained in a hollow-core photonic crystal�ber.
CG-4.1 WED 10:30Attosecond time delays in single andmulti-photon ionization�C. Cirelli1, M. Sabbar1, S. Heuser1, R.Boge1, M. Lucchini1, L. Gallmann1,2, and U.Keller1; 1ETH Zurich, Zurich, Switzerland;2University of Bern, Bern, SwitzerlandUsing attosecond streaking, we compareenergy-dependent photoionization time de-lays in argon and neon. Our results supportthe validity of recently calculatedWigner de-lays and provide an estimation for the elec-tron wavepacket formation time.
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ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14aEH-2.2 WED 10:45Optical Modes in the TopologicalInsulator Bi2Se3 Probed by RelativisticElectrons�N. Talebi, C. Özsoy Keskinbora, and P.van Aken; Stuttgart Center for Electron Mi-croscopy, Max Planck Institute forIntelligentSystems, Stuttgart, GermanyTetradymite structures like Bi2Se3 sustaintopological magnetoelectric e�ect and be-long to the class of hyperbolic materials.Here, we study the plasmons in nanostruc-tures composed of Bi2Se3 both theoreticallyand experimentally, using electron energyloss spectroscopy.
EB-4.2 WED 10:45Low cost, short range quantum keydistribution.�D. Lowndes, S. Frick, R. Nock, E. Linares-Vallejo, and J. Rarity; University of Bristol,Bristol, United KingdomWe present a quantum key distribution sys-tem comprising a small low cost handhelddevice suitable for distribution to the generalpublic by visiting a large “QuantumATM” toestablish key with a trusted party.
CJ-8.2 WED 10:45Testing hollow waveguides for nonlinearpulse compression in kilowatt averagepower operation�S. Hädrich1,2, A. Ho�mann1, M. Krebs1, O.deVries3, A. Liem3, S. Fabian3, M. Plötner3,R. Eberhardt3, T. Schreiber3, J. Limpert1,2,and A. Tünnermann1,2,3; 1Friedrich-Schiller-Universität Jena, Abbe Center of Photonics,Institute of Applied Physics, Jena, Germany;2Helmholtz-Institute Jena, Jena, Germany;3Fraunhofer Institute for Applied Optics andPrecision Engineering, Jena, Germany�e average power transmission of waveg-uides typically employed in nonlinear com-pression experiments is measured up to 1kW. Record high values of 900 W (Kagome�ber) and 700W (capillary) are achieved, re-spectively.
CK-11.2 WED 10:45On-�bre thin �lm lithium niobate high Qslow Bloch mode cavity�W. Qiu, A. Ndao, Z. Xie, T. Grojean, N.Courjal, X. Xu, G. Ulliac, R. Salut, F.I. Baida,andM.-P. Bernal; Femto-st, Besançon, FranceWe present here the design and fabricationof an hetero-structure high-Q Slow BlochMode (SBM) cavity based on a 2D square lat-tice air holes engraved in thin �lm lithiumniobate.
EH-2.3 WED 11:00Simultaneous Experimental Observationof the Quantization and Interference ofSurface Plasmon Polaritons�T.T.A. Lummen1, L. Piazza1, E. Quiñonez2,Y.Murooka1, B.W. Reed3, B. Barwick2, and F.Carbone1; 1École Polytechnique Fédérale deLausanne, Lausanne, Switzerland; 2TrinityCollege, Hartford, United States; 3LawrenceLivermore National Laboratory, Livermore,United StatesUsing a new hybrid modality of ultra-fast Photon-InducedNear-�eld ElectronMi-croscopy, we demonstrate the dual aspectsof surface plasmon polaritons by simultane-ously measuring both their spatial interfer-ence and quantization in a single TEM ex-periment.
EB-4.3 WED 11:00Long distance atom-atom entanglementfor device-independent quantumcommunication protocols�D. Burchardt1, N. Ortegel1, K. Redeker1,R. Gartho�1, W. Rosenfeld1,2, and H.Weinfurter1,2; 1Ludwig-Maximilians-Universität, Munich, Germany; 2Max-Plack-Institut für Quantenoptik, Garching,GermanyWe show how entanglement of two atomsover 400m together with a sub-microsecondatomic state detection enables a loophole-free violation of Bell’s inequality, whichwill be an essential step towards device-independent quantum communication.
CJ-8.3 WED (Invited) 11:00Coherent Addition of Ultrafast FiberLaser Pulses�J. Limpert; Friedrich-Schiller-UniversitätJena, Institute of Applied Physics, Jena,Germany; Helmholtz-Institute Jena, Jena,Germany; Fraunhofer IOF Jena, Jena,Germany�e presentation will review the recentachievements and potential of spatially andtemporally separated ampli�cation of ultra-short laser pulses followed by coherent beamcombination and coherent pulse stacking.
CLEO/ECBO-2.2 WED 11:00Acoustophoretic 2D-Prefocusing in aGlass Micro�uidic Chip forOptical-Stretching�G. Nava1,2, F. Bragheri3, T. Yang1, P.Minzioni1, R. Osellame3,4, I. Cristiani1, andK. Berg-Sørensen5; 1Università di Pavia,Dipartimento di Ingegneria Industriale edell’Informazione, Pavia, Italy; 2Universitàdi Milano, Department of Biomedical Sci-ence and Translational Medicine, Milano,Italy; 3Istituto di Fotonica e Nanotecnologie(IFN)-CNR,Milano, Italy; 4Politecnico diMi-lano, Dipartimento di Fisica, Milano, Italy;5Technical University of Denmark, Depart-ment of Physics, Kgs. Lyngby, DenmarkAcoustophoretic forces are used to focus the�ow in a micro�uidic channel of an opticalstretcher chip. Waveguides are integrated inthe micro�uidic chip by femtosecond laserwriting and acoustic prefocusing is obtainedwith a piezoelectric crystal.
CK-11.3 WED 11:001D crossed gratings for polarizationindependent high-Q �ltering:experimental demonstration and possibleimprovementsO. Gauthier-Lafaye1,2, P. Arguel1,2, A.Monmayrant1,2, �K. Sharshavina1,2,3,A.-L. Fehrembach4, F. Lemarchand4, andA. Sentenac4; 1CNRS, LAAS, 7 avenuedu colonel Roche, F-31400, Toulouse,France; 2Univ de Toulouse, LAAS, F-31400,Toulouse, France; 3Centre National desEtudes Spatiales, 18 avenue EdouardBelin, 31401, Toulouse, France; 4InstitutFresnel, CNRS, Ecole Centrale Marseille,Aix-Marseille Université, 13013, Marseille,FranceWe experimentally demonstrate record po-larization independance of high Q GuidedMode Resonance Filters using recently pro-posed 1D crossed gratings concepts. Perfor-mance achieved are discussed in view of thefabrication imperfections and ways of im-provement.
EH-2.4 WED 11:15E�ect of electron-phonon coupling on theplasmon lifetimes in nanographene�J.R. Martínez Saavedra1 and F.J. Garcíade Abajo1,2; 1ICFO Institut de Cie*nciesFoto*niques, Castelldefels, Spain; 2ICREA-Institucio* Catalana de Recerca i EstudisAvanc*ats, Barcelona, SpainWe study the plasmon-phonon coupling in
EB-4.4 WED 11:15A Novel Concept of EntanglementDistribution in Optical Networks�A. Poppe1, A. Ciurana2, J.Martinez-Mateo2,J.L. Rosales2, B. Schrenk1, M. Peev1, and V.Martin2; 1Optical Quantum Technology, DSSDepartment, AIT Austrian Institute of Tech-nology GmbH, Vienna, Austria; 2Facultadde Informática, Universidad Politécnica de
CLEO/ECBO-2.3 WED 11:15Femtosecond Laser Nanostructuring forHigh-Topological Charge VortexTweezers with Continuously TunableOrbital Angular Momentum�R. Drevinskas, M. Gecevičius, M. Beresna,and P. Kazansky; University of Southampton,Southampton, United KingdomFemtosecond laser fabrictated polarization
CK-11.4 WED 11:15Tunable Short-Wavelength InfraredRe�ection and Transmission Based onNanometric�in Film Structures�H. Kocer1, S. Butun2, and K. Aydin2;1Turkish Military Academy, Ankara, Turkey;2Northwestern University, Evanston, IL,United StatesWe proposed and demonstrated experimen-
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ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTESCE-11.2 WED 10:45High colour rendering dichromaticmonolithic light emitting diode withtuneable colour temperature�A. Yadav1, I.E. Titkov1, A.V. Sakharov2,W.V. Ludin2, A. Nikolave2, G.S. Sokolovskii2,A.F. Tsatsulnikov2, and E.U. Rafailov1;1AIPT, Aston University, Birmingham,United Kingdom; 2Io�e Physico-TechnicalInstitute, St. Petersburg, RussiaWe have demonstrated high colour ren-dering up to 67 and CCT variation from3600K to 13500K with monolithic dichro-matic LED. �e green/blue ratio is tuneableabout 2.5 times with current amplitude andpulse width modulation.
CB-5.2 WED 10:45All-Semiconductor Master OscillatorPower Ampli�er at 1.5 um for High PowerApplicationsM. Faugeron1, �M. Krakowski1, Y. Robert1,E. Vinet1, P. Primiani1, J.-P. Le Goëc1, O.Parillaud1, M. Vilera2, A. Perez-Serrano2,J.M.G. Tijero2, I. Esquivias2, and F.van Dijk1; 1III-V Lab, Palaiseau cedex,France; 2CEMDATIC-ETSIT, UniversidadPolitecnica de Madrid (UPM), Madrid,SpainWe demonstrate a monolithically integrated3-section MOPA at 1.5 um. We observe thatthe bent architecture is more stable than theusual straight one. We show single-modeemission with a SMSR better than 45 dB.
CH-7.2 WED 10:45Direct Comparison of PDH and SweptLocking Scheme for Cavity-EnhancedAbsorption SpectroscopyG. Kowzan1, K.F. Lee2, M. Paradowska1,M. Borkowski1, P. Ablewski1, S. Wójtewicz1,K. Stec1, D. Lisak1, M.E. Fermann2, R.S.Trawiński1, and �P. Maslowski1; 1Institute ofPhysics, Faculty of Physics, Astronomy andInformatics, Nicolaus Copernicus University,ul. Grudziadzka 5, 87-100, Torun, Poland;2IMRA America, Inc., 1044 Woodridge Ave,Ann Arbor, United StatesCavity enhanced optical frequency combspectrometer based on an Er:�ber femtosec-ond laser and VIPA etalon, operating in the1.5-1.6 �m range is presented. Implementedvarious locking schemes allows comparisonand determination of their performance lim-its.
CG-4.2 WED 10:45Interpreting attoclock measurements oftunnelling times�L. Torlina1, F. Morales1, J. Kaushal1, I.Ivanov2, A. Kheifets2, A. Zielinski3, A.Scrinzi3, H.G. Muller1, M. Ivanov1,4, and O.Smirnova1; 1Max Born Institute, Berlin, Ger-many; 2Australian National University, Can-berra, Australia; 3Ludwig Maximilians Uni-versity, Munich, Germany; 4Imperial College,London, United KingdomUsing ab-initio simulations and fully quan-tum analytical theory, we show that atto-clock delays for hydrogen are induced en-tirely by the interaction of the outgoing elec-tron with the core and do not result fromtunnelling delays.
CE-11.3 WED 11:00Improvement of external quantume�ciency of blue and green InGaN LEDsusing corrugated interface substrates�M. Zulonas1, T.J. Slight2, I.E. Titkov1, A.Sakharov3, K.A. Fedorova1, W. Lundin3, A.Nikolaev3, W. Meredith2, A. Tsatsulnikov3,and E.U. Rafailov1; 1Optoelectronics andBiomedical Photonics Group, Aston Uni-versity, Birmingham, United Kingdom;2Compound Semiconductor TechnologiesGlobal, Glasgow, United Kingdom; 3Io�ePhysico-Technical Institute, St. Petersburg,RussiaWe demonstrated an improvement of exter-nal quantum e�ciency in blue (20%) andgreen (34%) InGaN based light emittingdiodes by the use of the optimized coneshaped Corrugated Interface Substrate tech-nology.
CB-5.3 WED 11:00Coherent combining of twohigh-brightness laser diodes phase-lockedby a Michelson-type external cavityG. Schimmel1, I. Doyen1, P. Ramirez1, S.Janicot1, M. Hanna1, P. Georges1, �G. Lucas-Leclin1, V. Vilokkinen2, P. Melanen2, P.Uusimaa2, J. Decker3, P. Crump3, and G.Erbert3; 1Laboratoire Charles Fabry, In-stitut d’Optique, CNRS, Univ Paris-Sud11, Palaiseau, France; 2Modulight, Tam-pere, Finland; 3Ferdinand-Braun-Institut,Leibniz-Institut für Höchstfrequenztechnik,Berlin, GermanyWe describe a new coherent beam combin-ing architecture based on the passive phase-locking of two laser diodes in a Michelsonexternal cavity on their rear side, and theircoherent combination on their front side.
CH-7.3 WED 11:00Coherent Spectroscopy of Optical ActivityK. Hiramatsu1,2, �E. Plum1, J. Valente1,K.F. MacDonald1, and N.I. Zheludev1,3;1University of Southampton, Southampton,United Kingdom; 2�e University of Tokyo,Toyko, Japan; 3Nanyang Technological Uni-versity, Singapore, SingaporeWe demonstrate control of polarization oflight with light. Optical activity of metama-terials is controlled by coherent light wavesinteracting on a metamaterial nanostructureresulting in continuous control over polar-ization azimuth rotation and ellipticity.
CG-4.3 WED 11:00How far does an electron travel duringHigh-Order Harmonic Generation?�H.G. Kurz1, M. Kretschmar1, T.Binhammer2, T. Nagy1,3, D. Ristau1,4,M. Lein5, U. Morgner1,4, and M. Kovačev1;1Leibniz Universität Hannover - Institutfür Quantenoptik, Hannover, Germany;2Venteon GmbH, Hannover, Germany;3Laser-Laboratorium Göttingen, Göttingen,Germany; 4Laser Zentrum Hannover,Hannover, Germany; 5Leibniz UniversitätHannover - Institut für theoretische Physik,Hannover, GermanyWepresent in-situmeasurements of the elec-tronic motion during high-order harmonicgeneration (HHG) with Ångstrom spatialresolution by using liquid-water droplets asa target. �e measurements verify the semi-classical treatment of the electronic excur-sion during HHG.
CE-11.4 WED 11:15AlGaN-based MQWs emitting at 280nmfor Vertical Cavity Surface Emitting Laser�G. Le Gac1, X. Li2,3, S. Sundaram3, Y.El Gmili3, T. Moudakir3, P. Disseix1, F.Réveret1, D. Lagarde4, J. Leymarie1, S.Bouchoule5, G. Patriarche5, F. Genty6, J.-P.Salvestrini3,7, R.D. Dupuis8, P.L. Voss2,3,and A. Ougazzaden2,3; 1Institut Pascal,,
CB-5.4 WED 11:15High brightness narrow-stripe broad-arealaser with 7 W optical output at 910, 935& 970 nm for coarse spectral beamcombining�J. Decker, P. Crump, J. Fricke, A. Maaßdorf,G. Erbert, and G. Tränkle; Ferdinand-Braun-Institut, Leibniz-Institut für Höchstfrequen-ztechnik, Berlin, Germany
CH-7.4 WED 11:15Towards Planet Hunting on a Chip:On-Telescope Demonstration of anIntegrated 2D-3D Hybrid PhotonicSpectrograph�N. Cvetojevic1,2,3, N. Jovanovic4, S. Gross1,5,I. Spelaniak6, B. Norris3, C. Schwab7, O.Guyon4,8, F. Martinache9, M. Withford1,5,and J. Lawrence2; 1Centre for Ultrahighbandwidth Devices for Optical Systems(CUDOS), Sydney, Australia; 2AustralianAstronomical Observatory (AAO), Sydney,Australia; 3Sydney Institute for Astron-
CG-4.4 WED 11:15Attosecond Near-Field Streaking from AuNanotipsB. Förg1, J. Schötz1, F. Süßmann1,M. Förster2, M. Krüger2, B. Ahn3, K.Wintersperger1, M. Stockman4, D. Kim3, F.Krausz1, P. Hommelho�2, and �M. Kling1;1Laboratory for Attosecond Physics, MPQ &LMU, Garching, Germany; 2Department of
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graphene nanoislands through a perturba-tive RPA expansion and conclude that it con-tributes with a few millielectronvolts to theplasmon width, which increases with boththe island size and doping.
Madrid, Madrid, SpainWe propose a network design for entan-glement distribution to multiple users ina typical metropolitan area network. Wepropose a �xed wavelength plan usingstandard wavelength-division multiplexingequipment together with broadband sourcesof entangled photon-pairs.
converters for a high-topological charge op-tical vortices with tunable orbital angularmomentum are demonstrated. �e continu-ous control of torque without altering the in-tensity distribution was implemented in op-tical trapping.
tally realizable nanometric thin �lm struc-ture that is capable of tuning the re�ectionand transmission in the short-wavelengthinfrared spectrum based on thermally in-duced vanadium dioxide phase transition.
EH-2.5 WED 11:30Plasmene: An Arti�cial Graphene fromPlasmonic Nanoparticle Family�D. Sikdar1, K.J. Si2, W. Zhu1, W. Cheng2,and M. Premaratne1; 1Department of Elec-trical and Computer Systems Engineering,Monash University, Clayton, Australia;2Department of Chemical Engineering,Monash University, Clayton, AustraliaWe introduce ‘Plasmene’—in analogyto graphene—as freestanding, single-particle-thick, giant superlattice-sheetsof nanoparticles (‘meta-atoms’) from the‘plasmonic periodic table’, which featureboth programmable plasmon propagationand gap-mode resonance characteristics,besides many unique optical properties.
EB-4.5 WED 11:30Quantum Key Distribution (QKD) inOptical Networks: Does RamanScattering spoil things for Integration?F.Hipp1, �A. Poppe1, S. Aleksic2, D.Winkler2,B. Schrenk1, and G. Franzl2; 1Austrian In-stitute of Technology (AIT), Vienna, Austria;2Vienna University of Technology, Vienna,AustriaAn O-band centric integration of QKD ina 20-channel DWDM network is inves-tigated by analyzing the noise from on-o�-keyed communication signals down tosingle-photon-level.
CJ-8.4 WED 11:30High-power pulse compression ofmodelocked thin-disk lasers usingKagome-type HC-PCF: low-noise sourcefor HHG�F. Emaury1, A. Diebold1, B. Debord2, F.Gérôme2, C. Saraceno1,3, T. Südmeyer3, F.Benabid2, and U. Keller1; 1ETH Zurich,Zurich, Switzerland; 2GPPMM group,XLIM Research institute, Limoges, France;3Laboratoire Temps-Fréquence, Université deNeuchâtel, Neuchatel, SwitzerlandHigh average power pulse compressionin gas-�lled-Kagome-type HC-PCFs aredemonstrated for sub-100-fs pulse genera-tion with very low noise of <0.6% rms [1Hz,100 kHz].
CLEO/ECBO-2.4 WED (Invited) 11:30Accelerating Progress in BiomedicalImaging�K. Dholakia; University of St. Andrews,SUPA, North Haugh, Fife, United KingdomWe describe the use of propagation invari-ant light �elds for use in light sheet imaging.Studies in particular using Airy light beamsincluding generation of such beams in com-pact systems will be discussed
CK-11.5 WED 11:30On/O� Switching Photonic-CrystalLasers by Gate Control of Graphene�M.-S. Hwang1, J.-H. Choi1, K.-Y. Jeong1, S.-H. Kwon2, and H.-G. Park1; 1Departmentof Physics, Korea University, Seoul, Korea,South; 2Department of Physics, Chung-AngUniversity, Seoul, Korea, SouthWe demonstrate optically pumpedgraphene-integrated photonic crystal lasers.By applying gate voltage to the single-layergraphene, we tune the Fermi level ofgraphene and thus control lasing operatione�ciently.
EH-2.6 WED 11:45Experimental Demonstration of OpticalNonreciprocity Engineering UsingMagnetoplasmonic NanogratingsL. Halagacka1, �M. Vanwolleghem2, F.Vaurette2, J. Ben-Youssef3, K. Postava1, J.Pistora1, and B. Dagens4; 1Dept of Physicsand Nanotechnology Center, TechnicalUniversity Ostrava, Ostrava - Poruba,Czech Republic; 2Institut d’Electronique,de Microélectronique et de Nanotech-nologie, CNRS, Villeneuve d’Ascq, France;3Laboratoire de Magnétisme de Bretagne,Université de Bretagne Occidentale, CNRS,Brest, France; 4Institut d’ElectroniqueFondamentale, CNRS, Orsay, France
EB-4.6 WED 11:45Quantum-secure authentication of aphysical unclonable key�S. Goorden1, M. Horstmann1,2, A. Mosk1, B.Škorić3, and P. Pinkse1; 1Complex PhotonicSystems (COPS), MESA+ Institute for Nan-otechnology, University of Twente, Enschede,�e Netherlands; 2Laser Physics and Nonlin-ear Optics, MESA+ Institute for Nanotech-nology, University of Twente, Enschede, �eNetherlands; 3Eindhoven University of Tech-nology, Eindhoven,�e NetherlandsQuantum-Secure Authentication (QSA) ofa physical unclonable key is secure againstcopying due to technological limitationsand against digital emulation by virtue of
CJ-8.5 WED 11:451700-nm High-Energy All-Fiber FormatFemtosecond Laser�L. Kotov1,2,3, M. Likhachev2, M. Bubnov2,D. Lipatov4,5, A. Guryanov4, M. Tang6, A.Hideur6, and S. Février1; 1Univ. Limoges,CNRS, XLIM, UMR 7252, Limoges, France;2Fiber Optics Research Center RAS, Moscow,Russia; 3Moscow Institute of Physics andTechnology, Dolgoprudny, Russia; 4Instituteof Chemistry of High-Purity Substances RAS,Nizhny Novgorod, Russia; 5LobachevskyState University of Nizhnii Novgorod, NizhnyNovgorod, Russia; 6CORIA UMR 6614, Nor-mandie Université, CNRS-INSA-Universityof Rouen, Rouen, France
CK-11.6 WED 11:45Low Power All-Optical WavelengthConversion with Terahertz Refresh Ratesusing Colloidal Nanocrystals�P. Geiregat1,2,4, A. Houtepen2,3,4, D. Van�ourhout1,4, and Z. Hens2,3,4; 1Universityof Ghent, Department of Information Tech-nology, Photonics Research Group, Gent, Bel-gium; 2University of Ghent, Department ofInorganic and Physical Chemistry, Physicsand Chemistry of Nanostructures Group,Gent, Belgium; 3Technical University ofDel�, Department of Chemical Engineering,OEMS, Del�,�e Netherlands; 4University ofGhent, Center for Nano - and BioPhotonics,Gent, Belgium
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Aubière, France; 2School of Electrical andComputer Engineering, Georgia Insitute ofTechnology, Metz, France; 3UMI 2958 Geor-gia Tech CNRS, Metz, France; 4Universityof Toulouse, LPCNO, INSA-CNRS-UPS,Toulouse, France; 5LPN CNRS, UPR20,Marcoussis, France; 6Supelec, LMOPS, EA4423, Metz, France; 7University of Lorraine,LMOPS, EA 4423, Metz, France; 8Centerfor Compound Semiconductors and Schoolof Electrical and Computer Engineering,Georgia Institute of Technology, Atlanta,United StatesWe report on the design, fab-rication and characterization ofAl0.57Ga0.43N/Al0.37Ga0.63N MQWsgrown on a relaxed Al0.57Ga0.43N bu�eron AlN template by Metal Organic VaporPhase Epitaxy, for Vertical Cavity SurfaceEmitting Laser application.
We present the progress of narrow stripebroad area lasers operating at 910, 935 & 970nm, with P = 7W and in-plane BPP down to1.5 mm*mrad from a 30 �m wide stripe.
omy (SIfA), University of Sydney, Sydney,Australia; 4Subaru Telescope, NationalAstronomical Observatory of Japan (NAOJ),Hilo, United States; 5MQ Photonics ResearchCentre, Dept. of Physics and Astronomy,Macquarie University, Sydney, Australia;6School of Photonics & Quantum Sciences,Heriot-Watt University, Edinburgh, UnitedKingdom; 7Department of Astronomy &Astrophysics, Pennsylvania State University,Pennsylvania, United States; 8Department ofAstronomy and Steward Observatory, �eUniversity of Arizona, Tucson, United States;9Laboratoire Lagrange, Observatoire de laCote dAzur, Nice, FranceWe present the �rst successful demonstra-tion of an integrated photonic spectrograph,with a passive on-chip multimode-to-singlemode converter, on an 8 metre class tele-scope behind an adaptive optics system.
Physics, FAU Erlangen-Nürnberg, Erlangen,Germany; 3Physics Department, CASTECH,POSTECH, Pohang, Korea, South; 4Centerfor Nano-Optics, GSU Atlanta, Atlanta,United StatesWe demonstrate that attosecond streakingspectroscopy can be applied to measure thewaveform of the near-�eld of Au nanotipsthat results from their excitation with a few-cycle near-infrared laser pulse.
CE-11.5 WED 11:30Lasing Properties of SemiconductorMicrospheres with High SphericityFabricated by Laser Ablation inSuper�uid HeliumS. Okamoto1, S. Ichikawa2, Y. Minowa1,and �M. Ashida1; 1Graduate School of Engi-neering Science, Osaka University, Toyonaka,Japan; 2Institute for NanoScience Design, Os-aka University, Toyonaka, JapanWe successfully fabricated semiconductormicrospheres of ZnO, CdSe, etc. with highsphericity and good crystal quality by laserablation in super�uid helium and investi-gated their whispering gallery mode lasingat room temperature.
CB-5.5 WED 11:30Beam shaping of broad-area diode lasersusing 3D integrated optics�S. Gross, D. Coutts, and M.J. Withford; Cen-tre for Ultrahigh bandwidth Devices for Op-tical Systems (CUDOS), MQ Photonics Re-search Centre, Department of Physics and As-tronomy, Macquarie University, Sydney, Aus-traliaWe present a novel approach based on 3Dintegrated optics to shape the output ofa broad-area laser diode. Two photoniclanterns are used to create a circular sym-metric beam with uniform beam quality.
CH-7.5 WED 11:30Detailed analysis of laser-inducedbreakdown spectroscopy of singleparticles using electrodynamic balancetrappingS. Järvinen, S. Saari, J. Keskinen, and �J.Toivonen; Tampere University of Technology,Tampere, FinlandDetailed analysis of laser-induced break-down spectroscopy of single micron-sizedparticles is presented utilizing electrody-namic balance levitation to trap particles forstable analysis.
CG-4.5 WED 11:30Probe-Induced Time Delays in SinglePhoton Emission from a Copper(111)Surface�L. Kasmi1, M. Lucchini1, L. Castiglioni2,P. Kliuiev2, A. Ludwig1, M. Greif2,M. Hengsberger2, J. Osterwalder2, L.Gallmann1,3, and U. Keller1; 1ETH Zurich,Zurich, Switzerland; 2University of Zurich,Zurich, Switzerland; 3University of Bern,Bern, SwitzerlandWe investigate the dependence of photoe-mission delays from a copper (111) surfaceon the re�ection geometry of the infraredprobe �eld. �e Fresnel equations are foundto hold even on atomic length and timescales.
CE-11.6 WED 11:45Density of localized states in disorderedGa(AsBi)�M.K. Shakfa, M. Wiemer, P. Ludewig, K.Jandieri, K. Volz, W. Stolz, S. Baranovskii,andM. Koch;Department of Physics andMa-terial Sciences Center, Philipps-University ofMarburg, Marburg, Germany�e thermal quenching of the photolumi-nescence in disordered Ga(AsBi) shows anodd characteristic. Our study demonstratesthat an approach with a non-monotonoustwo-component density of localized statesis indispensable to theoretically reproducesuch a behavior.
CB-5.6 WED 11:45High-power, low-linewidth ridgewaveguide laser stabilized by compactVolume Holographic Grating externalcavity at 780 nmS. Rauch and �J. Sacher; Sacher LasertechnikGmbH, Marburg, GermanyWe present an external Volume grating-cavity ridge waveguide diode laser with anoutput power of 380 mW and a narrowlinewidth at a wavelength of 780 nm whichcan be continuously tuned by 5.2 GHz.
CH-7.6 WED 11:45Remote sensing of water temperature andsalinity using Raman spectroscopy�C. Artlett and H. Pask; Macquarie Univer-sity, Sydney, AustraliaWe have analysed the response of seawa-ter Raman spectra to changing temperatureand salinity, and developedmethods for pre-dicting these parameters (RMSE: 0.4 �C, 0.6PSU). Preliminary �eld trials of remote Ra-man sensing are described.
CG-4.6 WED 11:45Sub-Cycle Resolved Probe Retardation inStrong-Field Pumped DielectricsA.P. Pati, I.S.Wahyutama, and �A.N. Pfei�er;Institute of Optics and Quantum Electronics,Jena, Germany�e temporal retardation of a few-cycleprobe pulse in a strong-�eld pumped, bulkdielectric ismeasured. Sub-cycle oscillationsin the pump-probe delay scan reveal tran-sient conduction band populations and theinterband dephasing time.
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ROOM 4a ROOM 4b ROOM 13a ROOM 13b ROOM 14a
We demonstrate experimentally a disrup-tive approach to control both magnitudeand sign of nonreciprocal e�ects by couplingplasmonic and slit cavity resonances whenvarying only the geometry of a plasmonicnanograting on a magnetooptical substrate.
quantum-physical principles, even in caseattackers obtain all information about thekey.
We present an all-�ber format femtosecondlaser operating near 1700nm. �e laser isbased on soliton self-frequency shi� of highpower pulses at 1555nm in large mode area�bers. 7nJ, 160fs pulses are demonstrated
�e interplay between intraband andbandgap absorption in colloidal quantumdots leads to strong and ultrafast modula-tion of light absorption, enabling all-opticalwavelength conversion at terahertz refreshrates with cheap materials and strongerlight-matter interaction.
ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b14:00 – 15:30CN-1: Laser Sources for Defenceand SecurityChair: Joachim Wagner, IAF, Freiburg, Ger-many
14:00 – 15:30EH-3: Dielectrics and HyperbolicMetamaterialsChair: Sol Carretero Palacios, Institute ofMaterial Science of Sevilla, Sevilla, Spain
14:00 – 15:30EB-5: Quantum SimulationChair: Alessandro Fedrizzi, University ofQueensland, Brisbane, Australia
14:00 – 15:30CJ-9: Pulsed Fibre Laser SourcesChair: Tino Eidam, University of Jena, Jena,Germany
14:00 – 15:30CF-4: Novel Ultrafast LasersChair: �omas Südmeyer, University ofNeuchâtel, Neuchâtel, Switzerland
CN-1.1 WED 14:00Long-Wave Infrared Single-FrequencyOP-GaAs OPO Pumped by a PulsedTm:YAPMicrolaserQ. Clément1, J.-M. Melkonian1, �J.-B.Dherbecourt1, M. Raybaut1, A. Grisard2, E.Lallier2, B. Gérard3, B. Faure4, G. Souhaité4,and A. Godard1; 1ONERA, Palaiseau,France; 2�ales Research & Technology,Palaiseau, France; 3III-V Lab, Palaiseau,France; 4Teem Photonics, Meylan, FranceA single-frequency nested cavity OPO hasbeen developed for stand-o� detection ofhazardous chemicals in the 10.3-10.9micronrange. It is based on an OP-GaAs nonlinearcrystal pumped by a pulsed Tm:YAP micro-laser.
EH-3.1 WED (Invited) 14:00All-dielectric Nanophotonics: MagneticResponse, Fano Resonances, FunctionalMetasurfaces, and Nonlinear E�ects�I. Staude and Y. Kivshar; Nonlinear PhysicsCentre, Research School of Physics and Engi-neering, �e Australian National University,Canberra, AustraliaWe review recent advances in all-dielectricnanophotonics aiming at the manipula-tion of strong optically-induced electricand magnetic Mie resonances in dielectricnanostructures with high refractive index,including Fano resonances, Huygens meta-surfaces, and novel nonlinear e�ects.
EB-5.1 WED 14:00Observing Multi-Particle Decay and FanoResonances with Integrated Photonics�A. Crespi1,2, L. Sansoni3,4, G. Della Valle2,1,A. Ciamei3, R. Ramponi1,2, F. Sciarrino3, P.Mataloni3, S. Longhi2,1, and R. Osellame1,2;1Istituto di Fotonica e Nanotecnologie - Con-siglio Nazionale delle Ricerche, Milano, Italy;2Dip. di Fisica - Politecnico di Milano, Mi-lano, Italy; 3Dip. di Fisica - Sapienza Univer-sità di Roma, Roma, Italy; 4Integrated Quan-tum Optics - University of Paderborn, Pader-born, GermanyWe investigate experimentally the quantumdecay process of two particles, either bosonicor fermionic, by probing a femtosecond laserwritten waveguide array with two-photonstates. Manifestation of Fano resonancesstrongly depends on the particles’ statistics.
CJ-9.1 WED 14:00Passive Phase Locking of TwoMulti-Wavelength Fiber Lasers by MutualInjection Coupling and Spatial Filtering�B. Lei, J. Cao, W. Liu, and Y. Feng; Col-lege of Optoelectric Science and Engineering,National University of Defense Technology,Changsha, China, People’s Republic of (PRC)Passive phase locking of two multi-wavelength �ber lasers has been demon-strated using mutual injection couplingand single-mode �ber �ltering. Althoughseveral tens of longitudinal modes operatesimultaneously, stable interference patternis observed in experiment.
CF-4.1 WED (Invited) 14:00High-Power Sub-300-fs SemiconductorDisk Lasers�M. Mangold1, D. Waldburger1, S.M. Link1,M. Golling1, E. Gini2, B.W. Tilma1, and U.Keller1; 1Department of Physics, Institute forQuantum Electronics, ETH Zurich, Zurich,Switzerland; 2FIRST Center for Micro- andNanosicence, ETH Zurich, Zurich, Switzer-landWe present the �rst sub-150-fs SESAM-modelocked vertical-external-cavitysurface-emitting laser (VECSEL) with100-mW output power. Furthermore wereport on the �rst sub 300 fs modelockedintegrated external-cavity surface emittinglaser (MIXSEL), generating 180-mW ofoutput power.
CN-1.2 WED 14:15Rate equation modelling of thepower-versus-current characteristics ofhigh power mid-infrared quantumcascade lasers�H. �oll1, J. Wagner2, and Q. Yang2;1Diehl BGT Defence, Ueberlingen, Germany;2Fraunhofer Institute for Applied Solid StatePhysics, Freiburg, GermanyFrom a rate equation model an analyticalformula is derived, which is able to repro-duce experimental PI curves of high powerQCLs correctly for various design options.
EB-5.2 WED 14:15Validation of Boson Samplingexperiments�N. Spagnolo1, C. Vitelli1, M. Bentivegna1,D.J. Brod2, A. Crespi3, F. Flamini1, R.Ramponi3, P. Mataloni1, R. Osellame3, E.F.Galvao2, and F. Sciarrino1; 1Dipartimento diFisica, Sapienza Universita’ di Roma, Rome,Italy; 2Instituto de Fisica, Universidade Fed-eral Fluminense, Niteroi, Brazil; 3IFN-CNRand Dipartimento di Fisica, Politecnico diMilano, Milan, Italy�e experimental validation of photonicBoson Sampling experiments in integratedphotonic platforms is reported. We show theimplementation of statistical tests that canbe adopted to discriminate Boson Samplingdata from di�erent alternative hypotheses.
CJ-9.2 WED 14:155mJ pulsed Yb-doped all-�ber MOPAseeded by 0.2nm spectrally sliced superluminescent diode�M.O. Berendt, J. Spurrell, P. Barua, A.A.Umnikov, M.N. Velazquez, J.K. Sahu, S.-u.Alam, and D.J. Richardson; ORC, Universityof Southampton, Southampton, United King-domFiber MOPA system utilizing large core Yb-doped gain �ber to produce 100Hz rep-etition frequency 100ns, 5mJ rectangularpulses by ampli�cation of shaped seed pulsesfrom 0.2nm band pass �ltered Super Lumi-nescent Diode emission, is demonstrated.
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ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN14:00 – 15:30CK-12: Integrated Photonic SourcesChair: Lars Frandsen, Technical University ofDenmark, Lyngby, Denmark
14:00 – 15:30CE-12: �in FilmsChair: Bruno Viana, CNRS, Paris, France
14:00 – 15:30CB-6: Quantum Cascade LasersChair: Sven Hö�ing, University of St An-drews, St Andrews, United Kingdom
14:00 – 15:30CH-8: Optical Sources for Sensingand MetrologyChair: Vincenzo Spagnolo, Università e Po-litecnico di Bari, Bari, Italy
14:00 – 15:30CG-5: Attosecond PhotoionizationDynamicsChair: Matthias Kling, LMU München, Mu-nich, Germany
CK-12.1 WED (Tutorial) 14:00Rare-earth-doped Lasers on a SiliconChip�M. Pollnau; KTH-Royal Institute of Technol-ogy, Stockholm, SwedenRare-earth-doped lasers integrated on a sil-icon wafer are reviewed. �e theory ofcontinuous-wave lasers is extended by con-sidering spontaneous emission in the laserrate equation, thereby deriving the lasereigenvalue, coherence time, Q-factor, andlinewidth.
CE-12.1 WED 14:00Time-resolved microscopic study ofcharge carriers in newly developedperovskite thin �lms�K. Bader, R. Ciesielski, N. Giesbrecht, F.Hanusch, T. Bein, P. Docampo, M. Handloser,and A. Hartschuh; Department of Chem-istry and Center for NanoScience (CeNS),Ludwig-Maximilians-Universität München,81377 München, GermanyWe studied the photo-physical properties ofnewly developed perovskite thin �lms bytime-resolved laser scanning confocal mi-croscopy to correlate optical soaking e�ectsand charge carrier transport lengths with therespective �nal device e�ciencies.
CB-6.1 WED (Invited) 14:00Widely Tunable Interband Cascade Lasersfor the Mid-InfraredM. von Edlinger1, R. Weih2, J.Scheuermann1, L. Nähle1, M. Fischer1,S. Hö�ing2,3, J. Koeth1, and �M. Kamp2;1nanoplus GmbH, Gerbrunn, Germany;2Technische Physik, Universität Würzburg,Würzburg, Germany; 3School of Physics andAstronomy, St. Andrews, United Kingdom�e talk will present recent results on widelytunable interband cascade lasers in the mid-infrared. Design issues of these multi-segment devices, their fabrication and per-formance, and applications to gas sensingwill be discussed.
CH-8.1 WED 14:00E�ect of Injection Current on SignalStrength in a Single-Mode Laser DiodeOptical Feedback Interferometer Subjectto Weak Feedback�J. Al Roumy1,2, J. Perchoux1,2, Y.L. Lim3, T.Taimre4, A. Rakić3, and T. Bosch1,2; 1CNRS,LAAS, Toulouse, France; 2Univ de Toulouse,INP, LAAS, Toulouse, France; 3School of In-formation Technology and Electrical Engi-neering, �e University of Queensland, Bris-bane, Australia; 4School of Mathematics andPhysics, �e University of Queensland, Bris-bane, AustraliaWe present a simple analytical model thatdescribes the injection current dependenceof optical feedback interferometry powerand voltage signals strengths for a single-mode laser diode subject to weak feedback.
CG-5.1 WED (Invited) 14:00Attosecond Insight into ElectronCorrelation�M. Gisselbrecht1, D. Guénot1, E. Månsson1,D. Kroon1, M. Kotur1, E. Larsen1, S. Kasper1,M. Dahlström2, E. Lindroth2, A. Kheifets3,C. Arnold1, J. Mauritsson1, S. Sorensen1, andA. L’Huillier1; 1Department of Physics, LundUniversity, Lund, Sweden; 2Department ofPhysics, Stockholm University, Stockholm,Sweden; 3Research School of Physical Sci-ences, �e Australian National University,Canberra, AustraliaWe discuss how attosecond interferometryallows to shed light on the correlated elec-tron dynamics in a series of experiments onsingle and double ionization of noble gas.
CE-12.2 WED 14:15Lasing characteristics of an organic-inorganic halide perovskite thin �lm�Y.-H. Chou1, T.S. Kao2, J.-F. Huang2, C.-H.Chou2, K.-B. Hong2, F.-C. Chen2, and T.-C.Lu2; 1Inst. of Lighting and Energy Photonics,National Chiao Tung Univ., Tainan, China,Republic of (ROC); 2Dep. of Photonics andInst. of Electro-Optical Engineering, NationalChiao Tung Univ., Hsinchu, China, Republicof (ROC)We demonstrate lasing characteristics oforganic-inorganic halide perovskite pre-pared by solution process. �e excellent op-tical properties and versatility of these mate-rials show their promising potential to de-velop novel coherent light emitters in thenear future.
CH-8.2 WED 14:15Guidelines Towards Multi-100-W AveragePower Frequency Combs from�in-DiskLasers�F. Emaury1, A. Diebold1, A. Klenner1, C.Saraceno1,2, S. Schilt2, T. Sudmeyer2, and U.Keller1; 1ETHZURICH, Zurich, Switzerland;2Laboratoire Temps-Fréquence, Université deNeuchâtel, Neuchatel, SwitzerlandWe understand our complete noise and cav-ity dynamics characterization of the �rstCEO-referenceable 140-W laser based ona Yb:YAG SESAM modelocked thin-disk-laser and provide guidelines towards stabi-lized frequency combs in the >100W regime
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCN-1.3 WED (Invited) 14:30High Sensitive CMOS Image Sensor forLow Light Level Imaging�O. Nesher, E. Gross, and R. Ginat; AerospaceDivision, Elbit Systems Ltd., Haifa, IsraelElbit developed a digital low light levelCMOS sensor with similar sensitivity to GenII image intensi�er down to starlight. In thiswork we describe the the sensor, physicalmodel and results of �eld testing.
EH-3.2 WED 14:30Non-volatile Dielectric MetamaterialsRecon�gurable With LightQ. Wang1,2, E. Rogers1, �B. Gholipour1, T.Roy1, Y. Guanghui3, and N. Zheludev1,3;1University of Southampton, Southampton,United Kingdom; 2Institute of Materials Re-search and Engineering, Singapore, Singa-pore; 3Nanyang Technological University,Singapore, United KingdomHighly-controlled femtosecond-laser-induced phase changes in chalcogenide�lms allow us to write and erase arbitrarydielectric metamaterial patterns. �e tech-nology is further demonstrated by creatingdynamically re-focusable and chromaticallycorrectable lenses and super-oscillatorylenses.
EB-5.3 WED (Invited) 14:30Quantum simulation with optical lattices�U. Schneider; Cavendish Laboratory,University of Cambridge, Cambridge,United Kingdom; Fakultät für Physik,Ludwig-Maximilians-Universität München,München, Germany; Max-Planck-Institutfür Quantenoptik, Garching, Germany�e out-of-equilibrium dynamics of inter-acting many-body systems presents one ofthe most challenging problems in modernphysics. Ultracold atoms in optical latticeshave emerged as a powerful quantum simu-lator for these dynamics.
CJ-9.3 WED 14:301W ps master oscillator �ber ampli�ersystem continuously tunable from 740 nmto 910 nm�J. Lhermite1, R. Royon1, G. Santarelli2, J.-C. Delagnes1, and E. Cormier1; 1CELIA, Tal-ence, France; 2LP2N, Talence, FranceWe report on a MOPA system continuouslytunable from 740nm to 910nm. Such anemission covering 170nm is obtained bymeans of four-wave mixing in a microstru-tured �ber driven by an Ytterbium-dopedtunable �ber laser.
CF-4.2 WED 14:3015-GHz, Kerr-Lens Mode-Locked Laserand Fourier Synthesis of Each CombTooth�M. Endo1,2 and Y. Kobayashi1,2; 1�e In-stitute for Solid State Physics, �e Univer-sity of Tokyo, Kashiwa, Japan; 2ExploratoryResearch for Advanced Technology (ERATO),JST, Tokyo, JapanWe developed a Kerr-lens mode-lockedYb:Y2O3 ceramic laser with amode-spacingof 12 GHz (maximum 15 GHz). A�er select-ing a (several) user-speci�ed mode(s), weachieved the synthesis of up to six adjacentmodes.
EH-3.3 WED 14:45Emission of electromagnetic radiation intransformation-optical metamaterials�V. Ginis1, J. Danckaert1, I. Veretennico�1,and P. Tassin2; 1Vrije Universiteit Brus-sel, Brussel, Belgium; 2Chalmers University,Göteborg, SwedenUsing the tools of transformation optics,we show how realistic anisotropic metama-terials can decouple the intensity and thevelocity resolution of Cherenkov radiationfor high energy particle detectors with en-hanced sensitivity.
CJ-9.4 WED 14:45Modelling of Polarization E�ects inFourier Domain Mode-Locked (FDML)Lasers�C. Jirauschek1 and R. Huber2; 1TechnischeUniversität München, Munich, Germany;2Universität zu Lübeck, Lübeck, GermanyWe extend the theory of Fourier domainmode-locking (FDML) by including polar-ization e�ects such as �ber birefringence andcross-phase modulation. Comparison to ex-periment shows that these e�ects are impor-tant in standard non-polarization maintain-ing FDML lasers.
CF-4.3 WED 14:45Long-term, real-time correction ofcarrier-envelope phase �uctuations�M. Mero, N. Raabe, and G. Steinmeyer;Max-Born-Institut für Nichtlineare Optikund Kurzzeitspektroskopie, Berlin, GermanyAn improved version of the acoustic fre-quency comb based feed-forward CEP stabi-lization scheme is presented that enables vir-tually unlimited e�ective servo bandwidthsof several megahertz.
CN-1.4 WED 15:00A green pulsed lidar-radar transmitterbased on a frequency-shi�ed feedbacklaserM. Brunel1, H. Zhang1,2, �M. Romanelli1,and M. Vallet1; 1Institut de Physique deRennes, Rennes, France; 2Beijing Institute ofTechnology, Beijing, China, People’s Republicof (PRC)High-frequencymodulated pulses at 532 nmfor underwater lidar applications are emittedby frequency doubling the output of a FSFpassively Q switched laser
EH-3.4 WED 15:00Nonlinear Epsilon-Near-ZerometamaterialsR.K. Kaipurath1, M. Pietrzyk2, L. Caspani1,T. Roger1, M. Clerici1, �D. Faccio1, and A. DiFalco2; 1School of Engineering and PhysicalSciences, SUPA, Heriot-Watt University, Ed-inburgh, United Kingdom; 2School of Physicsand Astronomy, University of St. Andrews,Edinburgh, United KingdomMetamaterials composed of Silver-Glass lay-ers exhibit epsilon-near-zero behaviour witha huge Kerr optical nonlinearity, n2 ∼ 10−10
EB-5.4 WED 15:00Experimental Superposition of Orders ofQuantum GatesL. Procopio1, A. Moqanaki1, M. Araújo1,2,F. Costa1,2, I. Calafell1, E. Dowd1, D.Hamel1, �L. Rozema1, C. Brukner1,2, andP. Walther1; 1University of Vienna, Vienna,Austria; 2Institute for Quantum Optics andQuantum Information, Vienna, AustriaWe create a superposition of two quantumgates acting on the polarization of a singlephoton in both orders. �is allows us to ac-complish task which is impossible on a stan-
CJ-9.5 WED 15:00Discretely tunable pulsed �ber laser basedon tailored FBG arraysT. Tiess1, C. Chojetzki2, M. Rothhardt1, H.Bartelt1,3, and �M. Jäger1; 1Leibniz Instituteof Photonic Technology (IPHT), Jena, Ger-many; 2FBGS Technologies GmbH, Jena, Ger-many; 3Abbe Center of Photonics, FriedrichSchiller University Jena, Jena, GermanyWe present a discrete tuning concept forpulsed �ber laser using a �ber Bragg grat-ing (FBG) array as spectral�lter, which com-bines a �ber-integrated structure with excel-
CF-4.4 WED 15:00High-Power, Femtosecond Cr:LiCAFLasers Pumped by Multimode Diodes�U. Demirbas1, I. Baali1, D.A.E. Acar1,and A. Leitenstorfer2; 1Antalya InternationalUniversity, Antalya, Turkey; 2Department ofPhysics and Center for Applied Photonics atthe University of Konstanz, Konstanz, Ger-manyWe report a saturable Bragg re�ector mode-locked, multi-mode diode-pumped fem-tosecond Cr:LiCAF laser, producing 105-fslong pulses around 810 nm with 750 mW
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCE-12.3 WED 14:30CH3NH3PbI3 Perovskite Light EmittingField-E�ect Transistor�X.Y. Chin1, D. Cortecchia2,3, J. Yin1,4, A.Bruno1,3, and C. Soci1,4; 1Division of Physicsand Applied Physics, Nanyang Technologi-cal Univ., Singapore; 2Interdisciplinary Grad-uate School, Nanyang Technological Univ.,Singapore; 3Energy Research Inst. @ NTU(ERI@N), Nanyang Technological Univ., Sin-gapore; 4Centre for Disruptive Photonic Tech-nologies, Nanyang Technological Univ., Sin-gaporeWe demonstrate a CH3NH3PbI3 light-emitting �eld-e�ect transistor (LE-FET),a new concept in the �eld of solution-processable perovskite optoelectronicdevices. �is proves the potential ofperovskite materials for high-brightnessgate-assisted LEDs and electrical-injectionlasers.
CB-6.2 WED 14:30Quantum limited frequency noise of aquantum cascade laser frequency comb�F. Cappelli1,2, G. Villares1, S. Riedi1, A.Hugi1, and J. Faist1; 1Institute for QuantumElectronics, ETH Zurich, Zürich, Switzer-land; 2CNR-INO - Istituto Nazionale di Ot-tica and LENS - European Laboratory forNon-Linear Spectroscopy, Sesto Fiorentino,Italy�e measurement of the frequency noise ofa quantum cascade laser frequency combdown to the quantum limit is presented. �enoise spectrum is equivalent to the one ob-served in singlemode devices.
CH-8.3 WED 14:30Dual-Comb Modelocked Lasers�S.M. Link, A. Klenner, M. Mangold, M.Golling, B.W. Tilma, and U. Keller; ETHZürich, Zürich, SwitzerlandWepresent the �rst semiconductor disk lasersimultaneously emitting two gigahertzmod-elocked pulse trains. A simple link from theoptical domain to a microwave frequencycomb is established. �e relative carrier-envelope-o�set frequency is accessed di-rectly.
CG-5.2 WED 14:30Attosecond Two-photon TransitionsContaining Autoionizing States�A. Jiménez-Galán1, L. Argenti1, andF. Martín1,2; 1Universidad Autónoma deMadrid, Madrid, Spain; 2InstitutoMadrileñode Estudios Avanzados en Nanociencia,Madrid, SpainWe study attosecond-resolved two-photontransitions involving autoionizing statesby means of a time-dependent analyticalmodel.
�e e�ects of the autoionizing states arere�ected on the atomic phases and can bemeasured with current experimental resolu-tion.
CE-12.4 WED 14:45Second-harmonic generation fromthermally-evaporated indium selenidethin �lms�A. Slablab1, S. Divya2, K. Koskinen1,R. Czaplicki1, M. Kailasnath2, P.Radhakrishnan2, and M. Kauranen1;1Tampere University of Technology, Depart-ment of Physics, P.O.Box 692, FI-33101,Tampere, Finland; 2International School ofPhotonics, Cochin University of Science andTechnology, 682022, Kochi, IndiaWe investigated second-harmonic genera-tion from thin �lms of InSe chalcogenideprepared using thermal-evaporation tech-nique. Unexpectedly appreciable SHG signalwas observed. Our results suggest that ChG�lm is a promising nonlinear optical mate-rial for photonic applications.
CB-6.3 WED 14:45Advances Toward Quantum CascadeLaser Array Monolithically Multiplexedon Indium Phosphide for Mid-InfraredSpectroscopy�C. Gilles1, G. Maisons1, B. Simozrag1,L.J. Orbe2, G. Carpintero Del Bario2, andM. Carras1; 1III-V Lab, Palaiseau, France;2Universidad Carlos III de Madrid, Leganés,SpainIn this contribution, we present last devel-opments on monolithic widely tuneable ar-ray of distributed feedback quantum cascadelasers on indium phosphide wafers. We re-port complete characterization and analysisof adiabatic couplers and passive multiplex-ers.
CH-8.4 WED 14:45Measuring ultra-high power femtosecondlasers in space-time.�G. Pariente, V. Gallet, O. Gobert, and F.Quéré; CEA Saclay, Gif-sur-Yvette, France�e quest for ever more powerful femtosec-ond lasers leads to growing challenges inmetrology and optimization. In this presen-tation we will describe the �rst 3D spatial-temporal characterization of a femtosecondhigh power laser beam.
CG-5.3 WED 14:45Time-resolved Study of Helium ExcitedStates with Attosecond Quantum-BeatSpectroscopy�M. Lucchini1, T. Zimmermann1, A.Ludwig1, L. Kasmi1, J. Herrmann1, A.Landsman2, L. Gallmann1,3, and U. Keller1;1ETH Zurich, Zurich, Switzerland; 2MaxPlanck Institute for the Physics of ComplexSystems, Dresden, Germany; 3University ofBern, Bern, SwitzerlandWe study ionization of highly excited statesof helium with attosecond quantum-beatspectroscopy. Comparison of experimentaldata with numerical simulation reveals thespectral content and time evolution of theelectron wave-packet with sub-femtosecondresolution.
CK-12.2 WED 15:00Compact Rare-Earth-Doped MicroringLasers Monolithically Integrated onSilicon Chips�P. Purnawirman1, Z. Su1, J.D.B. Bradley1,E.S. Hosseini1, A. Baldycheva1, T.N. Adam2,G. Leake2, D. Coolbaugh2, M.R. Watts1, G.Singh1, and E.S. Magden1; 1Research Lab-oratory of Electronics, Massachusetts Insti-tute of Technology, Cambridge, United States;2College of Nanoscale Science and Engineer-ing, University at Albany, Albany, UnitedStates
CE-12.5 WED 15:00Novel Method of Sub-Wavelength�inFilm Growth for Single Photon Emissionfrom Dye Molecules�C. Polisseni, K.W. Kho, S. Grandi, K. Ma-jor, Y.-H. Lien, J. Hwang, A. Clark, andE. Hinds; Imperial College London, London,United KingdomWe have developed a method of growing or-ganic crystals to host stable, single-photonemitting molecules. �is o�ers single crys-talline sub-wavelength thin �lms with excel-lent homogeneity over large areas, making
CB-6.4 WED 15:00THz Quantum Cascade Lasers based on aHyperuniform Disordered Optical CavityDesign�R. Degl’Innocenti1, Y. Shah1, L. Masini2, A.Ronzani2, A. Pitanti2, Y. Ren1, D. Jessop1,A. Tredicucci3, H. Beere1, and D. Ritchie1;1Cavendish Laboratory, University of Cam-bridge, Cambridge, United Kingdom; 2NEST,CNR and Scuola Normale Superiore, Pisa,Italy; 3Dipartimento di Fisica E. Fermi, Uni-versita’ di Pisa, Pisa, ItalyWe realized a novel optical cavity design ter-
CH-8.5 WED 15:00Noise statistics in multi-heterodynespectrometers based on interband- andquantum cascade lasers�A. Hangauer1,3, J. Westberg1, M. Soskind1,2,E. Zhang1, and G. Wysocki1; 1Princeton Uni-versity, Princeton, United States; 2Rutgers,�e State University of New Jersey, NewBrunswick, United States; 3now at: SiemensAG, Corporate Technology, Munich, Ger-many�e noise statistics of two multi-heterodynespectrometers based on multi-mode semi-
CG-5.4 WED 15:00High Harmonics Spectroscopy inmolecules: reconstructing emission timefor Below�reshold Harmonics andelectron localization�F. Morales1, P. Rivière2, M. Richter1,L. Medisauskas1,3, A. Gubaydullin2, M.Ivanov1,3, F. Martin2, and O. Smirnova1;1Max-Born-Institut, Berlin, Germany;2Dpto. de Química, Universidad Autónomade Madrid, Madrid, Spain; 3Department ofPhysics, Imperial College London, London,United Kingdom
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cm2/W.�e measurements are in agreementwith theoretical predictions and pave theway to extreme, non-perturbative nonlinearoptics.
dard quantum computer. lent �exibility to implement tailored spectraltuning ranges.
of average and 65 kW of peak power at 96.4MHz repetition rate.
CN-1.5 WED 15:15Optical characterization of a single modemid infrared microstructured optical�ber up to 10 microns: Potential forsupercontinuum generation andapplications for QCLs based sensors�L. Brilland1, L. Provino1, S. Venck1, D.Méchin1, C. Caillaud2, S. Ferre3, C. Gilles3,L. Jumpertz3,4, M. Carras3, and J. Troles2;1Perfos, R&D platform of Photonics Bre-tagne, Lannion, France; 2Glasses and Ceram-ics Group, Institut des Sciences Chimiquesde Rennes, université de Rennes 1, Rennes,France; 3Alcatel�ales 3-5Lab, campus Poly-technique, Palaiseau, France; 4Telecom ParisTech, Ecole Nationale des Télécommunica-tions, CNRS LTCI, Paris, FranceWe present for the �rst time the attenuationof a chalcogenide AsSe microstructured op-tical �ber from 3 to 10 microns. �is �bercould �nd applications for the supercontin-uum generation and for sensors based onQCLs.
EH-3.5 WED 15:15Nano-opto-mechanical NonlinearDielectric Metamaterials�A. Karvounis1, W. Wu1, K.F. MacDonald1,and N.I. Zheludev1,2; 1University ofSouthampton, Southampton, United King-dom; 2Nanyang Technological University,Singapore, SingaporeWe introduce and experimentally demon-strate free-standing all-dielectric metama-terials providing resonant optical proper-ties at near-infrared wavelengths, which of-fer a path towards strong and fast opticalnonlinearities underpinned by nano-opto-mechanical forces.
EB-5.5 WED 15:15Towards Quantum Cloud Computing�X. Qiang, X.-Q. Zhou, K. Aungskunsiri, andJ. O’Brien; Centre for Quantum Photonics,University of Bristol, Bristol, United KingdomWe proposed a novel scheme for remoteconstruction of quantum gates using con�g-urable resources, which moves a major steptowards quantum cloud computing. And wedemonstrated it experimentally using pho-tonics system.
CJ-9.6 WED 15:15Nanosecond to Picosecond Fiber BraggGrating Compression of Giant-ChirpedPulses from an Ultra-Long Mode-LockedFiber Laser�R.I. Woodward1, E.J.R. Kelleher1, T.H.Runcorn1, S. Loranger2, D. Popa3, V.J.Wittwer3, A.C. Ferrari3, S.V. Popov1, R.Kashyap2,4, and J.R. Taylor1; 1FemtosecondOptics Group, Department of Physics, Impe-rial College London, London, United King-dom; 2Fabulas Laboratory, Department ofEngineering Physics, PolytechniqueMontréal,Montréal, Canada; 3Cambridge GrapheneCentre, University of Cambridge, Cambridge,United Kingdom; 4Fabulas Laboratory, De-partment of Electrical Engineering, Polytech-nique Montréal, Montréal, CanadaWe demonstrate compression of nanosec-ond giant-chirped pulses from an ultra-longall-normal dispersion mode-locked �berlaser by a factor of 100, o�ering a sim-ple route to short-pulse high-peak-powersources at low repetition rates by cavity elon-gation.
CF-4.5 WED 15:15Tm-doped All-�bre Soliton Laser with 3.1nJ Pulse Energy Using an EvanescentlyInteracted Mono-layer GrapheneSaturable Absorber�H. Jeong1,2, S.Y. Choi1, M.H. Kim1, F.Rotermund1, S.B. Lee2, K. Lee2, and D.-I.Yeom1; 1Department of Physics & Depart-ment of Energy Systems Research, Ajou Uni-versity, Suwon, Korea, South; 2Nono photon-ics research center, Korea Institute of ScienceTechnology, Seoul, Korea, SouthTm-doped all-�bre soliton laser is demon-strated using a mono-layer graphene sat-urable absorber with strong evanescent �eldinteraction, which stably generates the opti-cal pulse with 61 mW output power and 3.1nJ pulse energy
16:00 – 17:30CN-2: Optical Sensing for Defenceand SecurityChair: Hans Dieter �oll, Diehl BGT De-fense, Überlingen, Germany
16:00 – 17:30EH-4: Active Plasmonics andMetamaterialsChair: Yuri Kivshar, Australian NationalUniversity, Canberra, Australia
16:00 – 17:30CL-1: Low-cost LabelfreeDiagnostic DevicesChair: Sylvie Roke, EPFL, Lausanne, Switzer-land
16:00 – 17:30CJ-10: Mode Instabilities in HighPower Fibre Laser SystemsChair: Clemens Hönninger, Amplitude Sys-tems, Pessac, France
16:00 – 17:30CF-5: Ultrashort PulseMeasurement and FELsChair: LukasGallmann, ETHZurich, Zurich,Switzerland
CN-2.1 WED (Invited) 16:00Active Stand-O�Detection in theMid-Infrared Using BroadbandFemtosecond Optical ParametricOscillatorsZ. Zhang1, L. Maidment1, S. Lee3, R.Clewes2, C. Howle2, and �D. Reid1; 1Heriot-Watt University, Edinburgh, United King-dom; 2Defence Science and Technology Lab-oratory, Salisbury, United Kingdom; 3�alesOptronics, Glasgow, United Kingdom
EH-4.1 WED 16:00Ultrafast Self-Action in an Air/GoldPlasmonic Waveguide�A. Baron1,2, T.B. Hoang1,3, C. Fang1,2, M.H.Mikkelsen1,2,3, and D.R. Smith1,2,3; 1Centerfor Metamaterials and Integrated Plasmon-ics, Duke University, Durham, United States;2Department of Electrical and Computer En-gineering, Duke University, Durham, UnitedStates; 3Department of Physics, Duke Univer-sity, Durham, United States
CL-1.1 WED (Keynote) 16:00Lens-free On-chip Microscopy forBiomedical Imaging, Sensing andDiagnostics�A. Ozcan; UCLA, Los Angeles, United StatesWe review the recent progress on lens-freecomputationalmicroscopy tools for biomed-ical imaging, sensing and diagnostics appli-cations.
CJ-10.1 WED 16:00Mode Instabilities and the In�uence ofPhotodarkening in High-Power FiberLasers�H.-J. Otto1, N. Modsching1, C. Jauregui1,J. Limpert1,2, and A. Tünnermann1,2,3;1Institute of Applied Physics, Abbe Centerof Photonics, Friedrich-Schiller-UniversitätJena, Jena, Germany; 2Helmholtz-InstituteJena, Jena, Germany; 3Fraunhofer Institutefor Applied Optics and Precision Engineering,
CF-5.1 WED 16:00Regularization Approaches for PhaseRetrieval in Self-Di�raction SPIDER�S. Birkholz1, G. Steinmeyer1, S. Koke1,D. Gerth2, S. Buerger3, and B. Hofmann3;1Max-Born-Institut für Nichtlineare Optikund Kurzzeitspektroskopie, Berlin, Germany;2Johannes-Kepler-Universität, Doctoral Pro-gram Computational Mathematics, Linz,Austria; 3TU Chemnitz, Fakultät für Math-ematik, Chemnitz, Germany
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We report a compact monolithic rare-earth-doped microring lasers on silicon. Lasingwavelength at 1.0 and 1.5 *m are shown re-spectivelywith 980 nmpumping. We furtherdiscuss pulley-coupling design for 1480 nmpumping.
them compatible with integrated photonicdevices.
ahertz quantum cascade laser. �is is basedon an isotropic, disordered and hyperuni-form distribution of scatterers, which ex-hibits a photonic band gap.
conductor lasers (QCLs and ICLs) are in-vestigated to determine their detection per-formance limitations. Both follow the theo-retical Rice distribution and are suitable forspectroscopic measurements.
Using H+2 , we show how Coulomb explo-
sion, upon ionization, can be used to recon-struct the emission times of near and below-threshold-harmonics. We also show howelectron localization can be imprinted in theeven harmonics signal.
CK-12.3 WED 15:15�reshold estimate for dye-dopedpolymer micro-lasers�I. Gozhyk1,2, H. Rabbani3, S. Forget3,S. Chenais3, C. Ulysse3, J. Zyss1, andM. Lebental1; 1ENS de Cachan / CNRS,Cachan, France; 2CNRS, Marcoussis, France;3Université Paris 13 / CNRS, Villetaneuse,France�e relation between gain of a dye-dopedpolymer layer, mode losses and lasingthresholds are established on the exampleof planar Fabry-Perot micro-laser. Strongin�uence of pump beam polarization onthreshold is demonstrated and explained.
CE-12.6 WED 15:15Optomechanical Characterization ofSub-micron�ick Optical MaterialsE.A.A. Pogna1, G. Cerullo1, C. Ferrante2, and�T. Scopigno2; 1Physics Department - Politec-nico di Milano, Milano, Italy; 2Dipartimentodi Fisica, Roma, ItalyA novel approach to time resolved picosec-ond ultrasonics is presented as powerfultool to simultaneously determine the elasticmodulus and the refractive index dispersionin the visible range of ultrathin transparentmaterials.
CB-6.5 WED 15:15High power, widely tunable, mode-hopfree, continuous wave external cavityquantum cascade laser for multi-speciestrace gas detection�R. Centeno1, D. Marchenko1, J. Mandon1, S.Cristescu1, G. Wulterkens2, and F. Harren1;1Radboud University, Nijmegen, �e Nether-lands; 2TechnoCentrum, Radboud Univer-sity, Nijmegen,�e NetherlandsWe present an external cavity quantum cas-cade laser with a tunability of 303 cm-1 at 8um, an output power of 200mWand aNEAS= 3.7 x 10-8 cm-1Hz-1/2 with o�-axis ICOS.
CH-8.6 WED 15:15Silicon Nitride Chip-Based CoherentSupercontinuum for Highly E�cientSelf-Referencing of a 1-GHzDiode-Pumped Solid-State Laser�A.S. Mayer1, A. Klenner1, A.R. Johnson2,K. Luke3, M.R.E. Lamont2,3,4, Y. Okawachi2,M. Lipson3,4, A.L. Gaeta2,4, and U. Keller1;1Department of Physics, Institute of Quan-tum Electronics, ETH Zurich, Zurich,Switzerland; 2School of Applied and Engi-neering Physics, Cornell University, Ithaca,United States; 3School of Electrical andComputer Engineering, Cornell University,Ithaca, United States; 4Kavli Institute atCornell for Nanoscale Science, CornellUniversity, Ithaca, United StatesWe present the �rst carrier-envelope-o�set(CEO) frequency detection based on multi-octave-spanning supercontinuum genera-tion in a CMOS-compatible Si3N4 waveg-uide. Strong CEO-beat-signals (>30 dB) ofa gigahertz-Yb:CALGO-laser are obtainedwith only 36 pJ of coupled pulse energy.
CG-5.5 WED 15:15Origins of Very Low Energy Electrons inMid-IR Strong-Field Ionization�B. Wolter1, C. Lemell2, M. Baudisch1,M.G. Pullen1, X.-M. Tong3, M. Hemmer1,A. Sen�leben4, C.D. Schröter5, J. Ullrich5,6,R. Moshammer5, J. Burgdörfer2,7, and J.Biegert1,7,8; 1ICFO - Institut de CiènciesFotòniques, Castelldefels (Barcelona), Spain;2Institute for �eoretical Physics, ViennaUniversity of Technology, Vienna, Austria;3Center for Computational Sciences, Univer-sity of Tsukuba, Ibaraki, Japan; 4Institute ofPhysics, Center for Interdisciplinary Nanos-tructure Science and Technology (CINSaT),University of Kassel, Kassel, Germany; 5Max-Planck-Institut für Kernphysik, Heidelberg,Germany; 6Physikalisch-Technische Bunde-sanstalt, Braunschweig, Germany; 7Kavli In-stitute for �eoretical Physics, University ofCalifornia, Santa Barbara, CA, United States;8ICREA - Institució Catalana de Recerca i Es-tudis Avançats, Barcelona, SpainWe present a joint experimental and theo-retical investigation of atomic ionization byintense, ultrafast, mid-IR �elds which al-lows for a quantitative interpretation of therecently found low energy structures (LES,VLES and ZES).
16:00 – 17:30CK-13: Fundamental Interactionand Novel DevicesChair: Tapio Niemi, Tampere University ofTechnology, Tampere, Finland
16:00 – 17:30EA-8: Semiconductor QuantumLight SourcesChair: Christoph Becher, Universität desSaarlandes, Saarbrücken, Germany
16:00 – 17:30CB-7: Semiconductor LaserDynamicsChair: Guido Giuliani, University of Pavia,Pavia, Italy
16:00 – 17:30CH-9: Advanced MeasurementMethods and DevicesChair: Walter Lubeigt, M Squared LasersLtd., Glasgow, United Kingdom
16:00 – 17:30CG-6: Sub-fs Dynamics inMoleculesChair: Franck Lépine, Institut LumièreMatière, CNRS, Lyon, France
CK-13.1 WED 16:00Probing Topological Invariants in theBulk of Non-Hermitian Photonic Lattices�J.M. Zeuner1, M.C. Rechtsman2, Y. Plotnik2,Y. Lumer2, M.S. Rudner3, M. Segev2, andA. Szameit1; 1Insitute of Applied Physics,Friedrich-Schiller-Universität Jena, Jena,Germany; 2Department of Physics, Technion,Haifa, Israel; 3�e Niels Bohr InternationalAcademy, Niels Bohr Institute, Copenhagen,Denmark
EA-8.1 WED (Invited) 16:00Quantum Nanophotonics�J. Vuckovic; Ginzton Laboratory, StanfordUniversity, Stanford, CA, United StatesSemiconductor devices containing quantumdots or optically active impurities are used asa platform for fundamental studies of quan-tum optics and cavity QED, and for develop-ment of quantum technologies.
CB-7.1 WED 16:00Full scan phase reconstruction of sweptsource laserS. Slepneva1,2, B. O’Shaughnessy1,2, B.Kelleher1,2, S.P. Hegarty1,2, G. Huyet1,2,5, T.Butler1,2, A. Vladimirov3, M. Wojtkowski4,and �D. Goulding1,2; 1CAPPA, Cork Instituteof Technology, Cork, Republic of Ireland;2Tyndall National Institute, Cork, Republicof Ireland; 3Weierstrass Institute, Berlin,Germany; 4Institute of Physics, Torun,
CH-9.1 WED 16:00Broadband Cavity Enhancement withGraphene ModulatorK.F. Lee1, G. Kowzan1,2, C.-C. Lee3,C. Mohr1, J. Jiang1, T.R. Schibli3,4,5, P.Masłowski2, and �M.E. Fermann1; 1IMRAAmerica, Inc., Ann Arbor, United States;2Institute of Physics, Faculty of Physics,Astronomy and Informatics, NicolausCopernicus University, Torun, Poland;3Department of Physics, University of
CG-6.1 WED 16:00A Table Top Ultrashort Light Source inthe XUV for Time ResolvedMeasurements of Circular Dichroisms�R. Géneaux1, A. Ferré2, C. Handschin2,M. Dumergue2, F. Burgy2, A. Comby2, D.Descamps2, B. Fabre2, G.A. Garcia3, L.Merceron2, E. Mével2, L. Nahon3, S. Petit2,B. Pons2, D. Staedter4, S.Weber1, T. Ruchon1,V. Blanchet2, and Y. Mairesse2; 1CEA Saclay- LIDyL, Gif sur Yvette, France; 2CELIA
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�e application of a broadband femtosec-ond optical parametric oscillator to mid-infrared stand-o� detection of vapours andliquids is described, including thiodiglycol,nitromethane, water, D2O and polymers.Preliminary results achieving active hyper-spectral imaging are also presented.
We investigate theoretically and experimen-tally the nonlinear propagation of surfaceplasmons on an air/gold interface which re-veals large and ultrafast (100 fs) self-inducedabsorption. �e experiment enables a di-rect measurement of the third-order nonlin-ear susceptibility.
Jena, Germany�e latest results on investigating mode in-stabilities are presented. Its shown, that pho-todarkening is a major contributor of heateven in optimized �bers. �is opens a newpath to dramatically increase the mode in-stabilities threshold.
We present a novel SPIDER variant, basedon the third-order nonlinearity called self-di�raction. While our method greatly en-hances the capabilities of SPIDER, it requiresan additional deconvolution step, which weaddress by a regularization approach.
EH-4.2 WED 16:15Ultrafast All-Optical Switching of SurfacePlasmon Polariton Modes via FanoResonances�C. McPolin1, N. Olivier1, J.-S. Bouillard1,2,D. O’Connor1,3, A. Krasavin1, W. Dickson1,G. Wurtz1, and A. Zayats1; 1King’s Col-lege London, London, United Kingdom;2University of Hull, Hull, United King-dom; 3National Physical Laboratory, London,United KingdomWe experimentally demonstrate ultrafast,all-optical switching of plasmonic signalsusing optical cavity resonances. �e ob-served modulation occurs on a picosecondtimescale, yielding a change in transmissionof over 50%.
CJ-10.2 WED 16:15Raising the mode instability threshold inhigh-power �ber laser systems�C. Jauregui1, H.-J. Otto1, J. Limpert1,2, andA. Tünnermann1,2,3; 1Friedrich-Schiller Uni-versität, Jena, Germany; 2Helmholtz-IntituteJena, Jena, Germany; 3Fraunhofer Institutefor Applied Optics and Precision Engineering,Jena, GermanyBased on the recently revealed strong con-nection betweenmode instabilities and pho-todarkening, we provide new insights on thephysics of themode instability threshold andgive guidelines to signi�cantly increase it inthe near future.
CF-5.2 WED 16:15SEA-SPIDER apparatus for sub-cyclepulse characterization in the mid-IR�G. Fan1, T. Balciunas1, S. Hässler1, C.Fourcade-Dutin2, T. Witting3, A. Voronin4,A. Zheltikov4,5, F. Gerome2, A. Baltuska1,and F. Benabid2; 1Photonics Institute ViennaUniversity of Technology, Vienna, Austria;2GPPMM group, Xlim Research Institute,Limoges, France; 3Blackett Laboratory, Impe-rial College London, London, United King-dom; 4Physics Department, InternationalLaser Center, M.V. Lomonosov Moscow StateUniversity, Moscow, Russia; 5Department ofPhysics and Astronomy, Texas A & M Uni-versity, College Station, United StatesWe present a practical SEA-SPIDER imple-mentation for sub-cycle pulse characteriza-tion in the mid-IR spectral range which al-lows measurement of undistorted sub-cycleself-compressed pulses in Kagome �bre withspectrum spanning 1.1-2.6 �m range.
CN-2.2 WED 16:30Detection of Explosives and theirPrecursors using Imaging Mid-InfraredLaser Backscattering Spectroscopy�F. Fuchs, S. Hugger, J. Jarvis, Q. Yang, R. Os-tendorf, C. Schilling, R. Driad, R. Aidam, A.Bächle, W. Bronner, and J. Wagner; Fraun-hofer Institute for Applied Solid State Physics,Freiburg, Germany�e use of imaging mid-infrared laserbackscattering spectroscopy for the detec-tion of explosives and their precursors in arealistic outdoor scenario is reported. EC-QCLs providing a wide spectral coveragewere used for wavelength selective illumina-tion.
EH-4.3 WED 16:30Controlling Surface Plasmon Propagationusing Phase Change Materials�M. Rudé1, R.E. Simpson2, R. Quidant1,3, V.Pruneri1,3, and J. Renger4; 1ICFO - Institutde Ciències Fotòniques, Castelldefels, Spain;2SUTD - Singapore University of Technologyand Design, Singapore, Singapore; 3ICREA- Institució Catalana de Recerca i EstudisAvançats, Barcelona, Spain; 4ETH - Eid-genössische Technische Hochschule, Zürich,SpainWe demonstrate modulation of SPPs prop-agating along a Au waveguide. �is mod-ulation is induced by a laser driven transi-tion between the amorphous and crystalline
CJ-10.3 WED 16:30Investigations in Mode Instabilities inlow-NA Reduced Mode Overlap PhotonicCrystal Fibers�N. Haarlammert1, B. Sattler1, A. Liem1,M. Strecker1, J. Nold1, T. Schreiber1,R. Eberhardt1, A. Tünnermann1,2, K.Ludewigt3, and M. Jung3; 1FraunhoferInstitute for Applied Optics and PrecisionEngineering, Jena, Germany; 2Friedrich-Schiller-Universtitaet, Jena, Germany;3Rheinmetall Wa�e Munition GmbH,Unterluess, GermanyWe report on Investigations of mode in-stabilities in low-NA reduced mode over-lap photonic crystal �bers. �e MI limited
CF-5.3 WED 16:30Ultrashort pulse characterisation with thed-scan technique: a single-shotimplementation in the few- to single-cycleregime�D. Fabris1, W. Holgado2, F. Silva3, T.Witting1, J. Tisch1, and H. Crespo3; 1BlackettLaboratory, Imperial College, London, UnitedKingdom; 2Grupo de Investigación en ÓpticaExtrema (GIOE), Universidad de Salamanca,Salamanca, Spain; 3IFIMUP-IN and Depar-tamento de Física e Astronomia, Faculdadede Ciências, Universidade do Porto, Porto,PortugalWe demonstrate a novel single shot d-scandiagnostic based on a stationary glass prism
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We utilize non-hermiticity to experimen-tally demonstrate a topological transition inphotonic lattices. In contrast to standardmethods for examining topological proper-ties, which employ surface physics, we em-ploy bulk dynamics only.
Poland; 5National Research University ofInformation Technologies, Mechanics andOptics, St Petersburg, RussiaA swept source laser phase has been charac-terised using a self-referencing heterodynetechnique over a range > 10 THz reveal-ing mode-locking and chaotic laser dynam-ics across the sweep range.
Colorado at Boulder, Boulder, United States;4Department of Electrical, Computer andEnergy Engineering, University of Coloradoat Boulder, Boulder, United States; 5JILA,National Institute of Standards and Tech-nology and University of Colorado, Boulder,Boulder, United StatesWe lock a frequency comb to a high �nesseoptical cavity with stable repetition rate ando�set frequency using a graphene modula-tor. We comb-resolve the 175 nmwide trans-mitted spectrum with a Fourier transformspectrometer.
Bordeaux, Talence, France; 3SynchrotronSOLEIL, Gif sur Yvette, France; 4LCAR-IRSAMC Toulouse, Toulouse, FranceWe present an XUV light source based onhigh-harmonic generation producing ultra-short and quasi-circular pulses. �is sourceis used to measure photoelectron circulardichroism on chiral molecules, opening theroute to table-top time-resolved chiropticalexperiments.
CK-13.2 WED 16:15Enhancement of the Total Optical EnergyDensity inside a Scattering Medium�O. Ojambati, H. Yilmaz, A. Lagendijk, A.Mosk, andW. Vos;MESA+ Institute for Nan-otechnology, University of Twente, Enschede,�e NetherlandsWe investigate the total energy density oflight inside a scattering medium when theincident wavefront is spatially shaped. Weobserve that the energy density is enhancedcompared to unshaped light, in agreementwith theory.
CB-7.2 WED 16:15Experimental phase-space tomography ofsemiconductor laser dynamics�D. Brunner, M. Soriano, X. Porte, and I. Fis-cher; Instituto de Física Interdisciplinar y Sis-temas Complejos (IFISC), Universitat de lesIlles Balears,, Palma de Mallorca, SpainNonlinear semiconductor laser dynamics istypically described by the optical �eld, phaseand carrier inversion. We report the simul-taneous measurement of all three variableswith high temporal resolution for delayed-feedback dynamics in the LFF regime.
CH-9.2 WED 16:15Development of a space Laser Source formanipulation of cesium cold atomsaboard PHARAO�B. Faure1, T. Leveque1, D. Massonnet1, P.Laurent2, C. Salomon3, T. Bomer4, and S.�omin4; 1CNES, Toulouse, France; 2LNE-SYRTE, Paris, France; 3Laboratoire Kastler-Brossel, Paris, France; 4SODERN, Limeil-Brévannes, FranceDevelopment of the Laser Source forPHARAO cold cesium clock is presented.PHARAO is the main instrument of theESA mission ACES, that will be mountedaboard the International Space Station forfundamental physics tests.
CG-6.2 WED 16:15Physical Origins of Strong ChiralSensitivity of High Harmonic GenerationR. Cireasa1, A.E. Boguslavskiy2,5,8, B. Pons1,M.C.H. Wong2, D. Descamps3, S. Petit3,H. Ruf3, N. �ire1,4, A. Ferre3, J. Suarez6,J. Higuet3, B.E. Schmidt4, A.F. Alharbi2,F. Legare4, V. Blanchet1,3, B. Fabre3, S.Patchkovskii5,7, �O. Smirnova7, Y. Mairesse3,and V.R. Bhardwaj2; 1LCAR, Universite deToulouse, Toulouse, France; 2University ofOttawa, Ottawa, Canada; 3CELIA, Univer-site de Bordeaux - CNRS - CEA, Talence,France; 4INRS-EMT, Advanced Laser LightSource, Varennes, Canada; 5NRC Canada,Ottawa, Canada; 6Departamento de Quim-ica, Universidad Autonoma de Madrid,Madrid, Spain; 7Max-Born Institut, Berlin,Germany; 8Department of Physics, Queen’sUniversity, Ontario, CanadaWe describe high harmonic emission froma random ensemble of chiral molecules inmid-infrared �elds. We demonstrate and ex-plain extreme chiral sensitivity of the har-monic response and use it to time-resolve at-tosecond chiral dynamics.
CK-13.3 WED 16:30Light-induced conductive skin in siliconphotonic waveguidesS. Grillanda1, A. Melloni1, M. Sorel2, and�F. Morichetti1; 1Politecnico di Milano, Mi-lan, Italy; 2University of Glasgow, Glasgow,United KingdomWe show that at typical light intensity of lin-ear applications surface states induce mas-sive free carrier generation at the surface ofsilicon photonic waveguides, that becomesmore conductive than the bulk and inducesoptical absorption.
EA-8.2 WED 16:30Polarization Entangled Photons fromQuantum Dots Embedded in Nanowires�A. Predojevic1, T. Huber1, M. Khoshnegar2,D. Dalacu3, P.J. Poole3, H. Majedi2, and G.Weihs1; 1Institute for Experimental Physics,University of Innsbruck, Innsbruck, Aus-tria; 2Institute for Quantum Computingand Waterloo Institute for Nanotechnology,University of Waterloo, Waterloo, Canada;3National Research Council of Canada, Ot-tawa, CanadaWe present measurements on generation ofpolarization entangled photon pairs from asystem consisting of a quantum dot embed-ded in a nanowire.
CB-7.3 WED 16:30Long-Term Frequency Stability and NoiseEvolution of a Free-Running DistributedFeedback Quantum Cascade Laser�S. Schilt1, L. Tombez1, C. Tardy2, A.Bismuto2, S. Blaser2, R. Maulini2, R.Terazzi2, M. Rochat2, and T. Südmeyer1;1Laboratoire Temps-Fréquence, Neuchatel,Switzerland; 2Alpes Lasers SA, Neuchatel,SwitzerlandFrequency stability and noise variability ofa quantum-cascade-laser continuously mea-sured during two months showed a similarbehavior characterized by a dri� during the�rst month attributed to the laser contacts,followed by a stable regime.
CH-9.3 WED 16:30Adaptive, Hyperspectral Imager: Design,Modeling, and ControlS. McGregor, �A. Monmayrant, and S.Lacroix; LAAS-CNRS, Toulouse, FranceAn adaptive, hyperspectral imager is exper-imentally demonstrated, o�ering adaptablespectral and temporal resolutions, and highspatial resolution. It provides numerous ac-quisition schemes, including near snapshotacquisitions of the spectral content of severalregions of interest.
CG-6.3 WED 16:30Charge migration in Phenylalanineinitiated by attosecond pulses�A. Trabattoni1, D. Ayuso2, L. Belshaw3, S.De Camillis3, S. Anumula1, F. Frassetto4,L. Poletto4, A. Palacios2, P. Decleva5, J.B.Greenwood3, F. Martin2,6, F. Calegari7, andM. Nisoli1,7; 1Dep. of Physics, Politecnico diMilano, Milano, Italy; 2Dep. de Química,Modulo 13, Univ. Autónoma de Madrid,Madrid, Spain; 3Centre for Plasma Physics,School of Maths and Physics, Queen’s Univ.,Belfast, United Kingdom; 4IFN-CNR Padova,Padova, Italy; 5Dip. di Scienze Chimiche eFarmaceutiche, Univ. di Trieste and CNR-Istituto O�cina dei Materiali, Trieste, Italy;
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b
phases of Ge2Sb2Te5, which dramaticallyincreases its optical constants.
RMO �ber ampli�er output power of several�bers decreases with higher V-parameterand lower bending diameter.
and imaging spectrometer. Measurementsperformed with sub-3.5-fs pulses demon-strate the validity of this new implementa-tion down to the single-cycle regime.
CN-2.3 WED 16:45Scanning of radioluminescence emissionwith a PMT for remote detection of alphacontamination�J. Sand1, S. Ihantola1, A. Nicholl2, E.Hrnecek2, J. Toivonen3, H. Toivonen1, andK. Peräjärvi1; 1STUK - Radiation and Nu-clear Safety Authority, Helsinki, Finland;2European Commission, Joint Research Cen-tre, Institute for Transuranium Elements,Karlsruhe, Germany; 3Tampere University ofTechnology, Tampere, FinlandAn automated scanning system was devel-oped for the detection of radioluminescencelight induced by alpha particles in air. �e�rst results and detection capability underfull �uorescent lighting are presented.
EH-4.4 WED 16:45Bulk plasmon-polaritons in hyperbolicnanorod metamaterial waveguides�N. Vasilantonakis, M. Nasir, W. Dickson,G.A. Wurtz, and A.V. Zayats; Departmentof Physics, King’s College London, London,United KingdomWe show that light propagates in hyper-bolic metamaterial waveguide in the form ofbulk plasmon-polaritons. �e extraordinaryguided modes of the metamaterial slab havelow or negative group velocity with high ef-fective refractive indices.
CL-1.2 WED 16:45Label-free detection and quanti�cation ofEscherichia coli using an image cytometerbased on angular spatial frequencyprocessing�J.M. Perez1, M. Jofre1, P. Martinez1, andV. Pruneri1,2; 1�e Institute of PhotonicSciences, Castelldefels, Spain; 2InstitucioCatalana de Recerca i Estudis Avançats,Barcelona, SpainA newly designed image cytometer based onspatial Fourier analysis is proposed. It iscompact, low cost and can detect in a la-bel free format micro-organisms such as Es-cherichia coli in very low concentrations.
CJ-10.4 WED 16:45Mode-Instability Behavior in Yb3+-doped10-�m-core Fiber Ampli�ers�V. Tyrtyshnyy1, O. Vershinin1,2, D.Alekseev1,2, M. Kuznetsov3,4, and O.Antipov3,4; 1NTO IRE-Polus, Fryazino,Russia; 2Moscow Institute of Physics andTechnology, Dolgoprudny, Russia; 3Instituteof Applied Physics of Russian Academy ofScience, Nizhny Novgorod, Russia; 4NizhniyNovgorod State University, Nizhny Novgorod,RussiaMode instability with threshold of fewWattswas experimentally investigated in ampli-�ers based on Yb3+-doped �bers with 10 �mcore diameter. Numericalmodeling revealedpredominating role of population inversiongratings that account for mode instability.
CF-5.4 WED (Keynote) 16:45Ultrafast optics for X-ray free-electronlasers�F. Kärtner; Center for Free-Electron LaserScience, DESY and University of Hamburg,Hamburg, GermanyUltrafast optics in X-ray free-electron lasersis reviewed. Progress and needs in photo-injector, pump-probe and seed-lasers, tim-ing distribution, THz-pulse generation andits use for X-ray pulse characterization andpotentially driving attosecond free-electronlasers is discussed.
CN-2.4 WED 17:00Single-photon Sensitive Light-in-FlightImagingG. Gariepy1, N. Krstajic2, R. Henderson2, C.Li1, R.�omson1, G.S. Buller1, B. Heshmat3,R. Raskar3, J. Leach1, and �D. Faccio1;1Heriot-Watt University, Edinburgh, UnitedKingdom; 2University of Edinburgh, Edin-burgh, United Kingdom; 3MIT, Cambridge,United States�e �rst measurement of laser pulses prop-agating in air is performed using an ar-ray of single-photon avalanche diode detec-tors that can detect light scattered from airmolecules with picosecond timing resolu-tion.
EH-4.5 WED 17:00Tuneable Metamaterials Driven by Light�J.-Y. Ou1, E. Plum1, and N.I. Zheludev1,2;1University of Southampton, Southampton,United Kingdom; 2Nanyang TechnologicalUniversity, Singapore, SingaporeWe demonstrate optically driven mechani-cally recon�gurable metamaterials exhibit-ing optical nonlinearities 7 orders of magni-tude greater than GaAs in the telecom spec-tral range.
CL-1.3 WED 17:00Temperature E�ect on Cell Mechanics byOpto�uidic Microchips�T. Yang1, G. Nava1,2, F. Bragheri3,P. Paiè3,4, R. Martinez Vazquez3, P.Minzioni1, M. Veglione5, F. Lelii1, C.Mondello5, R. Osellame3,4, and I. Cristiani1;1Dipartimento di Ingegneria Industrialee dell’Informazione, Università di Pavia,Pavia, Italy; 2Department of Biomedical Sci-ence and Translational Medicine, Universitàdi Milano, Milano, Italy; 3Istituto di Fotonicae Nanotecnologie (IFN)-CNR, Milano, Italy;4Dipartimento di Fisica, Politecnico diMilano, Milano, Italy; 5Istituto di GeneticaMolecolare (IGM)-CNR, Pavia, ItalyWe analyze, using two di�erent opto-micro�uidic chips, the impact of tempera-ture on cellmechanical properties. Obtainedresults highlight a strong impact of tempera-ture on cell properties and allow comparingoptical-stretching and constriction-passingmeasurements.
CJ-10.5 WED 17:00Impact of axial pro�le of the gainmedium on the mode instability in lasers:regular versus tapered �bers�V. Filippov1, V. Ustimchik2, Y.Chamorovskii2, K. Golant2, A. Vorotynskii1,and O. Okhotnikov1; 1OptoelectronicsResearch Centre, Tampere University ofTechnology, Tampere, Finland; 2Instituteof Radio and Electronics of the RussianAcademy of Sciences, Moscow, Russia�e presented paper describes the new con-cept for suppression of mode instability inhigh power �ber lasers and ampli�ers basedon tapered (i.e. axially non-regular) double-clad few-mode gain architecture.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN6Inst. Madrileno de Estudios Avanzados enNanociencia, Madrid, Spain; 7Inst. of Pho-tonics and Nanotechnologies (IFN)-ConsiglioNazionale delle Ricerche (CNR),Milano, ItalyUltrafast charge dynamics initiated by at-tosecond pulses have been measured inphenylalanine. An oscillatory pattern inthe yield of a doubly-charged fragment wasmeasured with <4.3-fs period, represent-ing the �rst experimental demonstration ofcharge migration.
CK-13.4 WED 16:45Spatial soliton formation and guiding inazimuthally modulated Bessel-likenonlinear photonic latticesT. Dadalyan1, F. Diebel2, M. Boguslawski2,C. Denz2, and �R. Drampyan1; 1Institutefor Physical Research, National Academy ofSciences of Armenia, Ashtarak, Armenia;2University of Muenster, Muenster, Germany�e results of experimental study of con-trolled light propagation and soliton forma-tion in the optically induced 2d azimuthallymodulated Bessel-like 4-fold wave-guidingstructures in strontium bariumniobate crys-tal in self-focusing and defocusing regimesare presented.
EA-8.3 WED 16:45Single quantum dot laser-emission from amicropillar cavity in the strong couplingregime�F. Gericke1, C. Gies2, L. Messner1, S.Holzinger1, J. Wolters1, P. Gold3, C.Schneider3, S. Hö�ing3,4, F. Jahnke2, M.Kamp3, and S. Reitzenstein1; 1Institute ofSolid State Physics, Berlin University ofTechnology, Berlin, Germany; 2Institute for�eoretical Physics, University of Bremen,Bremen, Germany; 3Technische Physik, Uni-versity of Würzburg, Würzburg, Germany;4Present address: School of Physics andAstronomy, University of St. Andrews, St.Andrews, United KingdomWe show experimental studies of semicon-ductor micropillar cavities with embeddedsingle quantum dots in the strong couplingregime. With increasing excitation powerlasing oscillations start while the strong cou-pling remains.
CB-7.4 WED 16:45Phase Solitons in Semiconductor RingLaser with Coherent Forcing�F. Gustave1, L. Columbo2, F. Prati3, M.Brambilla2, B. Kelleher4, B. Tykalewicz4, G.Tissoni1, and S. Barland1; 1Université deNice-CNRS UMR7335 Institut Non Linéairede Nice, Valbonne, France; 2Dipartimento In-terateneo di Fisica, Università degli Studi ePolitecnico di Bari, Bari, Italy; 3Dipartimentodi Scienza e Alta Tecnologia, Universitàdell’Insubria, Via Valleggio 11, Como, Italy;4Centre for Advanced Photonics and ProcessAnalysis, Cork Institute of Technology, Cork,Republic of IrelandWe demonstrate the existence of phase soli-tons in a strongly multimode semiconduc-tor ring laser with coherent forcing. �ey aretemporal localized structures carrying a chi-ral charge, associated with a 2pi rotation ofthe optical phase.
CH-9.4 WED 16:45FPGA High Rate Pseudo-random SinglePhoton Counting Correlator�X. Ai, R. Nock, N. Dahnoun, and J. Rarity;University of Bristol, Bristol, United KingdomA FPGA-based correlator clocked at100MHz for Pseudo-random Single PhotonCounting LIDAR is presented. It performscorrelation of a random sequence withbipolar version of that sequence, hencezeroing the o�set of the correlation result.
CG-6.4 WED 16:45Direct Observation of AttosecondElectron Wavepacket in a NitrogenMolecule with a-Few-Pulse AttosecondPulse Train�T. Okino1, Y. Furukawa1, A.A. Eilanlou1, Y.Nabekawa1, S. Miyabe1, E.J. Takahashi1, K.Yamanouchi2, and K. Midorikawa1; 1RIKENCenter for Advanced Photonics, Saitama,Japan; 2Univ. of Tokyo, Tokyo, JapanAttosecond electron wavepacket in nitrogenmolecule is observed by intense a-few-pulseattosecond pulse train by recording the time-evolution of kinetic energy spectrumof frag-ment ion generated from two-photon disso-ciative ionization processes.
CK-13.5 WED 17:00Highly Sensitive Detection of CircularDichroism in 3D Pt-C Helices by Meansof a Photo-Acoustic Device�A. Benedetti1, G. Leahu1, R. LiVoti1, A. Belardini1, C. Sibilia1, M.Esposito2, V. Tasco2, and A. Passaseo2;1Sapienza:Università di Roma, DepartmentS.B.A.I., Roma, Italy; 2National Nanotech-nology Laboratory, CNR-Nano, Lecce,ItalyWe detect circular dichroism in an arrayof platinum-carbon helices by means of aphoto-acoustic detection system. Measure-ments of absorbed optical pulses con�rmnumerical calculations and all-optical mea-surements made on this sophisticated struc-tured device.
EA-8.4 WED 17:00Macroscopic Kerr Rotation from a BrightNegatively Charged Quantum Dot in aLow-QMicropillar CavityP. Androvitsaneas1, A. Young2, C. Schneider3,S. Hö�ing3,4, M. Kamp3, E. Harbord1, �J.Rarity2, and R. Oulton1,2; 1H. H. WillsPhysics Laboratory, University of Bristol,Bristol, United Kingdom; 2Merchant Ven-turers School of Engineering, University ofBristol, Bristol, United Kingdom; 3TechnischePhysik, Physikalisches Institut and WilhelmConrad Röntgen-Center for Complex Mate-rial Systems, UniversitätWürzburg, AmHub-land,Würzburg, Germany; 4School of Physicsand Astronomy, University of St Andrews, StAndrews, United KingdomWe report the measurement of macroscopicphase shi�s of several degrees for re�ectedincident light resonant with a bright nega-tively charged quantum dot in a micropillarstructure of Q-factor 150.
CB-7.5 WED 17:00Semiconductor Lasers with ContinuousTuning Bands Exceeding 100 nm in780-1000 nm Spectral Range�A. Chamorovskiy1, Y. Kostin2, M.Ladugin3, A. Lobintsov2, A. Marmalyuk3,M. Shramenko2, and S. Yakubovich4;1Superlum, Carrigtwohill, Republic ofIreland; 2Superlum Diodes Ltd, Moscow,Russia; 3OJSCM.F.Stelmakh Polyus ResearchInstitute, Moscow, Russia; 4Moscow StateTechnical University of Radioengineering,Electronics and Automation, Moscow, RussiaTunable lasers with �ber ring cavity withbroadband semiconductor optical ampli�ersare developed. Lasers possess tuning band-widths exceeding 100 nm in 780-1000 nmspectral range, 10000 nm/s mode-hop-freetuning and instantaneous linewidth below0.1 nm.
CH-9.5 WED 17:00Lithium Niobate Optical WaveguideSensing of RF Electromagnetic Pulses�A. Dzipalski1, A.J. Waddie1, I. �urston2,M. Moutrie2, J. Pottage2, and M.R.Taghizadeh1; 1IPAQS/EPS Heriot-WattUniversity, Edinburgh, United Kingdom;2Atomic Weapons Establishment, Aldermas-ton, United KingdomWe present the design, fabrication and ver-i�cation of an all-optical sensor for RFelectromagnetic pulse detection based uponLiNbO3 waveguides. �e sensor is capableof measuring both the peak �eld strengthand the pulse shape.
CG-6.5 WED 17:00Laser pulse duration can control thebreakage of multiple chemical bondsX. Xie1, E. Lötstedt2,3,4, S. Roither1, S.Erattupuzha1, S. Larimian1, D. Kartashov1,M. Schö�er1, K. Midorikawa2,3, A.Baltuška1, K. Yamanouchi4, and �M.Kitzler1; 1Photonics Institute, ViennaUniversity of Technology, Vienna, Austria;2Laser Technology Laboratory, RIKEN,Saitama, Japan; 3RIKEN Center forAdvanced Photonics, Saitama, Japan;4Department of Chemistry, School of Science,�e University of Tokyo, Tokyo, JapanWe show that the interplay of electron re-moval and nuclear dynamics on the few fem-tosecond range, controlled by the durationof few-cycle laser pulses, determines the ra-tio of C2H
3+4 fragmentation into two respec-
tively three moieties.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCN-2.5 WED 17:15A sensor for real-time monitoring of NO2using a diode laser and cavity enhancedmultiple line integrated absorptionspectroscopyA. Karpf and �G. Rao;Department of Physics,Adelphi University, Garden City, NY 11530,United StatesA trace gas sensor was developed using amultimode diode laser and cavity enhancedmultiple line integrated absorption spec-troscopy. NO2 was detected with 320 pptsensitivity over an integration time of 50 ms.
EH-4.6 WED 17:15High quality factor, fully switchable THzsuperconducting metasurface for cavityQED applications�G. Scalari1, C. Maissen1, S. Cibella2, J.Keller1, R. Leoni2, M. Beck1, and J. Faist1;1Institute for QuantumElectronics, Eidgenös-sische TechnischeHochschule Zürich,, Zürich,Switzerland; 2Istituto di Fotonica e Nanotec-nologie (IFN), CNR, via Cineto Romano 42,Rome, ItalyWe present a complementary THz metasur-face realised with Niobium thin �lm whichdisplays a quality factor Q=54 at 266 GHzand a fully switchable behaviour .We willshow such cavity employed in a QED exper-iment.
CL-1.4 WED 17:15Laser manufacturing for multi-analytepaper-based diagnostic sensors�I. Katis, P. He, R. Eason, and C. Sones;Optoelectronics Research Centre, Universityof Southampton, Southampton, United King-domWe present here our work on the fabrica-tion of paper-based multiplexed diagnosticsensors, using direct-write laser-based pro-cesses (Laser Induced Forward Transfer andphoto-polymerisation), for the detection ofglucose and proteins (BSA).
CJ-10.6 WED 17:15In situ Temperature Measurement inHigh Power Fiber Ampli�ers�F. Beier1,2, M. Heinzig2, N. Haarlammert2,J. Nold2, T. Schreiber2, R. Eberhardt2, andA. Tünnermann1,2; 1Friedrich-Schiller-Universitaet, Institute of Applied Physics,Jena, Germany; 2Fraunhofer Institute forApplied Optics and Precision Engineering,Jena, GermanyWe report on a setup for in situ tempera-ture measurement in high power ampli�er�bers based on an Optical Frequency Do-main Re�ectometer (OFDR). Suchmeasure-ment system allows analyzing the longitudi-nal �ber core temperature distribution.
ROOM 13a18:45 – 20:15PD-A: Postdeadline Session AChair: Valerio Pruneri, ICFO - �e Institute of PhotonicSciences and ICREA, Castelldefels, Spain
PD-A.1 WED 18:4549-fs Yb:YAG thin-disk oscillator with distributedKerr-lens mode-locking�J. Zhang1,2, J. Brons1, M. Seidel1, V. Pervak3, V.Kalashnikov4, Z. Wei2, A. Apolonski1,3, F. Krausz1,3,and O. Pronin1; 1Max-Planck-Institute of Quantum Op-tics, Garching, Germany; 2Institute of Physics, ChineseAcademy of Sciences, Beijing, China, People’s Republic of(PRC); 3Ludwig-Maximilians-University Munich, Garch-ing, Germany; 4Aston University, Institute of PhotonicTechnologies, Aston, United Kingdom�e concept of distributed Kerr-lens mode-locking anda thin-disk Yb:YAG oscillator based on this concept arepresented. �e described oscillator directly generatespulses with a duration of 49-fs and spectral width of 33nm.
PD-A.2 WED 18:55Development for Ultraviolet Vertical Cavity SurfaceEmitting LasersY.-S. Liu1, A.F.M.S. Haq1, T.-T. Kao1, K. Mehta1, S.-C.Shen1, T. Detchprohm1, P. Yoder1, H. Xie2, F. Ponce2, and�R.D. Dupuis1; 1Georgia Institute of Technology, Atlanta,United States; 2Arizona State University, Tempe, UnitedStatesWe present our current development toward an ultra-violet vertical cavity surface emitting laser, which in-cludes an electrically conducting distributed Bragg re-
�ector with peak re�ectivity of 91.6% and an opticallypumped VCSEL at 367.5 nm.
PD-A.3 WED 19:05Novel techniques for electrical tuning inquantum-cascade lasers.�A. Bismuto; Alpes Lasers SA, Neuchatel, SwitzerlandVernier basedDBRQCLs with integrated heaters to con-trol the mirror temperature are presented. Spectral tun-ing of 40cm-1 and 25cm-1 at 2000cm-1 and 1100cm-1were observed in cw. Tuning speeds of several kHz arepresented.
PD-A.4 WED 19:15Backward air lasing with femtosecond pumpingS. Alisauskas1, A. Baltuska1, R. Boyd2,3, and �P.Polynkin4; 1Photonics Institute Vienna, University ofTechnology, Vienna, Austria; 2Department of Physics,University of Ottawa, Ottawa, Canada; 3Institute of Op-tics, University of Rochester, Rochester, United States;4College of Optical Sciences, University of Arizona, Tuc-son, United StatesWe apply femtosecond laser pulses at 226nm to pumpbi-directional mirror-less lasing in air. Bene�cially forapplications, lasing is predominantly in the backward di-rection; forward lasing is suppressed through destructiveinterference between di�erent emission channels.
PD-A.5 WED 19:25Silicon Nitride Waveguides Enable Stabilization ofGigahertz Frequency Combs from Diode-PumpedSolid-State Lasers�A. Klenner1, A.S. Mayer1, A.R. Johnson2, K. Luke3,
M.R.E. Lamont2,3,4, Y. Okawachi2, M. Lipson3,4, A.L.Gaeta2,4, and U. Keller1; 1Department of Physics, In-stitute of Quantum Electronics, ETH Zurich, Zurich,Switzerland; 2School of Applied and Engineering Physics,Cornell University, Ithaca, United States; 3School ofElectrical and Computer Engineering, Cornell Univer-sity, Ithaca, United States; 4Kavli Institute at Cornellfor Nanoscale Science, Cornell University, Ithaca, UnitedStatesWe present the �rst carrier-envelope-o�set (CEO) sta-bilization of a gigahertz diode-pumped solid-state laserbased on direct supercontinuum generation in a CMOS-compatible silicon nitride waveguide and demonstrateexcellent noise properties of the tight CEO-lock.
PD-A.6 WED 19:35Mode-Resolved 10-GHz Frequency Comb from aFemtosecond Optical Parametric Oscillator�Z. Zhang, K. Balskus, R. McCracken, and D. Reid;Heriot-Watt University, Edinburgh, United KingdomWe report a mode-resolved 10-GHz frequency-combgenerated by �ltering an OPO comb with a stabilizedFabry-Pérot cavity. �is novel source opens up uniqueopportunities for precise frequency metrology and spec-troscopy in the near- and mid-IR.
PD-A.7 WED 19:45High Average-Power and Energy Deep-UltravioletFemtosecond Pulse Source Driven by 10 MHzFibre-Laser�F. Köttig, F. Tani, P. Uebel, P.S.J. Russell, and J.C. Travers;Max Planck Institute for the Science of Light, Erlangen,Germany
Femtosecond pulses, tunable between 270 and 320 nmwith up to 70 nJ energy, are generated by pumping adual-stage gas-�lled kagome-PCF system. �e 9.6 MHzrepetition-rate leads to average deep-UV powers of 693mW.
PD-A.8 WED 19:55Broadband azimuthal polarizer using gold nanowireenhanced step-index �bre�A. Tuniz1, C. Jain1,2, M. Potenz1,2, S. Weidlich1,3, andM. Schmidt1,2,4; 1Leibniz Institute of Photonic Technology(IPHT Jena), Jena, Germany; 2Abbe School of Photonicsand Faculty of Physics, Jena, Germany; 3Heraeus Quarz-glas GmbH & Co. KG, Hanau, Germany; 4Otto SchottInstitute of Materials Research, Jena, GermanyWe experimentally demonstrate that a step-index �brewith a central gold nanowire is an e�cient azimuthal po-larizer, providing broadband low-loss transmission forazimuthally polarized TE01 modes, with applications inSTED microscopy, laser tweezing and superfocussing.
PD-A.9 WED 20:05Optomechanical self-stabilization and hysteresis of afree-standing silica nanospike inside a hollow-corephotonic crystal �bre�S. Xie, R. Pennetta, D. Bykov, T. Euser, and P. Russell;Max Planck Institute for the Science of Light, Erlangen,GermanyA mechanically compliant silica nanospike can be self-stabilized at the core-center of a hollow-core photoniccrystal �bre by optical tweezer forces. Hysteresis behav-ior is measured indicating the system a promising plat-form for exploring optomechanical e�ects.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCK-13.6 WED 17:15Generation of Strong Electric Fields withPure Longitudinal Polarization by Using aDielectric Structure and a FocusedRadially Polarized Beam�K. Kitamura1,2 and S. Noda2,3; 1�e HakubiCenter for Advanced Research, Kyoto Univer-sity, Kyoto, Japan; 2Department of ElectronicScience and Engineering, Graduate School ofEngineering, Kyoto University, Kyoto, Japan;3Photonics and Electronics Science and Engi-neering, Kyoto University, Kyoto, JapanWepropose a new concept to generate strongelectric �elds by using a dielectric struc-ture and a focused radially polarized beam,which can lead the electric �elds with 0.4 λFWHM and pure longitudinal polarization.
EA-8.5 WED 17:15Indistinguishable Photons fromDeterministic Quantum Dot Microlenses�A. �oma1, P. Schnauber1, M. Gschrey1,R. Schmidt1, B. Wohlfeil2, M. Seifried1, J.-H. Schulze1, S. Burger2, F. Schmidt2, A.Strittmatter1, S. Rodt1, T. Heindel1, and S.Reitzenstein1; 1Institut für Festkörperphsik,Technische Universität Berlin, Berlin, Ger-many; 2Zuse-Institut Berlin, Berlin, GermanyWe explore the quantum optical proper-ties of single semiconductor quantum dots(QDs) deterministically integrated into mi-crolenses. In particular we address the in-�uence of the excitation power on single-photon purity and indistinguishability ofphotons.
CB-7.6 WED 17:15Longitudinal Multimode Dynamics inMonolithically Integrated MasterOscillator Power Ampli�ersM. Vilera1, �A. Perez-Serrano1, J. Javaloyes2,J.M.G. Tijero1, I. Esquivias1, and S. Balle2;1CEMDATIC-ETSIT, Universidad Politec-nica de Madrid (UPM), Madrid, Spain;2Departament de Fisica, Universitat de lesIlles Balears (UIB), Palma deMallorca, SpainWe investigate the observed longitudinalmultimode dynamics of a MOPA by meansof a travelling wave model that incorporatescoupled cavities and thermal e�ects. We dis-cuss their appearance and dependence ongeometrical factors and temperature.
CH-9.6 WED 17:15Frequency Domain Distance Measure-ment for Formation Flight in Space�B. Eder1, M. Hutterer2, L. Pedrosa2, S.Schweyer2, P. Putzer2, R. Kienberger3, andU. Hugentobler1; 1Technische UniversitätMünchen, FESG, Munich, Germany; 2OHBSystem AG, Munich, Germany; 3TechnischeUniversität München, Physik DepartmentE11, Garching, GermanyFor measuring huge absolute distances atechnique of Frequency Domain DistanceMeasurement without moving parts andfree-beam components can be used. Firstmeasurements prove the simple handling ofthe present setup compared to time-of-�ightmeasurements.
CG-6.6 WED 17:15Two-Pulse Control over DoubleIonization Pathways in CO2�S. Erattupuzha, S. Larimian, A. Baltuška, X.Xie, and M. Kitzler; Photonics Institute, Vi-enna University of Technology, Vienna, Aus-triaUsing a double-pulse scheme we visual-ize and control molecular dynamics takingplace on intermediate states populated dur-ing di�erent sequential double ionizationpathways of CO2. Exchanging the pulse-sequence can almost completely switch thepathway.
ROOM 13b18:45 – 20:15PD-B: Postdeadline Session BChair: �orsten Ackemann, University of Strathclyde,Glasgow, United Kingdom
PD-B.1 WED 18:45Rydberg excitation of trapped strontium ions�G. Higgins1, F. Pokorny1, F. Kress1, J. Haag1, C. Maier1,Y. Colombe1, and M. Hennrich1,2; 1Inst. für Exp.-Physik,Univ. Innsbruck, Innsbruck, Austria; 2Department ofPhysics, Stockholm Univ., Stockholm, SwedenWe report on the �rst trapped strontium Rydberg ions.Trapped Rydberg ions are a novel approach for quan-tum information processing which combines strong in-teraction between Rydberg states with advanced quan-tum control of trapped ions.
PD-B.2 WED 18:55Squeezed light and self-induced transparency inmercury-�lled hollow core photonic crystal �bers�U. Vogl1,2, N. Joly1,2, P. Russell1,2, C. Marquardt1,2, andG. Leuchs1,2; 1MPI for the Science of Light, Erlangen, Ger-many; 2Inst. for Optics, Information and Photonics, Univ.Erlangen-Nürnberg, Erlangen, GermanyWe successfully demonstrate squeezing of nanosecondpulses via self-induced transparency in a system of mer-cury vapor con�ned in a hollow core kagomé-style �ber.
PD-B.3 WED 19:05Universal Linear Optics for Quantum InformationProcessingJ. Carolan1, C. Harrold1, C. Sparrow1,2, E. Martin-Lopez1,3, N.J. Russell1, J.W. Silverstone1, P.J. Shadbolt1,2,N. Matsuda4, M. Oguma5, M. Itoh5, G.D. Marshall1,M.G. �ompson1, J.C.F. Matthews1, T. Hashimoto5, J.L.
O’Brien1, and �A. Laing1; 1Centre for Quantum Photon-ics, Univ. of Bristol, Bristol, United Kingdom; 2Dep. ofPhysics, Imperial College London, London, United King-dom; 3Nokia Research Centre, Cambridge, United King-dom; 4NTT Basic Research Lab., NTT Corporation, At-sugi, Japan; 5NTT Device Technology Lab., Atsugi, JapanWe demonstrate the longstanding goal that a single re-programmable optical chip is su�cient to implementall possible linear optical protocols, including quantumlogic and entangling gates.
PD-B.4 WED 19:15Active Temporal Multiplexing of a Silicon HeraldedSingle-Photon Source�C. Xiong1, X. Zhang1, Z. Liu2,3, A. Mahendra1,2, D.-Y. Choi4, C.J. Chae5, P. Leong2, M. Collins1, and B.Eggleton1; 1CUDOS, IPOS, School of Physics, Univ. ofSydney, Sydney, Australia; 2School of Electrical and In-formation Engineering, Univ. of Sydney, Sydney, Aus-tralia; 3Dep. of Communication Engineering, School of In-formation Engineering, Guangdong Univ. of Technology,Guangzhou, China, People’s Republic of (PRC); 4CUDOS,Laser Physics Centre, Australian Nat. Univ., Canberra,Australia; 5Advanced Photonics Research Inst., GwangjuInst. of Science and Technology, Gwangju, Korea, SouthUsing a fast �eld-programmable gate array, and low-lossoptical switches, we demonstrate a 100% enhancementto the heralded single-photon probability per clock cycleby active temporal multiplexing of a silicon nanowire-based heralded single-photon source.
PD-B.5 WED 19:25Van-der-Waals Explosion of Cold Rydberg AggregatesR. Faoro1,2, C. Simonelli1,3, M. Archimi1, G. Masella1,M. Valado1,3, R. Mannella1,4, D. Ciampini1,3,4, E.
Arimondo1,3,4, and �O. Morsch1,3; 1Dip. di Fisica, Pisa,Italy; 2Lab. Aimé Cotton, CNRS, Orsay, France; 3INO-CNR, Pisa, Italy; 4CNISM UdR Dip. di Fisica, Pisa, ItalyWe have measured the e�ect of the van-der-Waals forceon Rydberg atoms using a time-of-�ight technique. Inorder to produce aggregates of Rydberg atoms, o�-reso-nant excitation was used a�er creating an initial seed.
PD-B.6 WED 19:35Pure-Quartic Solitons�A. Blanco-Redondo1, T.F. Krauss2, B. Eggleton1, and C.Husko1; 1CUDOS, IPOS, School of Physics, Univ. of Syd-ney, Sydney, Australia; 2Dep. of Physics, University ofYork, York, United KingdomWe unveil a new class of solitons arising from the in-terplay of fourth-order dispersion and self-phase mod-ulation. �ese pure-quartic solitons enable soliton func-tionality in the normal GVD regime of optical media.
PD-B.7 WED 19:45Observation of Single-Photon Superradiance from aQuantum Dot�P. Tighineanu1, R. Daveau1, T. B. Lehmann1, H. E.Beere2, D. A. Ritchie2, P. Lodahl1, and S. Stobbe1; 1NielsBohr Inst., Copenhagen, Denmark; 2Cavendish Lab.,Cambridge, United KingdomWe demonstrate that single-photon superradiance is anew approach for dramatically increasing light-matterinteraction in quantum dots. We prepare the super-radiant state deterministically and measure a stronglyenhanced single-photon emission compared to conven-tional quantum dots.
PD-B.8 WED 19:55High-speed THz Metamaterial Modulators Exploit-
ing Strong Coupling between Split-ring Resonatorsand Graphene Plasmonic Resonators�P.Q. Liu1, I.J. Luxmoore2, S.A. Mikhailov3, N.A.Savostianova3, F. Valmorra1, J. Faist1, and G.R. Nash2;1Inst. for Quantum Electronics, ETH Zurich, Zurich,Switzerland; 2College of Engineering, Mathematics andPhysical Sciences, Univ. of Exeter, Exeter, United King-dom; 3Univ. of Augsburg, Augsburg, GermanyTunable THz hybrid metamaterials employing metal-based complementary split-ring resonators e�cientlycoupled to graphene plasmonic resonators are devel-oped. �e interaction between the two resonatorsreaches strong-coupling regime. State-of-the-art trans-mission modulation depth and modulation speed aredemonstrated.
PD-B.9 WED 20:05Frequency Comb of Time-Bin Entangled PhotonPairs on a ChipM. Kues1, C. Reimer1, P. Roztocki1, B. Wetzel1, F.Grazioso1, B.E. Little2, S.T. Chu3, D.J. Moss1,4, �L.Caspani1,5, and R. Morandotti1; 1INRS-EMT, Varennes,Canada; 2Xi’an Institute of Optics and Precision Mechan-ics of CAS, Xi’an, China, Republic of (ROC); 3Departmentof Physics and Material Science, City University of HongKong, Hong Kong, China, Republic of (ROC); 4School ofElectrical and Computer Engineering, RMIT University,Melbourne, Australia; 5School of Engineering and Phys-ical Sciences, Heriot-Watt University, Edinburgh, UnitedKingdomWe report the generation of multiple-frequency time-bin entangled photon pairs from a single integratedCMOS-compatible microring resonator. Entanglementon �ve channel pairs with visibilities above 82.6% (93.8%background-corrected) is demonstrated.
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HALL B013:00 – 14:00CF-P: CF Poster Session
CF-P.1 WEDPassively mode-locked erbium-doped �ber laserusing gold-nanosphere based on double cladding�ber as saturable absorber�J. Yuan, X. Bai, D. Fan, F. Pang, and X. Zeng; �e KeyLab of Specialty Fiber Optics and Optical Access Network,Shanghai, China, People’s Republic of (PRC)Wehave obtained a serial of 29 ns pulses at 1530 nmwitha repetition rate of 8.47 MHz by using a double cladding�ber coated with gold-nanosphere as saturable absorber.
CF-P.2 WEDQuantum-Dot Saturable Absorber and Kerr LensMode-Locked Yb:KGW Laser with >300 kW of PeakPowerR. Akbari1, H. Zhao1, K. Fedorova2, E. Rafailov2, and�A. Major1; 1University of Manitoba, Winnipeg, Canada;2Aston University, Birmingham, United KingdomDual action of quantum-dot saturable absorber and Kerrlens mode locking of a diode-pumped Yb:KGW laserwas demonstrated. �e laser delivered 105 fs pulses with2.5W of average power and >300 kW of peak power.
CF-P.3 WEDCoherent Mode-Locking: �eory and ExperimentR. Arkhipov1,2,3, �M. Arkhipov3, A. Shimko3, and I.Babushkin4; 1Weierstrass Institute, Berlin, Germany;2Humboldt-Universität zu Berlin, Mathematisch-Naturwissenscha�liche Fakultät, Berlin, Germany;3Faculty of Physics, St. Petersburg State University,St. Petersburg, Russia; 4Institute of Quantum Optics,Leibniz University, Hannover, GermanyWe consider theoretically and experimentally a nowellcoherent modelocking technique based on self-inducedtransparency in lasers. Our theory shows a possibility tosimpify drammatically the required setup. Experimentcon�rms at least SIT-related e�ects in the absorber.
CF-P.4 WEDUltrashort Optical Pulse Yb-doped Fiber GeneratorBased on Nonlinear Spectral Re-shaping�K. Regelskis, J. Želudevičius, and G. Račiukaitis; Depart-ment of Laser Technology, Center for Physical Sciences &Technology, Vilnius, LithuaniaWe present an ultrashort optical pulse Yb-doped �bergenerator based on nonlinear spectral re-shaping, oper-ating at a wavelength of 1060 nm. Pulses with the du-ration of 228 fs a�er compression were experimentallyachieved.
CF-P.5 WEDSub-200 fs dissipative soliton Er-doped �ber lasermode-locked by Sb2Te3 topological insulator�J. Boguslawski1, J. Sotor1, G. Sobon1, R. Zybala2, M.Kowalczyk1, J. Tarka1, D. Sliwinska1, and K. Abramski1;1Laser & Fiber Electronics Group, Wroclaw University ofTechnology, Wroclaw, Poland; 2Faculty of Materials Sci-ence and Engineering, Warsaw University of Technology,Warsaw, PolandWe present, for the �rst time, a dissipative soliton gener-ation in Er-doped �ber laser mode-locked bymonocrys-talline antimony telluride (Sb2Te3) topological insulatorsaturable absorber. Sub-200 fs pulses with 32.5 nm ofspectral bandwidth were achieved.
CF-P.6 WEDSoliton Molecules Generation in DWCNTMode-Locked�ulium-Doped Fibre Laser�M. Chernysheva1, C. Mou1, R. Howe2, G. Hu2, T.Hasan2, S. Turitsyn1, and A. Rozhin1; 1Aston Instituteof Photonics Technologies, Aston Unversity, Birmingham,United Kingdom; 2Cambridge Graphene Centre, Univer-sity of Cambridge, Cambridge, United KingdomWe have experimentally investigated power-dependantproperties of double-walled carbon nanotubes(DWCNT). We have realised DWCNT mode-locked�ulium-doped �bre laser and have achieved stable gen-eration of soliton molecules with up to 90-mW averageoutput power.
CF-P.7 WEDDri� and Noise of Carrier-Envelope Phase inTi:Sapphire Based Ultrashort Pulse Ampli�ersA. Borzsonyi1,2, �R.S. Nagymihaly1,2, and K. Osvay1,2;1Dept. of Optics and Quantum Electronics, Universityof Szeged, Szeged, Hungary; 2ELI-ALPS, ELI-HU Nk�.,Szeged, HungaryAbsolute CEP shi� of laser pulses originating from theampli�cation process in Ti:Sapphire is measured at dif-ferent repetition rates, gain, and thermal parameters.�e increase of CEP noise is <100mrad, depending onthe ampli�cation conditions.
CF-P.8 WEDAll-PM-�ber laser oscillator mode-locked with anonlinear optical loop mirror�J. Szczepanek1, T. Kardaś1, M. Michalska2, C.Radzewicz1, and Y. Stepanenko1,3; 1Institute of Ex-perimental Physics, Department of Physics, Universityof Warsaw, Warsaw, Poland; 2Institute of Optoelectron-ics, Military University of Technology, Warsaw, Poland;3Institute of Physical Chemistry, Polish Academy ofSciences, Warsaw, PolandWe demonstrate environmental stable, all-PM-�ber,
self-starting, all-normal dispersion Yb laser oscillatormode-locked with a nonlinear optical loopmirror. Non-linear processes a�ecting the electrical �eld temporal in-tensity of the pulse are investigated.
CF-P.9 WEDOptical arbitrary waveform characterization at thefew-photon level using dual-comb interferometryV. Durán1, �S. Tainta2, and V. Torres-Company1;1Chalmers University of Technology, Göteborg, Sweden;2Universidad Pública de Navarra, Pamplona, SpainWe present a dual-comb �ber system that enables sub-microsecond optical arbitrary waveform characteriza-tion with a sensitivity of a few photons per pulse. �isis achieved by combining electro-optic comb technologyand a pre-ampli�ed balanced receiver.
CF-P.10 WED80 fs Optical Pulse Generation UsingMach-Zehnder-Modulator-Based Flat CombGenerator and Dispersion-FlattenedDispersion-Decreasing Fibre�I. Morohashi, T. Sakamoto, N. Sekine, T. Kawanishi, A.Kasamatsu, and I. Hosako; National Institute of Informa-tion and Communications Technology, Tokyo, JapanBy compressing 468 GHz-width combs, which weregenerated by a Mach-Zehnder-modulator-based �atcomb generator (MZ-FCG), using a dispersion-�atteneddispersion-decreasing�bre, 80 fs-width pulses have beensuccessfully generated.
CF-P.11 WEDOptical Frequency Characteristics of a 10GHzAsynchronous Harmonic Mode-Locked Fiber SolitonLaser�D.-H. Yeh, S.-M. Wang, C.-J. Luo, and Y. Lai; Depart-ment of Photonic and Institute of Electro-Optical Engi-neering, National Chiao TungUniversity, Hsinchu, China,Republic of (ROC)Individual optical components of asynchronous mode-locked �ber lasers are shown to be not periodically os-cillating along with the lasing central wavelength. �eirrandom variation can be reduced by band-pass optical�ltering and/or optical injection.
CF-P.12 WEDComparison of di�erent carrier-envelope o�setfrequency stabilization methods for a highperformance DPSSL frequency comb�S. Kundermann and S. Lecomte; Centre Suissed’Electronique et de Microtechnique (CSEM), Neuchâtel,SwitzerlandAn optical frequency comb is fCEO locked using thetraditional pump power modulation and external fre-
quency shi�ing via an external acousto-optic frequencyshi�er in both feed forward and feedback architecture.A detailed comparison is provided.
CF-P.13 WEDGeneration of broadband femtosecond mid-IR pulsesin long KTA OPA in the vicinity of the edge oftransparency�F. Potemkin, A. Podshivalov, E. Migal, E. Mareev,and V. Gordienko; Faculty of Physics and InternationalLaser Center M.V. Lomonosov Moscow State University,Moscow, RussiaWe have realized the generation of femtosecond pulses,tunable in 1.8-4.9 um, from long KTA OPA, pumpedwith doubled Cr:forsterite laser (620 nm), with maxi-mal e�ciency close to the absorption edge of crystal (4.1um).
CF-P.14 WEDExperimental Observation of Dispersive WaveGeneration by Self-Defocusing Nonlinearity in BBOCrystal�B. Zhou and M. Bache; DTU Fotonik, Technical Univer-sity of Denmark, Kgs. Lyngby, DenmarkWe experimentally observe dispersive waves gener-ated by a self-defocusing soliton formed in a phase-mismatched BBO crystal. Tunable dispersive waves aregenerated around 2.0 to 2.1 �m with the NIR pumpwavelength of 1.3 �m.
CF-P.15 WEDFemtosecond Tunable Wavelength OPCPA SystemBased on Picosecond Fiber Laser Seed andPicosecond DPSS Laser Pump�R. Danilevičius1,2, A. Zaukevičius1, A. Michailovas1,2,and N. Rusteika1,2; 1Ekspla Ltd., Vilnius, Lithuania;2Center for Physical Sciences and Technology, Vilnius,LithuaniaIn this workwe constructed a compact femtosecond tun-able wavelength OPCPA system with a novel front-end.We measured up to 0.85 mJ, 30-50 fs duration pulses at680-930 nm wavelength tuning range.
CF-P.16 WEDVersatile Generation of Mid Infrared Pulses throughDi�erence Frequency Mixing in Super-ContinuumPulses�F. Isa, L. Fujii, T. Suzuki, K. Hirosawa, and F. Kannari;Keio university, Yokohama, JapanVersatile femtosecond mid infrared pulse generationwhere the bandwidth, center wavelength and pulse shapeare variable was achieved using a single supercontinuumlight shaped by a 4-f vector pulse shaper and a type-IBBO crystal.
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HALL B0CF-P.17 WEDE�cient Supercontinuum Generation in QuadraticNonlinear Waveguides withoutQuasi-Phase-Matching�H. Guo1, B. Zhou1, M. Steinert2, F. Setzpfandt2, T.Pertsch2, H.-P. Chung3, Y.-H. Chen3, and M. Bache1;1Group of Ultrafast Nonlinear Optics, DTU Fotonik,Technical University of Denmark (DTU), Kgs. Lyngby,Denmark; 2Institute of Applied Physics, Abbe Center ofPhotonics, Friedrich-Schiller-Universität Jena, Jena, Ger-many; 3Department of Optics and Photonics, NationalCentral University, Jhongli, China, Republic of (ROC)Soliton-induced supercontinuum generation (SCG)is experimentally accomplished in quadratic nonlin-ear waveguides without quasi-phase-matching, bydirectly pumping in the normal dispersion range,as negative-signed nonlinearity is produced throughphase-mismatched interactions. �e scheme promisese�cient mid-IR SCGs.
CF-P.18 WEDPicosecond Contrast of Recompressed CPA Pulses�M. Kalashnikov1,2 and N. Khodakovskiy1; 1Max-Born-Institute, Berlin, Germany; 2ELI-HU Non-Pro�t Ltd,Szeged, Hungary�ree types of stretcher-compressor con�gurations weretested aiming to investigate pedestals appearing on a pi-cosecond scale. It was found that the trailing front cangenerate the leading pedestal via self-phase modulationreproducing its substructure.
CF-P.19 WEDHigh Contrast Broadband Seeder for Multi-PW LaserSystem�O. Chalus1, A. Pellegrina1, O. Casagrande1, C. Derycke1,L. Boudjemaa1, C. Simon-Boisson1, S. Laux1, F. Lureau1,D. Sanchez2, J. Biegert2, J. Ahrens3, T. Binhammer3, O.Prochnow3, and S. Rausch3; 1�ales Optronique SAS,Elancourt, France; 2ICFO - Institut de Ciences Fotoniques,Castelldefels, Spain; 3Venteon Laser Technologies GmbH,Garbsen, GermanyHybrid Ti:Sa CPA/BBO OPCPA system with a XPW �l-ter inbetween the two has been developed to produce abroadband high contrast seeder of 10 mJ for the two 10PetaWatt beamlines of ELI NP infrastructure.
CF-P.20 WEDDesign and initial results of 10 PW laser for ELI-NP�F. Lureau1, S. Laux1, O. Casagrande1, O. Chalus1, P.-A. Duvochelle1, S. Herriot1, G. Matras1, C. Radier1, L.Boudjemaa1, C. Simon-Boisson1, R. Dabu3, I. Dancus3,and D. Ursescu2,3; 1�ales Optronique SAS, Elancourt,France; 2Horia Holubei National Research Institute forresearch and development in physics and nuclear engi-
neering, Magurele, Romania; 3National Institute for LaserPlasma and Radiation Physics, Magurele, RomaniaA laser system made of 2 beams of 10 PW each has beendesigned and is currently built for ELI-NP research in-frastructure. Design is presented as well as preliminaryresults
CF-P.21 WEDComparison of Linear Methods for AngularDispersion Measurement�M. Gstalter1, A. Borzsonyi1,2, and K. Osvay1,2; 1ELI-ALPS, ELI-Hu Nk�., Szeged, Hungary; 2Dept. of Opticsand Quantum Electronics, University of Szeged, Szeged,Hungary�ree angular dispersion measurement methods are ex-perimentally compared upon the alignment of a trans-mission grating compressor. We found that with similaraccuracies, the spectrally �ltered imaging provides 2Ddetection on-the-�y and ease of use.
CF-P.22 WEDA High-contrast Petawatt-class Ultrashort PulseLaser�N. Xie, Q. Zhu, J. Su, X. Wang, K. Zhou, X. Huang,X. Zeng, Y. Guo, L. Sun, and Q. Li; Research Center ofLaser Fusion, China Academy of Engineering Physics, Mi-anyang, China, People’s Republic of (PRC)�e paper presents a sub-petawatt femtosecond laser fa-cility, which is a multi-stage Ti:sapphire chirped pulseampli�cation (CPA) laser system. Cross-polarized wavegeneration was used to improve the temporal contrast.
CF-P.23 WEDSpace charge e�ects during ultrashort laser pulse�lament guided high voltage discharges in air�A. Schmitt-Sody1, A. Lucero2, V. Hasson3, and W.White1; 1Air Force Research Laboratory, Albuquerque,NM, United States; 2Boeing DES, Albuquerque, NM,United States; 3University of Arizona, Tucson, AZ, UnitedStatesWe present new experimental results that show the im-portant role of space charge e�ects during laser �lamentguided high voltage discharges at atmospheric pressurein air and explain the overall dynamics seen in experi-ments.
CF-P.24 WEDLaser Filament Induced Ice Multiplication Process�M. Matthew1, F. Pomel1, C. Wender2, J. Kasparian1,T. Liesner2, and J.-P. Wolf1; 1University of Geneva,Geneva, Switzerland; 2Karlsruhe Institute of Technology,Karslruhe, Germany�e contribution has been withdrawn by the authors.
CF-P.25 WEDCoherent Beam Recombination of Two FemtosecondLaser Beams�M. Galimberti, B. Parry, A. Jenson, A. Rogers, J. Phillips,C. Hernandez-Gomez, S. Hawkes, D. Symes, A. Sellers,N. Rodrigues, P. Foster, C. Hooker, R. Pattathil, A. Boyle,R. Heathcote, P. Brummitt, I. Musgrave, W. Shaikh, andJ. Collier; Central Laser Facility, STFC, Didcot, UnitedKingdomWe present the outcome from a proof of principle ex-periment on coherent beam recombinations of two fem-tosecond laser beams, a new scheme to overcome the is-sues and the plan for the next experimental campaign.
CF-P.26 WEDOptimization and coherent combining of Ramandissipative solitons in �ber laser�D. Kharenko1,2, A. Bednyakova2,3, E. Podivilov1,2, M.Fedoruk2,3, A. Apolonski1,4, and S. Babin1,2; 1Instituteof Automation and Electrometry SB RAS, Novosibirsk,Russia; 2Novosibirsk State University, Novosibirsk, Rus-sia; 3Institute of Computational Technologies SB RAS,Novosibirsk, Russia; 4Ludwig-Maximilians-UniversitaetMuenchen and Max-Planck-Institut fuer Quantenoptik,Garching, GermanySynchronous generation of a chirped dissipative solitonand a Raman dissipative soliton in an all-�ber laser cav-ity is optimized. Coherent combining of both solitons isperformed and a second-order Raman soliton is demon-strated.
CF-P.27 WEDSpectral and spatial shot-to-shot correlation analysisof bulk supercontinuum in the mid-infrared�A. van de Walle1,2, M. Hanna1, F. Guichard1,3, Y.Zaouter3, A. �ai2, N. Forget2, and P. Georges1;1Laboratoire Charles Fabry, Palaiseau, France; 2Fastlite,Valbonne, France; 3Amplitude Systemes, Pessac, FranceUsing the time-stretch dispersive Fourier transformtechnique, we report on full-bandwidth measurement ofspectral and spatial correlations in supercontinua gener-ated in bulk YAG by focusing femtosecond microjoulepulses, showing excellent stability in mid-IR wavelengthrange.
CF-P.28 WEDEigenmode expansion of optical vortices based onelectric-�eld reconstruction in spatial domain�K. Yamane1,2, S. Nakajim1, M. Suzuki1, Y. Toda1,2, andR. Morita1,2; 1Department of Applied Physics, HokkaidoUniversity, Sapporo, Japan; 2JST CREST, Sapporo, JapanA new fast method to expand electric �eld of opticalvortices into Laguerre-Gaussian modes, beyond orbital-angular-momentum resolution, is demonstrated. It is
based on electric-�eld reconstruction and applicable tocomplicated ultra-broadband light waves.
CF-P.29 WEDImproved Multiple Pulse Reconstruction from SHGFROG Spectrograms�A. Hause and F.Mitschke; Institut für Physik, UniversitätRostock, Rostock, GermanyA modi�ed algorithm is presented which signi�cantlyreduces the rate of false reconstructions of SHG FROGspectrograms. A procedure to obtain error bars is given;they allow to gauge the quality of the reconstruction.
CF-P.30 WEDSingle-shot attenuated total re�ectance infraredspectroscopy with chirped-pulse upconversion�T. Fuji1, H. Shirai1, C. Duchesne1,2, and Y. Furutani1;1Institute for Molecular Science, Okazaki, Japan; 2ChimieParisTech, Paris, FranceSingle-shot infrared absorption spectrum measurementat attenuated total re�ectance infrared spectroscopy hasbeen demonstrated. �e system was applied to observethe dynamics of exchanging process of bu�ers for bio-logical tissues.
CF-P.31 WEDUltrafast demagnetisation and precessional dynamicsin GdFeCo thin Films using a new pump-probesystem in the sub-8 femtosecond rangeC. Gonçalves1, A. Silva1, �D. Navas1, M. Miranda2, F.Silva1, H. Crespo1, and D. Schmool3; 1Department ofPhysics and Astronomy and IFIMUP-IN, Fac. de Ciên-cias, Univ. do Porto, Porto, Portugal; 2Department ofPhysics, Lund University, Lund, Sweden; 3LaboratoirePROMESCNRS (UPR 8521), Université de Perpignan ViaDomitia, Perpignan, FranceDevelop an ultrafast pump-probe apparatus based ona novel dual-colour scheme for the measurement ofspin dynamics, via the MOKE signal, with 8 fs pulse-durations in both pump and probe lines.
CF-P.32 WEDUltrafast coherent control of charge carriers insemiconductors�M.Wismer1, M. Ciappina1, S. Kruchinin1, V. Yakovlev2,and F. Krausz1; 1Max-Planck Institut für Quantenoptik,Garching, Germany; 2Center for Nano-Optics, GSU, At-lanta, United StatesWe investigate theoretically electron dynamics in bulksemiconductors caused by few cycle laser pulses that canbe generated through waveform synthesis. �e wave-forms are optimized to provide control over conductionband populations and interband polarisation.
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HALL B0CF-P.33 WEDOn the Role of Freeman Resonances in Pump-ProbeMeasurements of the Nonlinear Refractive Index�M. Hofmann and C. Brée; Weierstrass Institute for Ap-plied Analysis and Stochastics, Berlin, GermanyWe demonstrate the dramatic impact of Freeman res-
onances on the cross-induced transient refractive in-dex. Its nonperturbative charactermust be carefully con-sidered in pump-probe based measurements of the all-optical Kerr e�ect.
CF-P.34 WEDA novel pulse characterization method using timedomain ptychography�D.-M. Spangenberg1, P. Neethling1, E. Rohwer1, M.Brügmann2, and T. Feurer2; 1LRI, Stellenbosch Univer-sity, Stellenbosch, South Africa; 2IAP, Univeristy of Bern,
Bern, SwitzerlandUltrashort pulse characterization requires the recoveryof the spectral phase. A new method is discussed basedon ptychography, a spatial phase recovery techniquewhich we successfully extended to the temporal domainfor pulse characterization.
13:00 – 14:00CJ-P: CJ Poster Session
CJ-P.1 WEDA Novel Highly Birefringent Photonic Crystal Fiberfor THzWave Guidance�M.S. Habib1,2 and G.K.M. Hasanuzzaman2; 1DTU Fo-tonik, Department of Photonics Engineering, TechnicalUniversity of Denmark, DK-2800 Kgs. Lyngby, Den-mark, Lyngby, Denmark; 2Department of Electrical andElecreonic Enginerring, Rajshahi University of Engineer-ing & Technology, Rajshahi-6204, Bangladesh, Rajshahi,BangladeshIn this paper, a novel and relatively simple highly bire-fringent dual-hole unit based porous-core hexagonalphotonic crystal �ber in THz regime has been reported.�e proposed �ber con�rms birefringence around 0.033at 0.85 THz.
CJ-P.2 WEDInternal Gain in Er-doped As2S3 Planar WaveguideAmpli�ersK. Vu, K. Yan, and �S. Madden; Laser Physics Centre,Australian National University, Canberra, AustraliaLow loss Erbium doped As2S3 planar waveguides arefabricated by cothermal evaporation and plasma etching.Internal gain is demonstrated for the �rst time with Er-bium in chalcogenide glass, and additionally in a planarwaveguide ampli�er.
CJ-P.3 WEDGraphene Q-switched Yb:Yttria waveguide laser byevanescent-�eld interaction delivering an averageoutput power of 0.5 WA. Choudhary1, �S. Beecher1, S. Dhingra2, B. D’Urso2,T. Parsonage1, J. Grant-Jacob1, P. Hua1, J. Mackenzie1,R. Eason1, and D. Shepherd1; 1Optoelectronics ResearchCentre, University of Southampton, Southampton, UnitedKingdom; 2Department of Physics and Astronomy, Uni-versity of Pittsburgh, Pittsburgh, United StatesQ-switched operation of a PLD-grown planar Yb:Y2O3waveguide laser using evanescent interaction with asurface-covered graphene layer is presented . 310 nJpulses at an average power of 456 mW were obtainedduring operation.
CJ-P.4 WEDFemtosecond Fiber Laser Mode-Locked by HybridScheme of Nonlinear Polarization Rotation andSingle-Wall Carbon Nanotube�L. Jin1, K. Nonobe1, Y. Sakakibara2, E. Omoda2,H. Kataura2, and N. Nishizawa1; 1Nagoya University,Nagoya, Japan; 2National Institute of Advanced Indus-trial Science and Technology, Tsukuba, JapanWe proposed a femtosecond �ber laser mode-locked byhybrid scheme of nonlinear polarization rotation andsingle-wall carbon nanotube. �e superior performanceof hybrid scheme was con�rmed for power and pulsewidth both numerically and experimentally.
CJ-P.5 WEDSynchronously pumped 1120 nm short-pulse Raman�ber laser with �exible output dynamics andall-�berized format�H. Chen, S. Chen, Z. Jiang, and J. Hou; College of Op-toelectronic Science and Engineering, National Universityof Defense Technology, Changsha, China, People’s Repub-lic of (PRC)Based on a newly proposed all-�ber-integrated syn-chronously pumping scheme, we achieved highly e�-cient generation of short-pulse 1120 nm Raman laserwith widely tunable pulse duration and repetition rate.
CJ-P.6 WEDBroadband frequency quadrupling of a self-similarYb-�ber ampli�er with 254-268 nm tunable outputJ. Zhao, W. Li, D. Luo, Y. Liu, D. Bai, and �H. Zeng; EastChina Normal University, Shanghai, China, People’s Re-public of (PRC)We report on the generation of tunable pulse across 254-268 nm by frequency quadrupling of a self-similar Yb-�ber ampli�er. 1.33-W average power is achieved at 259nm with a spectral bandwidth of 4.7 nm.
CJ-P.7 WEDAdjustable High-repetition-rate Pulse Trains in aPassively Mode-locked Fiber Laser�R. Si Fodil1,2, F. Amrani1, A. Kellou2, and P. Grelu1;1Lab. ICB UMR 6303 CNRS, Université de Bourgogne,Dijon, France; 2Lab. Electronique Quantique, USTHB,Algiers, Algeria
We characterize experimentally an erbium-doped �berlaser that uses an intracavity Mach-Zehnder interferom-eter to produce an adjustable high-repetition-rate short-pulse output, highlighting its intrinsic pulse train insta-bility.
CJ-P.8 WEDReal-time Spectral Characterization of Random FiberLasers using a Scanning Fabry Perot Interferometer�S. Sugavanam1 and D. Churkin1,2,3; 1Aston Instituteof Photonic Technologies, Birmingham, United Kingdom;2Institute of Automation and Electrometry, Novosibirsk,Russia; 3Novosibirsk State University, Novisibirsk, Russia�e dynamic spectrum of a random �ber laser is mea-sured for the �rst time using a scanning Fabry-Perotinterferometer based real-time spectral measurementtechnique. Narrowband spectral components and cor-relations are revealed.
CJ-P.9 WEDSimple and Compact Visible Tunable Fiber Laser�Y. Fujimoto1, O. Ishii2, and M. Yamazaki3; 1Instituteof Laser Engineering, Osaka University, Suita, Japan;2Production Engineering Section, Optical Glass Produc-tion Department, Sumita Optical Glass, Inc.,, Minami-aizu, Japan; 3Glass Research Division, R&D Department,Sumita Optical Glass, Inc.,, Saitama City, JapanWe propose and demonstrate a novel design of simpleand compact tunable �ber laser skillfully using chro-matic aberration of a lens relay and a slit-like e�ect ofoptical �ber core.
CJ-P.10 WEDTm-doped �bre laser with radially-polarized outputbeam at 2�m�D. Lin, P. Shardlow, M. Beresna, P. Kazansky, and A.Clarkson; Optoelectronics Research Centre, University ofSouthampton, Southampton, United KingdomDirect excitation of the radially-polarized TM01 modein a cladding-pumped Tm �bre laser using a novel modeselection technique is reported. �e laser yielded 6.4Wof output at 1970nm for 27.6Wof absorbed pump power.
CJ-P.11 WEDUltra-broadband tuning of a cascaded Ramanrandom distributed feedback �ber laser�L. Zhang, J. Hu, H. Jiang, X. Yang, and Y. Feng; ShanghaiKey Laboratory of Solid State Laser and Application, andShanghai Institute of Optics and �ne Mechanics, ChineseAcademy of Sciences, Shanghai, China, People’s Republicof (PRC)Pumped with a tunable Yb-doped �ber laser, over 300nm continuously tuning of a cascaded Raman randomdistributed feedback �ber laser is achieved.
CJ-P.12 WEDLow Loss Double-clad Hollow Core Anti-ResonantFibers in the Mid-IR�M.S. Habib, O. Bang, and M. Bache; DTU Fotonik, De-partment of Photonics Engineering, Technical Universityof Denmark, DK-2800, Kgs. Lyngby, Denmark, Lyngby,DenmarkWe present double-clad hollow core anti-resonant �berwith low loss and low fraction of light in silica inmid-IR.Numerical simulations con�rmminimum leakage loss of0.003 dB/km and power fraction in silica around 6x10-5.
CJ-P.13 WEDAll-�ber single-mode laser at 977 nm with 5.5 Woutput powerS. Aleshkina1, �M. Likhachev1, D. Lipatov2,3, O.Medvedkov1, M. Bubnov1, and A. Guryanov2; 1Fiber Op-tics Research Center of the Russian Academy of Sciences,Moscow, Russia; 2Devyatykh G.G. Institute of Chemistryof High-Purity Substances of the Russian Academy ofSciences, Nizhny Novgorod, Russia; 3N.I.LobachevskyUniversity of Nizhny Novgorod, Nizhny Novgorod, RussiaIn this communication we realized the all-�ber single-mode laser scheme operating at 977 nm with a recordhigh output power of 5.5 W.
CJ-P.14 WEDImpact of di�erent order photonic bandgap inspectral �ltering photonic bandgap �ber ampli�er�M. Chen1, S. R. Petersen2, C. B. Olausson3, T. T.Alkeskjold3, and A. Shirakawa1; 1Institute for laser sci-ence, Tokyo, Japan; 2Technical University of Denmark,Lyngby, Denmark; 3NKT Photonics A/S, Birkerød, Den-mark
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HALL B0�e e�ect of di�erent-order bandgaps on parasitic lasingwas investigated in 1178nm photonic bandgap �ber am-pli�ers. Numerical calculations clearly explain the de-pendence on the orientation of the low-index stress rodsfor polarization maintenance against coiling.
CJ-P.15 WEDModelling and Optimization of High Repetition RateFiber Ampli�ers�R. Lindberg, P. Zeil, M.Malmström, V. Pasiskevicius, andF. Laurell; Department of Applied Physics, Royal Instituteof Technology, Stockholm, SwedenA model, correlating well with measurements, for pulseampli�cation in �ber ampli�ers was developed. �emodel suggests that pumping techniques and the seed’scarrier wavelength can be used to optimize the ampli�edpulse’s duration.
CJ-P.16 WEDCoherent Combining Of Single-Mode Pulses In ARing Cavity�I. Lobach1, S. Kablukov1, E. Podivilov1,2, A. Fotiadi3,4,and S. Babin1,2; 1Institute of Automation and Elec-trometry of SB RAS, Novosibirsk, Russia; 2NovosibirskState University, Novosibirsk, Russia; 3Serviced’Electromagnétisme et de Télécommunications, Mons,Belgium; 4Ulyanovsk State University, Ulyanovsk, RussiaWe demonstrate a new passive method of short pulsegeneration outside a laser cavity – combining of single-mode frequency pulses in an external cavity. A superpo-sition of 18 modes yields a train of nanosecond pulses.
CJ-P.17 WEDHigh Power Brightness Converter Realized By AMulti-Wavelengths Pumped Yb-Doped FiberAmpli�er�N.Haarlammert1, A. Liem1, C.Matzdorf2, T. Schreiber1,R. Eberhardt1, A. Tünnermann1,2, R. Koch3, H. Fritsche3,B. Kruschke3, A. Grohe3, and W. Gries3; 1Fraunhofer In-stitute for Applied Optics and Precision Engineering, Jena,Germany; 2Friedrich Schiller University Jena, Institute ofApplied Physics, Jena, Germany; 3DirectPhotonics Indus-tries GmbH, Berlin, GermanyA brightness enhancer based on multi-wavelengthsdiode-pumped �ber ampli�ers is presented. �e systemlinks together scalability of diode lasers and beamqualityof �ber ampli�ers, resulting in compact, high brightnesssystems with fast modulation capability.
CJ-P.18 WEDLarge-aperture erbium �uorozirconate glass-chipampli�ers and lasers�D.G. Lancaster1,2, Y. Li3, Y. Duan4, M.W. Withford4,and T.M. Monro1,2; 1University of South Australia, Ade-
laide, Australia; 2University of Adelaide, Adelaide, Aus-tralia; 3Maptek, Pty Ltd, Adelaide, Australia; 4MacquarieUniversity, Sydney, AustraliaWe report a large-aperture, erbium active, ytterbium-cerium co-doped �uorozirconate glass waveguide writ-ten via ultra-fast laser inscription. Con�gured as an am-pli�er the gain is 4.3 dB/cm (1545 nm); laser operationachieves 32% slope e�ciency.
CJ-P.19 WED1.7-GHz Intra-burst Repetition Rate Yb-FiberAmpli�er System�H. Kalaycioglu, P. Elahi, C. Kerse, D.K. Kesim, Ö.Akçaalan, and F.Ö. Ilday; Bilkent University, Ankara,TurkeyWe present all-�ber ultrafast Yb ampli�er that can pro-duce 20 ns long bursts of 175 �J repeated at 1 kHz, within-burst pulse repetition rate of 1.7 GHz, built to inves-tigate ultrafast material processing.
CJ-P.20 WEDBurst shaping in pico-second �ber lasers�R. Petkovšek1, J. Petelin2, and B. Podobnik2; 1Universityof Ljubljana, Ljubljana, Slovenia; 2LPKF Laser and Elec-tronics d.o.o., Naklo, Slovenia�eoretical model for burst shaping in �ber lasers is pre-sented. �e model is used to obtain input burst shapethat results in a �at output burst and is experimentallyevaluated in a four-stage �ber ampli�er.
CJ-P.21 WEDAnomalous RIN Transfer Figure in Random RamanLasers�J. Nuño and J.D. Ania-Castañón; Instituto de Óptica”Daza de Valdés”, IO-CSIC, Madrid, SpainWe show that under certain conditions, RIN transfer inrandom Raman �bre lasers can be highest for an inter-mediate frequency band, with potential impact on am-pli�cation applications. �e physical mechanisms be-hind this behaviour are analysed.
CJ-P.22 WEDImproved Low-loss Hollow Core Anti-ResonantSilica Mid-IR Fibers�M.S. Habib, O. Bang, and M. Bache; DTU Fotonik, De-partment of Photonics Engineering, Technical Universityof Denmark, DK-2800, Kgs. Lyngby, Denmark, Lyngby,DenmarkAn improved hollow core anti-resonant �ber with recordlow loss in the mid-IR regime is presented. Simulationresults promise to yield record minimum leakage andbending loss of about 0.0002 dB/km and 0.001 dB/kmrespectively.
CJ-P.23 WEDMono-Layer Graphene Saturable Absorbers withGreatly Enhanced Graphene-Evanescent FieldInteraction for Stable Passive Mode-Locking ofAll-Fibre LaserN.H. Park, H. Jeong, S.Y. Choi, M.H. Kim, J.-Y. Park, F.Rotermund, and �D.-I. Yeom; Department of Physics &Department of Energy Systems Research, Ajou University,Suwon, Korea, SouthWe demonstrate highly e�cient in-line mono-layergraphene saturable absorbers exhibiting large modula-tion depth and low scattering loss based on enhancedevanescent �eld interaction by employing over-claddingstructure for stable �bre laser mode-locking at highpower.
CJ-P.24 WEDActive Q-switching in Raman �ber laser with randomdistributed feedback�S. Babin1,2, A. Kuznetsov1, and E. Podivilov1,2; 1Instituteof Automation and Electrometry SB RAS, Novosibirsk,Russia; 2Novosibirsk State University, Novosibirsk, RussiaWe have demonstrated an actively Q-switched Raman�ber laser based on modulated loop-mirror feedbackand constant distributed feedback via Rayleigh backscat-tering. �e theory explaining the results has been devel-oped. Principal characteristics and advantages are dis-cussed.
CJ-P.25 WEDClustering and up-conversion e�ects in an Er3+:Yb3+co-doped fused silica �bre: A comparison betweenexperiment and models�M. Steinke1,2, D. Kracht1,2, J. Neumann1,2, and W.Peter1,2; 1Laser Zentrum Hannover e.V., Hannover, Ger-many; 2Centre forQuantum-Engineering and Space-TimeResearch - QUEST, Hannover, GermanyTo prove their validity, a stochastic model for the up-conversion and a model for the pair induced quench-ing have been compared to experimental slopes of anEr3+:Yb3+ co-doped silica �bre ampli�er.
CJ-P.26 WEDNonlinear Management of Fiber Oscillator withMultiple Gain Segments�T. Teamir1 and F. Ilday1,2; 1Bilkent University, De-partment of Physics, Ankara, Turkey; 2Bilkent Univer-sity, Department of Electrical and Electronics Engineer-ing, Ankara, TurkeyWe implement nonlinearity management in an oscilla-tor with two gain segments. Preliminary results sug-gest pulse evolution subject to an e�ective negativenonlinearity arising from the complex interaction oflarge chirp, gain �ltering, dispersion and self-phase-modulation.
CJ-P.27 WEDCMOS-Compatible High Index ContrastYtterbium-Doped Tantalum Pentoxide RibWaveguide Lasers�A. Aghajani1, G. Senthil Murugan1, N. Sessions1, V.Apostolopoulos2, and J. Wilkinson1; 1Optoelectronics Re-search Centre, University of Southampton, Southampton,United Kingdom; 2School of Physics and Astronomy, Uni-versity of Southampton, Southampton, United KingdomYtterbium-doped materials are common gain media inhigh performance laser systems. In this work we presenta Yb:Ta2O5 rib waveguide laser fabricated using CMOStechnology, with a cavity formed a�xing mirrors on theend facets.
CJ-P.28 WEDAcoustic and thermal e�ects in Brillouin RandomFiber Laser�A. Fotiadi1,3,4, I. Lobach2, and P. Mégret1; 1Universityof Mons, Mons, Belgium; 2Institute of Automation andElectrometry RAS, Novosibirsk, Russia; 3Io�e Physical-Technical Institute, St Petersburg, Russia; 4UlyanovskState University, Ulyanovsk, RussiaWe obseved competition between Brillouin scatteringand Brillouin lasing in long �bers driven by externalacoustic and temperature noise. �emodel of Brillouin -Rayleigh lasing process taking into account the environ-ment noise is developed.
CJ-P.29 WEDCladding Shaping of Optical Fiber Preforms via CO2Laser Machining�P. Shardlow, R. Standish, J. Sahu, and W.A. Clarkson;Optoelectronics Research Centre, Southampton, UnitedKingdomCO2 laser machining of silica preforms to providecladding shaping for double clad �bers is reported. Sig-ni�cant improvements in speed, automation, novel ge-ometry �exibility and removal of further �re polishingrequirements are demonstrated.
CJ-P.30 WEDHigh Power Spectrally-Tailorable�ulium-DopedFibre Ampli�ed Spontaneous Emission Source�A. Billaud, P. Shardlow, A. Butler, D. Jain, J. Sahu,and W.A. Clarkson; Optoelectronics Research Centre,Southampton, United KingdomAll �ber ampli�cation of a 2�m thulium-doped �bersource with a novel resonator architecture that producesampli�ed spontaneous emission output with spectralshape that can be tailored in an arbitrary manner is re-ported.
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HALL B0CJ-P.31 WED10 �J 150 fs All-Fiber Yb Laser Ampli�er System�O. Akcaalan, H. Kalaycioglu, D.K. Kesim, and F.O. Ilday;Bilkent University, Ankara, TurkeyWe present a monolithic Yb �ber laser ampli�er systemwhich is able to produce pulses of 10 �J compressible to150 fs, a record level for an all-�ber system built by com-mercially available components.
CJ-P.32 WEDMode-Locked Tm-Doped Fiber Lasers Based onHighly Ge-Doped Fibers�D. Klimentov, V. Dvoyrin, and I. Sorokina; NorwegianUniversity of Science and Technology, Trondheim, Nor-wayWe report three con�gurations of the SESAM mode-locked, linear-cavity femtosecond �ber MOPA operat-ing in the anomalous, nearly zero and normal dispersionregimes at around 1.88 �m based on a highly Ge-doped�ulium-doped normal dispersion �ber.
CJ-P.33 WED1180nm Bi-doped Aluminosilicate Fiber Ampli�er�N.K. �ipparapu, S. Jain, A. Umnikov, P. Barua, and J.Sahu; University of Southampton, Southampton, UnitedKingdomWe demonstrate for the �rst time 1120nm laser-diodepumped Bi-doped alumino-silicate �ber ampli�er at1180nm. �e ampli�er performance on pump wave-length was studied. 70% gain improvement was achievedwith 1120nm pumping, compared to 1047nm pump.
CJ-P.34 WEDPassive Mode-locked and SwitchableMultiwavelength Laser based on As2S3-PMMAMicrowires�A. Al-kadry1, M. El-Amraoui2, Y. Messaddeq2, and M.Rochette1; 1McGill University, Montreal, Canada; 2LavalUniversity, Québec City, CanadaWe demonstrate a passive mode-locked and spacing-switchable multiwavelength �ber laser using a 10cmlong As2S3-PMMA microwire. �e laser is based onnonlinear-polarization-rotation e�ect and provides twodi�erent operation regimes of pulse generation andmul-tiwavelength emissions.
CJ-P.35 WEDAll-normal-dispersion, all-PM-�bre laser at 1060 nmmode-locked with a nonlinear amplifying loopmirror�P.G. Bowen, H. Singh, A.F.J. Runge, and N.G.R. Brod-erick; Dodd-Walls Centre and Physics Department, �eUniversity of Auckland, Auckland, New ZealandWe report an all-normal-dispersion, all-�bre, all-PM,
laser operating at a central wavelength of 1060 nm. �elaser, mode-locked using a nonlinear amplifying loopmirror, generates linearly polarised pulses that can becompressed to 360 fs.
CJ-P.36 WEDGeneration of controlled optical spectra using phasemodulation and suppression of Stimulated Brillouinscattering�H.Achar and J. Nilsson;Optoelectronics ResearchCentre,University of Southampton, Southampton, United King-domAn arbitrary waveform generator drives a phasemodula-tor which broadens a single-line laser. �e periodic drivesignal is optimized to yield an optical spectrum suitablefor suppression of stimulated Brillouin scattering in anoptical �ber.
CJ-P.37 WEDDevelopment of high energy femtosecond �ber laserby all �ber coherent beam combining technology�Y. Kambayashi, M. Yoshida, T. Inoue, andM. Yoshikawa;Kinki University, Osaka, JapanWe have developed a novel all �ber coherent beam com-bining (CBC) system to scale up energies of femtosec-ond laser pulses. Our system has achieved a beam-combining e�ciency of 97.5% without �uctuations ofcombined powers.
CJ-P.38 WEDDevelopment of Multi-Color Visible Short PulseGlass Fiber Laser�S. Kajikawa1, Y. Fujimoto2, M. Yoshida1, O. Ishii3, andM. Yamazaki4; 1Fasility of Science and Engineering, KinkiUniversity, Higashi-Osaka, Japan; 2Institute for Laser En-gineering, Osaka University, Suita, Japan; 3ProductionEngineering Section, Optical Glass Productrion Depart-ment, Sumita Optical Glass, Minamiaizu-gun, Japan;4Glass Research Division, R&D Department, Sumita Op-tical Glass, Saitama, JapanWe demonstrated a multicolor (blue, green, orange, andred) ns-laser pulse generation in a Pr-doped waterproof�uoride glass �ber pumped by InGaN laser diodes. Agraphene thin �lm was used as a switching device.
CJ-P.39 WEDAll-�ber Picosecond Optical Pulse Generator Basedon Self-phase Modulation E�ect and SpectralFiltering using Narrowband FBG�J. Želudevičius, J. Petkelis, K. Regelskis, and G.Račiukaitis; Center for Physical Sciences & Technology,Vilnius, LithuaniaWe present experimental results of all-�ber picosecondpulse generator scheme based on self-phase modula-
tion e�ect and spectral �ltering using narrowband �berBragg gratings. Generation of pulses with duration of26ps and >3nJ energy is demonstrated.
CJ-P.40 WEDOptimal Order of Intra-Cavity Devices in RingCavity Fiber Lasers�O. Shtyrina1,2, I. Yarutkina1,2, A. Skidin1,2, M.Fedoruk1,2, and S. Turitsyn2,3; 1Novosibirsk State Uni-versity, Novosibirsk, Russia; 2Institute of ComputationalTechnologies SB RAS, Novosibirsk, Russia; 3Aston In-stitute of Photonic Technologies, Birmingham, UnitedKingdomWe study the impact of the intra-cavity elements orderon the output pulse energy in the all-normal ring �berlaser and�nd through intensive numericalmodelling theoptimal con�gurations with the highest energy.
CJ-P.41 WEDNarrowing the Linewidth of Yb:YAGWaveguideLasers Fabricated by Ultrafast Laser InscriptionP. Dekker1, �M. Ams1, T. Calmano2, S. Gross1, C.Kränkel2, G. Huber2, andM.Withford1; 1Macquarie Uni-versity, Sydney, Australia; 2Universität Hamburg, Institutfür Laser-Physik, Hamburg, GermanyWe report on the hybrid integration of a femtosecondlaser written Yb:YAG waveguide coupled to a passivewaveguide Bragg grating resulting in narrowed laseremission and single-ended laser output.
CJ-P.42 WEDSingle mode fused �ber couplers for high powerlasers and ampli�ers�C. Ottenhues1, T. �eeg1,2, K. Hausmann1,2, H.Sayinc1,2, J. Neumann1,2, and D. Kracht1,2; 1LaserZentrum Hannover e.V., Hannover, Germany; 2Centrefor Quantum Engineering and Space-Time Research(QUEST), Hannover, GermanyWe report a high power single mode fused �ber couplerwith a total power handling of 210 W for multiplexingdi�erent wavelengths. It can also be used as broadband�lter for ampli�ed spontaneous emission suppression.
CJ-P.43 WEDOptical pulse shaping by modulated Brillouin gain ina tellurite �berD. Deng, K. Nagasaka, T. Cheng, X. Xue, T. Suzuki, and�Y. Ohishi; Research Center for Advanced Photon Tech-nology, Toyota Technological Institute, Nagoya, JapanTunable all-optical �ne control of pulse width with astretching ratio of 1.17-0.36 accompanying a time delayvia doublet Brillouin gain lines was demonstrated in ashort 204-m-long nonlinear single-mode tellurite �ber.
CJ-P.44 WEDHo-doped �ber ampli�er of the weak signal at 2.1micron�V. Kamynin1,2, S. Antipov3, A. Baranikov4, and A.Kurkov1,2; 1Prokhorov General Physics Institute, RAS,Moscow, Russia; 2Photonics Laboratory of Perm Scienti�cCenter, Ural Branch, RAS, Perm, Russia; 3Departmentof Physics and Astronomy, Macquarie University, Sydney,Australia; 4Moscow Institute of Physics and Technology),Dolgoprudnyi, RussiaA small-signal holmium-doped�bre ampli�er is demon-strated. �e seed source is a cw holmium-doped �brelaser whose output power is modulated by an electro-optical modulator. �e maximum gain reached is 28.5dB.
CJ-P.45 WEDExperimental observation of tunable third-harmonicgeneration in a tellurite microstructured optical �ber�T. Cheng1, D. Deng1, X. Xue1, M. Matsumoto2, H.Tezuka2, T. Suzuki1, and Y. Ohishi1; 1Toyota Techno-logical Institute, Nagoya, Japan; 2Furukawa Denshi Co.,Tokyo, JapanWidely THG from 567 to 902 nmwas obtained when thetellurite microstructured optical �ber was pumped by anoptical parametric oscillator with the pump wavelengthchanging from 1700 to 2700 nm.
CJ-P.46 WEDGeneration of 80 W, 38 fs ultrashort pulse from aself-similar Yb-�ber ampli�erJ. Zhao, W. Li, Y. Liu, C. Wang, and �H. Zeng; East ChinaNormal University, Shanghai, China, People’s Republic of(PRC)We have demonstrated 38-fs laser pulse with 80-W aver-age power from a self-similar ampli�er. A broad spectralbandwidth of 104 nm (10-dB bandwidth) is achieved.
CJ-P.47 WEDDevelopment of Low Photo-Darkening Yb-DopedSilica Glass Fiber by Co-Doping of Group 2 Element�Y. Sakaguchi1, Y. Fujimoto1, M. Masuda1, N.Miyanaga1, and H. Nakano2; 1Institute of Laser En-gineering, Osaka University, Osaka, Japan; 2Faculty ofScience and Engineering, Kinki University, Osaka, JapanWe found that co-doping of group 2 element e�ectivelysuppresses the photo-darkening e�ect in Yb-doped silicaglass �ber.Mg co-doped Yb-doped silica �ber can workas a photo-darkening free over 50000 ppm of Yb concen-tration.
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HALL B0CJ-P.48 WEDRecord E�ciency kW-level Peak PowerSingle-frequency Er-doped Fiber Ampli�er�L. Kotov1,2, M. Likhachev1, M. Bubnov1, D. Lipatov3,4,and A. Guryanov3; 1Fiber Optics Research Center RAS,Moscow, Russia; 2Moscow Institute of Physics and Tech-nology, Dolgoprudny, Russia; 3Institute of Chemistry ofHigh Purity Substances RAS, Nizhny Novgorod, Rus-
sia; 4Lobachevsky State University of Nizhnii Novgorod,Nizhny Novgorod, RussiaWe present kW-peak power single-mode single-frequency Er-doped all-�ber ampli�er with a recordelectrical-to-optical conversion e�ciency of 8 %
CJ-P.49 WEDLaser emission in Yb3+ doped SiO2-ZrO2nanostructured optical �ber synthetized by thechemical sol-gel “inverse dip-coating” approach�G. Granger1, C. Restoin2, P. Roy2, R. Jamier2, S.Rougier2, A. Lecomte3, B. Beaudou4, and J.-M. Blondy2;1Institut für Strahlwerkzeuge (IFSW), Stuttgart, Ger-many; 2Xlim Research Institut UMR-CNRS n� 7252,
Limoges, France; 3SPCTS UMR-CNRS n� 7315, Limoges,France; 4GLOphotonics, Limoges, FranceWe report the microstructural and optical characteriza-tions of passive and ytterbium doped SiO2-ZrO2 nanos-tructured �bers. �e optimization of the chemical syn-thesis leads to e�cient laser emissions at 980 nm under915 nm pumping.
13:00 – 14:00EB-P: EB Poster SessionEB-P.1 WEDGeneration of general EPR-states on-chip�M. Gräfe, R. Heilmann, S. Nolte, and A. Szameit; In-stitute of Applied Physics, Abbe Center of Photonics,Friedrich-Schiller-Universität, Jena, GermanyWe present a novel method for generating arbitrarypath-encoded EPR-states on-chip by means of one sin-gle operation only. Such states can be exploited to mimicthe quantum statistics of fermions, bosons, and anyons.
EB-P.2 WEDCross-Phase Modulation in Gradient Echo Memoryusing Stationary Light�P. Vernaz-Gris1,2, J. Everett1, D. Higginbottom1, G.Campbell1, B. Buchler1, and P.K. Lam1; 1Centre forQuantum Computation and Communication Technology,�e Australian National University, Canberra, Australia;2Laboratoire Kastler Brossel, UPMC-Sorbonne Univer-sités, CNRS, ENS-PSL Research University, Collège deFrance, Paris, AustraliaWe study stationary light in a gradient echo memoryfor the enhancement of cross-phasemodulation betweenstored electric �elds. We present numerical simulationsthat support using a two-colour bidirectional control�eld.
EB-P.3 WEDGeneral Biphoton Time-bin Qutrit Generation andComplete Characterization for Hybrid QuantumInformation Processing�M. Fuwa1, T. Tohyama1, S. De Leseleuc1, J.-i.Yoshikawa1, S. Takeda2, P. van Loock3, and A.Furusawa1; 1�e University of Tokyo, Tokyo, Japan;2Institute for Molecular Science, Okazaki, Japan;3Johannes-Gutenberg Universität Mainz, Mainz, Ger-manyWe generate and fully characterize representatives ofbiphoton 2-mode time-bin qutrits compatible with ho-modyne measurements as a �rst step towards encodinga logical qubit into multi-photon superpositions manip-ulable with continuous-variable technologies.
EB-P.4 WEDA Di�erential Phase-Shi� Scheme for QKD inMulti-user Telecom Networks�M.Hentschel, A. Poppe, E. Querasser, R. Lieger, M. Peev,and B. Schrenk; Austrian Institute of Technology, Vienna,AustriaWe propose a scheme for quantum key distribution in apassive optical network based on di�erential phase shi�coding. A centralized station includes all expensive com-ponents, making it suitable for multi-user networks inlocal environments.
EB-P.5 WEDExperimental demonstration of multi-userentanglement distribution�J. Trapateau1, J. Ghalbouni2, E. Diamanti1, and I.Zaquine1; 1CNRS/ LTCI, Télécom Paristech, Paris,France; 2Université Libanaise, Beyrouth, LebanonEntanglement distribution based on double path SPDCin a PPLN crystal with a Michelson interferometer andphoton pair splitting with a commercial demultiplexerat telecom wavelength centered on ITU channel 24 hasbeen experimentally demonstrated.
EB-P.6 WEDSimulating quantum optical networks with ultrafastpulse shaping�Y. Cai, J. Roslund, C. Fabre, and N. Treps; Labora-toire Kastler Brossel, UPMC-Sorbonne Universités, CNRS,ENS-PSL Research University, Collège de France,, Paris,FranceWepresent on-demand quantum-network constructionsvia arbitrary shaping within the measurement process.Multimode entanglement is embedded within an opticalfrequency comb, and pulse shaping is used to simulateany photonic architecture.
EB-P.7 WEDA Photon-Photon Controlled-Phase Gate Using a ΛSystem�Y. Tokunaga1 and K. Koshino2; 1NTT Secure PlatformLaboratories, Tokyo, Japan; 2Tokyo Medical and DentalUniversity, Tokyo, Japan
We propose a scheme for implementing a photon-photon controlled-phase gate between polarizationqubits using a Λ-type atom, where the atom is used to-tally passively. It is also applicable to the photonic qubitsencoded in frequency.
EB-P.8 WEDDetecting Entanglement in Multipartite FrequencyEntangled Gaussian States�S. Gerke1, J. Sperling1, W. Vogel1, Y. Cai2, J. Roslund2, N.Trepes2, and C. Fabre2; 1Institut fur Physik, UniversitatRostock, Rostock, Germany; 2Laboratoire Kastler Brossel,Universite Pierre et Marie Curie, Paris 6, Paris, FranceMultimode radiation �elds may exhibit a variety of en-tangled partitions. We demonstrate a full entanglementanalysis of all non-trivial 115974 partitions for an exper-imentally prepared 10 mode frequency comb Gaussianstate.
EB-P.9 WEDSwitching on entanglement through local noiseA. Orieux1, �M.A. Ciampini1, P. Mataloni1, D. Bruß2, M.Rossi3, and C. Macchiavello3; 1Dipartimento di Fisica,Sapienza Università di Roma, Roma, Italy; 2Institut für�eoretische Physik III, Heinrich-Heine-Universität Düs-seldorf, Düsseldorf, Germany; 3Dipartimento di Fisicaand INFN-Sezione di Pavia, Pavia, ItalyWe show how entanglement can be turned on via a localnoisy device. We discuss two and four-qubit protocols inwhich an amplitude damping channel is used to produceentanglement starting from uncorrelated photons.
EB-P.10 WEDOptimization strategies in measurement-basedquantum computation�F. Arzani; Laboratoire Kastler Brossel, Paris, FranceWe show that optimizing the measured basis allows tomitigate imperfections due to �nite squeezing in thecluster-based model or to �nd the best possible compu-tation result using other entangled resource states.
EB-P.11 WEDHigh Capacity Fibonacci Protocol for Quantum KeyDistribution - Engineering Entangled States inHigh-Dimensional Hilbert Space�A. Sergienko1, D. Simon2, C. Fitzpatrick1, and O.Minaeva1; 1Boston University, Boston, United States;2Stonehill College, Easton, United StatesWe develop a novel approach to increased informationcapacity in quantum key distribution by means of al-gorithmic coding in high-dimensional Hilbert space, bymaking use of recurrent algebraic constructions such asthe Fibonacci sequence.
EB-P.12 WEDFast and e�cient state detection of single trappedatoms�K. Redeker1, D. Burchardt1, N. Ortegel1, R. Gartho�1,W. Rosenfeld1,2, and H. Weinfurter1,2; 1Ludwig-Maximilians-Universität, München, Germany; 2Max-Planck-Institut für Quantenoptik, Garching, GermanyFast and e�cient quantum measurements are essentialfor many applications in modern quantum technology.We present the experimental realization of an atomicstate detection for single atoms, based on photoioniza-tion and detection of ionization fragments.
EB-P.13 WEDCavity Quantum Electrodynamics with QuantumDots in MicrocavitiesM.P. Bakker1, A.V. Barve2, T. Ruitenbeek1, W. Lö�er1,L.A. Coldren2, D. Bouwmeester1,2, and �M.P. Van Exter1;1Huygens-Kamerlingh Onnes Laboratory, Leiden, �eNetherlands; 2University of California Santa Barbara,Santa Barbara, United StatesSingle quantumdots embedded in high-�nesse semicon-ductor microcavities are studied with resonant re�ec-tion and transmission spectroscopy. We demonstrate:polarization-resolved inspection of neutral and chargedstates, coherence measurements, and nonlinearity andhysteresis at larger injection power.
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CLEO®/Europe-EQEC 2015 ⋅ Wednesday 24 June 2015
HALL B013:00 – 14:00EH-P: EH Poster Session
EH-P.1 WEDTuning of multipole meta-atom response�M. Wenclawiak, J. Karaman, C. Hartl, K. Unterrainer,and J. Darmo; Vienna University of Technology, Vienna,AustriaMulti-pole type of meta-atoms is studied with respect tothe control of resonances. We used capacitive couplingand asymmetry for the normal mode splitting control upto 50% of the nominal value.
EH-P.2 WEDImaging and coupling plasmons to metallic selforganized crystalG. Binard1, C. Lethiec1, H. Frederich1, E. Yroala2, C.Schwob1, F. Charra3, L. Coolen1, and �A. Maitre1;1Institut des Nanosciences de Paris, Paris, France;2Universita Autonoma de Madrid, Madrid, Spain; 3Lydil,CEA, IRAMIS, Saclay, FranceFor a plasmonic crystal, e�cient coupling of light to plas-mons is demonstrated and imaged by Photo EmissionElectron Microscopy. For nanocrystals deposited at sur-face, increase of luminescence due to SPP coupling isquanti�ed.
EH-P.3 WEDFanned-out Plasmonic Waveguide Array forSubwavelength Line Imaging�N. Podoliak1, P. Horak1, J.C. Prangsma2, and P.W.H.Pinkse2; 1Optoelectronics Research Centre, University ofSouthampton, Southampton, United Kingdom; 2MESA+Institute for Nanotechnology, University of Twente, En-schede,�e NetherlandsWe design an array of air-guided plasmonic waveguidesfor high-resolution line imaging. With a coupling ef-�ciency of up to 90%, moderate losses and negligiblecross-talk, a resolution of λ/15 is demonstrated at near-infrared wavelengths.
EH-P.4 WEDColorimetric sensing using Fourier plane imaging ofsurface plasmons�P. Arora andA. Krishnan;Department of Electrical Engi-neering, Indian Institute of Technology Madras, Chennai,IndiaWe demonstrate simultaneous refractive index andthickness sensing using dark �eld Fourier plane imagingof surface plasmons for sub-wavelength thin �lms coatedon fabricated 1D and 2D plasmonic nanostructures.
EH-P.5 WEDPlasmonic nanostars as e�cient broadband scatterersfor random lasing�J. Ziegler, C. Wörister, C. Vidal, C. Hrelescu, and T.A.Klar; Institute of Applied Physics, Johannes Kepler Uni-versity Linz, Linz, AustriaWide spectral coverage of random lasing throughout thewhole visible range up to the near-infrared is demon-strated with star-shaped gold nanoparticles as broad-band scatterers for a variety of laser dyes.
EH-P.6 WEDTamm surface modes vs. surface plasmons inmetal-terminated 3-dimensional photonic crystals�S. Romanov1,4, A. Korovin2, and U. Peschel1,3;1University of Erlangen-Nuremberg, Erlangen, Germany;2Laboratoire de Génie Electrique de Paris, Paris, France;3FSU Jena, Jena, Germany; 4Io�e Physical TechnicalInstitute, St. Petersburg, RussiaTamm surface modes were for the �rst time studied inmetal �lm-terminated 3-dimensional photonic crystals.Compared to surface plasmon polaritons, these modesare more robust and allow for more e�cient tuning ofthe optical response.
EH-P.7 WEDAnalysis and Modeling of Metamaterial Absorbers�P. Bowen; Duke University, Durham, United StatesWe present a fully analytical model that describes idealabsorbing metasurfaces composed of �lm-coupled opti-cal nanoantennas. �e model predicts the spectrum andthe angular dependence of the absorption and is com-pared to full-wave numerical simulations.
EH-P.8 WEDPhase matching in layered hyperbolic metamaterials�C. de Sterke1,2, C. Duncan1, L. Perret2, S. Palomba2,M. Lapine1, and B. Kuhlmey1,2; 1Centre for Ultrahighbandwidth Devices for Optical System (CUDOS), Schoolof Physics, University of Sydney, Australia; 2Institute ofPhotonics and Optical Science (IPOS), School of Physics,University of Sydney, AustraliaWe �nd that hyperbolic metamaterials, which can sup-port propagating waves with arbitrarily large wavevec-tors, can phase match nonlinear frequency conversionprocesses that cannot be phase matched conventionally.We also consider the e�ect of Ohmic losses.
EH-P.9 WED50-fold SHG enhancement in RbTiOPO4 nonlinearcrystals by aggregates of silver nanostructures�L. Sánchez-García1, P. Molina1, M. Ramírez1, J.J.Carvajal2, M. Aguiló2, F. Díaz2, C. Heras1, and L.Bausá1; 1Dept. Física de Materiales and Instituto Nico-
las Cabrera, Universidad Autónoma de Madrid, Madrid,Spain; 2Física i Cristallogra�a de Materials, UniversitatRovira i Virgili, Tarragona, SpainAg nanostructures with plasmonic modes in the visible-NIR range are obtained on a nonlinear crystal. 50-foldenhancement of the blue SHG is achieved when the lo-calized surface plasmon is resonant with the fundamen-tal beam.
EH-P.10 WEDEnhancing LSP-mediated SHG conversion e�ciencywith NLO polymer�A. Sugita, T. Hirabayashi, S. Nihashi, A. Ono, and Y.Kawata; Shizuoka University, Hamamatsu, JapanWewill present LSP-mediated SHG fromNLO polymer-coated Au nanorods. �e 3.5-fold enhancement in theSHG conversion e�ciencies was involved by properlytuning the LSP resonance frequency to the NLO poly-mer’s transition frequency.
EH-P.11 WEDStrong enhancement of second-harmonic generationfrom silver nanoisland �lms through titaniumdioxide coating�K. Koskinen1, S. Chervinskii2,3, R. Czaplicki1, A.Lipovskii2,4, and M. Kauranen1; 1Tampere University ofTechnology, Tampere, Finland; 2St. Petersburg State Poly-technic University, St. Petersburg, Russia; 3University ofEastern Finland, Joensuu, Finland; 4St. Petersburg Aca-demic University, St. Petersburg, RussiaA nanolayer of titanium dioxide on a silver nanois-land �lm enhances second-harmonic generation fromthe nanoislands by a factor of 40 through tuning of theplasmon resonance close to the second-harmonic wave-length.
EH-P.12 WEDSecond Harmonic in Plasmonic Lithium NiobateWaveguides�V. Ng1,3, A. Boes2,3, A. Warrier1, J. Lin1, D. Spence1,A. Mitchell2,3, J. Downes1, D. Coutts1,3, and J. Dawes1,3;1MQ Photonics, Department of Physics and Astronomy,Macquarie University, Sydney, Australia; 2School of Elec-trical andComputer Engineering, RMIT,Melbourne, Aus-tralia; 3Centre for Ultrahigh bandwidth Devices and Op-tical Systems (CUDOS), Sydney, AustraliaGeneration of second harmonic plasmons in aair/gold/lithium niobate planar waveguide shows di-rect experimental evidence of a nonlinear plasmonicinteraction.
EH-P.13 WEDWire array metamaterial �bers based on so�-glass�J.G. Hayashi1, R. Lwin1, S. Fleming1, B.T. Kuhlmey1,2,
and A. Argyros1; 1IPOS, School of Physics, University ofSydney, Sydney, Australia; 2CUDOS, School of Physics,University of Sydney, Sydney, AustraliaWe fabricated tin/soda-limewire arraymetamaterials forthe MIR using �ber drawing, achieving wires 200 nmin diameter, ten times smaller than previous work. Nu-merical simulations show promising losses for use in theMIR.
EH-P.14 WEDAmetamaterial inspired microwave antenna designfor coplanar waveguides�L. Maple1, G. Stenning1,2, G. Bowden1, S. Berry1, P. deGroot1, andV. Apostolopoulos1; 1University of Southamp-ton, Southampton, United Kingdom; 2ISIS Pulsed Neu-torn and Muon Source, Didcot, United KingdomWepresent a hybridmetamolecule based on the �shscaleand split-ring resonator (SRR) designs. We demonstrateexperimentally that the SRRs enhance the �shscale res-onance, and modelling suggests antenna emission withapproximately 5.9 dBi gain.
EH-P.15 WEDSingular ampli�cation of light in non-normalstructures�K. Makris1,2, L. Ge3,4, S. Rotter1, and H. Tureci2;1Vienna University of Technology, Vienna, Austria;2Princeton University, Princeton, United States; 3Collegeof Staten Island, CUNY, New York, United States;4Graduate Center, CUNY, New York, United StatesWe study the e�ect of singular ampli�cation of light incoupled systems of optical waveguides that are com-posed of gain and loss. Singular values capture thephysics of transient ampli�cation.
EH-P.16 WEDChiral modes in 2D PT-symmetric nanostructures�M. Botey1, R. Herrero1, M. Turduev2, I. Giden2, H.Kurt2, and K. Staliunas2,3; 1Universitat Politècnica deCatalunya (UPC), Terrassa (Barcelona), Spain; 2TOBBUniversity of Economics and Technology, Ankara, Turkey;3Institució Catalana de Recerca i Estudis Avançats(ICREA), Barcelona, SpainWe propose a simple realistic 2D PT-symmetric pho-tonic structure from basic physical considerations. �estructure supports Bloch-like modes with opposite chi-rality, being its excitation input dependent, and holdsasymmetric transmission between in- and out-couplingchannels.
EH-P.17 WEDParity-Time Symmetry in Diluted Arrays of SplitRing Resonators�J.L. Garcia-Pomar1, C.Mejia-Cortes2, andM.I.Molina2;
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NOTES
CLEO®/Europe-EQEC 2015 ⋅ Wednesday 24 June 2015
HALL B01Institute of Optics (CSIC), Madrid, Spain; 2University ofSantiago, Santiago, ChileWe study the Parity-Time Symmetry in diluted arrays ofsplit ring resonators, showing the stability zone wherethe PT symmetry is unbroken; we calculate transmissionand re�ection of these systems and their dynamics.
EH-P.18 WEDParity-Time coupled microresonators:Kramers-Kronig limitation�S. Phang1, A. Vukovic1, S. Creagh2, T. Benson1, P.Sewell1, and G. Gradoni2; 1George Green Institute forElectromagnetics, Nottingham, United Kingdom; 2School
of Mathematical Sciences, Nottingham, United Kingdom�e paper demonstrates how realistic material modelbased on Kramers-Kroning relationships a�ects designrequirements for parity-time coupled microresonators.
E�ects of unbalancing gain and loss in this realisticscenario is also investigated.
175
CLEO®/Europe-EQEC 2015 ⋅ Thursday 25 June 2015
ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b8:30 – 10:00CD-11: Optical MicroscopyChair: Gregor Knopp, Paul Scherrer Institute,Villigen, Switzerland
8:30 – 10:00EH-5: Emission Control withNanoantennasChair: Niek van Hulst, ICFO, Barcelona,Spain
8:30 – 10:00CL-2: Fluorescence Imaging andOptical ManipulationChair: Monika Ritsch-Marte, Medical Uni-versity of Innsbruck, Innsbruck, Austria
8:30 – 10:00CJ-11: High-Power CW Fibre LaserSystemsChair: Cesar Jauregui, University of Jena,Jena, Germany
8:30 – 10:00CF-6: Characterization of UltrafastLasersChair: Rüdiger Paschotta, RP Photonics Con-sulting GmbH, Bad Dürrheim, Germany
CD-11.1 THU 8:30Stimulated Raman Scattering Microscopywith a Highly Versatile Fiber-FeedbackOptical Parametric Oscillator�T. Steinle1, V. Kumar2, A. Steinmann1, M.Marangoni2, G. Cerullo2, and H. Giessen1;14th Physics Institute, University of Stuttgart,Stuttgart, Germany; 2IFN-CNR, Diparti-mento di Fisica, Politecnico di Milano, Mi-lano, ItalyWe present a compact femtosecond �ber-feedback OPO featuring precise wavelengthcontrol and Watt-level output tunable from1.4 to 4.2 �m. �e system shows excellentnoise and dri� properties in a StimulatedRa-man scattering experiment.
EH-5.1 THU 8:30Metal-Dielectric Nanoantennas forEnhancement of Directional EmissionE. Rusak1, R. Guo1, �I. Staude1, M. Decker1,J. Sautter1, A. Miroshnichenko1, D. Powell1,I. Brener2, D. Neshev1, and Y. Kivshar1;1Nonlinear Physics Centre and Centre for Ul-trahigh Bandwidth Devices for Optical Sys-tems (CUDOS), Research School of Physicsand Engineering, �e Australian NationalUniversity, Canberra, Australia; 2Centerfor Integrated Nanotechnologies, Sandia Na-tional Laboratories, Albuquerque, UnitedStatesWe suggest a metal-dielectric nanoantenna,consisting of a gold nanorod and a siliconnanodisk, which provides giant enhance-ment of directional emission together withhigh radiation e�ciency. We demonstrateits fabrication by two-step electron-beamlithography.
CL-2.1 THU 8:30Nanophotonic measurement of the darkfraction in red �uorescent proteins�J.C. Prangsma1, R. Molenaar1, V.Subramaniam2, and C. Blum1; 1MESA+institute for nanotechnology, University ofTwente, Enschede, �e Netherlands; 2FOMinstitute for atomic and molecular physics(AMOLF), Amsterdam,�e NetherlandsNanophotonics-enabled quantum e�ciencymeasurements of a range of red �uores-cent proteins show that many of them havea considerable fraction of absorbing, butnot emitting, �uorophores, signi�cantly im-pacting quantitative microscopy and super-resolution experiments.
CJ-11.1 THU 8:30Low noise high power continuous waveMOPA Ytterbium doped �ber lasers at1064nm.�G. Guiraud1,2, R. Dubrasquet1, J. Boullet1,G. Santerelli2, and N. Traynor1; 1Azur LightSystems, Pessac, France; 2Laboratoire Pho-tonique, Numérique et Nanosciences , CNRS,Talence, FranceWe have developed a novel low noise, highe�ciency, high power (50W) continuouswave MOPA Ytterbium doped �ber laser at1064 nm for scienti�c and industrial appli-cations.
CF-6.1 THU 8:30Optimized Ancillae Generation forUltra-broadband Two-dimensionalSpectral Shearing Interferometry�R. Borrego-Varillas, A. Oriana, F. Branchi,G. Cerullo, and C. Manzoni; IFN-CNR, Di-partimento di Fisica, Politecnico di Milano,,Milano, ItalyWe introduce a new scheme which over-comes the challenges of ancillae preparationin traditional spectrally-sheared interferom-etry techniques. �e approach is applied to2DSI and reliably characterizes few-optical-cycle pulses from the UV to the IR.
CD-11.2 THU 8:45Visualizing of ferroelectric domaindynamics in random quadratic mediausing Cerenkov second-harmonicmicroscopy�M. Ayoub, J. Hanisch, J. Imbrock, and C.Denz; Institute of Applied Physics and Cen-ter for Nonlinear Science (CeNoS), Westfälis-che Wilhelms-Universität Münster, Münster,GermanyIn this contribution we use Čerenkov-typesecond-harmonic microscopy to monitorthe ferroelectric domain dynamics in ran-dom nonlinear media. �e measurementsare established in combination with record-ing the conventional hysteresis to determinethe current domain status.
EH-5.2 THU 8:45High directivity multipolar antennas astailored infrared nano thermal emitters.�M. Centini, A. Benedetti, M.C. Larciprete,A. Belardini, R. Li Voti, M. Bertolotti, andC. Sibilia; Sapienza University of Rome, Dept.SBAI, Roma, ItalyWe numerically calculated thermal relativeemissivity and spatial emission pattern ofcoupled nanoantenna ensembles showingthat multipolar contributions can be tailoredin order to produce highly directional ther-mal emissivity in the mid infrared.
CL-2.2 THU 8:45Observation of Atomic Dipole Forces inOptically Trapped NanodiamondsContaining NV Centres, in Liquid�C. Bradac, M. Juan, B. Besga, G. Molina-Terriza, and T. Volz; ARC Centre for Engi-neered Quantum Systems, Macquarie Uni-versity, Sydney, AustraliaWe present the e�ect of resonant forceson the manipulation, in liquid, of opticallytrapped nanodiamonds containing NV cen-tres, where these resonant forces are pro-duced by a laser slightly detuned from theNVs* dipole transition.
CJ-11.2 THU 8:45Novel, High-Brightness, Fibre LaserPlatform for kWMaterials ProcessingApplications�D. Kliner; nLIGHT Corp., Vancouver,United StatesWe report a new �bre laser architecturethat addresses key shortcomings of exist-ing designs, demonstrating 3.5-kW power(pump-power limited), M2 of 3.6 (highestbeam quality of an industrial multi-kW �berlaser), and 100-kHz modulation frequency.
CF-6.2 THU 8:45Generation and SpatiotemporalCharacterization of Ultrashort VortexPulses�M.Miranda, M. Kotur, P. Rudawski, C. Guo,A. Harth, A. L’Huillier, and C.L. Arnold; De-partment of Physics, Lund University, Lund,SwedenWe demonstrate the generation and spa-tiotemporal characterization of ultrashortvortex pulses.�e vortices are created us-ing lithographic spiral phase plates andmea-sured using a recently introduced techniquebased on spatially-resolved Fourier spec-trometry.
CD-11.3 THU 9:00Quadrature-phase modulation inheterodyne-detected coherent Ramanimaging�Y. Obara1, T. Suzuki1,2, M. Kawagishi3,M. Hayashi4, S. Terada3, and K. Misawa1,5;1Department of Applied Physics, Tokyo Uni-versity of Agriculture and Technology, Ko-ganei, Japan; 2Department of Physics, MeijiUniversity, Kawasaki, Japan; 3Departmentof Neuroanatomy and Cellular Neurobiol-
EH-5.3 THU 9:00Ultra-Compact On-chip Spectral-BandDemultiplexing with Plasmonic FanoNanoantennasR. Guo, �M. Decker, F. Setzpfandt, I. Staude,D. Neshev, and Y. Kivshar; Nonlinear PhysicsCentre and Centre for Ultrahigh-bandwidthDevices for Optical Systems (CUDOS), Aus-tralian National University, Canberra, Aus-traliaWe experimentally integrate a single-
CL-2.3 THU (Invited) 9:00Fluorescence lifetime imaging of cellular-level metabolic heterogeneity in cancer�M. Skala; Vanderbilt University, Nashville,United StatesCancer is a heterogeneous disease, and sub-populations of cells can drive drug resis-tance. Fluorescence lifetime imaging ofmetabolic co-factors is used tomonitor drugresponse on a cellular level, to optimize clin-ical treatment decisions.
CJ-11.3 THU 9:001 kW �ber laser oscillator with fs-written�ber Bragg gratings�C. Voigtländer1, R.G. Krämer1, A. Liem2,T. Schreiber2, A. Tünnermann1,2, andS. Nolte1,2; 1Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, Germany;2Fraunhofer Institute for Applied Optics andPrecision Engineering, Jena, GermanyWe present to the best of our knowledge
CF-6.3 THU 9:00Experimental Demonstration ofTemporal Ghost ImagingP. Ryczkowski1, �M. Barbier1, A.T. Friberg2,J.M. Dudley3, and G. Genty1; 1Departmentof Physics, Tampere University of Technology,Tampere, Finland; 2Department of Physicsand Mathematics, University of Eastern Fin-land, Joensuu, Finland; 3Institut FEMTO-ST, UMR 6174 CNRS-Université de Franche-Comté, Besançon, France
176
CLEO®/Europe-EQEC 2015 ⋅ Thursday 25 June 2015
ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN8:30 – 10:00CA-9: Yb3+-doped Solid State-lasersand Ampli�ersChair: �omas Calmano, Institut für Laser-Physik, Universität Hamburg, Hamburg, Ger-many
8:30 – 10:00EA-9: Controlled Light-matterInteractions IChair: Juan Perez Torres, �e Institute ofPhotonic Sciences ICFO, Barcelona, Spain
8:30 – 10:00CB-8: Optical Feedback and OpticalInjectionChair: Dimitris Syvridis, National andKapodestrian University of Athens, Athens,Greece
8:30 – 10:00EF-9: Mechanical Properties ofLight and Self-organisationChair: Gianluca Oppo, University of Strath-clyde, Glasgow, United Kingdom
8:30 – 10:00JSV-1: Photon Pair SourcesChair: Ian Walmsley, University of Oxford,Oxford, United-Kingdom
CA-9.1 THU 8:30160 W 800 fs Laser System without CPAfor High Speed Surface Texturing�V. Markovic, A. Rohrbacher, P. Hofmann,W. Pallmann, S. Pierrot, H. Ammann,and B. Resan; JDSU Ultrafast Lasers AG,Schlieren/Zurich, SwitzerlandWepresent a compact 160W800 fs laser sys-tem without the CPA technique, ideally suit-able for micromachining. �e laser is basedon the Yb:YAG crystal �ber ampli�ers fea-turing 32 dB small signal gain.
EA-9.1 THU 8:30Telecom-Heralded Single Photon Sourcefor Single-Atom, Single-Photon QuantumInterfaces�A. Lenhard, M. Bock, J. Brito, S. Kucera,P. Eich, P. Müller, J. Eschner, and C. Becher;Saarland University, Saarbrücken, GermanyWe report on a narrowband source of pho-ton pairs at near infrared and telecom wave-lengths. We demonstrate the absorption ofa single photon by a single trapped calciumion, heralded by a telecom photon.
CB-8.1 THU 8:30Solitary Pulse-on-Demand Production byOptical Injection Locking of PassivelyQ-Switched InGaN Laser DiodeX. Zeng1, L. Sulmoni2, N. Grandjean2, and�D. Boiko1; 1Centre Suisse d’Electronique etde Microtechnique SA (CSEM), Neuchâtel,Switzerland; 2Institute of Condensed MatterPhysics (ICMP), École Polytechnique Fédéralede Lausanne (EPFL), Lausanne, SwitzerlandWe report on optical injection locking of Q-switched InGaN multi-section diode laserfrom CW tunable laser to produce solitarypulses at precise wavelength. To the best ofour knowledge, this has never been done be-fore.
EF-9.1 THU (Keynote) 8:30Push and Twist: the MechanicalProperties of Light�S. Barnett1, R. Cameron1, A. Yao2, and R.Loudon3; 1University of Glasgow, Glasgow,United Kingdom; 2University of Strathclyde,Glasgow, United Kingdom; 3University of Es-sex, Colchester, United KingdomWe shall describe the two distinct momentathat light carries in a medium, includingmagnetic and meta materials. �e combina-tion of electric and magnetic e�ects is cru-cial, also, in exploiting the properties of chi-ral molecules.
JSV-1.1 THU (Invited) 8:30Silicon Quantum PhotonicsD. Bonneau, J.W. Silverstone, R. Santagati,J.L. O’Brien, and �M.G. �ompson; Centrefor Quantum Photonics, H. H. Wills PhysicsLaboratory and Department of Electrical andElectronic Engineering, University of Bristol,,Bristol, United KingdomSilicon photonics has the potential to trans-form quantum photonic technologies. Byutilising the silicon-on-insulator materialsystem, we are able to generate, manipulateand detect quantum states of light withina scalable and monolithic technology plat-form.
CA-9.2 THU 8:45High power (100W) Yb:YAGsingle-crystal �ber ampli�cation chain forsub-ps MHz systemF. Lesparre1,2, �J.-T. Gomes1, I. Martial2,X. Délen1, J. Didierjean2, W. Pallmann3,B. Resan3, A. Loscher4, J.-P. Negel4, T.Graf4, M. Abdou Ahmed4, F. Balembois1,and P. Georges1; 1Laboratoire Charles Fabry,Palaiseau, France; 2Fibercryst SAS, DecinesCharpieu, France; 3JDSU Ultrafast Lasers,Zurich, Switzerland; 4IFSW, Stuttgart, Ger-manyWe demonstrate the use of three successivesingle-crystal �ber ampli�er to implement aMOPA setup providing 709 fs, 20 MHz, 5muJ pulses with an average power of 100 W.
EA-9.2 THU 8:45Single-photon absorption by a singleatom, heralded by a telecom-convertedsingle photon�J. Brito, A. Lenhard, S. Kucera, P. Eich,P. Müller, C. Becher, and J. Eschner; Ex-perimentalphysik, Universität des Saarlan-des, Saarbrücken, GermanyA single trapped 40Ca+ ion absorbs a singleresonant photon from a photon pair gener-ated by spontaneous parametric down con-version, while the partner photon whose de-tection heralds the absorption is frequency-converted to a telecommunication wave-length.
CB-8.2 THU 8:45Suppressed Relaxation Oscillations in aDBR Laser Monolithically Integrated withWeakly Coupled Optical -Feedback DelaySection�L. Daan, D. Domenico, A. Huub, and S.Meint;COBRAResearch Institute, EindhovenUniversity of Technology, Eindhoven, �eNetherlands�e laser exhibits broad injection-currentregions of operation, free of relaxation-oscillation-induced instabilities and withhigh side-mode suppression above 40 dB, ir-respective of the feedback phase.
CA-9.3 THU 9:00Yb:YVO4-based regenerative ampli�er�A. Rudenkov1, V. Kisel1, A. Yasukevich1, V.Matrosov2, and N. Kuleshov1; 1Center forOptical Materials and Technologies,, Minsk,Belarus; 2Solix Ltd., Minsk, BelarusDiode-pumped femtosecond Yb:YVO re-generative ampli�er was demonstrated withmaximum pulse energy 100�J and aver-age output power 1.85W at pulse repetitionfrequencies up to 100kHz. 370 fs pulses
EA-9.3 THU 9:00Frequency-dependent Phase inPhoton-to-Atom Quantum-State Transfer�P. Eich, P. Mueller, S. Kucera, M. Schug, andJ. Eschner; Universitaet des Saarlandes, Saar-bruecken, GermanyWe investigate heralded single-photon tosingle-atom quantum-state transfer using asingle trapped 40Ca+ ion. We study how thephase of the �nal atomic state depends onthe detuning of the absorbed photon.
CB-8.3 THU 9:00Relation between fast phase response andchaos bandwidth enhancement insemiconductor lasers subject to opticalfeedback and injection�R.M. Nguimdo; Applied Physics ResearchGroup, Vrije Universiteit Brussel, 1050 Brus-sels Belgium, Brussels, BelgiumWe show the quantitative relation betweenthe chaos bandwidth enhancement and thefast phase dynamics in semiconductor lasers
JSV-1.2 THU 9:00On chip source of photon pairs withintegrated pump �ltering and signal/idlerdemultiplexing.N. Harris1, D. Grassani2, A. Simbula2,M. Pant1, M. Galli2, T. Baehr-Jones3, M.Hochberg3, D. Englund1, �D. Bajoni4,and C. Galland5; 1Department of Elec-trical Engineering and Computer Science,Massachusetts Institute of Technology,Cambridge, United States; 2Dipartimento
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ogy & �e Center for Brain Integration Re-search, Tokyo Medical and Dental Univer-sity, Bunkyo-ku, Japan; 4Wired Co.,Ltd., Ko-mae, Japan; 5Interdisciplinary Research Unitin Photon-Nano Science, Tokyo University ofAgriculture and Technology, Koganei, JapanWe realized two-dimensional imaging of in-halation anestheticmolecules in water by us-ing heterodyne-detected CARS microspec-troscopy. �e present method enables us tovisualize the localization and distribution ofsmall drug molecules in biological tissues.
element plasmonic Fano nanoantenna ontoa waveguide and demonstrate that this inte-grated nanoantenna can spatially separatewavelength-encoded optical signals. Assuch it can be used as an ultra-compacton-chip spectral-band demultiplexer.
the highest output power of a �ber laseroscillator with femtosecond written FBGs.�e gratings were inscribed with the phasemask scanning technique and a step-chirpedmask.
We report on the �rst experimental demon-stration of time-domain ghost imaging usingdi�erent types of temporally incoherent lightsources. Our results open novel perspectivesfor dynamic imaging of ultra-fast waveformswith high resolution.
CD-11.4 THU 9:15High-Resolution Sub-Surface Microscopyof CMOS Integrated Circuits UsingRadially Polarized Light�M. Rutkauskas1, C. Farrell1, C. Dorrer2, K.Marshall2, T. Lundquist3, P. Vedagarbha3,and D. Reid1; 1Scottish Universities PhysicsAlliance (SUPA), Institute of Photonics andQuantum Sciences, Heriot-Watt University,Edinburgh, United Kingdom; 2Laboratoryfor Laser Energetics, University of Rochester,Rochester, United States; 3DCG Systems Inc.,Fremont, United StatesComparison of high-resolution sub-surfacemicroscopy shows that illumination withlinear polarization resolves an edge with res-olutions of 95 nm and 120 nm, depending onE-�eld orientation, while radial polarizationachieves a resolution of 98 nm.
EH-5.4 THU 9:15Surface Plasmon Mediated SuperradianceGenerated from Ag Slit Array/InGaAsP atRoom Temperature�K.J. Ahn1, S.-H. Kim2, D.-S. Kim3, and K.-J. Yee2; 1Department of Energy Systems Re-search and Department of Physics, Ajou Uni-versity, Suwon, Korea, South; 2Departmentof Physics, Chungnam National University,Daejeon, Korea, South; 3Center for Subwave-length Optics and Department of Physics andAstronomy, Seoul National University, Seoul,Korea, SouthIn this presentation we studied surface plas-mon mediated superradiance from silver slitarrays attached on a InGaAsP bulk semicon-ductor at room temperature. Pump energy-dependent time delay and pulse width ofstrong pulses are discussed.
CJ-11.4 THU 9:15Narrow Linewidth Single Mode FiberAmpli�er With 2.3 kW Average Power�J. Nold1, M. Strecker1, A. Liem1, R.Eberhardt1, T. Schreiber1, and A.Tünnermann1,2; 1Fraunhofer Institutefor Applied Optics and Precision Engineer-ing, Jena, Germany; 2Friedrich-SchillerUniversität, Institute of Applied Physics,Jena, GermanyWe report on a high average power �berampli�er with a narrow spectral linewidth.We discuss issues to reach this power, whichare based on several high power componentsand strategies to avoid nonlinear e�ects.
CF-6.4 THU 9:15Sub-10fs jitter compensation system forfemtosecond ampli�ers for accelerators�A. Casanova1,2,3, Q. D’Acremont1,3, G.Santarelli2, S. Dilhaire3, and A. Courjaud1;1Amplitude-systèmes, Pessac, France;2Laboratoire Photonique, Numérique etNanosciences, Talence, France; 3LaboratoireOndes et Matière d’Aquitaine, Talence,FranceWe report a timing jitter compensation sys-tem allowing to achieve 3.5fs rms on short-term, and 8,9fs rms over 14h. �e sys-tem is based on noncolinear balanced cross-correlator, and is compatible with any sub-pslaser.
CD-11.5 THU (Invited) 9:30QuantumMicroscopy with NOON StatesY. Israel, S. Rosen, and �Y. Silberberg; Weiz-mann Institute of Science, Rehovot, IsraelImaging under low light conditions is partic-ularly challenging, due to the e�ect of noiseon the image. Quantum NOON states oflight illuminating an object, are shown toenhance the sensitivity of polarization mi-croscopy.
EH-5.5 THU 9:30Optical Activation of PlasmonicGermanium Nanoantennas Resonant inthe Mid-Infrared�M.P. Fischer1, C. Schmidt1, J. Stock1,E. Sakat2, A. Samarelli3, J. Frigerio4,P. Biagioni2, D.J. Paul3, G. Isella4, A.Leitenstorfer1, and D. Brida1; 1Departmentof Physics and Center for Applied Photonics,University of Konstanz, Konstanz, Germany;2Dipartimento di Fisica, Politecnico di Mi-lano, Milano, Italy; 3School of Engineering,University of Glasgow, Glasgow, UnitedKingdom; 4L-NESS, Dipartimento di Fisicadel Politecnico di Milano, Como, ItalyGermanium nanoantennas are activated bytriggering a mid-infrared plasma responsevia ultrafast optical interband excitation.Femtosecond control of the intrinsic semi-conductor allows activation of the localizedplasmonic resonance for hundreds of pi-coseconds.
CL-2.4 THU 9:30Probing Virus and ssDNA Vibrationsusing Nano-Optical TweezersA. Kotnala, S. Wheaton, R. Gelfand, and�R. Gordon; University of Victoria, Victoria,CanadaUsing our recently reported approach ofextraordinary acoustic Raman (EAR), weprobe the ~100 GHz vibration spectra ofthe MS2 bacteriophage virus and variouslengths of single-stranded DNA.
CJ-11.5 THU 9:30Narrowband super�uorescent �bersource with record 1.87 kW output powerin all-�ber MOPA structure�J. Xu, J. Leng, W. Liu, H. Xiao, S. Guo, P.Zhou, and J. Chen; College of OptoelectronicScience and Engineering, National Univer-sity of Defense Technology, Changsha, China,People’s Republic of (PRC)We demonstrate a narrowband all-�bermaster oscillator power ampli�er (MOPA)structured super�uorescent �ber source(SFS), which delivers a record power (1.87kW) up to now. Further power scaling isavailable with more powerful pump source.
CF-6.5 THU 9:30Asynchronous optical sampling withampli�ed laser systemsL. Antonucci1,2, A. Bonvalet1,2, X.Solinas1,2, L. Daniault1,2, and �M. Jo�re1,2;1Laboratoire d’Optique et Biosciences, EcolePolytechnique - CNRS UMR7645, Palaiseau,France; 2Institut National de la Santé et dela Recherche Médicale, U1182, Palaiseau,FranceWe extend arbitrary detuning asynchronousoptical sampling (AD-ASOPS) to two in-dependent femtosecond ampli�ed laser sys-tems, thus demonstrating a novel multiscalepump-probe spectroscopy approach span-ning from 400 fs up to 1 ms.
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at central wavelength 1014.7nm were ob-tained.
with optical feedback and optical injectionbased on numerical simulations of the laser’sresponse.
di Fisica, Universita degli Studi di di Pavia,Pavia, Italy; 3oriant Advanced Technol-ogy Group,, Naperville, United States;4Dipartimento di Ingegneria Industrialee Informazione, Universita degli Studi diPavia,, Pavia, Italy; 5Stuttgart University,Stuttgart, GermanyWe integrate a source of photon pairs (mi-croring) with Bragg mirrors and add-dropsfor pump �ltering and photon routing on thesame silicon chip, reducing the pump to lessthan the generated pairs intensities.
CA-9.4 THU 9:15High-energy, diode-pumped Yb:X disklaser-ampli�er with a KD*P pockels in amultipass relay imaging resonator�M. Loeser1,2, M. Siebold1, D. Albach1, F.Roeser1, and U. Schramm1,2; 1Helmholtz-Zentrum Dresden-Rossendorf, Dresden,Germany; 2Technische Universität Dresden,Dresden, GermanyWe present a diode-pumped high apertureregenerative disk laser ampli�er for pulse en-ergies up 1J. Yb:YAG, Yb:LuAG, Yb:CaF2and Yb:QX glass are used to study the evo-lution of the beam pro�le, pulse energy andspectrum.
EA-9.4 THU 9:15Nonequilibrium Phase Transition in aDilute Rydberg Ensemble�C. Wade, N. Šibalić, K. Weatherill, andC. Adams; Joint Quantum Centre (JQC)Durham-Newcastle, Department of Physics,Durham University, Durham, United King-domWe present observations of a nonequilib-rium phase transition between states of lowand high Rydberg atom number density.Induced by dipole-dipole interactions, thisstrong nonlinearity in room-temperatureCaesium vapour is accompanied by intrinsicoptical bistability.
CB-8.4 THU 9:15Timing jitter reduction of a two-sectionexternal-cavity semiconductor laser byharmonic mode-locking and opticalfeedback�S. Rauch1,3, L. Drzewietzki1, A. Klehr2,J. Sacher3, W. Elsäßer1, and S. Breuer1;1Institute of Applied Physics, Technische Uni-versität Darmstadt, Darmstadt, Germany;2Ferdinand-Braun-Institut, Berlin, Germany;3Sacher Lasertechnik GmbH, Marburg, Ger-manyLong-term timing jitter reduction of apassively mode-locked external �ber-cavitydiode laser by harmonic mode-locking andoptical feedback from an auxiliary cavityis experimentally demonstrated and con-�rmed by numerical simulations.
EF-9.2 THU 9:15Optical manipulation of mesoscopiclight-matter coherent wavefunctions in aplanar microcavity�A. Askitopoulos1, T. Liew2, H. Ohadi1,Z. Hatzopoulos3,5, P. Savvidis3,4, andP. Lagoudakis1; 1School of Physics andAstronomy, University of Southampton,Southampton, United Kingdom; 2NanyangTechnological University, Singapore, Sin-gapore; 3Foundation for Research andTechnology - Hellas, Institute of ElectronicStructure and Laser, Heraklion, Greece;4Department of Materials Science andTechnology, University of Crete, Heraklion,Greece; 5Department of Physics, Universityof Crete, Heraklion, GreeceWe studymode selectivity ofmesoscopic po-lariton condensates in optical traps. �e re-vealed physical mechanism consistently in-terprets spatial mode switching, while the-oretical simulations reproduce the observedresults, enabling the design of polaritonbased quantum circuits.
JSV-1.3 THU 9:15Six-photon experiments using an on-chiparray of heralded, pure single photonsourcesJ.B. Spring1, P.L. Mennea2, �B.J. Metcalf1,P.C. Humphreys1, J.C. Gates2, M. Moore1, S.Barz1, W.S. Kolthammer1, B.J. Smith1, P.G.R.Smith2, and I.A. Walmsley1; 1ClarendonLaboratory, University of Oxford, Oxford,United Kingdom; 2Optoelectronics Re-search Centre, University of Southampton,Southampton, United KingdomWe construct an array of on-chip, highly in-distinguishable, pure single photon sourcesbased on spontaneous fourwavemixing. Us-ing this source, we perform the �rst quan-tum interference experiment between threeheralded single photons.
CA-9.5 THU 9:30Diode-PumpedFemtosecond-Laser-Inscribed Yb:YAGChannel Waveguide Laser, Q-switched byCarbon Nanotubes�S.Y. Choi1, T. Calmano2,3, M.H. Kim1, D.-I. Yeom1, C. Kränkel2,3, G. Huber2,3, and F.Rotermund1; 1Ajou University, Suwon, Ko-rea, South; 2Universität Hamburg, Hamburg,Germany; 3�e Hamburg Centre for UltrafastImaging, Hamburg, GermanyWe demonstrate a diode-pumped,femtosecond-laser-inscribed Yb:YAGchannel waveguide Q-switched by carbonnanotubes (CNTs). Using CNT-coated dif-ferent output couplers acting simultaneouslyas saturable absorber mirrors, Q-switchingcharacteristics of a 9.3-mm-long waveguidelaser are systematically investigated.
EA-9.5 THU 9:30Quantum Nonlinear Cavity QEDWithCoherently Prepared Multilevel AtomsG. Yang1,3, W.-j. Gu2, G. Li2, B. Zou1, and�Y. Zhu1; 1Florida International University,miami, United States; 2Huazhong NormalUniversity, wuhan, China, People’s Republicof (PRC); 3Zhejiang University, Hangzhou,China, People’s Republic of (PRC)�e contribution has been withdrawn by theauthors.
CB-8.5 THU 9:30Optical feedback induced switchingbetween ground and excited stateemission in a quantum dot laser diode�M. Virte1, S. Breuer2, M. Sciamanna3, andK. Panajotov1,4; 1Brussels Photonics Team(B-Phot), Dept. of Applied Physics andPhotonics (TONA), Vrije Universiteit Brus-sel, Brussels, Belgium; 2Institute of AppliedPhysics, Technische Universität Darmstadt,Darmstadt, Germany; 3Centrale Supelec, OP-TEL Research Group, Metz, France; 4Instituteof Solid-state Physics, So�a, BulgariaRecurrent switching of a GS and ES emittingquantum-dot laser subject to time-delayedoptical feedback is studied theoretically andexperimentally and attributed to the evolu-tion of the GS,ES gain di�erence when vary-ing the optical feedback-phase.
EF-9.3 THU 9:30Optical pattern formation with a 2-levelnonlinearityA. Camara1, R. Kaiser1, G. Labeyrie1, W.Firth2, G.-L. Oppo2, G. Robb2, A. Arnold2,and �T. Ackemann2; 1Institut Non Linéaire deNice, Sophia Antipolis, France; 2University ofStrathclyde, Glasgow, United KingdomOptical pattern formation is studied in a coldatomic cloud using the single mirror feed-back scheme. We map the domain of exis-tence of this instability, due to a quasi-2-levelnonlinearity of scalar nature.
JSV-1.4 THU 9:30On-chip High Spectral Purity andBrightness Idler Single-Photon Source�Z. Yan, Y. Duan, L.G. Helt, M. Ams, M.J.Withford, and M.J. Steel; Centre for Ultra-high bandwidth Devices for Optical Systems(CUDOS) & MQ Photonics Research Centre,Department of Physics and Astronomy, Mac-quarie University, Sydney, Australia�e �rst side track induced birefringencewaveguide made by femtosecond laser writ-ten method for spontaneous four-wave mix-ing creates an on-chip single photon sourcewith genuine spectral purity of 94% and highbrightness of 250x10^3 pairs/nm*W*cm.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bEH-5.6 THU 9:453-D Skew Plasmonic Antenna Arrays�P. Zilio, M. Malerba, A. Toma, F. Tantussi,and F. DeAngelis; Istituto Italiano di Tecnolo-gia, Genova, ItalyWe investigate both theoretically and ex-perimentally the optical properties of high-aspect-ratio slanted metallic nanoantennadimers on metallic substrate. Strong �eldenhancements and collective e�ects resultfrom the inherent 3D spatial arrangement ofthese structures.
CL-2.5 THU 9:45�e optical vault: a recon�gurable opticalbottle beam for photophoretic trapping ofabsorbing macro-particles�A. Turpin1, V. Shvedov2, C. Hnatovsky2,Y. Loiko1,3, J. Mompart1, and W. Krolikow-ski2,4; 1Departament de Física, UniversitatAutònoma de Barcelona, Bellaterra, Spain;2Laser Physics Centre, Australian NationalUniversity, Canberra, Australia; 3Institute ofPhotonic Technologies, School of Engineer-ing& Applied Science Aston University, Birm-ingham, United Kingdom; 4Program, TexasA&M University at Qatar, Doha, QatarWe demonstrate the generation of a polar-ization tailored recon�gurable optical bottlecapable of trapping and unloading absorbingmacro-particles by means of conical refrac-tion and the photophoretic force.
CJ-11.6 THU 9:45Ultra-high Temperature Operation of aTuneable Ytterbium Fibre Laser�J. Daniel1,2, N. Simakov1,2, A. Hemming1,A. Clarkson2, and J. Haub1; 1Laser Tech-nologies Group, Cyber and Electronic War-fare Division, Defence Science and Tech-nology Organisation, Adelaide, Australia;2Optoelectronics Research Centre, Southamp-ton, United KingdomWe report on the performance of an ytter-bium �bre laser operating at ultra-high tem-peratures of up to 400�C, with a maximumoutput power of 33W and tuning range of124nm from 1036nm to 1160nm.
CF-6.6 THU 9:45On the Origin of Flicker noise inStabilized Frequency Combs�Y. Song1 and G. Steinmeyer2; 1UltrafastLaser Lab, School of Precision Instrumentsand Opto-electronics Engineering, TianjinUniversity, Tianjin, China, People’s Repub-lic of (PRC); 2Max-Born-Institut für Nichtlin-eare Optik und Kurzzeitspektroskopie, Berlin,GermanyWe discuss a quantum noise contributionthat is caused by ampli�ed spontaneousemission on the origin of a �icker noise inthe long-term carrier-envelope phase mea-surement of stabilized frequency combs.
10:30 – 12:00CD-12: Applications of OpticalFibres IIChair: Valerio Pruneri, ICFO - �e Instituteof Photonic Sciences and ICREA, Castellde-fels, Spain
10:30 – 12:00EH-6: Nanoantennas: From Sensingto�ermoplasmonicsChair: JérômeWenger, CNRS Institut Fresnel,Marseille, France
10:30 – 12:00CL-3: Multiphoton and MultimodalMicroscopyChair: Francesco Pavone, University of Flo-rence, Florence, Italy
10:30 – 12:00CJ-12: Erbium Fibre andWaveguideLasersChair: Jens Engholm Pedersen, NKT Photon-ics, Birkerød, Denmark
10:30 – 12:00CF-7: Ultrafast Spectroscopy andImagingChair: �omas Südmeyer, University ofNeuchâtel, Neuchâtel, Switzerland
CD-12.1 THU (Tutorial) 10:30Scienti�c Applications of PhotonicCrystal and Microstructured Fibres�P. Russell; MPI Science of Light, Erlangen,GermanyMicrostructured and photonic crystal �bresare making possible a whole range of novelexperiments on light-matter interactions,including supercontinuum generation, ul-trafast nonlinear dynamics in gases, en-hanced optomechanical e�ects, and manip-ulation of orbital angular momentum states.
EH-6.1 THU 10:30Hybrid optical antennas forsubnanometer multicolor localization ofsingle molecules�M.Mivelle1, T. van Zanten1, andM. Garcia-Parajo1,2; 1ICFO, Barcelona, Spain; 2ICREA,Barcelona, SpainWe demonstrate that our hybrid optical an-tenna allows broadband adiabatic �eld en-hancement and nanofocusing of light downto about 20 nm, together with Angstrom po-sition accuracy.
CL-3.1 THU 10:30Towards all-optical melanoma depthdetermination�M. Mazurenka, A. Varkentin, E. Blumen-roether, J. Stritzel, M. Otte, M. Rahlves, M.Meinhardt-Wollweber, and B. Roth; HanoverCentre for Optical Technologies, Leibniz Uni-versität Hannover, Hanover, GermanyWe present the progress towards a novelimaging system, based on OCT and optoa-coustic imaging modalities, combined withRaman spectroscopy, designed for a rapid,noninvasive, in-vivo melanoma boundaryassessment in 3D.
CJ-12.1 THU (Invited) 10:30Emerging Fiber Lasers and Ampli�ers forTelecoms�D. Richardson, Y. Jung, Q. Kang, J. Sahu,S. Jain, Z. Li, and S. Alam; OptoelectronicsResearch Centre, Southampton, United King-domWe review recent progress in the develop-ment of novel ampli�ers for future opticalcommunications systems including erbium-doped ampli�ers for Space Division Mul-tiplexed transmission and thulium-dopedampli�ers for long wavelength transmissionbeyond the L-band.
CF-7.1 THU 10:30Ultrafast �eld-resolved multi-terahertznano-spectroscopy�M.A. Huber1, M. Eisele1, T.L. Cocker1, M.Plankl1, L. Viti2, D. Ercolani2, L. Sorba2,M.S. Vitiello2, and R. Huber1; 1Departmentof Physics, University of Regensburg, Re-gensburg, Germany; 2NEST, CNR-InstitutoNanoscienze and Scuola Normale Superiore,Pisa, ItalyWe present a novel multi-terahertz near-�eld microscope that combines high spatialresolution (10 nanometers) with sub-cycletemporal resolution (10 femtoseconds). �isconcept allows for �eld-resolved detectionof femtosecond carrier dynamics at an InAsnanowire surface.
EH-6.2 THU 10:45Getting more Photons from SingleMolecules with DNA-sca�oldedNanophotonic StructuresG. Acuna, A. Puchkova, C. Vietz, B. Wünsch,E. Pibiri, B. Lalkens, D. Wang, and �P. Tin-nefeld; Institute for Physical and �eoreticalChemistry, Braunschweig University of Tech-
CL-3.2 THU 10:45Single shot polarimetric contrastmicroscopy by circular polarizationorthogonality breaking imaging�N. Ortega-Quijano, J. Fade, E. Schaub, F.Parnet, and M. Alouini; Institut de Physiquede Rennes (CNRS/Université de Rennes 1),Rennes, France
CF-7.2 THU 10:45Exploring Ultrafast Physics with InfraredNear-Field Nanoscopy�F. Keilmann; Lasnix, Berg, Germany;Ludwig-Maximilians-Universität, München,Germany; Neaspec GmbH, Martinsried,GermanyPump-probe mid-infrared spectroscopy at
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCA-9.6 THU 9:45Radiation hard optical frequency combfrom a diode-pumped solid-statefemtosecond laser�G. Buchs, S. Kundermann, E. Portuondo-Campa, and S. Lecomte; Centre Suissed’Electronique et de Microtechnique (CSEM),Neuchâtel, SwitzerlandWe report on a radiation hard frequencycomb based on Yb:KYW gain mediumfemtosecond diode-pumped solid-state lasertechnology. Ground level gamma and pro-ton radiation tests with high doses are pre-sented and their e�ects are discussed.
EA-9.6 THU 9:45Overcoming Decoherence to GenerateIndistinguishable Single Photons�T. Grange1, G. Hornecker1, D. Hunger2, J.-P. Poizat1, J.-M. Gérard3, P. Senellart4, andA. Au�èves1; 1Institut Néel, Grenoble, France;2LMU, Munich, Germany; 3CEA, Grenoble,France; 4LPN, Marcoussis, FranceWe investigate theoretically the generationof indistinguishable single photons from astrongly dissipative quantum system placedinside an optical cavity. Our calculations re-veal an unconventional regime of high in-distinguishability for moderate emitter cav-ity coupling strengths and high quality factorcavities.
CB-8.6 THU 9:45Single-sideband characteristics ofphotonic microwave signals generatedwith optically injected quantum-dot andquantum-well semiconductor lasers�C.-Y. Chen, C.-H. Cheng, and F.-Y. Lin; In-stitute of Photonics Technologies, National Ts-ing HuaUniversity, Hsinchu, China, Republicof (ROC)Photonic microwave signals generatedby optically injected quantum-dot andquantum-well lasers are investigated andcompared. �e QD laser shows 15 dBhigher sideband rejection ratio in mi-crowave frequencies ranging from 10 to 22GHz.
EF-9.4 THU 9:45An experimental proposal for patternformation in optomechanical cavities�J. Ruiz-Rivas1, C. Navarrete-f2, G.Patera3, E. Roldán1, and G.J. de Valcárcel1;1Universitat de Valencia, Valencia, Spain;2Max-Panck Institut für Quantenoptik,Garching, Germany; 3Laboraoire dePhysique des Lasers, atomes et molécules,Lille, FranceIn this work we address the possibility of ob-serving pattern formation experimentally inoptomechanical resonators, proposing im-plementations that are compatible with cur-rent membrane setups.
JSV-1.5 THU 9:45Directly measuring nonclassical states ofup to 50 photons at telecommwavelengths�T. Bartley1,2, G. Harder2, A. Lita1, S.W.Nam1, T. Gerrits1, and C. Silberhorn2;1National Institute for Standards and Tech-nology, Boulder, United States; 2University ofPaderborn, Paderborn, GermanyUsing spontaneous parametric down-conversion in ppKTP waveguides, wedirectly measure nonclassical states ofup to 50 photons at telecommunicationwavelengths with a Klyshko e�ciencyof >60% and a generation rate of ~1 persecond.
10:30 – 12:00CA-10: �in Disk Lasers andAmpli�ersChair: Martin Schellhorn, French-GermanResearch Institute (ISL), Saint-Louis, France
10:30 – 12:00EA-10: Controlled Light-matterInteractions IIChair: OlivierMorin, Max Planck Institute ofQuantum Optics, Garching, Germany
10:30 – 12:00CB-9: Quantum-dot LasersChair: Maria Ana Cataluna, University ofDundee, Nethergate, Dundee, United King-dom
10:30 – 12:00EI-1: Structured Light andStructured MaterialsChair: Uwe Bandelow, WIAS, Berlin, Ger-many
10:30 – 12:00JSV-2: Source EngineeringChair: Robert Keil, from the University ofInnsbruck, Innsbruck, Austria
CA-10.1 THU 10:30220mJ, 1 kHz Picosecond Regenerative�in-Disk Ampli�er�S. Klingebiel1, M. Schultze1, C.Y. Teisset1,R. Bessing1, M. Häfner1, S. Prinz1, M.Gorjan2,3, D. Sutter4, K. Michel1, H.G.Barros2, Z. Major2, F. Krausz2,3, and T.Metzger1; 1TRUMPF Scienti�c Lasers GmbH+ Co. KG, Unterföhring, Germany; 2Ludwig-Maximilians-Universität München, Depart-ment für Physik, Garching, Germany; 3Max-Planck-Institut für Quantenoptik, Garching,Germany; 4TRUMPF Laser GmbH + Co. KG,Schramberg, GermanyWe report on a chirped-pulse regenerativethin-disk ampli�er generating 220 mJ pulseenergy at 1 kHz repetition rate with a pulseduration of 1.9 ps for pumping few-cycle op-tical parametric ampli�ers (OPA).
EA-10.1 THU 10:30Storage and retrieval of ultrafast singlephotons using a room-temperaturediamond quantummemory�J.-P. MacLean1, K. Fisher1, D. England2, P.Bustard2, R. Lausten2, K. Resch1, and B.Sussman2; 1Institute of Quantum Comput-ing, Department of Physics and Astronomy,University of Waterloo, Waterloo, Canada;2National Research Council of Canada, Ot-tawa, Canada�e contribution has been withdrawn by theauthors.
CB-9.1 THU (Invited) 10:30InGaN/GaN Quantum Dot Lasers: �eNext Frontier�P. Bhattacharya, T. Frost, and A. Hazari;University of Michigan, Ann Arbor, UnitedStatesDue to the reduced strain, InGaN/GaNquantum dots can be incorporated intolasers emitting across the visible spectrumwith superior performance. �e DC and dy-namic characteristics of such green- and red-emitting lasers are demonstrated.
EI-1.1 THU (Invited) 10:30Graphene Nanophotonics�J. De Abajo; ICFO Institut de CiènciesFotòniques, Castelldefels (Barcelona), SpainWe review di�erent strategies and recent ad-vances in the achievement of strong opti-cal tunability in the vis-NIR usinggrapheneplasmons, as well as their potential applica-tion for quantum optics, light manipulation,and sensing
JSV-2.1 THU 10:30A single non-linear directional coupler togenerate N00N states�R. Kruse1, L. Sansoni1, S. Brauner1, R.Ricken1, C.S. Hamilton2, I. Jex2, and C.Silberhorn1; 1Integrated Quantum Optics,University of Paderborn, Paderborn, Ger-many; 2FNSPE, Czech Technical University inPrague, Prague, Czech RepublicWe present a non-linear directional couplerwhich generates post-processing free N00Nstates without the need of narrowband �l-tering. We demonstrate a state �delity ofF = (84.1 ± 2.3)% and the double fringefrequency of a 2-photon N00N state.
CA-10.2 THU 10:45100 mJ, 200 Hz, Cryogenic Yb:YAGComposite�in-Disk Laser Ampli�er�F. Reichert1, M. Hemmer1, A.-L.Calendron1,2, H. Cankaya1,2, K. Zapata1,M. Smrz1,3, L.E. Zapata1,4, and F.X.Kärtner1,2,4; 1CFEL/DESY, Hamburg, Ger-many; 2�e Hamburg Centre for Ultrafast
EA-10.2 THU 10:45Coherent Population Trapping withDefect Spin Ensembles in Silicon Carbide�D. O’Shea, O. Zwier, A. Onur, X. Yang, andC. van der Wal; Zernike Institute for Ad-vanced Materials, University of Groningen,Groningen,�e NetherlandsWe demonstrate coherent optical control
JSV-2.2 THU 10:45Hyperentangled photon states on a chipA. Orieux1, �M.A. Ciampini1, G. Corrielli2,3,A. Crespi2,3, R. Osellame2,3, F. Sciarrino1,and P. Mataloni1; 1Dipartimento di Fisica,Sapienza Università di Roma, Roma, Italy;2Istituto di Fotonica e Nanotecnologie, Con-siglio Nazionale delle Ricerche (IFN-CHNR),
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nology, Braunschweig, GermanyWe present DNA origami nano-antennas.Besides recent progress in the achievable�uorescence enhancement we discuss howsingle-molecule measurements help to re-veal the details of the dye-nanostructure in-teraction.
We report a novel method to fully charac-terize linear dichroism from a single mea-surement using a dedicated dual-frequencydual-circular-polarization coherent source.�is method entails a high potential forminimally-invasive polarimetric imaging ofbiological tissues.
200 fs temporal resolution is demonstratedat 20 nm spatial resolution, far below thedi�raction limit, by combining near-�eldmicroscopy with a 100 fs �ber-laser basedsupercontinuum.
EH-6.3 THU 11:00Controlling Light Emission withPercolating Plasmonic Networks�M. Gaio1, M. Castro-Lopez1,2, J. Renger2,N. van Hulst2,3, and R. Sapienza1; 1King’sCollege London, London, United Kingdom;2ICFO - Institut de Ciencies Fotoniques,Barcelona, Spain; 3ICREA - InstitucióCatalana de Recerca i Estudis Avançats,Barcelona, SpainSelf-assembled and lithographic gold net-works characterised by large density of states(LDOS) �uctuations around the electricalpercolation threshold are studied through�uorescence dynamics experiments. We dis-cuss the role of global long-range and localnear-�eld contributions.
CL-3.3 THU 11:00Absolute measurements of SecondHarmonic Generation signal fromCollagen �brils with unresolved diameterS. Bancelin1, C. Aimé2, I. Gusachenko1, L.Kowalczuk3, G. Latour1, T. Coradin2, and�M.-C. Schanne-Klein1; 1Lab. for Opticsand Biosciences, Ecole Polytechnique, CNRS,Inserm, Palaiseau, France; 2Laboratoire deChimie de la Matière Condensée de Paris,Sorbonne Universités, UPMC Univ Paris 06,CNRS, Collège de France, Paris, France;3Physiopathology of Ocular Diseases, �er-apeutic Innovations, Centre de Recherchedes Cordeliers, Sorbonne Universités, UPMCUniv Paris 06, INSERM UMRS 872, Paris,FranceWe correlated SHG and Electron Micro-scopies to calibrate SHG signals as a func-tion of collagen �bril diameter, down to 30nm. We observed a fourth power depen-dence, in agreement with analytical and nu-merical calculations.
CJ-12.2 THU 11:00Glass waveguide-semiconductor hybridlasers�Y. Fan1, R. Oldenbeuving2, D. Geuzebroek3,A. Leinse4, P. van der Slot1, and K. Boller1;1Laser Physics and Nonlinear Optics group,MESA+ Research Institute for Nanotechnol-ogy, University of Twente, Enschede, �eNetherlands; 2SATRAX B.V., Enschede, �eNetherlands; 3XiO photonics B.V., Enschede,�e Netherlands; 4LioniX B.V., Enschede,�eNetherlandsWe present a novel glass waveguide-semiconductor hybrid laser. Near 1.55 umwavelength the laser is widely tunable andshows a spectral bandwidth of 24 kHz. Op-eration at around 694 nm is demonstratedas well.
CF-7.3 THU (Invited) 11:00Mapping Atomic Motions withUltrabright Electrons�R.J.D. Miller; Max Planck Institute for theStructure andDynamics ofMatter, Hamburg,Germany; University of Toronto, Toronto,Canada�e electron sources are now capable ofresolving nuclear motions on the 10 fstimescale (sub-Å spatial resolution) withsingle shot structure capabilities and soonsingle shot full movies of atomic motionswith the same resolution.
EH-6.4 THU 11:15Investigation of combined one- andtwo-photon NIR excitedsurface-enhanced Raman scatteringnanosensors for bio-applications�Z. Heiner, M. Gühlke, and J. Kneipp;Humboldt-Universität zu Berlin, Berlin, Ger-manyWe present a novel, simultaneous mul-timodal confocal Raman microscopic ap-proach operating at 1064 nm for bio-applications and demonstrate its excellentfeasibility for all-optical nanosensing basedon surface-enhanced Raman and hyper-Raman scattering over a wide pH-range.
CL-3.4 THU 11:15A femtosecond-pulsed tunable OpticalParametric Generator at 1530-1790 nmfor Label-free�ird HarmonicGeneration Imaging�J. Trägårdh1, G. Robb1, K. Gadalla2, S.Cobb2, C. Travis3, G.-L. Oppo3, and G.McConnell1; 1Centre for Biophotonics,SIPBS, University of Strathclyde, Glasgow,United Kingdom; 2Institute of Neuroscienceand Psychology College of Medical, Veteri-nary and Life Sciences, University of Glasgow,Glasgow, United Kingdom; 3Department ofPhysics, University of Strathclyde, Glasgow,United KingdomWe have developed a simple tunable opti-cal parametric generator, emitting ultrashortpulses at 1530-1790 nm, for label-free thirdharmonic generation imaging. We demon-strate imaging of a thick (200 micrometer)brain slice.
CJ-12.3 THU 11:15Fully Phase Stabilized SESAMMode-locked Erbium Fiber LaserFrequency Comb Oscillator with anIntegrated Electro-optic Modulator�S. Schweyer1, U. Hugentobler1, R.Kienberger2, B. Eder3, P. Putzer3, L.Pedrosa3, J. Obermaier3, S. Wick3, T.Unterholzer3, and N. Lemke3; 1TechnischeUniversität München - FESG, Munich, Ger-many; 2Technische Universität München -Physics Department E11, Munich, Germany;3OHB System AG, Munich, GermanyIn this paper the fully phase stabilizationof an all-in-�ber SESAM mode locked Er-bium frequency comb laser with an inte-grated electro-optic modulator is demon-strated
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Imaging, Hamburg, Germany; 3HilaseCenter, Dolni Brezany, Czech Republic;4Massachusetts Institute of Technology,Cambridge, United StatesWe report on a chirped pulse ampli�er basedon a cryogenic Yb:YAG composite thin-diskwhich delivered pulses with an energy of 106mJ at a repetition rate of 200 Hz.
of the spin of defects in silicon carbideand identify the S=1 spin structure of theground and optically excited states, reveal-ing a role for relaxation pathways via inter-system crossing.
Milano, Italy; 3Dipartimento di Fisica, Po-litecnico di Milano, Milano, Italy2-photon 4-qubit hyperentangled photonstates have been injected within a glass chipfabricated by femtosecond laser writing. Us-ing path- and polarization- degrees of free-dom we have exploited both product andcluster states.
CA-10.3 THU 11:00Carrier-envelope-phase Stabilization viaDual Wavelength Pumping�M. Seidel1, J. Brons1, F. Lücking2, I.Angelov1, V. Pervak2, A. Apolonski1,2, T.Udem1, and O. Pronin1; 1Max-Planck-Institut für Quantenoptik, Garching,Germany; 2Ludwig-Maximilians-UniversitätMünchen, Garching, GermanyMulti-wavelength diode pumping is pro-posed as a novel concept for carrier-envelope-phase stabilizing high-power os-cillators. In a proof-of-principle exper-iment the residual carrier-envelope-phasenoise of a 17-W Kerr-lens mode-lockedYb:YAG thin-disk oscillator was reduced to235-mrad.
EA-10.3 THU 11:00Step-by-step Coherent PopulationTrapping with Coupled Single Spins inDiamond�G. Hétet2, P. Jamonneau1, A. Dréau3, J.-F.Roch1, and V. Jacques1; 1Laboratoire AiméCotton, CNRS, Orsay, France; 2LaboratoirePierre Aigrain, Paris, France; 3Kavli Instituteof Nanoscience, Del�,�e NetherlandsWe demonstrate room temperature coher-ent population trapping (CPT) with singlespins in diamonds. Using a laser controlledrelaxation we could observe multiple CPTpreparation conditions and the step-by-steppumping to the dark state.
CB-9.2 THU 11:00High Performance of InAs/GaAsQuantum Dot Lasers MonolithicallyGrown on Si substrate with InAlAs/GaAsDislocation Filter Layers Introducing�M. Tang, S. Chen, Q. Jiang, J. Wu, A. Seeds,and H. Liu; University College London, Lon-don, United KingdomWe have established an InAs/GaAs quantumdot lasers monolithically grown on Si sub-strate with high output power (>100 mW)and high operation temperature (110 C) byusing molecular beam epitaxy system.
EI-1.2 THU 11:00Composite multi-vortex di�raction-freebeams and van Hove singularities inhoneycomb latticesV. Paltoglou1, Z. Chen2, and �N. Efremidis1;1University of Crete, Heraclion, Greece; 2SanFrancisco State University, San Francisco,United StatesWe �nd that honeycomb lattices supportdi�raction-free multi-vortices above thevan-Hove singularity. Exact solutions for thespinor components are obtained in the Diraclimit. Right at the singularity the solutionsbecome in�nite extend stripes.
JSV-2.3 THU 11:00Tunable Entangled Photon States from aNonlinear Directional Coupler�F. Setzpfandt1,2, A.S. Solntsev1, J.Titchener1, C.W. Wu1, C. Xiong3, T.Pertsch2, R. Schiek4, D.N. Neshev1, andA.A. Sukhorukov1; 1Centre for UltrahighBandwidth Devices for Optical Systems(CUDOS) and Nonlinear Physics Centre,Research School of Physics and Engineering,Australian National University, Canberra,Australia; 2Institute of Applied Physics,Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, Germany; 3CUDOS,the Institute of Photonics and Optical Science(IPOS), School of Physics, University ofSydney, Sydney, Australia; 4University ofApplied Sciences Regensburg, Regensburg,GermanyWe propose and experimentally demon-strate all-optically tunable biphoton genera-tion using a nonlinear directional coupler asquantum light source. �e source can gen-erate high-�delity N00N states, completelysplit states, and states with variable degreesof entanglement.
CA-10.4 THU 11:15Novel�in Disk Lens Shaped CompositeNd:YAG/YAG Ceramic Laser�T. Dascalu1, A. Ionescu1, G. Salamu1,2,O. Grigore1,2, M. Dinca1,2, F. Voicu1,2, C.Brandus1,2, and N. Pavel1; 1National Insti-tute for Laser, Plasma and Radiation Physics,Solid-State Quantum Electronics Laboratory,Bucharest 077125, Romania, Magurele, Ro-mania; 2University of Bucharest, Facultyof Physics, Bucharest 077125, Romania,Magurele, RomaniaA novel thin-disk lens-shaped compositeNd:YAG/YAG ceramic laser is proposed.Under the pump by a three-fold �ber-coupled diode lasers this device delivers 16-mJ output energy with overall optical-to-optical e�ciency of ~0.26, at 0.31 slope ef-�ciency.
EA-10.4 THU 11:15Controlling Quantum States of Lightusing Light-Shi�s in Photon EchoQuantumMemories�G. Hétet1, T. Chanelière2, and D. Guéry-Odelin3; 1Laboratoire Pierre-Agrain, Paris,France; 2Laboratoire Aimé-Cotton, Paris,France; 3Laboratoire Collision-Agrégats-Réactivité, Toulouse, FranceWe present a scheme for di�raction controland read-out of spin waves using a gradi-ent echo quantum memory. We show an ex-perimental demonstration of photon echoescontrol using light shi�s in rare earth dopedmaterials.
CB-9.3 THU 11:15Modulation Response Enhancement byTwo-State Lasing in Quantum Dot Lasers�A. Röhm1, B. Lingnau1, and K. Lüdge2;1Institut f. �eoretische Physik, Technis-che Universität Berlin, Berlin, Germany;2Fachbereich Physik, Freie Universität Berlin,Berlin, GermanyWe present our theoretical results on the re-lation between two-state lasing and signalmodulation in quantum dot lasers, whichshow a sharp increase in themaximummod-ulation frequency a�er the excited state las-ing threshold.
EI-1.3 THU 11:15Electronic and Optical Properties ofPlasmonic Topological Insulators�J. Yin1, Z. Wang1,2, W. Wu3, G. Adamo2,N.I. Zheludev2,3, and C. Soci1,2; 1Division ofPhysics and Applied Physics, School of Phys-ical and Mathematical Sciences, NanyangTechnological University, Singapore, Singa-pore; 2Centre for Disruptive Photonic Tech-nologies, Nanyang Technological University,Singapore, Singapore; 3Optoelectronics Re-search Centre, University of Southampton,Southampton, United KingdomBand structure and dielectric functions ofvarious topological insulator materials areobtained by many-body perturbation the-ory, elucidating origin and composition de-pendence of the bulk plasma wavelength inthe visible and near-infrared parts of thespectrum.
JSV-2.4 THU 11:15Engineering time-frequency properties ofphoton pairs generated by a tranversallypumped semiconductor device�G. Boucher, T. Douce, A. Eckstein, I. Favero,G. Leo, T. Coudreau, P.Milman, and S. Ducci;LaboratoireMatériaux et Phénomènes Quan-tiques Université Paris Diderot/CNRS, Paris,FranceWe present an ultra-versatile AlGaAs sourceof photon pairs; the spatial properties ofthe pump beam control the degree of thebi-photon frequency correlations. A noveltechnique to generate and characterize non-gaussian states is proposed.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCD-12.2 THU 11:30UV Light Generation in the FundamentalMode of a Multimode Photonic CrystalFiber Via Four-Wave Mixing at 532*nm�B. Sévigny, A. Cassez, O. Vanvincq, Y.Quiquempois, and G. Bouwmans; PhLAMLaboratory, Villeneuve d’Ascq, FranceA method is introduced by which UV lightcan be generated in the fundamental modevia four-wavemixing by pumping in a super-position of modes at 532 nm. Fiber designand experimental results are presented.
EH-6.5 THU 11:30Spontaneous�ermal Cycles in MetallicNano�uids with Heat Dissipation viaNanobubbles�J.L. Dominguez-Juarez1,4, S. Vallone1, M.Moocarme1,2, A. Lempel1, H.D. Gafney3, andL.T. Vuong1,2; 1Dept. of Physics, City Univer-sity of New York- Queens College, NY, UnitedStates; 2Dept. of Physics, City University ofNew York- �e Graduate Center, NY, UnitedStates; 3Dept. of Chemistry, City Univer-sity of New York- Queens College and theGraduate Center, NY, United States; 4Centrode Fisica Aplicada y Tecnologia Avanzada,UNAM Campus Juriquilla, Qro, MexicoWe present an experiments of spontaneousoscillatory behavior in binary-solventplasmonically-absorbing nano�uids, whichoccurs when collimated light grazesmenisci. �e robust heat cycles identifynanobubbles, new mechanisms for probingnanoparticle-solvent chemistry, and novelthermo-mechanical dynamics.
CL-3.5 THU (Invited) 11:30High-�roughput Second HarmonicImaging�S. Roke, C. Macias-Romero, and M. Di-dier; Laboratory for fundamental BioPho-tonics, École Polytechnique Fédérale de Lau-sanne, Lausanne, SwitzerlandHigh throughput multiphoton imaging canbe achieved with wide-�eld second har-monic microscopy. We demonstrate dy-namics in living cells with image acquisi-tion times of 50 microseconds. Low �uenceimaging of cultured primary neurons is alsopossible.
CJ-12.4 THU 11:30Wideband-tunable, soliton �bre lasermode-locked at 1.88 GHz by optoacousticinteractions in solid-core PCF�W. He, M. Pang, and P. St.J. Russell; MaxPlanck Institute for the Science of Light, Er-langen, GermanyWe report a wavelength-tunable soliton �brelaser stably mode-locked at 1.88 GHz (the188th harmonic of the cavity round-trip fre-quency) by an optically-driven acoustic res-onance in a solid-core photonic crystal �bre.
CF-7.4 THU 11:30Photocurrent Coherent Control in GaAsUsing Femtosecond Phase-locked Pulses�H. Tahara and Y. Kanemitsu; Institute forChemical Research, Kyoto University, Uji, Ky-oto, JapanWe report coherently controlled photocur-rent in subpicosecond dynamics. �e peri-odic change of photocurrent intensity wasobserved by using phase-locked pulses. Wecontrolled the carrier generation due to shal-low acceptors in bulk GaAs.
CD-12.3 THU 11:45Temporal Crystals in Gas-�lled PhotonicCrystal Fibers�M. Saleh1,2, A. Armaroli2, A. Marini2, T.Tran2, F. Belli2, A. Abdolvand2, and F.Biancalana1,2; 1Heriot-Watt University, Ed-inburgh, United Kingdom; 2Max-Planck In-stitute for the Science of Light, Erlangen, Ger-manyCondensed-matter phenomena such asWannier-Stark ladders, Bloch oscillations,and Zener tunneling can be inferredduring the propagation of a delayed probefollowing an ultrashort strong soliton inhollow-core photonic crystal �bers �lled byRaman-active gases.
EH-6.6 THU 11:45Optically induced heating in metallicnanowire systems.�D. McCloskey1,2,3, A.P. Bell2,3,4, J.A.Fair�eld2,3,4, S. Mills2,3,4, E. McCarthy2,3,4,J. Boland2,3,4, and G. Ba�ou5; 1School ofPhysics, Trinity College Dublin, Dublin,Republic of Ireland; 2Centre for research onadaptive nanostructures and nanodevices(CRANN)), Dublin, Republic of Ireland;3Advanced materials and bioengineeringcentre (AMBER), Dublin, Republic of Ireland;4School of Chemistry, Trinity College Dublin,Dublin, Republic of Ireland; 5Institut Fresnel,CNRS, Aix Marseille Université, CentraleMarseille, UMR 7249, 13013, Marseille,France�ermal imaging based on quadriwaveshearing interferometry (TIQSI) is em-ployed to make quantitative measurementsof the local temperature rise, and heat sourcedensity, in complex systems composed frommetallic nanowires, under focused optical il-lumination.
CJ-12.5 THU 11:45High peak power single frequencyampli�ers based on e�cientErbium-Ytterbium doped LMA �bers�G. Canat1, W. Renard1, T. Robin2, B.Cadier2, J. Le Gouët1, L. Lombard1, A.Durécu1, and P. Bourdon1; 1Onera, �eFrench aerospace lab, Palaiseau, France;2iXFiber SAS, Lannion, FranceWe report on various single-frequencyMOPA based on new Erbium-Ytterbiumphosphoaluminosilicate �bers. We obtained1450W peak power with 102 ns pulse du-ration and 770W for 650 ns pulse durationwith 23% e�ciency and M2<1.4.
CF-7.5 THU 11:45Electro-Optic Sampling of InfraredWaveforms up to 200 THz�S. Keiber1,2, S. Sederberg1, A. Schwarz1,O. Razskazovskaya1, M. Trubetskov1,2, V.Pervak1,2, F. Krausz1,2, and N. Karpowicz1;1Max-Planck-Institut für Quantenoptik,Garching, Germany; 2Fakultät für Physik,Ludwig-Maximilians-Universität, Garching,GermanyElectro-optic sampling is a sensitive tech-nique for electric �eld measurements in theTHz range. We show that it can be used tounambiguously characterize broadband in-frared pulses up to a frequency of 200 THz.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCA-10.5 THU (Invited) 11:30High-power femtosecond thin-diskoscillators�O. Pronin1, J. Brons1, M. Seidel1, J. Zhang1,M. Trubetskov2, D. Bauer3, D. Sutter3, V.Kalashnikov4, A. Apolonski1,2, V. Pervak2,and F. Krausz1,2; 1Max-Planck-Instituteof Quantum Optics, Garching, Germany;2Ludwig-Maximilians-University Munich,Garching, Germany; 3TRUMPF-LaserGmbH and Co. KG, Schramberg, Germany;4Aston University, Institute of PhotonicTechnologies, Birmingham, United KingdomAn overview of the progress on femtosec-ond thin-disk oscillator development overthe two last years is presented. Possible lim-itations of technical and fundamental char-acter as well as future prospects of few-cycle,>100-MW oscillators are discussed.
EA-10.5 THU 11:30Large reduction of quantum �uctuationsof light from a single emitter by an opticalnanostructure�D. Martin-Cano1,3, H.R. Haakh1, K.Murr2,3,4,5, and M. Agio2,3,4; 1Max PlanckInstitute for the Science of Light, Erlangen,Germany; 2National Institute of Optics(CNR-INO), Florence, Italy; 3Center forQuantum Science and Technology in Arcetri(QSTAR), Florence, Italy; 4European Lab-oratory for Nonlinear Spectroscopy (LENS),Sesto Fiorentino, Italy; 5Università di Firenze,Dipartimento di Fisica ed Astronomia, SestoFiorentino, GermanyWe research reduced quantum �uctuationsin the resonance �uorescence from a sin-gle emitter mediated by an optical nanos-tructure. A high control over such squeezedstates of light is feasible, allowing its manip-ulation at the nanoscale.
CB-9.4 THU 11:30Amplitude stability of a two-statequantum dot laser�R. Pawlus1, M. Gioannini2, L. Drzewietzki1,W. Elsäßer1, and S. Breuer1; 1Institute of Ap-plied Physics, Technische Universität Darm-stadt, Darmstadt, Germany; 2Dipartimentodi Elettronica e Telecomunicazioni, Politec-nico di Torino, Torino, Italy�e spectrally-resolved amplitude stabilityof a free-running quantum-dot laser is stud-ied by relative-intensity-noise analysis. Fortwo-state emission a noise-compensation upto 10 dB is found which can be attributedto the unique QD anticorrelated carrier-coupling.
EI-1.4 THU 11:30New enantiomeric phenomena in toroidalmedia�T.A. Raybould1, V.A. Fedotov1, N.Papsimakis1, I.J. Youngs2, W.T. Chen3, D.P.Tsai3, and N.I. Zheludev1,4; 1University ofSouthampton, Southampton, United King-dom; 2DSTL, Salisbury, United Kingdom;3National Taiwan University, Taipei, China,Republic of (ROC); 4Nanyang TechnologicalUniversity, Singapore, SingaporeWe report on the �rst computational studyof a peculiar type of optical activity in ametamaterial structure, underpinned by theexotic resonant combination of an electricquadrupole and a non-negligible toroidaldipole.
JSV-2.5 THU 11:30Waveguide-Coupled Electrically-TunableCavity-Emitter System�M. Petruzzella1, T. Xia1, F.M. Pagliano1, S.Birindelli1, L. Midolo1, Ž. Zobenica1, L. Li2,E. Lin�eld2, and A. Fiore1; 1Eindhoven Uni-versity of Technology, Eindhoven,�e Nether-lands; 2School of Electronic and Electrical En-gineering, University of Leeds, Leeds, UnitedKingdomBy independently controlling the energy ofquantum dots and photonic crystal cavities,we demonstrate the �rst fully-tunable semi-conductor cavity-emitter system. Purcell-enhancement is observed at tunable wave-lengths and the integration with ridgewaveguides is discussed.
EA-10.6 THU 11:45“Ultra” Manipulation: Taking Advantageof Both Conventional Tweezers and AtomOptical Manipulation�M. Juan1, C. Bradac1, B. Besga1, J.Berthelot2, R. Quidant2, G. Molina-Terriza1,and T. Volz1; 1Macquarie University, Sydney,Australia; 2ICFO - �e Institute of PhotonicScience, Barcelona, SpainIn the context of optical manipulation, tworegimes have evolved independently: con-ventional optical tweezers, and laser manip-ulation of atoms. We report on a set of ex-periments capitalizing on the simultaneoususe of those two regimes.
CB-9.5 THU 11:45Repetition rate deviations and timingjitter of passively mode-locked laserssubject to optical feedback from twoexternal optical cavities�O. Nikiforov1, L. Jaurigue2, L. Drzewietzki1,K. Lüdge2, and S. Breuer1; 1Institute of Ap-plied Physics, Technische Universität Darm-stadt, Darmstadt, Germany; 2Institute of�eoretical Physics, Technische UniversitätBerlin, Berlin, GermanyWe study the pulse repetition rate and tim-ing jitter dependencies of a passively mode-locked quantum-dot laser on time-delayedoptical feedback from two external cavitiesand �nd a good qualitative agreement be-tween experiment and simulation.
EI-1.5 THU 11:45Nonparaxial accelerating beams withpre-engineered trajectoriesR.-S. Penciu, V. Paltoglou, and �N. Efremidis;University of Crete, Heraclion, GreeceWepropose a generalmethod for the genera-tion of nonparaxial accelerating beams withprede�ned convex trajectories. Besides cir-cular, elliptic, and parabolic, we �nd for the�rst time power-law and exponential trajec-tories.
JSV-2.6 THU 11:45Light-Emitting Diodes of Non-ClassicalLight Based on Site-Controlled PyramidalQuantum Dots�G. Juska; Tyndall National Institute, Cork,Republic of IrelandA site-controlled, electrically driven sourceof single photons is presented. �e source isbased on highly symmetric Pyramidal quan-tum dots and it has high potential for brightelectroluminescence of single and entangledphotons.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13b14:00 – 15:30CD-13: Nonlinear Phenomena IIIChair: Marco Centini, La Sapienza Univer-sita’ di Roma, Roma, Italy
14:00 – 15:30EH-7: Coherent E�ects inNanophotonicsChair: Kristjan Leosson, University of Ice-land, Reykjavík, Iceland
14:00 – 15:30CL-4: Vibrational and HighResolution Imaging and SensingChair: Herrman O�erhaus, University ofTwente, Enschede,�e Netherlands
14:00 – 15:30CJ-13: �ulium-doped Fibre LaserSystems IChair: W. Andrew Clarkson, University ofSouthampton, Southampton, United King-dom
14:00 – 15:30CF-8: High Harmonic GenerationUltrafast TechnologyChair: Rodrigo Lopez Martens, ENSTA ofParis, Paris, France
CD-13.1 THU 14:00Spontaneous emergence anddisappearance of temporal cavity solitonsin a continuously-driven passive �berresonator�M. Erkintalo, K. Luo, J.K. Jang, S. Coen,and S.G. Murdoch; Dodd-Walls Centre andPhysics Department, �e University of Auck-land, Auckland, New ZealandWe report real-time observations of spon-taneous formation and annihilation of tem-poral cavity solitons in a coherently-driven�ber resonator. Our observations agree withsimulations, and theymatch the route to sta-ble frequency combs observed in microres-onators.
EH-7.1 THU 14:00Unidirectional emission from sphericalnanoparticles: ab-initio simulations andspatial dynamics of a core-shell spaser�J.S. Totero Gongora1, A.E. Miroshnichenko2,Y.S. Kivshar2, and A. Fratalocchi1;1PRIMALIGHT, King Abdullah University ofScience and Technology (KAUST), �uwal,Saudi Arabia; 2Nonlinear Physics Centre,Research School of Physics and Engineering,Australian National University, Canberra,AustraliaWe study the dynamics of a spaser by cou-pling ab-initio simulations and thermody-namic analysis. Spasing action exhibits dif-ferent phases, which produce rotational evo-lution that can be used to achieve unidi-rectional emission from spherical nanopar-ticles.
CL-4.1 THU 14:00Diamond waveguides for mid-IRchemical sensing�M. Malmström1,2, P. Forsberg1, Y. Cai1, M.Karlsson1, F. Nikolaje�1, and F. Laurell2;1Department of Engineering Sciences, Ap-plied Materials Science, Uppsala University,Uppsala, Sweden; 2Department of AppliedPhysics, Laser Physics, Royal Institute ofTechnology (KTH), Stockholm, SwedenMulimode diamondwavegides aremanufac-tured and characterized in terms of propa-gation loss and mode dependence as a �ststep in realizing MIR-spectroscopic mea-surement technique to enable super sensi-tive, label-free detection of chemicals andbiomolecular interactions.
CJ-13.1 THU 14:00200 MW peak power Tm-based �ber CPAsystem and prospects for further powerscaling�F. Stutzki1, C. Gaida1, M. Gebhardt1,2,C. Jauregui1, J. Limpert1,2, and A.Tünnermann1,2,3; 1Institute of AppliedPhysics, Jena, Germany; 2Helmholtz-Institute Jena, Jena, Germany; 3FraunhoferInstitute for Applied Optics and PrecisionEngineering, Jena, GermanyA �ber CPA system with a record peakpower of more than 200MW and an averagepower of 24W is presented. �e further scal-ing potential towards GW-level peak powersis discussed.
CF-8.1 THU 14:00Coherent ultrafast di�raction imaging atthe Abbe limit using a compact highaverage power high harmonic source�M. Zürch1, J. Rothhardt2,3, S. Hädrich2,3,S. Demmler2, M. Krebs2, J. Limpert2,3,A. Tünnermann2,3,4, A. Guggenmos5,6, U.Kleineberg5,6, and C. Spielmann1,3; 1Instituteof Optics and Quantum Electronics, AbbeCenter of Photonics, Jena University, Jena,Germany; 2Institute of Applied Physics, AbbeCenter of Photonics, Jena University, Jena,Germany; 3Helmholtz Institute Jena, Jena,Germany; 4Fraunhofer Institute for AppliedOptics and Precision Engineering, Jena,Germany; 5Ludwig-Maximilians-UniversitätMünchen, Garching, Germany; 6Max-Planck-Institut für Quantenoptik, Garching,GermanyWe demonstrate ultra-high resolution imag-ing at the Abbe limit using high numericalaperture coherent di�raction imaging. �eused �ltered high-average power high har-monic source operated at 33nm wavelengthfurther provides su�cient �ux for real-timeimaging.
CD-13.2 THU 14:15Broadband Fourier-TransformStimulated Raman ScatteringJ. Rehault, F. Crisa�, V. Kumar, M.Marangoni, G. Cerullo, and �D. Polli; Di-partimento di Fisica, Politecnico di Milano,Milano, ItalyWe demonstrate a new approach to broad-band stimulated Raman scattering basedon time-domain-Fourier-transform detec-tion of the stimulated Raman gain. Ourmethod blends the sensitivity of single-channel lock-in detection with the spec-tral resolution of Fourier-transform spec-troscopy.
EH-7.2 THU 14:15Blackbody metamaterial lasers�C. Liu1, J. Huang2, S. Masala3, E.Alarousu3, Y. Han2, and A. Fratalocchi1;1PRIMALIGHT, Faculty of ElectricalEngineering; Applied Mathematics andComputational Science, King Abdullah Uni-versity of Science and Technology., �uwal,Saudi Arabia; 2Advanced Membranesand Porous Materials Center, Divisionof Physical Sciences and Engineering,King Abdullah University of Science andTechnology, �uwal, Saudi Arabia; 3Solarand Photovoltaics Engineering ResearchCenter, Division of Physical Sciences andEngineering, King Abdullah University ofScience and Technology, �uwal, SaudiArabiaWe investigate both theoretically and exper-imentally a new type of laser, which exploitsa broadband light ”condensation” processsustained by the stimulated ampli�cation ofan optical blackbody metamaterial.
CL-4.2 THU 14:15Highly compact, low-noise all-solid-statelaser system for stimulated Ramanscattering microscopy�T. Steinle1, V. Kumar2, A. Steinmann1, M.Marangoni2, G. Cerullo2, and H. Giessen1;14th Physics Institute, University of Stuttgart,Stuttgart, Germany; 2IFN-CNR, Diparti-mento di Fisica, Politecnico di Milano, Mi-lano, ItalyWe present a simple, compact and very ro-bust laser source for low-noise stimulatedRaman scatteringmicroscopy using a single-stage optical parametric ampli�er seededwith tunable cw radiation from an external-cavity diode laser.
CJ-13.2 THU 14:15170 W Single-mode Large Pedestal�ulium-doped Fibre LaserN. Simakov1, �A. Hemming1, A. Carter2,K. Farley2, A. Davidson1, N. Carmody1,J. Daniel1, M. Hughes1, L. Corena1, D.Stepanov1, and J. Haub1; 1Defence Scienceand Technology Organisation, Edinburgh,SA, Australia; 2Nufern Inc., East Granby, CT,United StatesWe present a new large pedestal thulium-doped �bre which enables the constructionof high power, robust, monolithic, all-�brelasers suitable for the optical pumping ofholmium-doped gain media.
CF-8.2 THU 14:15Generation of energetic compressed laserpulses in a planar hollow waveguide forHigh-order Harmonic Generation�A. Jarnac2, F. Brizuela1, C.M. Heyl1, P.Rudawski1, F. Campi1, B. Kim1, L. Rading1,P. Johnsson1, A. Mysyrowicz2, A. L’Huillier1,A. Houard2, and C.L. Arnold1; 1Departmentof Physics, Lund University, P.O. Box 118,22100 Lund, Sweden; 2Laboratoire d’OptiqueAppliquée, ENSTA Paristech, Ecole Polytech-nique, CNRS, 91762 Palaiseau, FranceWe present post-compression of a TW classlaser in a planar hollow waveguide. �e vi-ability of the compressed pulses for applica-tions in strong-�eld physics is demonstratedby generating high-order harmonics in a gasjet.
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEIN14:00 – 15:30CA-11: Nd3+-doped Solid-stateLasers and Ampli�ersChair: Jacob Mackenzie, University ofSouthampton, Southampton, UnitedKingdom
14:00 – 15:30CK-14: Fabrication and Sources inMicro/Nano OpticsChair: Peter G. R. Smith, University ofSouthampton, Southampton, United King-dom
14:00 – 15:30CB-10: Ultrafast SemiconductorLasers and Frequency CombsChair: Stefan Breuer, Technische UniversitätDarmstadt, Darmstadt, Germany
14:00 – 15:30EI-2: Nonlinear DynamicsChair: Gian-Luca Oppo, University of Strath-clyde, Glasgow, United Kingdom
14:00 – 15:30JSV-3: Complex Interferences inWaveguidesChair: Fabio Sciarrino, La Sapienza Univer-sita’ di Roma, Roma, Italy
CA-11.1 THU 14:0011-GHzWaveguide Nd:YAG Laser CWMode-Locked with Monolayer Graphene�A. Okhrimchuk1,2, P. Obraztsov3, M.Rybin3, S. Garnov3, and E. Obraztsova3;1International Center of Laser Technologies,D.Mendeleyev University of ChemicalTechnology of Russia, Moscow, Russia; 2FiberOptics Research Center of RAS, Moscow,Russia; 3Prokhorov General Physics Instituteof RAS, Moscow, RussiaWe report on CW passive mode-lockingin the waveguide Nd:YAG laser inscribedby femtosecond pulses. An atomic layergraphene is used as saturable absorber. CWmode-locking is achieved by controlling theGVD with Gires-Tournois interferometer.
CK-14.1 THU 14:00Integrated Polymer Micro-ball Lenses forTwo-dimensional Divergence Reductionof Light from Single-mode OpticalWaveguides�L. Chang1, M. Dijkstra2, R.M. de Ridder3,K. Worho�4, V. Subramaniam1,5, and H.Kanger1; 1University of Twente, Enschede,�e Netherlands; 2University of Twente,Enschede, �e Netherlands; 3University ofTwente, Enschede,�e Netherlands; 4LioniX,Enschede, �e Netherlands; 5FOM InstituteAMOLF, Amsterdam,�e NetherlandsWe demonstrate a fabrication procedurewhich is suitable for integrating micro-balllenses onto planar channel waveguide chips.In addition, we describe a design procedureand give an optical characterization of themicro-ball lenses.
CB-10.1 THU 14:00An Ultrafast Photonic Crystal Fano Laser�J. Mork, Y. Yu, Y. Chen, M. Heuck, andK. Yvind; Technical University of Denmark,Kongens Lyngby, DenmarkWepropose and analyze a novel type of laser,where one of themirrors is formed by a Fanointerference between a waveguide mode anda nanocavity. �e laser can operate at ultra-high speed.
EI-2.1 THU 14:00Towards a Generalized Weak LangmuirOptical Turbulence�G. Xu1, J. Garnier2, S. Trillo3, M. Conforti4,D. Churkin5, S. Turitsyn5, and A. Picozzi1;1Laboratoire Interdisciplinaire Carnot deBourgogne (ICB), CNRS-University of Bur-gundy, Dijon, France; 2Laboratoire de Prob-abilités et Modèles Aléatoires Université ParisDiderot, Paris, France; 3Department of Engi-neering, University of Ferrara, Ferrara, Italy;4Laboratoire de Physique des Lasers, Atomeset Molécules (PhLAM), CNRS-University ofLille 1, Lille, France; 5Aston Institute of Pho-tonic Technologies, Aston University, Birm-ingham, United KingdomWe show that nonlinear dispersion e�ectsdramatically in�uence the dynamics of in-coherent waves, e.g., by regularizing spec-tral incoherent solitons, or removing spec-tral collapse singularities. �ese results aredescribed by a generalized optical Langmuirturbulence formalism.
JSV-3.1 THU (Invited) 14:00Multiphoton quantum interference inmultiport integrated optical circuits:from teleportation to Boson Sampling�I. Walmsley1, B. Metcalf1, J. Spring1, P.Humphreys1, M. Barbieri3, S. Kolthammer1,J. Gates2, and P. Smith2; 1University of Ox-ford, Oxford, United Kingdom; 2Universityof Southampton, Southampton, United King-dom; 3Universita degli Studi Roma Tre,Roma, ItalyWe describe progress toward multiphotonoperation of integrated optical systems withapplications in quantum information pro-cessing.
CA-11.2 THU 14:15Neodymium Doped Active MediumBased CPA Laser System for OPCPAPumping With Average Output Power of100W and 20ps Output Pulse DurationOperating at 1 kHz repetition rateA. Michailovas1,2, A. Zaukevicius1, �K.Michailovas1, and V. Smilgevicius3;1EKSPLA, Vilnius, Lithuania; 2Institute ofPhysics of Center for Physical Sciences andTechnology, Vilnius, Lithuania; 3VilniusUniversity Laser Research Center, Vilnius,LithuaniaWe present a Neodymium doped activemedium based chirped pulse ampli�er sys-tem providing 100mJ pulses of 20ps in dura-tion at repetition rate of 1kHz that is meantas a pump source for an OPCPA system.
CK-14.2 THU 14:15Enhanced performance ofplasmon-assisted resonant-cavity mid-IRAlxIn�−xSb LEDs�L. Meriggi1, M. Steer1,2, Y. Ding1, A.Samarelli1, I. �ayne1, C. MacGregor2, C.Ironside3, andM. Sorel1; 1School of Engineer-ing, University of Glasgow, Glasgow, UnitedKingdom; 2Quantum Device Solutions, Glas-gow, United Kingdom; 3Department of Imag-ing and Applied Physics, Curtin University,Perth, AustraliaAlxIn�−xSb LED and photodiodes are an ef-fective platform for low cost and fast mid-infrared optical sensors. Extraction e�-ciency and spectral selectivity are signi�-cantly enhanced by resonant-cavity DBR de-sign and surface plasmonic grating.
CB-10.2 THU 14:15Experimental comparison ofextended-cavity passively mode-locked1.5 um quantum well lasers withanti-colliding design and self-collidingdesign�V. Moskalenko; Eindhoven University ofTechnology, Eindhoven,�e NetherlandsWe present a con�rmation of the theoreti-cal prediction of superiority of anti-collidingpulse passive mode-locking design over self-colliding pulse design. Increase of the outputoptical power, reduction of RF linewidth andpulse duration was demonstrated
EI-2.2 THU 14:15Wave Kinetics of Random Fibre Lasers�D. Churkin1,2,3, I. Kolokolov4,5, E.Podivilov2,3, I. Vatnik2,3, M. Nukulin2, S.Vergeles4,5, I. Terekhov3,6, V. Lebedev4,5, G.Falkovich7,8, S. Babin2,3, and S. Turitsyn1,3;1Aston Institute of Photonic Technologies,Aston University, Birmingham, UnitedKingdom; 2Institute of Automation andElectrometry, Siberian Branch of the RussianAcademy of Sciences, Novosibirsk, Russia;3Novosibirsk State University, Novosibirsk,Russia; 4Landau Inst. for �eoreticalPhysics, Russian Academy of Sciences,Chernogolovka, Russia; 5Moscow Inst.of Physics and Technology, Dolgoprudny,Russia; 6�e Budker Inst. of Nuclear Physics,Novosibirsk, Russia; 7Weizmann Inst. of Sci-ence, Rehovot, Israel; 8Inst. for InformationTransmission Problems, Moscow, RussiaWe propose the concept of the wave kineticsof active cyclic systems and formulate �rstever nonlinear kinetic theory of the laser’sspectrum. As an example, we describe thespectrum of random �ber laser.
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ROOM 1 ROOM 4a ROOM 4b ROOM 13a ROOM 13bCD-13.3 THU 14:30Conjugate �elds and negative frequenciesin nonlinear optics�F. Biancalana; Heriot-Watt University, Ed-inburgh, United KingdomWe formulate a conceptually newmodel thatis able to treat the nonlinear interaction be-tween positive and negative frequency com-ponents in pulse propagation.
EH-7.3 THU 14:30Coherent and Incoherent NonlinearEmission from Single Gold Nanorods�V. Knittel, M. Fischer, M. Vennekel, A.Leitenstorfer, and D. Brida; Department ofPhysics and Center for Applied Photonics,University of Konstanz, Konstanz, GermanyWe drive third-harmonic generation andmulti-photon photoluminescence in singlegold nanoantennas with ultrashort pulses.�e comparison between these processesleads to fundamental insights into the ori-gin of the nonlinear-optical response in no-ble metals.
CL-4.3 THU 14:30Innovative nanostructured biochips tocombine SPRI and SERS�A. Olivéro1,4,2, J.-F. Bryche1,3, J.Moreau1, R. Gillibert2,4, G. Barbillon3,M. Sarkar1, M. Lamy de la Chapelle2, B.Bartenlian3, E. Maillart4, and M. Canva1;1Laboratoire Charles Fabry, Palaiseau,France; 2Laboratoire Chimie, Structures,Propriétés de Biomatériaux et d’Agents�érapeutiques, Bobigny, France; 3Institutd’Electronique Fondamentale, Orsay, France;4Horiba Scienti�c, Palaiseau, FranceCoupling SPRI and SERS measurementson a common metallic substrate, in orderto monitor biomolecular interactions andidentify target molecules, is a promising toolfor early diagnosis.
CJ-13.3 THU 14:30�ulium Doped Fibre Laser based on�eta Cavity Lasing DirectionRecti�cation�S. Kharitonov and C.-S. Brès; Ecole Poly-technique Fédérale de Lausanne, Lausanne,SwitzerlandA unidirectional �ulium doped �ber laserexploiting the properties of theta cavity isreported. Uniform operation in the 1880-2055nm range is observed. More than700mW of output power is measured for a25% slope e�ciency.
CF-8.3 THU 14:30Plasma-Mirror Frequency-ResolvedOptical Gating for Characterization ofVUV Pulses�R. Itakura, T. Kumada, M. Nakano, andH. Akagi; Kansai Photon Science Institute,Japan Atomic Energy Agency, Kizugawa, Ky-oto, JapanWe propose and demonstrate a new methodfor characterizing VUV waveform basedon time-resolved re�ection spectra using aplasma mirror formed by an intense laserpulse. �e VUV waveform is retrieved us-ing the FROG algorithm.
CD-13.4 THU 14:45Non Local Binding and IntertwinedDissipative Solitons in Time DelayedVCSELs�M. Marconi1, M. Giudici1, S. Balle2, andJ. Javaloyes3; 1Institut Non Lineaire deNice, Valbonne, France; 2Institut Mediter-rani d’Estudis Avançats, Esporles, Spain;3Departament de Fisica, Universitat de lesIlles Baleares, Palma de Mallorca, SpainWe demonstrate experimentally and theo-retically how a VCSEL submitted to a dou-ble time delayed feedback loop is capable ofgenerating dissipative solitons as polariza-tion slips with, in addition, controlable, nonlocal, interactions for information process-ing.
EH-7.4 THU 14:45Second-harmonic light generated bydipole nanoantennas�D. de Ceglia1, M.A. Vincenti1, C.De Angelis2, A. Locatelli2, J. Haus3,and M. Scalora4; 1National ResearchCouncil, Charles M. Bowden ResearchCenter, RDECOM, Huntsville, UnitedStates; 2Dipartimento di Ingegneriadell’Informazione, Università degli Studidi Brescia, Brescia, Italy; 3Electro-OpticsProgram, University of Dayton, Dayton,United States; 4Charles M. Bowden ResearchCenter, RDECOM, Huntsville, United StatesWe study second-harmonic scattering fromisolated and arrayed dipole nanoantennas.We clarify the role of �eld enhancement andantennamodes for symmetric and asymmet-ric antenna con�gurations, and show how tocontrol the multipolar nonlinear response.
CL-4.4 THU 14:45Coherent Anti-stokes RamanSpectroscopic System withDual-Wavelength OscillatedElectronically Tuned Laser�Y. Maeda1, Y. Nishimoto2, S. Wada1, andH. Sato1; 1RIKEN, Saitama, Japan; 2KwanseiGakuin University, Hyogo, JapanWe have developed a Coherent Anti-stokesRaman Scattering (CARS) spectroscopicsystem by using a dual-wavelength oscil-lated electronically tuned laser and obtainedCARS spectra from chemical materials in�ngerprint region.
CJ-13.4 THU 14:45Coherent combination of two Tm-based�ber ampli�ers at sub-ps pulse duration�C. Gaida1, M. Gebhardt1,3, M. Kienel1,3,M. Müller1,3, A. Klenke1,3, F. Stutzki1,C. Jauregui-Misas1, J. Limpert1,2,3, andA. Tünnermann1,2,3; 1Institute of AppliedPhysics, Jena, Germany; 2Fraunhofer Insti-tute for Applied Optics and Precision Engi-neering, Jena, Germany; 3Helmoltz-Institute,Jena, GermanyCoherent combination of two ultrafast,thulium-based �ber ampli�ers is demon-strated around 2000 nm wavelength for the�rst time. An output of 25 MW at 860 fspulse duration is achieved by successfullymitigating nonlinear e�ects.
CF-8.4 THU 14:45High-throughput and microfocusingcapabilities of a beamline for attosecondpulses based on toroidal mirrors�F. Frassetto1, A. Trabattoni2, G. Sansone2,F. Calegari3, M. Nisoli2,3, and L. Poletto1;1National Research Council, Institute of Pho-tonics and Nanotechnologies, via Trasea7, 35131, Padova, Italy; 2Department ofPhysics, Politecnico di Milano, Piazza L. DaVinci 32, 20133, Milano, Italy; 3National Re-search Council, Institute of Photonics andNanotechnologies, Piazza L. da Vinci 32,20133, Milano, ItalyWe present a novel attosecond beamline de-signed for XUV-XUV pump/probe experi-ments. Microfocusing capabilities, long exitarm at the target area, and high throughputare obtained using only toroidal mirrors.
CD-13.5 THU 15:00Experimental Signature of RiemannWaveShoaling in Optical Fiber�B. Wetzel1, D. Bongiovanni1, M. Kues1, Y.Hu2, Z. Chen2,3, J.M. Dudley4, S. Wabnitz5,and R. Morandotti1; 1INRS-EMT, Varennes,Québec, Canada; 2Nankai University, Tian-jin, China, People’s Republic of (PRC); 3Deptof Physics & Astronomy, San Francisco State
EH-7.5 THU 15:00Coherent Perfect Absorption in a HybridSilicon-Metal Photonic Circuit�S. Zanotto and A.Melloni; Politecnico diMi-lano, Milano, ItalyWe propose the design of a compact and ef-�cient coherent perfect absorber based on ahybrid dielectric-plasmonic waveguide cou-pler, with potential applications in integrated
CL-4.5 THU 15:00Resolution enhancement of wide-�eld�uorescence microscopy with a scatteringlens�H. Yilmaz1, E.G. van Putten1,2, J.Bertolotti1,3, A. Lagendijk1, W.L. Vos1, andA.P. Mosk1; 1Complex Photonic Systems(COPS), MESA+ Institute for Nanotechnol-ogy, University of Twente, P.O. Box 217, 7500
CJ-13.5 THU 15:00Nonlinear compression of ultrashortpulses from a thulium-based �ber laser ina gas-�lled Kagome-type HC-PCF�M. Gebhardt1, C. Gaida1, S. Hädrich1,3, F.Stutzki1, C. Jauregui1, J. Limpert1,2,3, andA. Tünnermann1,2,3; 1Institute of AppliedPhysics, Abbe Center of Photonics, Jena, Ger-many; 2Fraunhofer Institute for Applied Op-
CF-8.5 THU (Invited) 15:00Multidimensional harmonic phasespectroscopyA. Camper, N. Lin, B. Manschwetus, R.Géneaux, E. Skantzakis, V. Gruson, B. Carré,T. Auguste, �P. Salières, and T. Ruchon; CEA,IRAMIS, Lasers, Interactions and DynamicsLaboratory - LIDyL, CEA-SACLAY, Gif-sur-Yvette, France
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ROOM 14a ROOM 14b ROOM 21 ROOM CURIE ROOM EINSTEINCA-11.3 THU 14:30240-GHz smoothly tunablesingle-frequency Nd:YVO4/LBO laser�D. Radnatarov, S. Khripunov, S. Kobtsev,and V. Lunin; Novosibirsk State University,Novosibirsk, Russia�is work has for the �rst time developedand tested a method of automatic contin-uous tuning of second harmonic outputof a CW single-mode and single-frequencyNd:YVO4/LBO laser across a record-widerange of 240 GHz.
CK-14.3 THU 14:30Optical Characteristics of Purely SidewallInGaN/GaN Core-Shell Nanorods GreenLight-Emitting Diodes�T.-P. Chen1, T.S. Kao1, D.-W. Lin1, J.-K. Huang1, A.-J. Tzou2, W.-C. Hsu1, S.-W. Chang3, H.-C. Kuo1, and Y.-F. Chen4;1Department of Photonic & Institute ofElectro-Optical Engineering, National ChiaoTung University, Hsinchu, China, Repub-lic of (ROC); 2Department of Electrophysics,National Chiao Tung University, Hsinchu,China, Republic of (ROC); 3Research Centerfor Applied Sciences, Academia Sinica, Taipei,China, Republic of (ROC); 4Department ofPhysics, National Taiwan University, Taipei,China, Republic of (ROC)Purely-sidewall core-shell nonpolar greenInGaN/GaN LEDs have been successfullydesigned. Electroluminescence measure-ment showed a slight blue-shi� as injectedpower increases. �rough 3-dimention cur-rent spreading layer, a high e�cient 3Dgreen LED device could be achieved.
CB-10.3 THU 14:30Mode-Locked Double Active Region LaserDiode�A. Forrest1, H. Wang2, J. Mi2, B. Cui3,J. Pan2, Y. Ding1,4, and M.A. Cataluna1;1University of Dundee, Dundee, United King-dom; 2Chinese Academy of Science, Beijing,China, Republic of (ROC); 3Beijing Univer-sity of Technology, Beijing, China, Republicof (ROC); 4University of Glasgow, Glasgow,United KingdomWepresent the �rstmonolithicmode-lockedlaser diode with two quantum well active re-gions connected by a GaAs tunnel junction(PiNPiN). Picosecond pulses were achievedat 1040 nm, with a 24 GHz repetition rate.
EI-2.3 THU 14:30Limitation for ultrashort solitons innonlinear optical �bers by cusp formation�U. Bandelow1, S. Amiranashvili1, andN. Akhmediev2; 1Weierstrass Institute forApplied Analysis and Stochastics (WIAS),Berlin, Germany; 2�e Australian NationalUniversity, Canberra, AustraliaA new mechanism preventing formation ofultrashort optical solitons below 1.5 opticalcycles is demonstrated. Indicating univer-sal behavior, many examples exhibit the ap-pearance of unphysical cusp envelopes forshorter solitons, such that they cannot exist.
JSV-3.2 THU 14:30Noise-Enhanced Transport on QuantumMazes�A. Crespi1,2, F. Caruso3,4,5, A.G. Ciriolo2,F. Sciarrino6, and R. Osellame1,2; 1Istitutodi Fotonica e Nanotecnologie - ConsiglioNazionale delle Ricerche, Milano, Italy; 2Dip.di Fisica - Politecnico di Milano, Milano,Italy; 3LENS & Dip. di Fisica e Astronomia -Univ. di Firenze, Sesto Fiorentino (FI), Italy;4QSTAR, Firenze, Italy; 5Istituto Nazionaledi Ottica - Consiglio Nazionale delle Ricerche,Firenze, Italy; 6Dip. di Fisica - Sapienza Uni-versità di Roma, Roma, ItalyWe experimentally demonstrate the role ofnoise in strongly enhancing the transport ef-�ciency on a complex network, by study-ing coherent light propagation in three-dimensional waveguide arrays, fabricated inglass by femtosecond laser pulses.
CA-11.4 THU 14:45Single-frequency Q-switched Nd:YAGMicro-laser with 1.7-ns, 1.6-mJ Pulses at 1kHzH. Iliev1, B. Oreshkov2, D. Chuchumishev2,A. Trifonov2, I. Stefanov2, and �I.Buchvarov3; 1IBPhotonics Ltd., So�a,Bulgaria; 2So�a University, So�a, Bulgaria;3ITMO University, St. Petersburg, RussiaWe present an Nd:YAG micro laser generat-ing 1.7 ns, 1.6 mJ pulses at 1kHz repetitionrate . An RTP Pockels cell is used to obtainsingle frequency output with 470 ps pulse-to-pulse timing jitter.
CK-14.4 THU 14:45Femtosecond Laser Printed Microopticsin Hydrogenated Amorphous Silicon�R. Drevinskas1, M. Beresna1, M.Gecevičius1, M. Khenkin2, A. Kazanskii2,O. Konkov3, Y. Svirko4, and P. Kazansky1;1University of Southampton, Southampton,United Kingdom; 2M.V. Lomonosov MoscowState University, Moscow, Russia; 3A.F. Io�ePhysicotechnical Institute, St. Petersburg,Russia; 4University of Eastern Finland,Joensuu, FinlandFemtosecond laser assisted nanostructuringof hydrogenated amorphous silicon (a-Si:H)is demonstrated. �e laser-induced periodicsub-wavelength structures exhibit dichroismand giant form birefringence giving extra di-mensions to the polarization sensitive print-ing of microoptic elements.
CB-10.4 THU 14:45Spectral broadening of mode-lockedsemiconductor lasers byresonator-internal pulse shaping�B. Döpke1, R.H. Pilny1, C. Brenner1, J.C.Balzer1, A. Klehr2, G. Erbert2, G. Tränkle2,and M.R. Hofmann1; 1Ruhr-UniversityBochum, Bochum, Germany; 2Ferdinand-Braun Institute, Berlin, GermanyIn a modelocked semiconductor laser,resonator-internal phase- and amplitude�lters are optimized for maximum spectralbandwidth using an evolutionary algorithm.Modes of operation of the laser emittingpulses with variable dispersion have beenfound.
EI-2.4 THU 14:45Rogue waves of the Sasa-Satsumaequation in a chaotic wave �eld�N. Akhmediev1, J.-M. Soto-Crespo2, N.Devine1, and N. Ho�mann3,4; 1the Aus-tralian National University, Canberra, Aus-tralia; 2Instituto de Optica, Madrid, Spain;3Hamburg University of Technology, Ham-burg, Germany; 4Imperial College, London,United KingdomWe have found an explanation for theskewed shape of the rogue waves given bythe exact solutions of Sasa-Satsuma equationand calculated the probability density func-tions for various values of the propagationconstant.
JSV-3.3 THU 14:45Bloch Oscillations ofEinstein-Podolsky-Rosen StatesM. Lebugle, M. Gräfe, R. Heilmann, A. Perez-Leija, S. Nolte, and �A. Szameit; Institute ofApplied Physics, Abbe School of Photonics,Friedrich-Schiller Universität Jena, Jena, Ger-manyBloch oscillations of nonlocal quantumstates are experimentally demonstrated.Singular transitions between particleantibunching and bunching are reported,and the results are further linked to thequantum simulation of bosonic, anyonicand fermionic particles.
CA-11.5 THU 15:00Characteristics of a Nd:YAG/diamondComposite Laser Fabricated with theRoom-Temperature Bonding�Y. Okuyama, T. Yamauchi, T. Onda, and I.Shoji; Chuo University, Tokyo, JapanWe have succeeded in cw oscillation ofa Nd:YAG/diamond composite laser fabri-cated with the room-temperature bonding.
CK-14.5 THU 15:00Back-Focal Plane Interferometry ofTrapped Dielectric Particles in a ResonantHollow Photonic Crystal Optical Trap�T. Mario, M. Flavio, D. Nicolas, D. Peru-mal, F. László, J. Sylvia, and H. Romuald;École polytechnique Fédérale de Lausanne,Lausanne, SwitzerlandWe trap sub-micron sized dielectric particle
CB-10.5 THU 15:00Optical Frequency Comb Generatorbased on Quantum-Dash PassivelyMode-Locked Lasers Stabilized withResonant Optical Feedback�K. Merghem1, V. Panapakkam1, C. Calo1,A. Martinez1, F. Lelarge2, and A. Ramdane1;1CNRS Laboratory for Photonics and Nanos-tructures, Marcoussis, France; 2III-V lab, a
EI-2.5 THU 15:00Optical Frequency Comb Generationbeyond the Lugiato-Lefever Equation�T. Hansson1,2 and S. Wabnitz2; 1ChalmersUniversity of Technology, Göteborg, Sweden;2Università degli Studi di Brescia, Brescia,Italy�e generation of optical frequency combsin microresonators with large nonlinear
JSV-3.4 THU 15:00Experimental Realization of ScattershotBoson Sampling�M. Bentivegna1, N. Spagnolo1, C. Vitelli1,F. Flamini1, N. Viggianiello1, L. Latmiral1,P. Mataloni1, D. Brod2, E. Galvão3, A.Crespi4,5, R. Ramponi4,5, R. Osellame4,5,and F. Sciarrino1; 1Sapienza Università diRoma, Rome, Italy; 2Perimeter Institute
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University, San Francisco, United States;4Institut FEMTO-ST / Université de Franche-Comté, Besançon, France; 5Universitá degliStudi di Brescia / INO-CNR, Brescia, ItalyWe report on the generation of Riemannwaves in nonlinear optical �ber. �esepropagation dynamics, associated with theshoaling of appropriately pre-chirped opti-cal pulses, are investigated both numericallyand experimentally.
quantum optics and optical signal process-ing.
AE, Enschede, �e Netherlands; 2Presentaddress: Philips Research Laboratories, 5656AE, Eindhoven, �e Netherlands; 3Presentaddress: Physics and AstronomyDepartment,University of Exeter, Exeter, United KingdomWe present a new wide-�eld microscopymethod that reaches a high-resolution basedon speckle correlations in a high-index im-mersion medium for visible light. Wedemonstrate a two times better resolutioncompared to conventional microscopy.
tics and Precision Engineering, Jena, Ger-many; 3Helmholtz-Institute, Jena, GermanyWe report on nonlinear compressionof ultrashort pulses around two micronwavelength using a gas-�lled Kagome-typehollow-core PCF. Pulse shortening by morethan a factor of two was achieved in a �rstproof-of-principle experiment.
We report on simultaneous measurementsof phase and amplitude of high order har-monics generated in a pumped sample alongseveral space parameter dimensions. Us-ing quantum and optical interferometries,we provide bi-dimensionnal maps of the at-tosecond radiation.
CD-13.6 THU 15:15Phase-Locked, Multiwavelength,Distributed Feedback Brillouin Laser�T.F.S. Buettner, D.D.Hudson, I.V. Kabakova,and B.J. Eggleton; CUDOS, IPOS, School ofphysics, �e University of Sydney, Sydney,AustraliaWe numerically investigate the interplay ofcascaded stimulated Brillouin scattering andKerr-nonlinear four-wave mixing in a su-perstructured Bragg grating for frequencycomb generation. We demonstrate phase-locking between pump and generated Stokesand anti-Stokes waves.
EH-7.6 THU 15:15Hotspot-Induced Vacuum-Field RabiSplitting in a Semiconducting Nanodimeras a Photonic Cavity�M. Uemoto1 and H. Ajiki2; 1Department ofMaterials Engineering Science, Osaka Uni-versity, Osaka, Japan; 2Photon Pioneers Cen-ter, Osaka University, Osaka, JapanWe theoretically study a Rabi splitting of atwo-level emitter placed at the hotspot gen-erated by exciton resonance. In contrast toa plasmonic nanodimer, well-de�ned Rabisplitting spectra appear, maintaining largesplitting energy.
CL-4.6 THU 15:15Temporal Focusing Microscopy with 3DStructured Illumination for EnhancedAxial Resolution in Deep Imaging�Q. Song1,2, K. Isobe1,3, F. Kannari2, H.Kawano4, A. Kumagai4, A. Miyawaki1,4, andK. Midorikawa1; 1RIKEN Center for Ad-vanced Photonics, Wako, Japan; 2Keio Uni-versity, Yokohama, Japan; 3JST, PRESTO,Kawaguchi, Japan; 4RIKEN Brain Science In-stitute, Wako, JapanWe demonstrate multiphoton 3D structuredillumination microscopy by utilizing thetemporal focusing technique to axially con-�ne the excitation in deep imaging. �e axialresolution improvement is available throughspatial intensity modulation along the axialdirection.
CJ-13.6 THU 15:15High-power wavelength-tunablethulium-doped all-�ber super�uorescentsource�J. Liu, H. Shi, C. Liu, and P. Wang; BeijingUniversity of Technology, Beijing, China, Peo-ple’s Republic of (PRC)We demonstrated the power scaling ofnarrow-linewidth thulium-doped all-�bersuper�uorescent source with wavelength-tunable from 1940~2020nm. �e all-�ber super�uorescent source yielded 364Wof output power at central wavelength of1990nm with 3dB spectral bandwidth of2.1nm
ROOM 4b ROOM 13a ROOM 13b ROOM 14a16:00 – 17:30CL-5: Fibre-based Bioimaging and SensingChair: Robert Huber, Universität zu Lübeck, Lübeck, Ger-many
16:00 – 17:30CJ-14: �ulium-doped Fibre Laser Systems IIChair: Fabian Stutzki, University of Jena, Jena, Germany
16:00 – 17:30CF-9: Novel Trends in Ultrafast OpticsChair: Takao Fuji, Institute for Molecular Science ofOkazaki, Okazaki, Japan
16:00 – 17:30CA-12: In-band Pumped Solid-state LasersChair: Yasutake Ohishi, Toyota Technological Institute ofNagoya, Nagoya, Japan
CL-5.1 THU 16:00All-Fiber Burst Mode Femtosecond Laser SystemIntegrated with OCT for Cataract Surgery�D.K. Kesim, H. Kalaycioglu, C. Kerse, and F.O. Ilday;Bilkent University, Ankara, TurkeyWe demonstrate a burst-mode Yb all-�ber femtosecondlaser system integrated with OCT for cataract surgeryand aim to enhance further the procedure with lower col-lateral tissue damage, cleaner, e�cient cuts with compactand robust structure.
CJ-14.1 THU 16:002050 nm Pulse Picker Based Femtosecond ChirpedPulse Fiber Ampli�er System at 362 nJ and 800 kHz�H. Hoogland1,2 and R. Holzwarth1,3; 1Menlo SystemsGmbH, Martinsried, Germany; 2Department of Physics,University of Erlangen-Nuremberg, Erlangen, Germany;3Max-Planck-Institute of Quantum Optics, Garching,GermanyWe report on an all-PM �ber based CPA system at 2050nm emitting ultrashort pulses at 362 nJ pulse energy and392 fs pulse duration at 800 kHz repetition rate.
CF-9.1 THU 16:00Towards dual-channel Yb-pumped broadbandOPCPA synthesizer�A.-L. Calendron1,2,3, H. Cankaya1,2, G. Cirmi1,2, andF.X. Kärtner1,2,3,4; 1Center for Free-Electron Laser Sci-ence, DESY, Hamburg, Germany; 2�e Hamburg Centrefor Ultrafast Imaging, Hamburg, Germany; 3Departmentof Physics, University of Hamburg, Hamburg, Germany;4Department of Electrical Engineering and Computer Sci-ence and Research Laboratory of Electronics, Cambridge,United StatesTwo broadband channels of a passively carrier-envelope
CA-12.1 THU 16:00Highly e�cient Tm3+:Sc2O3 Laser in-band Pumpedby a 1611.5 nm Er Fiber Laser�M. Tokurakawa1, Y. Mashiko1, and C. Kränkel2,3;1Institute for Laser Science, University of Electro-Communications, Tokyo, Japan; 2Institute of Laser-Physics, University of Hamburg, Hamburg, Germany;3�e Hamburg Centre for Ultrafast Imaging, Hamburg,GermanyWe have demonstrated Tm3+:Sc2O3 laser in-bandpumped by a 1611.5 nm Er-�ber laser. �e maximumoutput power of 403 mW and the slope e�ciencies
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�e composite achieved high output powerat high pump power under which the non-composite Nd:YAG was broken.
using hollow photonic crystal cavities withvery low power. �e Brownianmotion of thesingly trapped particles is studied using backfocal plane interferometry.
joint Lab of Alcatel Lucent Bell Labs, �alesResearch & Technology and CEA-LETI, Mar-coussis, FranceAn optical frequency comb generated byan InAs/InP quantum dash based passivelymode-locked laser is investigated. �e combspans ~1.5THz, with 147 modes spaced by~10GHz, and shows a long-term stability of1.5x10-9 over 1230s.
phase-shi�s is considered. We report on nu-merical simulations of the Ikeda map anddiscuss conditions for the validity of the LLEapproximation.
for �eoretical Physics, Waterloo, Canada;3Universidade Federal Fluminense, Niteròi,Brazil; 4Istituto di Fotonica e Nanotecnologie- Consiglio Nazionale delle Ricerche, Milano,Italy; 5Politecnico di Milano, Milano, ItalyWe present an experimental realization ofBoson Sampling with random heralded in-puts, recording up to three-photon events,generated by six di�erent SPDC sources, in-terfering in a 13-mode integrated interfer-ometer.
CA-11.6 THU 15:1556 W cw Nd:YAG solar laser by a heliostat- parabolic mirror system�J. Almeida1, D. Liang1, C. Vistas1, andE. Guillot2; 1CEFITEC, Departamento deFísica, FCT, Universidade Nova de Lisboa,2829-516 Campus de Caparica, Portugal, Ca-parica, Portugal; 2PROMES-CNRS, 7 rue duFour Solaire, 66120, Font Romeu, Odeillo,France, Odeillo, France56W cw solar laser was produced by end-side-pumping a Nd:YAG rod through aheliostat-parabolic mirror system, reach-ing 21.1W/m2 record collection e�ciency.175% enhancement in slope e�ciency overthe previous record was also reported.
CK-14.6 THU 15:151D and 2D photonic structures made bysimple liquid-based process�J. Teisseire1, B. Brudieu1,2, A. Le Bris1,3,I. Gozhyk1, F. Guillemot4, G. Dantelle2, F.Sorin3, and T. Gacoin2; 1Laboratoire deSurface du Verre et Interfaces, Unité mixtede Saint-Gobain/CNRS UMR 125, Aubervil-liers, France; 2Laboratoire de Physique dela Matière Condensée, Ecole Polytechnique,Palaiseau, France; 3Institut des Matériaux,Ecole Polytechnique Fédérale de Lausanne,Lausanne, Switzerland; 4Produits Compos-ites et Revêtements de Surface, Saint-GobainRecherche, Aubervilliers, FranceWe report a sol-gel process resulting in thelarge-areaDistributed Bragg Re�ectors, withexcellent and tunable optical properties andhigh stability, easily integrated within exist-ing optoelectronic architectures and com-patible with other liquid-based techniques.
CB-10.6 THU 15:15Quantum cascade laser Kerr frequencycomb�C. Lecaplain, C. Javerzac-Galy, E. Lucas, J.D.Jost, and T.J. Kippenberg; EPFL-SB-ICMP-LPQM, Lausanne, SwitzerlandWe report quantum cascade laser Kerr combgeneration. For the �rst time QCL lightis coupled into a microresonator via a ta-pered chalcogenide �ber allowing mid-IRKerr comb generation.
EI-2.6 THU 15:15Long-Wavelength Radiation fromFemtosecond Filaments in Gases�O. Kosareva1, V. Andreeva1, N. Panov1,D. Shipilo1, A. Savel’ev1, A. Shkurinov1,L. Bergé2, and S.L. Chin3; 1Departmentof Physics and International Laser Center,Lomonosov MSU, Moscow, Russia; 2CEA,DAM, DIF, Arpajon cedex, France; 3COPLand Departement de physique, UniversiteLaval, Quebec, Canada�e self-consistent 3D+time simulationsidenti�ed new physical mechanisms sup-porting experimentally observed phenom-ena such as 3D Raman light bullet, single-cycle midinfrared pulse generation andenhancement, ring-type transverse shapeof terahertz radiation from the air-basedplasma.
JSV-3.5 THU 15:15E�cient Certi�cation of Boson Samplingin Waveguide Lattices with parity-likeSymmetry�C. Dittel1, R. Keil1, M. Tichy2, A. Perez-Leija3, T. Kauten1, S. Weimann3, M.Lebugle3, A. Szameit3, and G. Weihs1;1Institut für Experimentalphysik, UniversitätInnsbruck, Innsbruck, Austria; 2Departmentof Physics and Astronomy, University ofAarhus, Aarhus, Denmark; 3Institute ofApplied Physics, Abbe Center of Photonics,Friedrich-Schiller-Universität Jena, Jena,GermanyWe present a stringent and e�cient cer-ti�cation method to verify the functional-ity of boson-sampling devices with symmet-ric transformation behavior. �e resultingsuppression law ensures the functionality ofboson-samplers and is applicable even inlarge systems.
ROOM 21 ROOM CURIE ROOM EINSTEIN NOTES16:00 – 17:30CB-11: Advanced Fabrication ofSemiconductor LasersChair: Michel Krakowski, III-V Lab, Palaiseau, France
16:00 – 16:45EI-3a: Multi-physics ModelingChair: Javier de Abajo, ICFO - �e Institute of PhotonicSciences, Barcelona, Spain
16:00 – 17:30JSV-4: Manipulation of QuantumInformation on ChipChair: Mark �ompson, University of Bristol, Bristol,United Kingdom
CB-11.1 THU 16:00DBR based cavities in strained Ge microbridge on200 mm Germanium-On-Insulator (GeOI) substratestowards CMOS compatible laser applications�A. Gassenq1, G. Osvaldo Dias2, K. Guilloy1, S. tardif1,N. Pauc1, D. Rouchon2, J. Widiez2, J.M. Hartmann2,D. Fowler2, A. Chelnokov2, J. Escalante1, I. Duchemin1,Y.M. Niquet1, R. Geiger3, T. Zabel3, H. Sigg3, J. Faist3,F. Rieutors1, V. Reboud2, and V. Calvo1; 1UniversityGrenoble Alpes, INAC-SP2M and CEA, Grenoble, France;2University Grenoble Alpes, CEA-Leti Minatec, Grenoble,France; 3Laboratory for Micro- and Nanotechnology, Paul
EI-3a.1 THU 16:00Simulation of Multi-Scale Optical Devices -Challenging Simulation Applications Handled with aRay-Tracing-FDTD Interface MethodC. Leiner, �W. Nemitz, S. Schweitzer, F.P. Wenzl, G. Pe-harz, P. Hartmann, and C. Sommer; Institute of Sur-face Technologies and Photonics, Joanneum ResearchForschungsges.m.b.H, Weiz, AustriaWe present simulations of optical devices, which arecomposed of di�ractive and refractive optical elements.�ese particular cases require multiple bidirectional in-terfacing between Ray-Tracing and Finite-Di�erence-
JSV-4.1 THU 16:00Quantum phase estimation algorithm on arecon�gurable silicon photonic chip�R. Santagati1, J.W. Silverstone1, M.J. Strain2, M. Sorel2,S. Miki3, T. Yamashita3, M. Fujiwara3, M. Sasaki4, H.Terai3, M.G. Tanner2, C.M. Natarajan2, R.H. Had�eld2,J.L. O’Brien1, and M.G. �ompson1; 1Centre for Quan-tum Photonics, H. H. Wills Physics Laboratory & Depart-ment of Electrical and Electronic Engineering, Universityof Bristol, Bristol, United Kingdom; 2School of Engineer-ing, James Watt South Building, University of Glasgow,,Glasgow, United Kingdom; 3National Institute of Infor-
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phase stabilized Ytterbium-pumped synthesizer with24�J (MIR) and 22�J (NIR) are demonstrated. Synthe-sized pulses as short as 2.3 fs are enabled which can beampli�ed to high energies.
against the 1611.5 nm absorbed pump power of 74%were obtained.
CL-5.2 THU 16:15Development of ultrahigh-resolutionspectral-domain OCT system using supercontinuumsource in 1.7 um wavelength region�H. Kawagoe, M. Yamanaka, and N. Nishizawa; Dept.Quantum Engineering, Nagoya University, Furo-cho,Chikusa-ku, Nagoya 464-8603, JapanUltrahigh resolution spectral domain optical coherencetomography at 1.7 um region was developed for the �rsttime using �ber laser based supercontinuum. Deep tis-sue imaging with axial resolution of less than 5 um wasrealized.
CJ-14.2 THU 16:15150WMOPA Tm3+-doped all-�ber laser system at1908nmC. Yang, Y. Ju, B. Yao, and �T. Dai; Harbin Institute ofTechnology, Harbin, China, People’s Republic of (PRC)We reported a high power Tm3+-doped all-�ber laserwith MOPA architecture. Up to 152W laser operating at1908.1nm was obtained with a total 434W 790nm pumppower, corresponding to the FWHM was 0.13nm.
CF-9.2 THU 16:15Balancing thermal lensing in enhancement cavities�N. Lilienfein1,2, H. Carstens1,2, S. Holzberger1,2, C.Jocher3, T. Eidam3, J. Limpert3, A. Tünnermann3, A.Apolonski1,2, F. Krausz1,2, and I. Pupeza1,2; 1Max-Planck-Institut für Quantenoptik, Garching, Germany;2Ludwig-Maximilians-Universität, Munich, Germany;3Friedrich-Schiller-Universität, Jena, Germany�e compensation of the thermal lensing of an enhance-ment cavity’s mirrors is demonstrated for up to 160 kilo-watt of average power with picosecond pulses using athin fused silica Brewster plate cooled by forced convec-tion.
CA-12.2 THU 16:15Highly e�cient 2066-nm Tm:Lu2O3 ceramic lasersin-band pumped by Raman-shi�ed erbium �ber laserat 1670 nm�O. Antipov1,2, A. Novikov1,2, R. Kositsyn2, S. Larin3,and I. Obronov3; 1Insitute of Applied Physics RAS, NizhnyNovgorod, Russia; 2Nizhny Novgorod State University,Nizhny Novgorod, Russia; 3NTO IRE-Polus, Enterprise,Fryasino Moscow region, RussiaHighly e�cient laser oscillations at 2066 nm inTm:Lu2O3 ceramics in-band pumped at 1670 nm byRaman-shi�ed erbium �ber laser were investigated.Both CW and Q-switched oscillations were achieved inhigh-quality 16-W-power beams.
CL-5.3 THU 16:30Re�ection-mode Confocal Microscopy via aMultimode Fiber�D. Loterie, S. Farahi, D. Psaltis, and C.Moser; École poly-technique fédérale de Lausanne, Lausanne, SwitzerlandWe implement digital confocal microscopy through amultimode �ber. Using a transmission matrix, we canaccurately transmit images through the �ber. A digitalpinhole �ltering method is used to enhance contrast inspot-scanned images.
CJ-14.3 THU 16:30Optimising Tm-Doped Silica Fibres for High LasingE�ciency�P. Shardlow, D. Jain, R. Parker, J. Sahu, and W.A.Clarkson; Optoelectronics Research Centre, Southampton,United KingdomOptimisation of Tm �ber core composition for 70% slopee�ciency at >100W from 793nm pumping is reported.Spatial dopant distribution variations are shown to be thelimiting factor that should be overcome for greater e�-ciency.
CF-9.3 THU 16:30Novel Optimized SESAMs for Kilowatt UltrafastLasersT. Zengerle1, A. Diebold1, M. Mangold1, C. Schriber1, C.Al�eri1, �F. Emaury1, M. Ho�mann2, C.J. Saraceno1,2,M. Golling1, D. Follman3, G.D. Cole3,4, M. Aspelmeyer5,T. Südmeyer2, and U. Keller1; 1Department of Physics,Institute for Quantum Electronics, ETH Zurich, Zurich,Switzerland; 2Laboratoire Temps-Fréquence, Universitéde Neuchâtel, Neuchâtel, Switzerland; 3Crystalline MirrorSolutions LLC, Santa Barbara, United States; 4CrystallineMirror Solutions GmbH, Vienna, Austria; 5Vienna Cen-ter for Quantum Science and Technology (VCQ), Facultyof Physics, University of Vienna, Vienna, AustriaWe present novel high-power SESAMs using a substrateremoval technique. Optimized for kW-level operation,they show signi�cant improvement in terms of surface�atness and provide ideal parameters for high-powermodelocking.
CA-12.3 THU 16:30Compact Sub-Picosecond Multi-mJ Multi-kHzYb:YAG Ampli�er�M. Ue�ng1, T. Pleyer1, R. Lange1, H.G. Barros1, D.Sutter2, T. Metzger3, Z. Major1,4, and F. Krausz1,4;1Ludwig-Maximilians-Universität München, Garching,Germany; 2TRUMPF Laser GmbH, Schramberg, Ger-many; 3TRUMPF Scienti�c Lasers GmbH + Co. KG,München-Unterföhring, Germany; 4Max-Planck-Institutfür Quantenoptik, Garching, GermanyWe present a novel thin-disk laser scheme merging re-generative and multipass ampli�cation without the needfor chirped-pulse ampli�cation. We have generated6.5mJ, 5kHz pulses with potential for further scaling to15-20mJ.
CL-5.4 THU 16:45Rare-earth thermometry using functionalised optical�bre tips for in vivo measurements of braintemperature�E. Schartner1,2, S. Musolino1,3, A. Salem3, M.Hutchinson1,3, and T. Monro1,2; 1ARC Centre of excel-lence for Nanoscale BioPhotonics, Institute for Photonicsand Advanced Sensing, �e University of Adelaide,Adelaide, Australia; 2School of Physical Sciences, �eUniversity of Adelaide, Adelaide, Australia; 3School ofMedical Sciences, �e University of Adelaide, Adelaide,Australia
CJ-14.4 THU 16:45A watt-class narrow-linewidth MOFPA system at 813nm by using a Tm3+ -doped �uoride �ber for the Sroptical lattice clock�E. Kajikawa1, Y.-i. Takeuchi1, K. Kohno1, K. Nakagawa1,and M. Musha1,2; 1Institute for Laser Science, Univer-sity of Electro-communications, Tokyo, Japan; 2InnovativeSpace-time Project, ERATO, JST, Tokyo, JapanA narrow-linewidth MOFPA system at 813 nm using aTm3+ -doped �uoride �ber has been developed with themaximum output power of 1.68 W for the Sr optical lat-tice clock.
CF-9.4 THU 16:45Time Series Analysis of Mode-locked Oscillator CEPNoise�N. Raabe1,2, S. Birkholz1, M. Mero1, Y. Song3, F. Bach1,and G. Steinmeyer1; 1Max-Born-Institut, Berlin, Ger-many; 2Amplitude Technologies, Evry, France; 3School ofPrecision Instruments and Opto-electronics Engineering,Tianjin University, Tianjin, China, People’s Republic of(PRC)Applying the Grassberger-Procaccia algorithm, we an-alyze free-running CEP measurements taken from dif-ferent laser oscillators. We �nd that the utilized �ber
CA-12.4 THU 16:45Graphene mode-locked diode-pumped Cr:LiSAFlaser at 857 nm�F. Canbaz1, N. Kakenov2, C. Kocabas2, U. Demirbas3,and A. Sennaroglu1; 1Koç University, Istanbul, Turkey;2Bilkent University, Ankara, Turkey; 3Antalya Interna-tional University, Antalya, TurkeyWe report, for the �rst time to our knowledge, graphene-based mode-locked operation of a Cr:LiSAF laser. Alow-threshold resonator design enabled the generation of100-fs pulses at 857 nm with only 270 mW of pump.
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Scherrer Institut, Villigen, SwitzerlandIn this work, we will present our processing e�orts onGeOI wafers and highly strained Ge micro-bridges withintegrated distributed Bragg re�ector, in order to fabri-cate suspended strained Ge laser cavities.
Time-Domain simulation methods to achieve physicallycorrect simulation results.
mation and Communications Technology (NICT), Kobe,Japan; 4National Institute of Information and Communi-cations Technology (NICT), Tokyo, JapanWe show a new device and scheme for generating entan-gled two-qubit photonic states on a silicon-on-insulatorchip, and use this system to execute the quantum phaseestimation algorithm.
CB-11.2 THU 16:15Controllable dual-wavelength-stabilized Y-branchDBR diode lasers at 785 nm for shi�ed excitationRaman di�erence spectroscopy�B. Sumpf, M. Maiwald, A. Müller, J. Fricke, P. Res-sel, F. Bugge, G. Erbert, and G. Tränkle; Ferdinand-Braun-Institut, Leibniz Institut für Höchstfrequenztech-nik, Berlin, GermanyIn this contribution controllable dual-wavelength-stabilized Y-branch DBR diode lasers at 785 nm with anoutput power of 215 mW and a side-mode-suppression-ratio better 50 dB suitable for shi�ed excitation Ramandi�erence spectroscopy will be presented.
EI-3a.2 THU 16:15Multiple ionization of noble gases by intensefemtosecond laser pulses enhances THz generation�P. Gonzalez de AlaizaMartinez, A. Debayle, L. Gremillet,and L. Bergé; CEA-DAM-DIF, Arpajon, FranceMultiple ionization of gases is shown to enhance THzgeneration by intense, femtosecond laser pulses. For in-creasing intensities, we demonstrate a cyclic growth inthe THz signal associated with the binding energies ofionized atoms.
JSV-4.2 THU 16:15Towards On-Chip Continuous-Variable QuantumKey DistributionM. Ziebell1,2, �M. Persechino1,3, N. Harris4, C. Galland5,D. Marris-Morini2, L. Vivien2, E. Diamanti3, and P.Grangier1; 1Laboratoire Charles Fabry, Institut d’Optique,CNRS, Univ Paris Sud, Palaiseau, France; 2Institutd’Electronique Fondamentale, Univ Paris Sud, CNRS, Or-say, France; 3Laboratoire Traitement et Communicationde l’Information, CNRS, Télécom ParisTech, Paris, France;4Department of Electrical Engineering and ComputerScience, MIT, Cambridge, United States; 5UniversitätStuttgart, Stuttgart, GermanyWe present experimental progress towards the imple-mentation of continuous-variable quantum key distribu-tion integrated on silicon photonics. �is includes thedesign, fabrication and characterization of a chip imple-menting all the main functionalities of this protocol.
CB-11.3 THU 16:30Monolithic integrated InP distributed Bragg re�ector(DBR) lasers on (001) silicon�B. Tian1, Z. Wang1, M. Pantouvaki2, W. Guo2, P. Absil2,J.V. Campenhout2, C. Merckling2, and D.V. �ourhout1;1INTEC Department, Ghent University, Ghent, Belgium;2IMEC, Leuven, BelgiumWe presented a room temperature optical-pumped InPin-plain DBR laser monolithic integrated on (001)-silicon substrate. �is is also our �rst device demonstra-tion based on the selectively grown InP with high crys-talline quality.
EI-3a.3 THU 16:30Classical Entanglement: �eory and Application�F. Töppel1,2, A. Aiello1,2, C. Marquardt1,2, E.Giacobino1,3, and G. Leuchs1,2; 1Max Planck Insti-tute for the Science of Light, Erlangen, Germany;2Institute for Optics, Information and Photonics,Universität Erlangen-Nürnberg, Erlangen, Germany;3Laboratoire Kastler Brossel, Université Pierre et MarieCurie, Ecole Normale Supérieure, CNRS, Paris, FranceCylindrically polarized beams of light exhibit the re-markable feature of non-separability (“classical entangle-ment”) between di�erent degrees of freedom. Borrow-ing ideas from quantum information theory, we showclassical-optics applications that bene�t from this uniqueproperty.
JSV-4.3 THU 16:30Toward an Optically-Integrated Quantum RandomNumber Generator�C. Abellán1, W. Amaya1, M.W. Mitchell1,2, andV. Pruneri1,2; 1ICFO-Institut de Ciencies Fotoniques,Castelldefels, Spain; 2ICREA-Institució Catalana de Re-cerca i Estudis Avançats, Barcelona, SpainA new quantum random number generator based on thebeating of two semiconductor lasers is proposed. Initialexperimental results indicate the possibility to achievemulti-Gb rates using photonics integrated circuits
CB-11.4 THU 16:45Single-mode 1180 nm GaInNAs/GaAs DBR laserdiode for frequency doubling to 590 nm�V.-M. Korpijärvi, J. Viheriälä, A. Aho, and M. Guina;Optoelectronics Research Centre (ORC) / Tampere Univer-sity of Technology, Tampere, FinlandWe report a single-mode dilute nitride GaInNAs/GaAsdistributed Bragg re�ector laser diode emitting at 1180nm. �e laser exhibited an output power of 290 mW at adriving current of 1060 mA.
JSV-4.4 THU 16:45Towards On-Chip Quantum Networks based on SpinQubits in Diamond�T. Schröder1, L. Li1, E.H. Chen1, S. Mouradian1,M. Walsh1, I. Bayn1, M.E. Trusheim1, J. Zheng1,M. Lu2, M. Cotlet2, H. Bakhru3, M.L. Markham4,D.L. Twitchen4, C.B. Poitras5, M. Lipson5, and D.Englund1; 1Massachusetts Institute of Technology, Cam-bridge, United States; 2Brookhaven National Laboratory,Upton, United States; 3SUNY Polytechnic Institute, Al-bany, United States; 4Element Six, Santa Clara, UnitedStates; 5Cornell University, Ithaca, United States
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ROOM 4b ROOM 13a ROOM 13b ROOM 14a
We report on the fabrication of a temperature sensorbased on a thin layer of erbium:ytterbium doped tellu-rite glass on the tip of an optical �bre, and its use in an invivo setting.
lasers exhibit stochastic behavior, while the Ti:Sa oscilla-tormeasurements surprisingly indicate deterministic dy-namics.
CL-5.5 THU 17:00Towards a multimode �ber two-photon endoscope�E.E. Morales Delgado1, S. Farahi1,2, I. Papadopoulos2,D. Psaltis2, and C. Moser1; 1Laboratory of Applied Pho-tonics Devices, School of Engineering, École Polytech-nique Fédéral de Lausanne (EPFL), Lausanne, Switzer-land; 2Laboratory of Optics, School of Engineering, ÉcolePolytechnique Fédéral de Lausanne (EPFL), Lausanne,SwitzerlandWe generate spatially focused femtosecond pulses with-out modal dispersion through a multimode �ber usingdigital phase conjugation. Scanning of the focus and two-photon absorption is demonstrated, showing the feasibil-ity of ultra-thin multiphoton endoscopy.
CJ-14.5 THU 17:00Targeting di�erent pulsing regimes in Tm �ber laserwith a nonlinear amplifying loop mirror�J. Peng, Z. Yu, M. Malmström, F. Laurell, and V. Pasiske-vicius; Royal Institute of Technology, KTH, Stockholm,SwedenDi�erent pulsed oscillation regimes in Tm-doped �gure-8 �ber laser with amplifying nonlinear loop mirrorcan be selectively and reliably targeted by adjusting theroundtrip gain and the amplifying Sagnac loop polariza-tion bias.
CF-9.5 THU 17:00Dual-comb femtosecond enhancement cavity forprecise study of ionization dynamics and intracavityhigh harmonic generationD. Carlson, T.-H. Wu, and �R.J. Jones; University of Ari-zona, Tucson, United StatesWe show two high power phase coherent fs frequencycombs can be coupled to the same enhancement cavityfor performing precise time-resolved measurements ofoptical nonlinearities and potentially simplifying dual-comb spectroscopy in the XUV.
CA-12.5 THU 17:00Frequency-Agile Ti:Sapphire Laser System with HighPower and High Pulse Energy for SpectroscopicApplications�S. Metzendorf, V. Wulfmeyer, A. Behrendt, F. Späth, andA. Riede; University of Hohenheim, Institute of Physicsand Meteorology, Stuttgart, GermanyA high-power frequency-stabilized pulsed Tita-nium:Sapphire laser system operating via injection-seeding alternately at two wavelengths near 818 nm ispresented. It is applied as transmitter for a mobile watervapor Di�erential Absorption Lidar.
CL-5.6 THU 17:15Fiber-optic control and thermometry of single-cellthermosensation logic with NV-centers�I. Fedotov; Physics Department, International Laser Cen-ter, M.V. Lomonosov Moscow State University, Moscow,Russia; Russian Quantum Center,, Skolkovo, Russia; De-partment of Physics and Astronomy, Texas A&M Univer-sity, College Station, United States�ermal activation and online thermometry of individ-ual cells have been demonstrated using a �ber-opticprobe integrated with an NV-diamond quantum sensor.A diamond microcrystal heated by laser radiation trans-mitted through the �ber provides a local heating of thecell culture.
CJ-14.6 THU 17:15Null-frequency-shi� acousto-optic tunable �lter forwavelength tuning of a Tm �bre laser�P. Shardlow1, J. Ward2, C. Pannell2, S. Valle2, and W.A.Clarkson1; 1Optoelectronics Research Centre, Southamp-ton, United Kingdom; 2Gooch and Housego (UK), Ilmin-ster, United KingdomA novel null-frequency shi� acouto-optic tunable �lter isdeveloped and utilised for tuning a thulium doped �brelaser for rapid electronic control of output spectrum from1940-2115nm at >20W output power.
CF-9.6 THU 17:15100 THz optical switching with plasmonicmetamaterial�V. Nalla1, S. Vezzoli1, J. Valente2, S. Handong1, andN. Zheludev1,2; 1Centre for Disruptive Photonic Tech-nologies, Nanyang Technological University, Singapore,Singapore; 2Optoelectronics Research Centre and Centrefor Photonic Metamaterials, University of Southampton,Southampton, United KingdomUsing femtosecond laser with variable pulse duration weprobe the limits of switching that exploits coherent ab-sorption in nanostructured gold �lms. Switching con-trast ratios of 7:1 with a modulation bandwidth exceed-ing 100THz has been observed.
CA-12.6 THU 17:15Electro-optic Q-switching using PolarisationDependant�ermal Lensing�L. Maweza, G. King, N. Du Preez, and H. Strauss; Na-tional Laser Center, CSIR, Pretoria, South AfricaWe introduce an Electro-optic Q switching techniquethat reduces the need for a polariser by exploiting the po-larisation dependence of the thermal lens e�ect of a cutuniaxial gain materials. It was experimentally demon-strated with success.
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Wediscuss progress towards on-chip quantumnetworks.We describe NV-nanocavity systems in the strong Pur-cell regime and electron spin-coherence exceeding 200*s;NV creation in cavity-�eld maxima; and hybrid on-chipnetworks for integration of NV-cavity systems.
CB-11.5 THU 17:00Array with 24 distributed Bragg re�ector lasers forscanning applications: Fabrication andcharacterisation�O. Brox, J. Fricke, A. Klehr, A. Maaßdorf, M. Matalla,H. Wenzel, and G. Erbert; Ferdinand-Braun-Institut,Leibniz-Institut für Höchstfrequenztechnik, Berlin, Ger-manyWe present a diode laser array with small footprint in-corporating 24 individually addressable ridge waveguideDBR lasers. For wavelengths stabilisation around 905 nmwe apply 3rd order E-beam de�ned surface Bragg grat-ings.
JSV-4.5 THU 17:00Integrated Photonic Transmitter and Receiver forQuantum Key Distribution�P. Sibson1, M. Godfrey1, C. Erven1, S. Miki2, T.Yamashita2, M. Fujiwara3, M. Sasaki3, H. Terai2, M.Tanner4, C. Natarajan4, R. Had�eld4, J. O’Brien1, and M.�ompson1; 1Centre for Quantum Photonics, Universityof Bristol, Bristol, United Kingdom; 2National Instituteof Information and Communications Technology, Kobe,Japan; 3National Institute of Information and Communi-cations Technology, Tokyo, Japan; 4University of Glasgow,Glasgow, United KingdomWe demonstrate an integrated photonic transmitter andreceiver for multi-protocol quantum key distribution.�is Indium Phosphide device prepares states for Coher-ent One Way, Di�erential Phase Shi�, and BB84 proto-cols, decoded by a Silicon Oxynitride receiver.
CB-11.6 THU 17:15�-Stripes Quantum Cascade Lasers Arrays at 4.6�m�S. Ferré, B. Simozrag, V. Trinité, and M. Carras; III-VLab, Palaiseau, FranceWepresent a step towards high-powerQuantumCascadeLasers (QCLs) in the 3-5�mwavelength range in contin-uous mode. We report �-stripes QCLs arrays emittingat 4.6�m, with electrical an optical characterization andanalysis.
JSV-4.6 THU 17:15Implementation of the Fourier-Kravchuk transformin Photonic LatticesS. Weimann1, A. Perez-Leija1, M. Lebugle1, M.C. Tichy2,R. Keil3, and �A. Szameit1; 1Institut für AngewandtePhysik, Jena, Germany; 2Department of Physics and As-tronomy, Aarhus, Denmark; 3Institut für Experimental-physik, Innsbruck, AustriaWe report on the experimental realization of a discreteand �nite Fourier transform using photonic lattices. Oursystem operates integrated and independent of the input.We investigate the transformation of classical and quan-tum light.
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HALL B013:00 – 14:00CG-P: CG Poster Session
CG-P.1 THUUltra-Broadband Spectral Phase Control in theVulcan 20PW Upgrade Front End�A. Wyatt, P. Oliveira, A. Boyle, Y. Tang, M. Galimberti,I. Ross, I. Musgrave, C. Hernandez-Gomez, and J. Collier;STFC Central Laser Facility, Didcot, United KingdomOptimal compression from a CP-OPCPA is demon-strated numerically and experimentally via simultaneousadaptive spectral shaping of the pump and signal pulses.A new design for the Vulcan 20PW front end based onthis is presented.
CG-P.2 THUGenetic optimization of attosecond–pulse generationin light–�eld synthesizers�B. Bódi1, E. Balogh2, V. Tosa3, E. Goulielmakis4,K. Varjú2, and P. Dombi1; 1MTA Lendület UltrafastNanooptics Group, Wigner Research Centre for Physics,Budapest, Hungary; 2Department of Optics and Quan-tum Electronics, University of Szeged, Szeged, Hungary;3National Institute for R&D of Isotopic and MolecularTechnologies, Cluj–Napoca, Romania; 4Max Planck Insti-tut für Quantenoptik, Garching, GermanyWeoptimized an existing light-�eld-synthesizer with ge-netic algorithm to achieve di�erent (single and double)atto-pulse shapes based on single-atom response. Ro-bustness of results was checked with 3D propagationcode.
CG-P.3 THUTowards controlled sub-cycle waveforms in the nearinfrared�A. Schwarz1,2, X. Geng3,4, H. Fattahi1,2, O.Razskazovskaya1, S. Keiber1,2, D.E. Kim3,4, F. Krausz1,2,and N. Karpowicz1; 1Max-Planck-Institut für Quan-tenoptik, Garching, Germany; 2Ludwigs-Maximilians-Universität, München, Germany; 3Center for AttosecondScience and Technology, POSTECH, Pohang, Korea,South; 4Max Planck Center for Attosecond Science,Pohang, Korea, SouthSpectral broadening of a 2.1 �mOPCPA source in a hol-low core �ber yields a super-continuum spanning overalmost 3 octaves. �e carrier-envelope phase-stabilitywas characterized and the pulses appear to be partlycompressed.
CG-P.4 THUSub-Cycle Timing Lock in a Multi-mJ ParametricWaveform Synthesizer�S. Fang1, R. Mainz1,2, G.M. Rossi1,2, Y. Yang1,2, G.Cirmi1, S.-H. Chia1,2, C. Manzoni3, G. Cerullo3, O.D.
Mücke1, and F.X. Kärtner1,2,4; 1Center for Free-ElectronLaser Science, DESY, and the Hamburg Center for Ul-trafast Imaging, Hamburg, Germany; 2Physics Depart-ment, University of Hamburg, Hamburg, Germany; 3IFN-CNR, Dipartimento di Fisica, Politecnico di Milano, Mi-lan, Italy; 4Department of Electrical Engineering andComputer Science and Research Laboratory of Electronics,Massachusetts Institute of Technology, Cambridge, UnitedStatesWe actively stabilize the timing jitter of a multi-mJ, >2-octave-wide optical parametric waveform synthesizerwith a balanced optical cross-correlator. We obtain aresidual rms timing jitter of 360 as measured over thewhole Nyquist range.
CG-P.5 THUSpatio-temporal Isolation of Attosecond Pulses at300 eV: Attosecond Lighthouse at the Water Window�F. Silva1, S.M. Teichmann1, S.L. Cousin1, M. Hemmer1,and J. Biegert1,2; 1ICFO-Institut de Ciencies Fotoniques,Barcelona, Spain; 2ICREA-Institució Catalana de Recercai Estudis Avançats, Barcelona, SpainWe demonstrate spatio-temporal isolation of attosecondpulses in the water window through the combination oflong-wavelength driven high-harmonic generation andthe attosecond lighthouse e�ect, generating so�-Xraysup to 300 eV.
CG-P.6 THU�e High-intensity HHG beamline at the Lund LaserCentre: towards XUV-pump XUV-probe experiments�H. Coudert-Alteirac1, F. Campi1, M. Miranda1, L.Rading1, B. Manschwetus1, B. Farkas2, P. Rudawski1, S.Maclot1, C.M. Heyl1, F. Brizuela1, B. Kim1, A. L’Huillier1,and P. Johnsson1; 1Department of Physics, Lund Univer-sity, Lund, Sweden; 22ELI-HU Non-Pro�t Ltd, Szeged,HungaryIn our high-intensity HHG beamline, we present a newsetup which splits and delays XUV attosecond pulses. Itwill lead towards XUV-autocorrelation and XUV pump-probe experiments, allowing probing attosecond dy-namics in molecules through nonlinear ionization.
CG-P.7 THUGeneration of XUV supercontinua through control ofattosecond pulse interferences�W. Holgado1, C. Hernández-García1,2, B. Alonso1,3, M.Miranda4, F. Silva3, L. Plaja1, H. Crespo3, and Í.J. Sola1;1Universidad de Salamanca, Salamanca, Spain; 2JILA,University of Colorado at Boulder, Boulder, United States;3Universidade do Porto, Porto, Portugal; 4Lund Univer-sity, Lund, SwedenBy controlling NIR pulse chirp and phase matching con-ditions, it is possible to generate XUV supercontinua in
a standardHHG setup. Such a spectrum arises from par-ticular interference conditions of the di�erent generatedattosecond pulses.
CG-P.8 THUResonant high-order harmonic generation andampli�cation of XUV pulses�M. Khokhlova1,2 and V.V. Strelkov1; 1�eoretical De-partment, General Physics Institute of Russian Academyof Sciences, Moscow, Russia; 2Department of Physics, M.V. Lomonosov Moscow State University, Moscow, RussiaWe suggest analytical quantum-mechanical theory de-scribing generation of harmonic resonant with the tran-sition between ground and autoionizing state of the gen-erating particle. �is theory describes both harmonicamplitudes and phases needed for attopulse generationimproving.
CG-P.9 THUDirect High-Order Harmonic Radiation as a Tool forthe Characterization of Femtosecond Filaments�M. Kretschmar1, C. Brée2, T. Nagy1,3, H.G. Kurz1, U.Morgner1, and M. Kovacev1; 1Leibniz Universität Han-nover, Institut für Quantenoptik, Hannover, Germany;2Weierstrass Institut für Angewande Analysis, Berlin,Germany; 3Laser-Laboratorium Göttingen e.V., Göttin-gen, GermanyWepresent themeasurement of high-order harmonic ra-diation directly from a �lament. �e XUV-radiation al-lows for the determination of the on-axis intensity as wellas a conclusion on pulse characteristics along the �la-ment’s propagation axis.
CG-P.10 THUCarrier-wave Rabi �opping signatures in high-orderharmonic generation�M. Ciappina1, J.A. Pérez-Hernández2, A. Landsman3,T. Zimmermann4, M. Lewenstein5,6, L. Roso2, andF. Krausz1,7; 1Max-Planck Institut für Quantenop-tik, Garching, Germany; 2Centro de Láseres Pulsa-dos (CLPU), Salamanca, Spain; 3Max-Planck Insti-tut für Physik complexer Systeme, Dresden, Germany;4Physics Department, ETH Zurich, Zurich, Switzer-land; 5ICFO-Institut de Ciènces Fotòniques, Castellde-fels, Spain; 6ICREA-Institució Catalana de Recercai Estudis AvanÇats, Barcelona, Spain; 7Departmentfür Physik, Ludwig-Maximilians-Universität München,Garching, GermanyWe perform numerical simulations of high-order har-monic generation (HHG) in order to demonstrate sig-natures of the carrier-wave Rabi �opping phenomenon(CWRF) in real atoms. We show peculiar structures ap-pears in the spectra in this regime.
CG-P.11 THUNear-Ionization-�reshold Emission inHigh-Harmonic Generation Driven by Single-CyclePulses�W.-C. Chu, F. Tani, K.F. Mak, J. Travers, and P. Russell;Max Planck Institute for the Science of Light, Erlangen,GermanyWemodel high-harmonic generation driven by a single-cycle pulse. A delayed monochromatic signal slightlyabove the ionization-threshold frequency is seen, corre-sponding to the emission from nearly-bound electronsfollowing the driving pulse.
CG-P.12 THUNonlinear Phase Measurements in FemtosecondEnhancement Cavities�S. Holzberger1,2, N. Lilienfein1,2, H. Carstens1,2, T.Saule1,2, F. Lücking2, M. Trubetskov1, V. Pervak2,T. Eidam3, J. Limpert3, A. Tünnermann3, E. Fill1,2,F. Krausz1,2, and I. Pupeza1,2; 1Max-Planck-Institutfür Quantenoptik, Garching, Germany; 2Ludwig-Maximilians-Universität München, Garching, Germany;3Friedrich-Schiller-Universität Jena, Jena, GermanyWe investigate enhancement limitations of femtosecondpulses in a passive optical resonator with a gas target.Using spatial-spectral-interferometry we quantitativelyvalidate a �t-parameter-free model predicting the cavityperformance in a broad parameter range.
CG-P.13 THUSub-femtosecond control at conical intersections�M. Richter1,2, F. Bouakline1, J. González-Vázquez3, L.Martínez-Fernández3, I. Corral3, S. Patchkovskii1, F.Morales1, M. Ivanov1,2, F. Martín3, and O. Smirnova1;1Max-Born Institute, Berlin, Germany; 2Department ofPhysics, Imperial College London, London, United King-dom; 3Departmento de Química, Universidad Autónomade Madrid, Madrid, SpainWe present numerical evidence of the sub-femtosecondcontrol over a conical intersection (CI) topology, usingan ultrashort near-infrared laser pulse as a carving toolto sculpt the nuclear wavepacket while passing throughthe CI region.
CG-P.14 THUTime-resolved Dynamical Franz-Keldysh e�ect�T. Otobe1, K. Yabana2, Y. Shinohara3, S. Sato2, and G.Bertsch4; 1Japan Atomic Energy Agency, Kyoto, Japan;2Univ. of Tsukuba, Tukuba, Japan; 3Max-Planck Insti-tute, Halle, Germany; 4Univ. of Washington, Seattle,United StatesWe present theoretical investigation for the dynamicFranz-Keldysh e�ect in sub-femtosecond time resolu-tion. Our ab-inito simulation and the analytical formula
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HALL B0predict the phase shi� between themodulation of the di-electric function and the electric �eld.
CG-P.15 THUBohmian-trajectory Analysis of Enhanced Ionizationof Molecules in Intense Laser Fields�R. Sawada1,2, T. Sato2,3, and K. Ishikawa1,2,3;1Department of Applied Physics, Graduate School ofEngineering, �e University of Tokyo, Tokyo, Japan;2Photon Science Center, Graduate School of Engineering,�e University of Tokyo, Tokyo, Japan; 3Department ofNuclear Engineering and Management, Graduate Schoolof Engineering,�e University of Tokyo, Tokyo, JapanWe theoretically investigated the mechanism of en-hanced ionization using Bohmian trajectory for one-dimensional hydrogen molecule. We �nd the ionizationfrom down-�eld core contributes as well although theionization from up-�eld core has been o�en highlighted.
CG-P.16 THUAdiabatic and Dynamic Stabilisation of Ionisation:Hunting for Kramers-Henneberger states�M. Matthews1, J. Gateau1, A. Patas2, N. Berti1, A.Lindinger2, S. Hermelin1, J. Kasparian2, L.Woste1, and J.-P.Wolf1; 1Geneva University, Geneva, Switzerland; 2FreieUniversitat, Berlin, Germany�e contribution has been withdrawn by the authors.
CG-P.17 THU�eoretical Study of Ultrafast Electron Dynamics inAmino AcidsD. Ayuso1, A. Palacios1, P. Decleva2, and �F. Martín1,3;1Departamento de Química, Módulo 13, Universidad Au-tonoma de Madrid, Madrid, Spain; 2Dipartimento diScienze Chimiche e Farmaceutiche, Università di Trieste,Trieste, Italy; 3InstitutoMadrileño de Estudios Avanzadosen Nanociencia, Cantoblanco, Madrid, Spain
We present a theoretical study of ultrafast electron dy-namics initiated upon attosecond excitation in the aminoacids glycine and phenylalanine, occurring in a sub-femtosecond time scale and therefore preceding any nu-clear rearrangement.
CG-P.18 THUFrequency-resolved optical gating technique to re-trieve the amplitude of a vibrational wavepacket of H+
2�Y. Nabekawa1, Y. Furukawa1, T. Okino1, A. AmaniEilanlou1, E. Takahashi1, K. Yamanouchi2, and K.Midorikawa1; 1RIKEN, Saitama, Japan; 2University ofTokyo, Tokyo, JapanWe propose a novel algorithm to retrieve the com-plex amplitude of each wavefunction in the vibrationalwavepacket of H+
2 , which is based on the frequency-resolved optical gating technique used for characterizingultrashort optical pulses.
CG-P.19 THUE�ect of Chirp on Direct Electron Acceleration byTightly Focused TM01 Laser Pulses�P. Hogan-Lamarre1, V. Marceau1, C. Varin2, T. Brabec2,and M. Piché1; 1Centre d’Optique, Photonique et Laser,Université Laval, Québec, Canada; 2Center for Researchin Photonics, University of Ottawa, Ottawa, CanadaNumerical simulations using exact solutions toMaxwell’s equations for radially polarized chirpedlaser pulses reveal that chirp can reduce the maximumenergy achievable by direct electron acceleration inmostpractical situations.
13:00 – 14:00CH-P: CH Poster Session
CH-P.1 THUAutocollimation architecture of all-�ber Dopplervelocity meterA. Pavlov1,2, Y. Pyrkov1,2, and �V. Tsvetkov2; 1MoscowInstitute of Physics and Technology (State University),Moscow, Russia; 2General Physics Institute, Moscow, Rus-siaTest measurements with use of air ri�e IZh-61 bulletwere made. �e speed resolution of set-up is estimatedto be about 5 cm/s. Both high-speed and low-speed phe-nomena accompanying a ri�e shot were analyzed.
CH-P.2 THUSimulation and design of compact photoacoustic gassensors�B. Parvitte, C. Risser, R. Vallon, and V. Zéninari; Groupede Spectrométrie Moléculaire et Atmosphérique, UMR7331 CNRS Université de Reims, Reims, France�is paper present the design and simulation of com-pact photoacoustic gas sensors using the �ermoacous-tics module of Comsol Multiphysics as the equations ofpressure acoustics are not accurate enough for small res-onant cells.
CH-P.3 THUCoherent beam combining using an internally sensedoptical phased array with multiple phase locked slavelasers�L. Roberts1, R. Ward1, R. Fleddermann1, S. Raj1, A.Sutton2, G. de Vine2, D. McClelland1, and D. Shaddock1;
1�e Australian National University, Canberra, Aus-tralia; 2Jet Propulsion Laboratory, Pasadena, UnitedStatesWe present the design and characterisation of an inter-nally sensed optical phased array that uses three individ-ually phase locked lasers for coherent beam combining,demonstrating quadratic intensity scaling and excellentoutput beam stability.
CH-P.4 THUBeam Quality Deterioration Due to AngularDispersion of Optical Elements�S. Mokhov; CREOL - the College of Optics and Photonics,UCF, Orlando, United States�e deterioration of M2 from unity due to angulardispersion for non-monochromatic Gaussian beam isfound analytically. It depends on beam size and mean-square variation of optical element angular dispersionaveraged with beam spectral distribution.
CH-P.5 THUFibre Bragg Grating Sensor Interrogation Systemusing a VCSEL and Correlation Techniques�C. Triana1,2, M. Varón-Durán2, andD. Pastor1; 1Optical& Quantum Communications Group, ITEAM ResearchInstitute, Universidad Politécnica de Valencia, Valencia,Spain; 2High Frecuency Electronics and CommunicationsResearch Group, Universidad Nacional de Colombia, Bo-gotá, ColombiaWe report a low-cost interrogator for FBG sensors basedon a VCSEL source. �e system is able to identify theinitial and �nal points of the time-wavelength readoutby using a correlation procedure.
CH-P.6 THUUltrafast IR Laser Written FBG Sensors for NuclearEnvironments�M. Ams1,2, M. Fabian2, S. Antipov1, A. Pal3, R. Sen3,A. Fuerbach1, M. Withford1, T. Sun2, and K. Grattan2;1Macquarie University, Sydney, Australia; 2City Univer-sity London, London, United Kingdom; 3Central Glassand Ceramic Research Institute (CGCRI), Kolkata, Aus-traliaWe report the feasibility of using optical sensors in nu-clear environments where the presence of highly ener-getic radiation is a concern. �e response of various �breBragg gratings exposed to gamma radiation is presented.
CH-P.7 THUCharacterising a Re�ection Grating for a VUVSpectrometer Using Optical Surface Pro�ling�D. Kane, D. Little, and R. Carman; Macquarie Univer-sity, Sydney, AustraliaOptical surface pro�ling of a grating (~2000 square mi-crons) allows the distribution of step height to be quan-ti�ed. �e distribution has a positive impact for VUVgratings because wavelengths yielding zero di�ractione�ciency are avoided.
CH-P.8 THUA New Approach to Design of a Mach-ZehnderInterferometer with a Porous-FilmWaveguide�N. Raicevic1,2, A. Maluckov1, and J. Petrovic1; 1VincaInstitute of Nuclear Sciences, Belgrade, Serbia and Mon-tenegro; 2School of Electrical Engineering, University ofBelgrade, Belgrade, Serbia and MontenegroA porous-�lm based waveguide interferometer is pro-
posed as a sensor of �uid concentration. Its nonlinearresponse yields the maximum sensitivity at a particular�uid refractive index. �e maximum sensitivity is esti-mated via the Fisher information.
CH-P.9 THUErbium-doped Y2O3 nanocrystals for temperaturesensingA.C. Brandão-Silva, M. Gomes, �J. Ávila, J.J. RodriguesJr., Z. Macedo, and M. Alencar; Universidade Federal deSergipe, São Cristóvão, Brazil�e performance of Y2O3 nanocrystals, produced viaPVA-assisted sol-gel route, in which polyvinyl alcohol isemployed in the polymerization step, as nanothermome-ters was investigated and the crystals size’s in�uence onthe sensor sensitivity was evaluated.
CH-P.10 THUWhispering-Gallery Modes in Multimode Fibres:Experimental evidence and ray tracing model�Y. Padilla Michel1,2, P. Steglich1,2, S. Schrader1, andM. Casalboni2; 1Technical University of Applied ScienceWildau, Wildau, Germany; 2University of Rome Tor Ver-gata, Rome, ItalyHere, we show that it is possible to produceWGM in thecoating of a bent MMF.�is WGM in MMF are suitableto develop high-sensitive resonators exploiting the coat-ing modes, resembling a coil resonator.
CH-P.11 THUSingle micro-particle scattering detection based onEdge Filter Enhanced Self-Mixing Interferometry�V. Contreras1, J. Lonnqvist2, and J. Toivonen1; 1Tampere
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HALL B0University of Technology, Tampere, Finland; 2VaisalaOyj,Helsinki, FinlandWe describe a novel self-mixing interferometer capa-ble of detecting single microparticle scattering events.�e signal detection, based on frequency to intensitymodulation mapping, yields to about two orders ofmagnitude larger SNR than conventional self-mixing-interferometry.
CH-P.12 THUNear-infrared adaptive interferometric sensing basedon liquid crystal light valve�A. Peigné1,2,3, U. Bortolozzo2, S. Residori2, S. Molin3, P.Nouchi3, D. Dol�3, and J.-P. Huignard4; 1�ales Under-water Systems, Sophia Antipolis, France; 2INLN, Univer-sité de Nice-Sophia Antipolis, Valbonne, France; 3�alesResearch and Technology France, Palaiseau, France;4Jphopto, Paris, FranceAdaptive interferometry o�ers new possibilities in vi-brometry applications. Our technique, based on a liquidcrystal light valve, is presented. It leads to low frequencyphase perturbations �ltering such as those coming fromtemperature or vibrations.
CH-P.13 THUSpatial Heterodyne Spectrometer for LIBSApplications�M. Lenzner1, C. Feng2, and J.-C. Diels2; 1Lenzner Re-search LLC, Tucson, United States; 2University of NewMexico, Albuquerque, United StatesA modi�ed Spatial Heterodyne Spectrometer (SHS) isused for measuring the spectrum in LIBS experiments.�e resolution of the device is su�cient to resolve com-mon isotopic lines.
CH-P.14 THUNoise Modelling and Measurement of HighSensitivity Photonic Crystal Fibre-optic Gyroscope�F. Teng, J. Jin, Z. Zhang, and C. Zhang; Beihang Uni-vercity, Beijing, China, People’s Republic of (PRC)�e incoherent back-re�ected and backscattered lightin photonic crystal �bre interferometer �bre-optic gy-roscope was investigated quantitatively. An accuratenoise model which takes incoherent back-re�ection andbackscattering noise into account was proposed and ver-i�ed by experiments.
CH-P.15 THUDirect Detection Doppler Lidar using a ScanningFabry-Perot Interferometer and a Single-PhotonCounting Module�P.J. Rodrigo and C. Pedersen; DTU Fotonik, Departmentof Photonics Engineering, Technical University of Den-mark, Roskilde, Denmark
A monostatic coaxial direct detection Doppler lidar us-ing a scanning Fabry-Perot interferometer and a single-photon counting module is experimentally demon-strated at 787 nm operating wavelength.
CH-P.16 THUIncoherent Broadband Cavity Enhanced AbsorptionSpectroscopy with a Supercontinuum Source�C. Amiot1,2, A. Aalto1, G. Genty1, and J. Toivonen1;1Physics Department, Tampere University of Technol-ogy, Tampere, Finland; 2Institut FEMTO-ST, UMR 6174CNRS-Université de Franche-Comté,, Besançon, FranceWe demonstrate cavity enhanced absorption spec-troscopy in the near/mid-IR using a supercontinuumsource. �e full absorption band of methane at 1.65 umwasmeasuredwith excellent dynamic range achieved us-ing a careful data �tting procedure
CH-P.17 THUCharacterization of axial non-uniformities insingle-mode �bers at the subnanometer scale byedge-interrogated time-resolved acousto-optics�E. Alcusa-Sáez1, A. Díez1, M. González-Herráez2, andM.V. Andrés1; 1Universidad de Valencia, Burjassot,Spain; 2Universidad de Alcalá, Alcalá de Henares, SpainAn edge interrogation approach is introduced to im-prove the performance of the time-resolved acousto-optic technique for axial non-uniformity analysis insingle-mode �bers. Detection of subnanometer diam-eter changes, or sub-ppm core refractive index changesis demonstrated.
CH-P.18 THUSpectroscopy of liquid-�lled microstructured optical�bres.B. Wajnchold1, �A. Uminska1, M. Grabka1, A. Rygula2,3,D. Kotas1, M. Golunski1, S. Pustelny1, and W. Gawlik1;1Marian Smoluchowski Institute of Physics, JagiellonianUniversity, Krakow, Poland; 2Faculty of Chemistry, Jagiel-lonian University, Krakow, Poland; 3Jagiellonian Centerfor Experimental �erapeutics, JAgiellonian University,Krakow, Poland�e absorption measurements of the liquid-�lled pure-silica microstructured optical �bres were performed.�e measurements concentrate on spectroscopic analy-sis of the water solutions of cationic dyes, oxazine 725perchlorate and bromophenol blue sodium salt.
CH-P.19 THUOptical Comb-Based, Wide Bandwidth HybridElectro-Optic Probing System�B. Gouhier, K.-L. Lee, A. Nirmalathas, C. Lim, and E.Ska�das; Dep. of Electrical and Electronic Engineering,�e University of Melbourne, Melbourne, Australia
In this paper, we study the performance of a novelelectro-optic probing system which aims at providingTHz bandwidth without the need of a complex pump-probe set-up used in conventional EO sampling systems.
CH-P.20 THUAnalysis of the Angle Dependency in Inscription ofthe Fiber Bragg Gratings in the MicrostructuredPolymer Optical Fibers�I.-L. Bundalo, K. Nielsen, and O. Bang; Technical Uni-versity of Denmark (DTU Fotonik), Lyngby, Denmark24 Fiber Bragg Gratings were inscribed in Microstruc-tured Polymer Optical Fibers (mPOFs) with randominscription angle. We investigated grating quality andspeed of writing dependency to the laser inscription an-gle in mPOFs.
CH-P.21 THUBeam Focalization in Re�ections from FlatSubwavelength Gratings�Y.C. Cheng1, H. Zeng2, J. Trull1, C. Cojocaru1, M.Malinauskas3, T. Jukna4, D. Wiersma2, J. Redondo5,and K. Staliunas1,6; 1Departament de Física i Enginy-eria Nuclear, Universitat Politècnica de Catalunya, Ter-rassa, Spain; 2European Laboratory for Non Linear Spec-troscopy (LENS), University of Florence, Sesto Fiorentino,Italy; 3Laser Research Center, Department of Quan-tum Electronics, Vilnius University, Vilnius, Lithuania;4Department of Technologies, Panevezys Faculty of Tech-nologies and Business, Kaunas University of Technologies,Panevezys, Lithuania; 5Instituto de Investigacion para laGestion Integrada de Zonas Costeras, Universitat Politec-nica de Valencia, Gandia, Spain; 6Institucio Catalana deReserca i Estudis Avançats (ICREA), Barcelona, Spain�e �at focusing mirror without an optical axis has beendemonstrated with subwavelength gratings based on lat-eral di�usion of a narrow beam. A focal length of 10micrometers is achieved for visible light.
CH-P.22 THUEstimation of an Unknown Phase using SqueezedStates and Real-Time Feedback Control�T. Gehring1, A.A. Berni1, B.M. Nielsen1, V. Händchen2,M.G.A. Paris3, andU.L. Andersen1; 1Technical Universityof Denmark, Kgs. Lyngby, Denmark; 2Albert-Einstein-Institut, Hannover, Germany; 3Universit degli Studi diMilano, Milano, ItalyWe demonstrate phase estimation beyond the coherentstate limit by using squeezed light as probe states, ho-modyne detection and Bayesian estimation. We use real-time feedback to the homodyne detector to achieve op-timal estimation performance.
CH-P.23 THUSmall refractive index, high performance:magnesium �uoride whispering gallery moderesonators for refractometric sensingF. Sedlmeir1,2,3, R. Zeltner1,2, G. Leuchs1,2, and �H.G.L.Schwefel1,2; 1Max Planck Institute for the Science of Light,Günther-Scharowsky-Str. 1, Bau 24, Erlangen, Germany;2Institut für Optik, Information und Photonik, Univer-sity of Erlangen-Nuremberg, Staudtstraße 7/B2, Erlangen,Germany; 3SAOT, School in Advanced Optical Technolo-gies, Paul-Gordan-Straße 6, Erlangen, GermanyFor refractometric sensingMgF2WGM-resonators haveadvantages over silica microspheres: their refractive in-dex is close to that of water and they are birefrigent. Weshow why this may be bene�cial and present �rst exper-imental results.
CH-P.24 THUOptical Microbubble Resonator�icknessMeasurements by Means of Re�ectance ConfocalMicroscopyA. Cosci1,2, F. Quercioli3, D. Farnesi1,2, S. Berneschi2, A.Giannetti2, F. Cosi2, A. Barucci2, F. Baldini2, G. NunziConti2, S. Soria2, �S. Pelli1,2, and G. Righini1,2; 1MuseoStorico della Fisica e Centro Studi e Ricerche EnricoFermi, Roma, Italy; 2IFAC-CNR, Istituto di Fisica Appli-cata ’Nello Carrara’, Consiglio Nazionale delle Ricerche,Firenze, Italy; 3INO-CNR, Istituto Nazionale di Ottica,Consiglio Nazionale delle Ricerche, Firenze, ItalyOptical Microbubble Resonators are new emerging op-tical sensors. Simulations show strong relationship be-tween the resonator thickness and its sensitivity. Wepropose a new non-destructive method to evaluate theMicrobubble thickness using confocal re�ectance mi-croscopy.
CH-P.25 THUStrong antiresonant re�ection guiding in apoly(methyl-methacrylate) hollow-core optical �berC. Markos, �J.K. Mølgaard Pedersen, K. Nielsen, and O.Bang;DTUFotonik, Department of Photonic Engineering,Technical University of Denmark, Kgs. Lyngby, DenmarkWe report the fabrication and characterization of an an-tiresonant hollow coremicro-structured polymer optical�ber. �e �ber revealed strong resonances in the range480-900nm. �e thermal sensitivity of the �ber is ~256pm/C.
CH-P.26 THUFerro�uid in�ltrated multicapillary microstructuredoptical �bers for endoscopic applications�E. Tagoudi1, H. Ottevaere2, D. Pysz3, R. Buczynski3, andS. Pissadakis1; 1Foundation for Research and Technology-Hellas,Institute of Electronic Structure and Laser, Her-
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HALL B0aklion, Creta, Greece; 2Vrije Universiteit Brussel, Brus-sels Photonics Team, Brussels, Belgium; 3Institute of Elec-tronic Materials Technology, Warsaw, Poland�is paper outlines preliminary experimental results onthe use ofmagnetic�eld for tuning the spectral transmis-sion properties of amulti-capillary glass optical �ber uti-lizing in�ltrated ferro�uids, while targeting endoscopicimaging applications.
CH-P.27 THUMeasurement of�ermal Pro�les of FBGs UsingWhispering Gallery ModesM. Delgado-Pinar, I.L. Villegas, �A. Díez, J.L. Cruz, andM.V. Andrés; Universidad de Valencia, Valencia, SpainWe present a technique that enables the measurementof inhomogeneous temperature pro�les of FBGs, basedon the use of whispering gallery modes. �e techniquerelies on the high sensitivity of WGMs to temperaturevariations.
CH-P.28 THUSimultaneous super-resolution and multichannelblind deconvolution of Raman spectra calibrated byan optical frequency comb�K. Chen, T. Wu, H. Wei, and Y. Li; Key Lab of PrecisionMeasurement Technology & Instrument, Beijing, China,People’s Republic of (PRC)A unifying approach to high resolution Raman spec-troscopy based on simultaneous blind deconvolutionand sub-pixel shi� of multiple degraded spectra is estab-lished. Both �ne structure of isotopic e�ect and poly-morphs are retrieved in our framework.
CH-P.29 THULaser Absorption Trace Gas Monitor with a TunableHigh Finesse External Cavity for Clinical BreathAnalysis�R. Someya1, T. Imamura1, T. Okamoto1, N. Toyoshima2,M. Asobe3, K. Tei3, and S. Yamaguchi3; 1Power and
Industrial System R&D Center, Toshiba Corp., kana-gawa, Japan; 2Healthcare Company, Toshiba Corp., tokyo,Japan; 3Tokai University, kanagawa, JapanA tunable cavity enhanced absorption spectroscopic sys-tem is successfully demonstrated for trace gas sensor.Multiple gas detection can be achieved with a single lightsource using a simple tuning schematic between 1.5umand 1.7um.
CH-P.30 THUDual frequency comb interferometer for fast andhigh resolution optical spectroscopy�E. Portuondo-Campa, J. Bènnes, S. Kundermann, andS. Lecomte; Centre Suisse d’Electronique et de Microtech-nique (CSEM), Neuchâtel, SwitzerlandA dual comb fourier interferometer was built for NIRspectroscopy. �e system provides a unique combina-tion of high resolution (0.07 /cm) with high speed scan-ning (2 ms/scan), based on non-stabilized femtosecondlasers.
CH-P.31 THUTemperature Sensing and Sensor Design using a New�ermographic Phosphor for a Wide Range ofApplications�F. Venturini1, R. Bürgi1, S. Borisov2, and I. Klimant2;1Institute of Applied Mathematics and Physics, ZurichUniversity of Applied Sciences, Winterthur, Switzerland;2Institute of Analytical Chemistry and Food Chemistry,Graz University of Technology, Graz, Austria�e luminescence emission of the new phosphorChromium(III)-doped yttrium aluminum borate wasanalyzed in a broad temperature range. �e resultsdemonstrate the high suitability of this material to de-velop a robust, inexpensive but sensitive sensor.
CH-P.32 THUExperimental Characterization of the Anisotropy ofthe Elasto-Optic E�ect in Optical Fibers under AxialStrainX. Roselló-Mechó, M. Delgado-Pinar, A. Díez, and �M.V.Andrés; Universidad de Valencia, Burjassot, Spain�e experimental characterization of the elasto-opticanisotropy, generated in a standard optical �ber underaxial strain, is carried out by means of the TE- and TM-polarized whispering gallery modes of the �ber itself.
CH-P.33 THUIn-line extraction of an ultra-stable frequency signalover an optical �ber link�A. Bercy1,2, F. Stefani2,1, S. Guellati-Khelifa3, G.Santarelli4, C. Chardonnet1, P.-E. Pottie2, O. Lopez1,and A. Amy-Klein1; 1Laboratoire de Physique des Lasers,Université Paris 13, Sorbonne Paris Cité, CNRS, Vil-letaneuse, France; 2Laboratoire National de Métrolo-gie et d’Essais Système de Références Temps-Espace,UMR 8630 Observatoire de Paris, CNRS, UPMC, Paris,France; 3Laboratoire Kastler-Brossel, UPMC, ENS, CNRS,Paris, France; 4Laboratoire Photonique, Numériqueet Nanosciences, Université de Bordeaux 1, Institutd’Optique and CNRS, Talence, FranceOptical frequency links give the possibility to transfer anultrastable frequency reference to a distant laboratory.We demonstrate the extraction of an ultrastable signalalong an urban �ber link, opening the way to multiple-users dissemination.
CH-P.34 THUE�ects of 1/f frequency noise in self-heterodynelinewidth measurement system with various delaylengths�Q. Hu, P.J. Rodrigo, and C. Pedersen; Technical Univer-sity of Denmark, Roskilde, Denmark�e e�ect of 1/f frequency noise on self-heterodyne de-tection and its implication on laser linewidth measure-
ments are demonstrated experimentally. �e results areapplied to remote wind sensing measurements using co-herent Doppler LIDARs.
CH-P.35 THUMultilayer Filter Using the Borrmann E�ect for EUVSource Monitoring�J. Barreaux1, I. Kozhevnikov3, B. Bastiaens1, R. van deKruijs2, F. Bijkerk2, and K. Boller1; 1Laser Physics andNonlinear Optics, MESA+ Institute for Nanotechnology,University of Twente, Enschede, �e Netherlands; 2XUVOptics, MESA+ Institute for Nanotechnology, Universityof Twente, Enschede, �e Netherlands; 3Institute of Crys-tallography, Russian Academy of Sciences, Moscow, Rus-siaWe present the design of narrow-band multilayer �ltersbased on the Borrmann e�ect for monitoring of EUVsources. For 13.5 nm, �lters with a narrow spectral trans-mission of 0.23 nm are feasible.
CH-P.36 THUComb-Assisted Sub-kHz-Linewidth OpticalParametric Oscillator for High-PrecisionSpectroscopy�I. Ricciardi1, S. Mosca1, M. Parisi1, P. Maddaloni1, L.Santamaria1, G. Giusfredi2, P. De Natale2, and M. DeRosa1; 1CNR-INO, Istituto Nazionale di Ottica, Poz-zuoli (NA), Italy; 2CNR-INO, Istituto Nazionale di Ottica,Firenze, ItalyWe demonstrate a comb-assisted transfer-oscillatorscheme for sub-kHz line narrowing of the idler mode ofa singly-resonant optical parametric oscillator, emittingin the frequency range between 2.7 and 4.2 �m.
13:00 – 14:00EA-P: EA Poster Session
EA-P.1 THUFocusing characteristics of a 4 π parabolic mirror forhighly e�cient light matter interaction�L. Alber1,2, M. Fischer1,2, M. Bader1,2, S. Heugel1,2,K. Mantel1, M. Sondermann1,2, and G. Leuchs1,2,3;1Max Planck Institute for the Science of Light, Erlangen,Germany; 2Friedrich-Alexander University Erlangen-Nürnberg, Erlangen, Germany; 3University of Ottawa,Ottawa, Canada
We characterize the focusing properties of a parabolicmirror scanning the focus with an ion. �e results are re-produced by simulations based on interferometric testsof the mirror. We demonstrate light-matter couplingwith 27% e�ciency.
EA-P.2 THUQuantum state control with atoms and cavities�M. Penasa, T. Rybarczyk, B. Peaudecerf, S. Gerlich, S.Gleyzes, J.-M. Raimond, M. Brune, S. Haroche, and I.Dotsenko; Collège de France, Paris, FranceWe measure the photon number in a microwave cavityprobed by circular Rydberg atoms using the Past Quan-
tum State approach. It leads to a considerable noise re-duction and allows us to access normally hidden infor-mation.
EA-P.3 THUPhotoionizing 174Yb+ to 174Yb2+�M. Fischer1,2, S. Heugel1,2, V. Elman2, M.Sondermann1,2, and G. Leuchs1,2,3; 1Max Planck In-stitute for the Science of Light, Erlangen, Germany;2Institute of Optics, Information and Photonics, Uni-versity of Erlangen-Nuremberg, Department of Physics,Erlangen, Germany; 3Department of Physics, Universityof Ottawa, Ottawa, Canada
We demonstrate the fully-resonant photo-ionization of174Yb+ to 174Yb2+ with weak continuous-wave lasers atultraviolet-wavelengths. �e successful ionization is ver-i�ed by checking the motional dynamics of the mixed-species ion-crystal.
EA-P.4 THUOptical trapping of quantum dots in a deep parabolicmirror�V. Salakhutdinov1,2, M. Manceau3, A. Bramati3, E.Giacobino3, M. Sondermann1,2, and G. Leuchs1,2; 1MaxPlanck Institute of the Science of Light, Erlangen, Ger-many; 2University Erlangen-Nuremberg, Institut of Op-
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HALL B0tics, Information and Photonics, Erlangen, Germany;3Laboratoire Kastler Brossel, Universit Pierre et MarieCurie, Paris, FranceWe demonstrate the optical trapping of ’dots-in-rods’nano-crystals in the focus of a deep parabolic mirror.�is approach promises to enable e�cient light-matterinteraction in free space for various solid-state basedquantum emitters.
EA-P.5 THUMultimode Semiconductor WaveguideCharacterization by Fourier Analysis of the OpticalTransmission Spectrum�B. Pressl1, T. Günthner1, K. Laiho1, J. Geßler2, S.Hö�ing2,3, M. Kamp2, C. Schneider2, and G. Weihs1,4;1Institut für Experimentalphysik, Universität Innsbruck,Innsbruck, Austria; 2Technische Physik, UniversitätWürzburg, Würzburg, Germany; 3School of Physics & As-tronomy, University of St Andrews, St Andrews, UnitedKingdom; 4Institute for Quantum Computing, Waterloo,CanadaFourier analysis of the optical transmission spectra ofmultimode semiconductor waveguides reveal informa-tion beyond the well-known Fabry-Pérot technique.Characteristics important for quantum photonics, likerelative modal excitation, propagation loss or dispersionare easily estimated in-situ.
EA-P.6 THUMode Splittings in Microscopic Fabry-PerotResonators�M. Upho�, M. Brekenfeld, S. Ritter, and G. Rempe; MaxPlanck Institut für Quantenoptik, Garching, Germany�e frequency splitting of polarization eigenmodes inmicrofabricated Fabry-Perot cavities is investigated. We�nd e�ects of the mirror geometry to be the dominantsource and present a theory in excellent agreement withour experimental results.
EA-P.7 THUNanowire quantum dot molecules�T. Huber1, A. Predojević1, M. Khoshnegar2, D. Dalacu3,P.J. Poole3, H. Majedi2, and G. Weihs1,2; 1Institut für Ex-perimentalphysik, Universität Innsbruck, Innsbruck, Aus-tria; 2Institute for Quantum Computing, University ofWaterloo, Waterloo, Canada; 3National Research Coun-cil of Canada, Ottawa, CanadaWe present optical investigations of quantum dotmolecules embedded into nanowires.
EA-P.8 THUTime-bin Entangled Photons from a SemiconductorQuantum DotA. Predojević1, L. Ostermann2, T. Huber1, �M. Pril-
müller1, G.S. Solomon3, H. Ritsch2, and G. Weihs1;1Institut für Experimentalphysik, Universität Innsbruck,Innsbruck, Austria; 2Institut für�eoretische Physik, Uni-versität Innsbruck, Innsbruck, Austria; 3Joint Quantuminsitute, National Institute of Standards and Technology,Gaithersburg, United StatesWe present our latest results on time-bin entangled pho-tons from a single semiconductor quantum emitter.
EA-P.9 THUBiphoton evolution equation for discrete opticalsystems�A. Perez-Leija1, M. Gräfe1, M. Lebugle1, R. Heilmann1,S. Nolte1, H. Moya-Cessa2, D. N. Christodoulides3, andA. Szameit1; 1Institute of Applied Physics, Abbe School ofPhotonics, Friedrich-SchillerUniversität Jena, Jena, Ger-many; 2INAOE, Coordinacion de Optica,, Tonantzintla,Puebla, Mexico; 3CREOL, �e College of Optics & Pho-tonics, University of Central Florida, Orlando, Florida,United StatesIn this work we demonstrate, theoretically and exper-imentally, that two-photon probability amplitudes de-scribing propagation of light in any two-photon stateare governed by an evolution equation identical to a 2Dtight-binding equation.
EA-P.10 THUTemporal coherence and correlation ofcounter-propagating twin photons�A. Gatti1,2, T. Corti2, and E. Brambilla2; 1Istitutodi Fotonica e Nanotecnologie del CNR, Milano, Italy;2Dipartimento di Scienza e Alta Tecnologia, Universitàdell’Insubria, Milano, ItalyWe investigate the quantum correlation and the tempo-ral coherence of twin photons counterpropagating in pe-riodically poled crystals, showing a peculiar transitionfrom a high temporal entanglement to a separable stateas the pump spectrum broaden
EA-P.11 THUTemporal shaping of heralded photons in aresonator-assisted parametric down-conversion withmodulated pump pulses�V.A. Averchenko1,2, M. Förtsch1,2, M. Fischer1,2, A.Aiello1,2, C. Marquardt1,2, and G. Leuchs1,2; 1Max-Planck Institute for the Science of Light, Erlangen, Ger-many; 2Institute for Optics, Information and Photonics,University of Erlangen-Nuernberg, Erlangen, GermanyWe theoretically study temporal shaping of heraldedphotons via the modulation of pump pulses driving theparametric process in the resonator-assisted con�gura-tion. Agreement with the corresponding experimentwith nonlinear whispering gallery mode resonator is ob-tained
EA-P.12 THUPhoton-Number Squeezed Pulse Generation withSymmetric Mach-Zehnder Interferometer�A. Hosaka, K. Hirosawa, R. Sawada, and F. Kannari;Keio University, Yokohama, JapanA -3.1dB photon-number squeezed state was generatedwith a symmetric �ber interferometer instead of com-monly used asymmetric interferometers in the normaldispersion regime. We numerically proved the merit ofthis scheme.
EA-P.13 THUAdvances in vacuummagnetic linear birefringenceusing pulsed �elds�R. Battesti, A. Cadène, A. Rivère, M. Fouché, and C.Rizzo; Laboratoire National Champs Magnétiques In-tenses (CNRS UPR3228), Toulouse, FranceIn this contribution we will present the advances on themeasurement of the vacuummagnetic birefringence ob-tained using pulsed magnetic �elds at the National HighMagnetic Field Laboratory of Toulouse, France.
EA-P.14 THUImportance of excitation and trapping conditions inphotosynthetic energy transportR. Leon-Montiel1,2, I. Kassal3, and �J. Torres1,4; 1ICFO- �e Institute of Photonic Sciences, Barcelona, Spain;2Instituto Nacional de Astro�sica, Optica y Electronica,Puebla, Mexico; 3Centre for Engineered Quantum Sys-tems, Brisbane, Australia; 4Universitat Politecnica deCatalunya, Barcelona, SpainWe discuss how realistic models of excitation and trap-ping for modelling energy transport in photosyntheticsystems can lead to very di�erent predictions about theimportance of environment-assisted quantum transport(ENAQT).
EA-P.15 THUQuantum Process Estimation with an UnknownDetectorB. Smith, �M. Cooper, and M. Karpinski; University ofOxford, Oxford, United KingdomQuantumprocess estimationwithout assumptions aboutmeasurements used is presented. �e detector responseis characterized with a �nite set of probe states. Numeri-cal simulations for quantum optical processes demon-strate the technique for complex systems.
EA-P.16 THUCoherence studies of broadband light states emittedby quantum-dot superluminescent diodes�F. Friedrich1, S. Hartmann1, W. Elsäßer1,2, and R.Walser1; 1Institute of Applied Physics, Technical Univer-sity Darmstadt, Darmstadt, Germany; 2also with Cen-
ter of Smart Interfaces, Technical University Darmstadt,Darmstadt, GermanyWe show that multi-mode phase-randomized Gaussianstates are well suited to describe broadband light emittedby quantum-dot superluminescent diodes. �is is veri-�ed by comparison of their �eld- and intensity correla-tion functions with experimental results.
EA-P.17 THUExperiments on the quantum statistics of broadbandlight states from quantum-dot superluminescentdiodes�S. Hartmann1, F. Friedrich1, A. Molitor1, M. Reichert1,W. Elsäßer1,2, and R. Walser1; 1Institute of AppliedPhysics, Technical University Darmstadt, Darmstadt,Germany; 2also with Center of Smart Interfaces, Techni-cal University Darmstadt, Darmstadt, GermanyWe perform two experiments in which tunable photonstatistics on femtosecond timescales are realized withampli�ed spontaneous emission from quantum-dot su-perluminescent diodes. �e results are discussed in thecontext of an analytical quantum theoretical approach.
EA-P.18 THUFrequency-Dependent Squeezed Light for Surpassingthe Standard-Quantum-Limit in a MacroscopicOptomechanical System�S. Chua, L. Neuhaus, S. Zerkani, T. Briant, S. Deleglise,P.-F. Cohadon, and A. Heidmann; Laboratoire KastlerBrossel, Paris, FranceWe present the design of a Frequency-dependentsqueezed light source for surpassing the Standard Quan-tum Limit of a macroscopic quartz-micropillar optome-chanical cavity. We also present the squeezing-ellipse an-gle controls that allow choice of squeezed quadrature.
EA-P.19 THUPrecision inference of a mechanical element using aMach-Zender interferometer with an optomechanicalcavity.�R. Garcés1 and G.J. Milburn2; 1Departament d’Òptica,Universitat de València, València, Spain; 2ARC Centrefor Engineered Quantum Systems, School of Mathemat-ics and Physics, �e University of Queensland, Brisbane,AustraliaWe show an increase in the precision in the inference ofthe position of a mechanical element, using N-photonwave packets in a Mach-Zender interferometer with anoptomechanical cavity in one of its inner arms.
EA-P.20 THUDegenerate parametric oscillation in membranecavity optomechanics�C. Navarrete-Benlloch1, C. Sánchez Muñoz2, and M.
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HALL B0Benito3; 1Max-Planck-Institut für Quantenoptik, Garch-ing, Germany; 2Universidad Autónoma de Madrid,Madrid, Spain; 3Instituto de Ciencia de Materiales,Madrid, Spain�e contribution has been withdrawn by the authors.
EA-P.21 THUGeneration of squeezed light in optomechanicaldevices by injection of two close optical frequencies.�R. Garcés and G.J. de Valcárcel; Departament d’Òptica,Universitat de València, València, SpainA method for reducing the quantum �uctuations of alight quadrature in an optomechanical cavity is pro-posed. We use a bichromatic driving that induces theappearance of a bistable phase state. We present the an-alytical and numerical analysis.
EA-P.22 THUEnhancement of photon indistinguishability at 1550nm using long-range surface plasmon polaritonnanowire waveguides�R. Kobayashi, T. Sakaidani, N. Namekata, and S. Inoue;Institute of Quantum Science, Nihon University, Tokyo,Japan�e photon-indistinguishability enhancement �lterusing long-range surface plasmon polariton waveg-uides was presented. Using the �lter, the photon-indistinguishability higher than 98 % was achievedirrespective of the polarization of input photons.
EA-P.23 THUQuantum Dirac Phase Interferometer in a PlasmonicWaveguide�V. Savinov1 and N.I. Zheludev1,2; 1Optoelectronics Re-search Centre & Centre for Photonic Metamaterials,Southampton, United Kingdom; 2Centre for DisruptivePhotonic Technologies, Nanyang Technological University,Singapore, SingaporeWewill show that, according to the laws of quantumme-chanics, the phase of guided surface plasmon polaritonsin a plasmonic waveguide shall change under the in�u-ence of applied magnetic �eld.
EA-P.24 THUWhich-Path Information in a Nested Mach-ZehnderInterferometer with Partially Marked Paths�G. Ferenczi, V. Potocek, and S.M. Barnett; University ofGlasgow, Glasgow, United Kingdom
We demonstrate that a standard quantum-optical de-scription of a recent broadly discussed experiment byDanan et al. provides an intuitive picture of the work-ing of the interferometer when spectral decompositionof the signal is considered.
EA-P.25 THUObservation of Hong-Ou-Mandel interference byusing a frequency-domain beamsplitter�T. Kobayashi1, R. Ikuta1, S. Yasui1, S. Miki2, T.Yamashita2, H. Terai2, M. Fujiwara3, T. Yamamoto1, M.Sasaki3, Z.Wang2, M. Koashi4, andN. Imoto1; 1GraduateSchool of Engineering Science, Osaka University, Toyon-aka, Osaka 560-8531, Japan; 2Advanced ICT ResearchInstitute, National Institute of Information and Com-munications Technology (NICT), Kobe 651-2492, Japan;3Advanced ICT Research Institute, National Institute ofInformation and Communications Technology (NICT),Koganei, Tokyo 184-8795, Japan; 4Photon Science Cen-ter,�e University of Tokyo, Bunkyo-ku, Tokyo 113-8656,JapanWe �rst demonstrated the Hong-Ou-Mandel interfer-ence of two photons of di�erent colors in an optical rangeby using a partial frequency converter. An observed vis-ibility is 0.71±0.04, which clearly shows the nonclassicalinterference.
EA-P.26 THUPrecision Tests of the Foundations of QuantumMechanics with Single Photons and Multi-PathInterferometers�T. Kauten, T. Kaufmann, B. Pressl, R. Keil, and G.Weihs;Institut für Experimentalphysik, Universität Innsbruck,Innsbruck, AustriaWe present results from �ve-path interferometer exper-iments to determine an upper bound on possible higherorder interference terms and to test for the possibility ofquantum mechanical wave-functions based on quater-nions rather than complex numbers.
EA-P.27 THUMultiparameter quantum estimation in integratedinterferometersM.A. Ciampini1, �N. Spagnolo1, C. Vitelli1, L. Pezzè2,A. Smerzi2, and F. Sciarrino1; 1Dipartimento di Fisica,Sapienza Universita’ di Roma, Rome, Italy; 2QSTAR,INO-CNR and LENS, Firenze, ItalyWe discuss the conditions of useful entanglement to ob-tain quantum enhanced sensitivity inmultiparameter es-
timation, and we describe a benchmark of multimodeFock states in multiarm integrated interferometers withthree and four modes.
EA-P.28 THUPhoton Pair Generation in an Amorphous SiliconMicro-ring Resonator�E. Hemsley1, D. Bonneau1, G. Sinclair1, J. Pelc2, R.Beausoleil2, M.G. �ompson1, S. Miki3, T. Yamashita3,M. Fujiwara4, M. Sasaki4, H. Terai3, M.G. Tanner5,C.M. Natarajan5, R.H. Had�eld5, and J.L. O’Brien1;1Centre for Quantum Photonics, Bristol, United King-dom; 2Hewlett-Packard Lab., Palo Alto, United States;3National Inst. of Information and CommunicationsTechnology (NICT), Kobe, Japan; 4National Inst. of Infor-mation and Communications Technology, Tokyo, Japan;5School of Engineering, Glasgow, United KingdomWe compare the performance of an a-Si micro-ring res-onator photon source to a waveguide photon source, inboth continuous and pulsed regimes, and characterizethe purity of the generated photons.
EA-P.29 THUEntangled Photon States Generated from a PlanarCuCl Microcavity�H. Ajiki; Photon Pioneers Center, Osaka University, Os-aka, JapanWave vectors of entangled photons from a planar micro-cavity are theoretically studied in a dressed-state pictureof two energy quanta. Wave vectors of entangled pho-tons strongly depend on cavity detuning and incident-�eld angle.
EA-P.30 THUAnomalous phonon-broadened spectra of localisednanotube-excitons�I. Wilson-Rae1, A. Imamoglu2, and W. Zwerger3;1Department of Physics, University of York, York, UnitedKingdom; 2Institute of QuantumElectronics, ETHZurich,Zurich, Switzerland; 3Physik Department, TechnischeUniversitaet Muenchen, Garching, GermanyWe analyse the decoherence of localised excitons in sus-pended nanotubes induced by �exural phonons, andshow that it results in a “collapse” of the zero-phononline realising the “localised” phase of a subohmic spin-boson model.
EA-P.31 THUTowards e�cient quantummemory with very longstorage time.�C. Laplane1, P. Jobez1, I. Usmani2, N. Timoney1, N.Gisin1, A. Ferrier3,4, P. Goldner3, and M. Afzelius1;1Group of Apllied Physics, Geneva, Switzerland;2Laboratoire Charles Fabry, Institut d’Optique, CNRS,Université Paris-Sud, Paris, France; 3PSL Research Uni-versity, Chimie ParisTech CNRS, Institut de Recherchede Chimie Paris, Paris, France; 4Sorbonne Universités,UPMC Univ Paris 06, Paris, FranceWe are developing two techniques to enhance both thee�ciency and the storage time in ensemble-based mem-ories. In our work, we reached an e�ciency of 12% anda coherence time of 7 minutes.
EA-P.32 THUA post-processing free Si nanocrystals basedquantum random number generatorZ. Bisadi1, A. Meneghetti2, A. Tomasi2, G. Fontana1, A.Tengattini1, �P. Bettotti1, G. Pucker3, M. Sala2, and L.Pavesi1; 1Department of Physics, University of Trento,Trento, Italy; 2Department of Mathematics, University ofTrento, Trento, Italy; 3Center for Materials and Microsys-tems , Bruno Kessler Foundation, Trento, ItalyWe present a quantum random number generator basedon silicon nanocrystals LED. �e device generates highquality random sequences that pass all the statistical testswithout any post-processing at a speed of 0.5 Mbs.
EA-P.33 THUNegative Rays and Optical Orbital AngularMomentum�V. Potoček and S.M. Barnett; University of Glasgow,Glasgow, United KingdomWe de�ne a generalization of ray optics featuring rays ofnegative intensity contribution. We provide an intuitiveyet mathematically exact representation of Laguerre-Gaussian beams in this picture. �e properties and pos-sible uses are thoroughly discussed.
13:00 – 14:00EF-P: EF Poster Session
EF-P.1 THUExcitable chaotic pulses in a dual-frequency laser�M. Romanelli1, M. Vallet1, T. Erneux2, and M.
Brunel1; 1Institut de Physique de Rennes, Rennes, France;2Universite Libre de Bruxelles, Bruxelles, BelgiumWe report a new excitable behaviour in a laser, close to a
bifurcation towards a chaotic state. �e excitable pulsesdo not display phase-slips as in the standard Adler pic-ture, and have heavy-tailed statistics.
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HALL B0EF-P.2 THUEmergence of chaotic behavior from frequency combregime in dissipative systems�S. Coulibaly1, Z. Liu1, M. Taki1, and M. Clerc2;1Laboratoire de Physique des Lasers, Atomes etMolécules,CNRS UMR 8523, Université de Lille - Sciences et Tech-nologie - 59655 Villeneuve d’Ascq Cedex, France, Vil-leneuve d’Ascq, France; 2Departamento de Física, Facul-tad de Ciencias Físicas y Matemáticas, Universidad deChile, Casilla 487-3, Santiago, Chile, Santiago, Chile�e transition from Kerr cavity frequency comb to achaotic regime in the Lugiato-Levefer equation is stud-ied through the spectrum of Lyapunov exponents of theperiodic state resulting from modulation instability.
EF-P.3 THUPhoto-isomerization induces pattern instability,labyrinth and foam textures�V. Odent1,2, I. Andrade-Silva2, M.G. Clerc2, and D.Esca�3; 1Laboratoire de Physique des Lasers, Atomes etMolécules, CNRSUMR8523, Université Lille 1, Villeneuved’Ascq, France; 2Departamento de Fisica, Facultad deCiencias Fisicas y Matematicas, Universidad de Chile,Santiago, Chile; 3Complex Systems Group, Facultad de In-geniería, Universidad de los Andes, Santiago, ChileWe report experimental observation of crown splash,labyrinth and foam textures, induced by photo-isomerization process in an azo dye liquid crystal.Numerical simulations performed with a genericbistable and di�usive model reproduce qualitativelyexperimental dynamics.
EF-P.4 THUInstabilities of Laser Cavity Solitons Induced byDelayed Feedback�A. Vladimirov1,2, D. Puzyrev3, S. Yanchuk1, andS. Gurevich4; 1Weierstrass Institute, Berlin, Germany;2Lobachevsky State University, Nizhny Novgorod, Rus-sia; 3Humboldt University of Berlin, Berlin, Germany;4Institute for �eoretical Physics, University of Münster,Münster, GermanyWe study analytically and numerically the e�ect of de-layed feedback on the dynamics of cavity solitons inbroad area lasers with a saturable absorber. We analyzeinstabilities leading to dri�ing and oscillating soliton for-mation.
EF-P.5 THUControl and generation of dri�ing pattern usingasymmetrical Fourier �lteringE. Louvergneaux1, �V. Odent1, S. Coulibaly1, U.Borlolozzo2, and S. Residori2; 1Laboratoire de Physiquedes Lasers, Atomes et Molécules, CNRS UMR8523, Uni-versité Lille 1, Villeneuve d’scq, France; 2Institut Non
Linéaire de Nice, UMR 6618, 1361 Route des Lucioles,Valbonnes, FranceWe show that asymmetrical Fourier �ltering applied onan optical feedback system allows to generate new dy-namics characterized by dri�ing patterns. �e dynamicsis controlled by the cuto� spatial frequency value.
EF-P.6 THUOptical Turbulence and Polarization Rogue Waves inExperiments and Ginzburg-Landau Model ofQuasi-CW Fiber LaserS. Sugavanam1, N. Tarasov1,2, S. Wabnitz3, and �D.Churkin1,4,5; 1Aston Institute of Photonic Technologies,Birmingham, United Kingdom; 2Institute of Computa-tional Technologies, Novisibirsk, Russia; 3Dipartimentodi Ingegneria dell’Informazione, Universita di Brescia,Brescia, Italy; 4Institute of Automation and Electrometry,Novosibirsk, Russia; 5Novisibirsk State University, Novis-ibirsk, RussiaComplex Ginzburg-Landau equations being e�cient formodelling of mode-locked �ber lasers are surprisinglyfound to describe the turbulent generation of quasi-CW�ber laser and emergence of polarization rogue waves intheir radiation.
EF-P.7 THUCharacteristics of Peregrine Soliton in thegeneralized nonlinear Schrödinger equation withperiodic coe�cients�G.C. Tiofack, S. Coulibaly, and M. Taki; Laboratoire dePhysique des Lasers, Atomes et Molécules, Université deLille 1 Sciences et Technologies, Lille, FranceWe study the properties of rogue wave in the nonlin-ear Schrödinger equation with periodic coe�cients. Ourpredictions allow controlling the characteristics of Pere-grine solutions (number of peaks, size) and are in excel-lent agreement with simulations.
EF-P.8 THUNonlinear plasmonic slot waveguides: stationarystates, bifurcation, stability and temporal evolutionW. Walasik1, F. Ye2, A. Rodriguez3, and �G. Renversez1;1Aix-Marseille University & Institut Fresnel CNRS, Mar-seille, France; 2Shanghai Jiao Tong University, Shangai,China, People’s Republic of (PRC); 3Princeton University,Princeton, United StatesUsing our newmodels, we study the stationary and tem-poral solutions (including asymmetric ones) in nonlin-ear plasmonic symmetric slot waveguides where a non-linear dielectric core of Kerr type is surrounded by twosemi-in�nite metal regions.
EF-P.9 THUImpact of noise on solitary waves dynamics innon-local non-instantaneous Kerr medium�H. Louis1, M. Tlidi2, and E. Louvergneaux1; 1Universitéde Lille 1, Villeneuve d’Ascq cedex, France; 2Faculté desSciences, Université Libre de Bruxelles (U.L.B.), Bruxelles,BelgiumWe show that the undulation dynamics of localizedstructures propagating in non-local non-instantaneousKerr media are induced by the noise. Numerical resultsare in agreement with our experiments in a nematic liq-uid crystal cell.
EF-P.10 THU�e Role of Carrier Di�usion in RNGH Instabilitiesof Quantum Cascade Lasers�N. Vuković1, J. Radovanović1, V. Milanović1, and D.Boiko2; 1School of Electrical Engineering, University ofBelgrade, Belgrade, Serbia and Montenegro; 2CentreSuisse d’Electronique et de Microtechnique (CSEM),Neuchâtel, SwitzerlandWe report the carrier di�usion e�ect on multimodeRisken-Nummedal-Graham-Haken instabilities inquantum cascade lasers and compare these to con-ventional laser diodes. We show the superradianceemission and regular self-pulsations are possible inshort cavity samples.
EF-P.11 THUUni�ed Photonic Implementation of ReservoirComputing and Extreme Learning Machines basedon a Single Time-delayed NodeS. Ortïn1, D. San-Martín2, �L. Pesquera1, M.C. Soriano3,D. Brunner3, I. Fischer3, C.R. Mirasso3, and J.M.Gutiérrez1; 1Instituto de Física de Cantabria (CSIC-UC),Santander, Spain; 2Predictia Intelligent Data SolutionsS.L., Santander, Spain; 3Instituto de Física Interdisciplinary Sistemas Complejos (CSIC-UIB), Palma de Mallorca,SpainWe present a uni�ed photonic implementation of Reser-voir Computing (ESN)and ELM based on a single non-linear node subject to delayed feedback. Switching be-tween ESN and ELM is easily obtained by opening thefeedback loop.
EF-P.12 THUMicrowave Signal Generation Using along-wavelength VCSEL under Dual-BeamOrthogonal Optical InjectionP. Pérez1,5, A. Quirce2, �Á. Valle1, L. Pesquera1, A.Consoli3, and I. Esquivias4; 1Instituto de Física deCantabria,CSIC-Universidad de Cantabria, Santander,Spain; 2Vrije Universiteit Brussel, Faculty of EngineeringSciences, Brussels Photonics Team (B-PHOT), Brussels,
Belgium; 3Instituto de Ciencia de Materiales de Madrid,CSIC, Madrid, Spain; 4Departamento de TecnologíaFotónica, Universidad Politécnica de Madrid, ETSI deTelecomunicación, Madrid, Spain; 5Departamento deFísica Moderna, Universidad de Cantabria, Santander,SpainWe experimentally and theoretically investigate mi-crowave signal generation using a 1550nm VCSEL sub-ject to two-frequency orthogonal optical injection. It isfound that microwave linewidth is given by the sum ofthe two master lasers linewidths.
EF-P.13 THUSpontaneous mode locking in the superradiantlasers: Intrinsic losses in an active medium instead ofresonant losses in a saturable absorber�V. Kocharovsky1, V. Kocharovsky1,2, E. Kocharovskaya1,and V. Kukushkin1; 1Institute of Applied Physics RAS,Nizhny Novgorod, Russia; 2Texas A&M University, Col-lege Station, RussiaWe �nd that a self-mode-locking in a DFB Fabry-Perotcavity may exist without using any mode-locking tech-nique if a mode superradiance takes place in a laser withan active-center polarization lifetime exceeding a cavitylifetime.
EF-P.14 THUTemperature-Dependent Double PolarizationSwitching in long-wavelength VCSELsA. Quirce1, �Á. Valle2, L. Pesquera2, H. �ienpont1,and K. Panajotov1,3; 1Vrije Universiteit Brussel, Fac-ulty of Engineering Sciences, Brussels Photonics Team(B-PHOT), Brussels, Belgium; 2Instituto de Física deCantabria, CSIC-Universidad de Cantabria, Santander,Spain; 3Institute of Solid State Physics, So�a, BulgariaCharacterization of double polarization switchings (PS),type II followed by type I and vice-versa, observed in aVCSEL at di�erent temperatures, is used to measure thetemperature dependence of VCSEL parameters like thespin-�ip rate.
EF-P.15 THUHigh- Power Vortex Light Bullets in Kerr Media�O. Fedotova1, O. Khasanov1, T. Smirnova2, G. Rusetsky1,and E. Gaižauskas3; 1Scienti�c-Practical Material Re-search CentreScienti�c-Practical Material Research Cen-tre, Minsk, Belarus; 2International Sakharov Environ-mental University, Minsk, Belarus; 3Vilnius universityLaser research center, Vilnius, LithuaniaSpatio-temporal localization conditions for high-powerfemtosecond vortex pulsed beams in Kerr medium withanomalous group velocity dispersion and plasma non-linearity depending on topological charge and the ratioof input pulse power to critical one are studied.
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HALL B0EF-P.16 THUSolitonic cavities in conservative and dissipativesystems�R. Driben1,2 and A. Yulin1; 1ITMO University, St. Pe-tersburg, Russia; 2University of Paderborn, Paderborn,GermanyWedemonstrate nonlinear dynamics of cavity consistingof two solitons and trapped dispersive waves in conser-vative and dissipativemodels with the applications to thegeneration of supercontinuum and formation of the fre-quency combs respectively.
EF-P.17 THUModulation instability in periodically dispersionkicked optical �bersM. Conforti1, S. Rota Nodari2, G. Dujardin2,3, �A.Mussot1, S. Trillo4, and S. DE Biévre2,3; 1CNRS-Universite Lille 1, Villeneuve d’Ascq, France; 2UMR 8524et UFR de Mathématiques, Université Lille 1, Villeneuved’Ascq, France; 3Équipe MÉPHYSTO, Inria Lille Nord-Europe Parc Scienti�que de la Haute-Borne, Villeneuved’Ascq, France; 4Dipartimento di Ingegneria, Universit‘adi Ferrara,Via Saragat, Ferrara, FranceModulation instability has been investigated theoreti-cally and experimentally in dispersion kicked �bers. Anexpression of parametric gain has been obtained allow-ing predicting the experimental behavior. �ese �bersconstitute a platform to investigate fundamental physi-cal phenomena.
EF-P.18 THUReal-time Spectral Evolution of Breathing TemporalCavity SolitonsK. Luo, J. Jang, M. Erkintalo, �S. Murdoch, and S. Coen;Physics Dept, University of Auckland, Auckland, NewZealandWe present the �rst real-time measurement of the spec-tral evolution of a breathing temporal cavity soliton. Wemeasure the roundtrip by roundtrip evolution of thesenonlinear localised structures observing excellent agree-ment with their simulated evolution.
EF-P.19 THUNonlinear spectral compression in optical �berS. Papernyi1, �A. Bednyakova2,3, S. Turitsyn2,4, W.Clements1, and M. Fedoruk2,3; 1MPB CommunicationsInc., Pointe-Claire, Canada; 2Novosibirsk State Univer-sity, Novosibirsk, Russia; 3Institute of ComputationalTechnologies, Novosibirsk, Russia; 4Aston Institute of Pho-tonic Technologies, Birmingham, United KingdomWe present experimental observation of spectral com-pression of a powerful wave produced by a Raman �berlaser in normal dispersion �ber. �e results of numerical
modeling fully con�rm experimentally observed spec-tral behavior of nonlinear waves.
EF-P.20 THUBaseband Modulation Instability as the Origin ofRogue Waves�F. Baronio1, S. Wabnitz1, S. Chen2, P. Grelu3, andM. Conforti4; 1University of Brescia, Brescia, Italy;2Southeast University, Nanjing, China, Republic of(ROC); 3CNRS-Universitè de Bourgogne, Dijon, France;4CNRS-Universitè Lille 1, Lille, FranceWe study the existence of rogue wave solutions in di�er-ent nonlinear wave evolutionmodels, commonly used inoptics and hydrodynamics, showing the connection withbaseband modulation instability.
EF-P.21 THUDiscrete Nonlocal Nonlinearity inQuadraticWaveguide Arrays�F. Setzpfandt1, W. Sohler2, R. Schiek3, and T. Pertsch1;1Institute of Applied Physics, Abbe Center of Photon-ics, Friedrich-Schiller-Universität Jena, Jena, Germany;2Angewandte Physik, Universität Paderborn, Paderborn,Germany; 3University of Applied Sciences Regensburg,Regensburg, GermanyWe investigate direct nonlinear interactions betweenneighboring waveguides in discrete quadratic waveguidearrays. Usingmode symmetries to suppress local nonlin-earities, we experimentally show the profound e�ect ofsuch nonlocal interactions on second-harmonic genera-tion.
EF-P.22 THUConsistency Properties of a Chaotic Laser to InputPulse Trains�N. Oliver1, T. Jüngling1, D. Brunner1, A.J. Pons2, J.Tiana-Alsina3, J. Buldú4, M.d.C. Torrent2, J. García-Ojalvo5, and I. Fischer1; 1Instituto de Física Interdisci-plinar y Sistemas Complejos (IFISC) CSIC-UIB, Palma deMallorca, Spain; 2Universitat Politècnica de Catalunya,Departament de Física i Enginyeria nuclear, Terrassa,Spain; 3Universitat Politècnica de Catalunya, Departa-mento de Teoría de la Señal y Comunicaciones, Barcelona,Spain; 4Universidad Rey Juan Carlos & Centro de Tec-nología Biomédica, Madrid, Spain; 5Universitat PompeuFabra, Department of Experimental and Health Sciences,Barcelona, SpainWe experimentally study consistency properties of asemiconductor laser subject to optical feedback. By in-jecting short electrical pulses into the chaotic laser, char-acteristic responses are induced. �eir degree of consis-tency is studied via correlations.
EF-P.23 THUSpontaneous Spatial Patterns in Discrete NonlinearSchrödinger Equations: Ring Cavities andCounterpropagating BeamsA.B. Leite, �J.M. Christian, G.S. McDonald, C. Dickinson,andA.S. Heyes;University of Salford, GreaterManchester,United KingdomWe propose two new contexts for modelling spon-taneous optical patterns with discrete nonlinearSchrödinger equations beyond mean-�eld theory: ringcavities and counterpropagating beams. Linear analysispredicts threshold instability spectra, which are testedagainst extensive simulations.
EF-P.24 THUStimulated Brillouin Scattering in hybridsilicon-chalcogenide slot waveguides�S.R. Mirnaziry1,2, C. Wol�1,2, M. Steel1,3, B. Eggleton1,4,and C. Poulton1,2; 1Centre for Ultrahigh bandwidth De-vices for Optical Systems (CUDOS), Sydney, Australia;2School of Mathematical Sciences, University of Technol-ogy Sydney, Sydney, Australia; 3School of Physics, Mac-quarie University, Sydney, Australia; 4School of Physics,University of Sydney, Sydney, AustraliaStimulated Brillouin Scattering is studied in hybridsilicon-chalcogenide slot waveguides. �e physics ofinteractions between acoustic and optical waves is ex-plained in detail. Furthermore, parameters which canenhance the strength of the nonlinearity are investigated.
EF-P.25 THUBreathers Emergence in Spontaneous ModulationInstability�S. Toenger1, T. Godin1, C. Billet1, F. Dias2, M. Erkintalo3,G. Genty4, and J. Dudley1; 1FEMTO-ST, Besancon,France; 2University College Dublin, Dublin, Republicof Ireland; 3University of Auckland, Auckland, NewZealand; 4Tampere University of Technology, Tampere,FinlandSimulations of the stochastic nonlinear Schrödingerequation show that localized structures emerging spon-taneously from chaotic modulation instability �eld arewell-described by analytic soliton on �nite backgroundor breather solutions and their superpositions.
EF-P.26 THUMagneto-Optical Switch Based on the High-ContrastResonance of Electromagnetically InducedAbsorption�D. Brazhnikov1,2, A. Taichenachev1,2, A. Tumaikin1,and V. Yudin1,2,3,4; 1Novosibirsk State University, Novosi-birsk, Russia; 2Institute of Laser Physics SB RAS, Novosi-birsk, Russia; 3Novosibirsk State Technical University,
Novosibirsk, Russia; 4Russian QuantumCenter, Skolkovo,Moscow Region, Russia�e device for switching probe laser beam intensity by aweak static magnetic �eld is proposed. Its performancebased on the new scheme for observing the high-contrastand ultra-narrow resonance of electromagnetically in-duced absorption.
EF-P.27 THUNonlinear parametric resonances in aperiodicdispersion oscillating �bers�C. Finot1, A. Sysoliatin2, and S. Wabnitz3; 1LaboratoireInterdisciplinaire Carnot de Bourgogne, Dijon, France;2Fiber Optics Research Center, Moscow, Russia;3Dipartimento di Ingegneria dell Informazione, Bres-cia, ItalyWe numerically study the evolution of parametric res-onance sidebands in aperiodic dispersion oscillating�bers. We separately consider a linear variation of var-ious parameters and highlight di�erent novel mecha-nisms for the splitting of the resonance sidebands.
EF-P.28 THUTuning Synchronized Square-Wave Pulses withOptoelectronic Oscillators�J. Martínez-Llinàs1, P. Colet1, and T. Erneux2; 1IFISC,Instituto de Física Interdisciplinar y Sistemas Complejos(CSIC-UIB), Palma de Mallorca, Spain; 2Université Librede Bruxelles, Optique Nonlinéaire �éorique, Bruxelles,BelgiumWe show that two mutually delay-coupled optoelec-tronic oscillators can generate stable in and out-of-phasetunable square-wave solutions, including those with anarbitrary duty cycle. Furthermore, multiple solutionswith di�erent periods coexist.
EF-P.29 THUSpatio-temporal Dynamics of Raman Fibre Lasers�N. Tarasov1, S. Sugavanam1, and D. Churkin1,2,3;1Aston Institute of Photonic Technologies, Aston Univer-sity, Birmingham, United Kingdom; 2Institute of Automa-tion and Electrometry, Siberian Branch of the RussianAcademy of Sciences, Novosibirsk, Russia; 3NovosibirskState University, Novosibirsk, RussiaWe experimentally measure in real-time spatio-temporal dynamics of quasi-CW Raman �bre laser.We found that despite intensity dynamics is stochasticat all powers, the laser operates in di�erent dynamicspatio-temporal regimes of di�erent nature.
203
Authors’ Index
A. Kaminskii, Alexander . . . . CA-2.4 SUNA. Ritchie, David . . . . . . . . . .PD-B.7 WEDAalto, Antti . . . . . . . . . . . . . . CH-P.16 THUAalto, Timo . .CI-P.7 TUE, �CH-6.1 WEDAbal, Miguel . . . . . . . . . . . . . CM-P.11 SUNAbdolvand, Amin . . . . . . . . . �CM-P.6 SUN,�CM-3.5 SUN, CD-P.30 TUE,
CE-P.1 TUEAbdolvand, Amir . . . . . . . . . . CD-1.1 SUN,�EE-1.2 SUN, EF-6.5 MON,
CD-12.3 THUAbdou Ahmed, Marwan . . . CB-P.2 MON,
CB-P.16 MON, CA-9.2 THUAbdul Kudus, Muhammad I.M.
CE-2.5 SUNAbdulhalim, Ibrahim . . . . . . . .CH-4.5 SUNAbe, Masashi . . . . . . . . . . . . . .�CA-3.1 SUNAbegão, Luis . . . . . . . . . . . . . . . CE-9.5 TUEAbel, Stefan . . . . . . . . . . . . . . �CD-P.1 TUEAbellán, Carlos . . . . . . . . . . . �JSV-4.3 THUAblewski, Piotr . . . . . . . . . . . . CH-7.2 WEDAboud Ahmed, Marwan . . . .CA-7.3 MONAbraham, Emmanuel . . . . . . .CC-P.9 SUN,
CC-P.10 SUNAbram, Izo . . . . . . . . . . . . . . .CK-4a.2 MONAbramski, Krzysztof . . . . . . . CF-P.5 WEDAbrate, Silvio . . . . . . . . . . . . . CE-P.24 TUEAbsil, Philippe CJ-1.4 SUN, CB-11.3 THUAbu Saa, Muayad . . . . . . . . CB-P.22 MONAcar, Durmus Alp Emre . . . . CF-4.4 WEDAcar, Hakki . . . . . . . . . . . . . . . EH-1.3 WEDAcedo, Pablo . . . . . . . . . . . . .CB-P.11 MONAceves, Alejandro . . . . . . . . .EF-4b.3 MONAchar, Harish . . . . . . . . . . . . �CJ-P.36 WEDAchim, Alexandru . . . . . . . . . CA-P.32 SUNAchouche, Mohand . . . . . . . . .CK-7.1 TUEAckemann, Thorsten . . . . . . . EF-1.3 SUN,
EF-1.5 SUN, CB-P.15 MON,EC-P.6 TUE, EC-3.3 TUE, �EF-9.3 THU
Acuna, Guillermo . . . . . . . . . CL-P.18 SUN,EH-6.2 THU
Adam, Thomas N. . . . . . . . .CK-12.2 WEDAdamo, Giorgio . . . . . . . . . . . . EG-2.1 SUN,
CK-6.5 MON, EH-2.1 WED, EI-1.3 THUAdams, Charles . . . . . . . . . . . . EA-9.4 THUAdinolfi, Barbara . . . . . . . . . �CL-P.13 SUNAdler, Steffen . . . . . . . . . . . . . CB-P.7 MONAfshinmanesh, Farzaneh . �CK-P.29 MONAfzelius, Mikael . . . . . . . . . . . .EA-2.4 SUN,
EA-P.31 THUAgazzi, Laura . . . . . . . . . . . . .CJ-6a.3 MONAghajani, Armen . . . . . . . . . �CJ-P.27 WEDAgio, Mario . . . . . . . . . . . . . . .EA-10.5 THUAgnesi, Antonio . . . . . . . . . . . CA-1.4 SUN,�CA-2.1 SUNAgranat, Aharon . . . . . . . . . . CD-7.5 MONAgranat, Aharon J. . . . . . . . . .EF-1.6 SUN,
EF-7.2 TUEAgranat, Mikhail . . . . . . . . . . . CC-3.2 SUNAgrawal, Govind . . . . . . . . . .EG-5b.3 MONAgruzov, Petr . . . . . . . . . . . �CK-P.13 MONAguilar, Alberto . . . . . . . . . . . .CM-2.4 SUNAguiló, Magdalena . . . . . . . .CA-P.31 SUN,
CA-4.5 SUN, CA-5a.1 MON,CA-5a.2 MON, CA-5b.3 MON,
EH-P.9 WEDAharonovich, Igal . . . . . . . . . EE-5b.1 MONAhn, Byung-Nam . . . . . . . . .EG-5b.1 MONAhn, Byungnam . . . . . . . . . . . CG-4.4 WEDAhn, Kwang Jun . . . . . . . . . . .CE-P.6 TUE,�EH-5.4 THUAhn, Yeong Hwan . . . . . . . . . . CC-4.4 SUNAho, Antti CB-P.26 MON, CB-5.1 WED,
CB-11.4 THUAhrens, Jan . . . . . . . . . . . . . . CF-P.19 WEDAhufinger, Veronica . . . . . . . . EC-P.8 TUEAhuja, Jatin . . . . . . . . . . . . . . EF-4a.2 MONAi, Xiao . . . . . . . . . . . . . . . . . . �CH-9.4 WEDAidam, Rolf . CB-P.7 MON, CN-2.2 WEDAiello, Andrea . . . . . . . . . . . . . EA-1.2 SUN,
EG-P.1 MON, EA-P.11 THU,EI-3a.3 THU
Aimé, Carole . . . . . . . . . . . . . . . CL-3.3 THUAizitiaili, Abulikemu . . . . . . . CA-7.6 MONAjiki, Hiroshi . . . . . . . . . . . . �EA-P.29 THU,
EH-7.6 THUAka, Gerard . . . . . . . . . . . . . . . CE-7.4 MONAkagi, Hiroshi . . . . . . . . . . . . . .CF-8.3 THUAkahane, Kouichi . . . . . . . . . . . CI-3.6 SUNAkbari, Reza . . . . . . . . . . . . . . CF-P.2 WEDAkçaalan, Önder . . . . . . . . . CJ-P.19 WED,�CJ-P.31 WEDAkhmediev, Nail . . . . . . . . . . . EF-3.2 SUN,
EI-2.3 THU, �EI-2.4 THUAkiyama, Jun . . . . . . . . . . . . . . CA-P.8 SUNAkozbek, Neset . . . . . . . . . . . . CK-1.6 SUNAktürk, Selçuk . . . . . . . . . . . . �SH-1.1 SUN,�CM-7.1 MONAkulov, Katherine . . . . . . . . . CK-6.4 MONAl Balushi, Ahmed . . . . . . . . .EG-7.1 MONAl-kadry, Alaa . . . . . . . . . . . �CJ-P.34 WEDAl Nakdali, Dalia . . . . . . . . . . �CB-3.2 TUEAl Roumy, Jalal . . . . . . . . . . .�CH-8.1 WEDAlam, Shaif-ul . . . . . . . . . . . CD-P.17 TUE,
CJ-9.2 WEDAlam, Shaiful . . . . . . . . . . . . . CJ-12.1 THUAlarousu, Erkki . . . . . . . . . . . . EH-7.2 THUAlbach, Daniel . . . . . . . . . . . CA-P.21 SUN,
CA-9.4 THUAlber, Lucas . . . . . . . . . . . . . . �EA-P.1 THUAlberucci, Alessandro . . . . . . CD-7.2 MONAlbrecht, Bernhard . . . . . . . . �EA-2.5 SUNAlbrecht, Boris . . . . . . . . . . . EB/EG.2 TUEAlcubilla, Ramón . . . . . . . . . . . JSI-1.2 SUNAlcusa-Sáez, Erica . . . . . . . �CH-P.17 THUAleksandrov, Veselin . . . . . . CA-P.40 SUNAlekseev, Dmitriy . . . . . . . . . CJ-10.4 WEDAlekseeva, Irina . . . . . . . . . . . . CE-P.5 TUEAleksic, Slavisa . . . . . . . . . . . . EB-4.5 WEDAlencar, Márcio . . . . . . . . . . . .CE-9.5 TUE,
CH-P.9 THUAleshkina, Svetlana . . . . . . . . CJ-3.1 SUN,
CJ-P.13 WEDAlessio, Stefani . . . . . . . . . . . CE-P.20 TUEAlexaki, Konstantina . . . . . . . CM-1.3 SUNAlexander, Oliver . . . . . . . . . . CG-3.3 WEDAlfieri, Cesare . . . . . . . . . . . . . . CF-9.3 THUAlharbi, Abdullah F. . . . . . . . CG-6.2 WEDAli, Jalil . . . . . . . . . . . . . . . . . . . CC-6.5 TUEAlighanbari, Soroosh . . . . . . .ED-P.9 MON
Alisauskas, Skirmantas . . . . . CF-2.1 TUE,CF-3.5 TUE, PD-A.4 WED
Alismail, Ayman . . . . . . . . . . . .CA-P.1 SUNAljunid, Syed Abdullah . . . . . EG-2.1 SUNAlloncle, Anne-Patricia . . . .CM-P.20 SUNAlmeida, Gustavo Foresto Brito de�CM-P.14 SUNAlmeida, Joana . . . . . . . . . . .CE-P.26 TUE,�CA-11.6 THUAlmeida, Juliana M. P. . . . . �CE-6.3 MONAlonso, Benjamín . . . . . . . . . . CG-P.7 THUAlouini, Mehdi . . . . . . . . . . . . . CL-3.2 THUAlsaleh, Magda . . . . . . . . . . . . .�EI-P.3 TUEAlshehri, A.M . . . . . . . . . . . . . �CM-P.1 SUNAlshehri, Ali . . . . . . . . . . . . . . . CM-P.2 SUNAltabas, Jose A . . . . . . . . . . . JSIV-2.4 SUNAltabas, Jose Antonio . . . . . . �CI-2.4 SUNAltan, Hakan . . . . . . . . . . . . �CC-P.18 SUN,
CE-P.11 TUEAltmann, Robert . . . . . . . . . �ED-2.1 MONAltpeter, Philipp . . . . . . . . . . .EG-P.2 MONAltug, Hatice . . . . . . . . . . . JSII-1a.3 MON,
JSII-2.3 MONAltuzarra, Charles . . . . . . . . . . EG-3.5 SUNAlvarez, Daniel . . . . . . . . . . JSII-1a.3 MONAmani Eilanlou, Abdolreza CG-P.18 THUAmann, Markus-Christian . . . CC-1.1 SUNAmanti, Maria . . . . . . . . . . . . . CC-1.3 SUNAmaral, Anderson . . . . . . . . . . CH-2.2 SUNAmaya, Waldimar . . . . . . . . . CH-6.6 WED,
JSV-4.3 THUAmbrogio, Stefano . . . . . . . . JSIV-1.2 SUNAmin, Haider . . . . . . . . . . . . . . .CL-P.6 SUNAmiot, Caroline . . . . . . . . . . . . EE-3.1 SUN,�CH-P.16 THUAmiranashvili, Shalva . . . . . . . .EI-2.3 THUAmmann, Hubert . . . . . . . . . . CA-9.1 THUAmoah, Timothy . . . . . . . . �CK-P.14 MONAmodio, Pasquale . . . . . . . . . ED-2.6 MONAmrani, Foued . . . . . . . . . . . . . CJ-2.1 SUN,
CD-6.1 MON, EF-8.3 TUE, CJ-P.7 WEDAms, Martin CM-P.8 SUN, CM-4.3 SUN,�CJ-P.41 WED, JSV-1.4 THU,�CH-P.6 THUAmthor, Matthias . . . . . . . . . . CB-1.1 TUEAmy-Klein, Anne . . . . . . . . . ED-3.3 MON,
CH-P.33 THUAnastasiou, Antonios . . . . . . CM-7.5 MONAnders, Krzysztof . . . . . . . . . .CH-6.3 WEDAndersen, Mikkel . . . . . . . . . . . EC-1.5 TUEAndersen, Ulrik L. . . . . . . . . CH-P.22 THUAnderson, Mitchell David . . EG-P.5 MONAndrade-Silva, Ignacio . . . . . EF-8.5 TUE,
EF-P.3 THUAndral, Ugo . .�CJ-2.1 SUN, �EF-8.3 TUEAndré, Yves-Bernard . . . . . . . .CD-3.5 SUNAndreeva, Vera . . . . . . . . . . . . . EI-2.6 THUAndrés, Miguel . . . . . . . . . . . . . CL-P.7 SUNAndrés, Miguel V. . . . . . . . .CH-P.17 THU,�CH-P.32 THUAndrés, Miguel Vicente . . . CH-P.27 THUAndrés, Pedro . . . . . . . . . . . . . CM-P.4 SUNAndrews, Aaron Maxwell . . . .CC-1.4 SUNAndrews, David . . . . . . . . . . �CD-7.1 MONAndriukaitis, Giedrius . . . . . . �CA-3.3 SUN
Andriuskaitis, Giedrius . . . . . . CF-2.1 TUEAndrovitsaneas, Petros . . . . . EA-8.4 WEDAndryieuski, Andrei . . . . . . �CK-P.40 MONAngela, Vella . . . . . . . . . . . . .�CM-7.6 MONAngelov, Ivan . . . . . . . . . . . . . CA-10.3 THUAnia-Castañón, Juan Diego CI-P.12 TUE,
CJ-P.21 WEDAnoikin, Eugene . . . . . . . . . �CE-10.2 WEDAntier, Marie . .CJ-1.4 SUN, CD-4.2 SUNAntipov, Oleg . . . . . . . . . . . . CJ-10.4 WED,�CA-12.2 THUAntipov, Sergei . . . . . . . . . . . �CM-4.3 SUN,
CH-P.6 THUAntipov, Sergey . . . . . . . . . . CJ-P.44 WEDAntonosyan, Diana . . . . . . . .�CD-3.2 SUN,
CD-P.12 TUEAntonucci, Laura . . . . . . . . . . .CF-6.5 THUAnumula, Sunilkumar . . . . . . CG-6.3 WEDAolita, Leandro . . . . . . . . . . . . .EA-7.1 TUEAono, Masashi . . . . . . . . . . . EG-P.15 MONApolonski, Alexander . . . . . CA-P.12 SUN,
CA-P.22 SUN, CA-P.34 SUN,CD-8.4 TUE, CD-P.18 TUE,CF-P.26 WED, PD-A.1 WED,CA-10.3 THU, CA-10.5 THU,CF-9.2 THU
Apostolopoulos, Vasilis . . . .CC-P.13 SUN,CC-P.17 SUN, CJ-P.27 WED,EH-P.14 WED
Appelfelder, Michael . . . . . . . CM-4.1 SUNArantchouk, Leonid . . . . . . . . CD-3.5 SUNArar, Bassem . . . . . . . . . . . . �CD-P.40 TUEAraújo, Mateus . . . . . . . . . . . . EB-5.4 WEDAravazhi, Sanmugam . . . . . CJ-6a.3 MONAravazhi, Shanmugam . . . . . CE-7.3 MONArbabzadah, Emma . . . . . . . �CA-6.4 MONArchimi, Matteo . . . . . . . . . . PD-B.5 WEDArcizet, Olivier . . . . . . . . . . . .�EG-1.3 SUN,
EG-1.5 SUN, CK-2.4 SUNArend, Carsten . . . . . . . . . . . . . CE-4.4 SUNArgenti, Luca . . . . . . . . . . . . . .CG-5.2 WEDArguel, Philippe . . . . . . . . . . CK-11.3 WEDArgyris, Apostolos . . . . . . . �CB-P.31 MONArgyros, Alexander . . . . . . . EH-P.13 WEDArimondo, Ennio . . . . . . . . . . PD-B.5 WEDArion, Vladimir . . . . . . . . . . . CE-P.14 TUE,
CE-P.15 TUEArkhipov, Mikhail . . . . . . . . . �CF-P.3 WEDArkhipov, Rostislav . . . . . . . . CF-P.3 WEDArmaroli, Andrea . . . . . . . . . CD-12.3 THUArmas Rivera, Ivan . . . . . . . .CD-P.26 TUEArnaud, Garnache . . . . . . . CB-P.32 MON,
CB-1.3 TUEArndt, Markus . . . . . . . . . . . . . �EA-3.1 SUNArnold, Aidan EC-P.2 TUE, EC-3.3 TUE,
EF-9.3 THUArnold, Cord . . . . . . . . . . . . . . CG-5.1 WEDArnold, Cord L. . . . . . . . . . . . .CG-1.5 TUE,
CF-6.2 THU, CF-8.2 THUArnold, Craig B. . . . . . . . . . . . CE-6.3 MONArnoldi, Laurent . . . . . . . . . CM-5b.1 MONArora, Pankaj . . . . . . . . . . . . �EH-P.4 WEDArriola, Alexander . . . . . . . . . CM-P.8 SUNArthaber, Holger . . . . . . . . . . . CC-2.4 SUNArtlett, Christopher . . . . . . . �CH-7.6 WED
Arzani, Francesco . . . . . . . . �EB-P.10 WEDAschieri, Pierre . . . . . . . . . . . . . CI-P.4 TUEAshida, Masaaki . . . . . . . . . . CC-P.15 SUN,�CE-11.5 WEDAshitkov, Sergey . . . . . . . . . . . CC-3.2 SUNAsif, Rameez . . . . . . . . . . . . . .�CI-P.10 TUEAskitopoulos, Alexis . . . . . . . �EF-9.2 THUAsobe, Masaki . . . . . . . . . . . .CH-P.29 THUAspelmeyer, Markus . . . . . . . �EA-4.1 SUN,
CF-9.3 THUAssanto, Gaetano . . . . . . . . . CD-7.2 MONAtatüre, Mete . . . . . . . . . . . . . . CE-4.4 SUNAtorf, Bernhard . . . . . . . . . . CK-P.16 MONAtvarz, Tereza . . . . . . . . . . . . CE-P.16 TUEAuffèves, Alexia . . . . . . . . . . . . EA-9.6 THUAugé, Sylvain . . . . . . . . . . . . CB-P.17 MONAuguste, T . . . . . . . . . . . . . . . . CF-8.5 THUAujard, Isabelle . . CLEO/ECBO-1.2 WEDAung, Yan Lin . . . . . . . . . . . . .CE-7.4 MONAungskunsiri, Kanin . . . . . . . EB-5.5 WEDAus der Au, Juerg . . . . . . . . . . CA-2.1 SUNAustin, Dane R. . . . . . . . . . . .CG-3.2 WED,
CG-3.3 WEDAutebert, Claire . . . . . . . . �JSV-P.10 MONAverchenko, Valentin A. . . �EA-P.11 THUAvila, Abundio . . . . . . . . . . . . .CM-2.4 SUNÁvila, Jhon . . . . . . . . . . . . . . . �CH-P.9 THUAvo, Ricardo . . . . . . . . . . . . . . . CI-5.2 MONAydin, Koray . . . . . . . . . . . . . CK-11.4 WEDAyoub, Mousa . . . . . . . . . . . �CD-11.2 THUAyuso, David . . . . . . . . . . . . . CG-6.3 WED,
CG-P.17 THUAzami, Shunya . . . . . . . . . . . . . CK-9.6 TUEAzana, Jose . . . . . . . . . . . . . . . . �CI-4.1 SUNAzhar, Mohiudeen . . . . . . . . . �CH-4.3 SUNAzzini, Stefano . . . . . . . . . . . JSV-P.3 MONB. Lehmann, Tau . . . . . . . . . PD-B.7 WEDB. Olausson, Christina . . . . CJ-P.14 WEDB Ovchinnikov, Yuri . . . . . . . ED-P.9 MONBa, Dexin . . . . . . . . . . . . . . . . CA-P.13 SUNBaali, Ilyes . . . . . . . . . . . . . . . . CF-4.4 WEDBaaske, Martin . . . . . . . . . . . . .CH-4.2 SUNBabakiray, Sercan . . . . . . . . . . CC-4.1 SUNBabazadeh, Nasser . . . . . . . CE-11.1 WEDBabin, Sergey . . . . . . . . . . . .CF-P.26 WED,
CJ-P.16 WED, �CJ-P.24 WED,EI-2.2 THU
Babin, Sergey A. . . . . . . . . . . .CM-4.2 SUNBabushkin, Ihar . . . . . . . . . . . . EE-2.5 SUN,
EE-P.14 SUN, �EF-3.3 SUN,CF-P.3 WED
Bach, Florian . . . . . . . . . . . . . . CF-9.4 THUBache, Morten . . . . . . . . . . . EE-P.11 SUN,
EF-3.6 SUN, CF-3.3 TUE, �CF-3.6 TUE,CF-P.14 WED, CF-P.17 WED,CJ-P.12 WED, CJ-P.22 WED
Bächle, Andreas . . . . . . . . . . CB-P.7 MON,CN-2.2 WED
Bachmann, Dominic . . . . . . . CC-2.4 SUN,CC-P.4 SUN
Bachtold, Adrian . . . . . . . . . . CH-1.1 SUN,CK-10.3 WED
Bader, Kathrin . . . . . . . . . . .�CE-12.1 WEDBader, Marianne . . . . . . . . . . . EA-P.1 THUBader, Sven . . . . . . . . . . . . . . . �CB-2.6 TUE
204
Authors’ Index
Badioli, Michela . . . . . . . . . .�JSIV-2.2 SUNBaehr-Jones, Tom . . . . . . . CK-4b.1 MON,
EA-7.6 TUE, JSV-1.2 THUBaets, Roel . . . . . . . . . . . . . . . .�CE-4.1 SUNBaffou, Guillaume . . . . . . . . . . EH-6.6 THUBagaev, Sergei . . . . . . . . . . . . . CA-8.5 TUEBaghban, Mohammad Amin�CK-5.3 MONBagniuk, Jacek . . . . . . . . . . . . .CC-P.6 SUNBai, Dongbi . . . . . . . . . . . . . . . CJ-P.6 WEDBai, Xunkun . . . . . . . . . . . . . . .CF-P.1 WEDBai, Zhenxu . . . . . . . . . . . . . . CA-P.13 SUNBaida, F.I. . . . . . . . . . . . . . . . CK-11.2 WEDBaier, Moritz . . . . . . . . . . . . . . .CK-7.1 TUEBajoni, Daniele . . . . . . . . . . �EG-P.4 MON,�JSV-P.3 MON, �EA-7.6 TUE,�JSV-1.2 THUBakhru, Hassaram . . . . . . . . .JSV-4.4 THUBakhtiari Gorajoobi, Shahab�CK-10.6 WEDBakker, Morten P. . . . . . . . . EB-P.13 WEDBakshaev, Ilia O. . . . . . . . . . .CD-P.28 TUEBakunov, Michael . . . . . . . . . .CC-6.1 TUE,�CC-6.2 TUEBalci, Osman . . . . . . . . . . . . . CC-P.18 SUNBalciunas, Tadas . . . . . . . . . . .CF-2.1 TUE,�CG-2.3 TUE, CF-5.2 WEDBaldini, Francesco . . . . . . . . CL-P.13 SUN,
CH-P.24 THUBaldycheva, Anna . . . . . . . . CK-12.2 WEDBalembois, François . . . . . . . . CA-9.2 THUBallato, John . CH-4.4 SUN, CE-P.8 TUEBalle, Salvador EF-1.2 SUN, EI-P.2 TUE,
CB-2.5 TUE, CB-7.6 WED,CD-13.4 THU
Balogh, Emeric . . . . . . . . . . . �CG-1.4 TUE,CG-P.2 THU
Balskus, Karolis . . . . . . . . . . �ED-P.6 MON,PD-A.6 WED
Baltensperger, Urs . . . . . . . . CD-P.14 TUEBaltuska, Andrius . . . . . . . . . . CJ-2.5 SUN,
EE-P.8 SUN, CA-3.3 SUN, CD-4.5 SUN,EE-4.3 SUN, �CF-2.1 TUE, CF-2.4 TUE,CF-3.5 TUE, CG-2.3 TUE, CF-5.2 WED,CG-6.5 WED, CG-6.6 WED,PD-A.4 WED
Balzer, Jan C. . . . . . . . . . . . CB-P.21 MON,CB-10.4 THU
Bañares, Luis . . . . . . . . . . . . . . CM-2.2 SUNBancal, Jean Daniel . . . . . . . EB-1.4 MONBancelin, Stéphane . . . . . . . . . CL-3.3 THUBandelow, Uwe . . . . . . . . . . . . �EI-2.3 THUBanerjee, Saumyabrata . . . . . CA-3.6 SUNBanfi, Francesco . . . . . . . . . . EE-P.17 SUNBang, Ole CK-P.39 MON, CE-P.20 TUE,
CH-5.4 TUE, CJ-P.12 WED,CJ-P.22 WED, CH-P.20 THU,CH-P.25 THU
Bannerman, Rex H.S. . . . . . . �CE-2.3 SUNBanzer, Peter EA-1.2 SUN, EG-P.1 MONBarach, Gilad . . . . . . . . . . . . . . CA-P.4 SUNBaranchikov, Alexander . . . . . CL-P.3 SUNBaranikov, Anton . . . . . . . . . CJ-P.44 WEDBaranov, Andrey . . . . . . . . . �CE-P.23 TUEBaranovskii, Sergei . . . . . . . CE-11.6 WED
Barbano, Emerson . . . . . . . CD-5b.2 MON,CD-P.15 TUE, CE-9.5 TUE
Barbay, Sylvain . . . . . . . . . .�EF-4a.3 MON,EF-8.1 TUE
Barbier, Margaux . . . . . . . . . . �CF-6.3 THUBarbieri, Marco . . . . . . . . . . . JSV-3.1 THUBarbieri, Stefano . . . . . . . . . . . CC-2.2 SUNBarbillon, Grégory . . . . . . . . . . CL-4.3 THUBarbosa, Cristina . . . . . . . . . .CE-P.16 TUEBardou, Nathalie . . . . . . . . . . . CD-8.6 TUEBargigia, Ilaria . . . . . . . . . . . . JSIV-1.2 SUNBarilleau, Ludovic . . . . . . . . . . �EI-P.1 TUEBarillot, Thomas . . . . . . . . . . . CG-1.2 TUEBarland, Stéphane . . . . . . . . . EF-1.4 SUN,
EE-3.6 SUN, CB-7.4 WEDBarmenkov, Yuri . . . . . . . . . . . .CL-P.7 SUNBarnes, Mark . . . . . . . . . . . . . CC-P.13 SUNBarnett, Stephen . . . . . . . . . . EC-P.3 TUE,�EF-9.1 THUBarnett, Stephen M. . . . . . .EA-P.24 THU,
EA-P.33 THUBarnett, Stephen Mark . . . . . EC-2.3 TUEBaron, Alexandre . . . . . . . �CK-11.1 WED,�EH-4.1 WEDBaronio, Fabio . . . . . . . . . . . EF-4b.2 MON,�EF-P.20 THUBarré, Nicolas . . . . . . . . . . . . .CA-P.20 SUNBarreaux, Jonathan . . . . . . �CH-P.35 THUBarrera, David . . . . . . . . . . . . CH-6.6 WEDBarros, Helena G. . . . . . . . . . .CA-P.1 SUN,
CA-10.1 THU, CA-12.3 THUBarry, Liam P. . . . . . . . . . . . . . . CI-2.1 SUNBarry, Liam Paul . . . . . . . . . . . . CI-2.5 SUNBartalini, Saverio . . . . . . . . . . . CC-4.5 SUNBartels, Randy . . . . . . . . . . . . .CM-3.3 SUNBartelt, Hartmut . . . . . . . . . . . CJ-9.5 WEDBartenlian, Bernard . . . . . . . . .CL-4.3 THUBarthélémy, Alain . . . . . . . . . . CJ-1.3 SUN,
CJ-1.5 SUNBartley, Tim . . . . . . . . . . . . . JSV-P.6 MON,�JSV-1.5 THUBartley, Tim J. . . . . . . . . . . . JSV-P.7 MONBarua, Pranabesh . . . . . . . . . . CJ-3.2 SUN,
CJ-P.33 WED, CJ-9.2 WEDBarucci, Andrea . . . . . . . . . . CH-P.24 THUBarve, Ajit V. . . . . . . . . . . . . EB-P.13 WEDBarwick, Brett . . . . . . . . . . . . .EH-2.3 WEDBarz, Stefanie . . . . . . . . . . . . . JSV-1.3 THUBas, Derek . . . . . . . . . . . . . . . . �CC-4.1 SUNBashan, Gil . . . . . . . . . . . . . . . . EA-7.5 TUEBassignot, Florent . . . . . . . . . . EF-7.5 TUEBastiaens, Bert . . . . . . . . . . CM-P.19 SUN,
CH-P.35 THUBastock, Paul CE-2.6 SUN, CD-P.11 TUEBateman, James . . . . . . . . . CK-P.18 MONBateman, Sam . . . . . . . . . . . . .CJ-5.1 MONBatentschuk, Mirowslaw . . . . JSI-2.1 SUNBattesti, Rémy . . . . . . . . . . . �EA-P.13 THUBaudin, Emmanuel . . . . . . . . . EG-3.4 SUNBaudisch, Matthias . . . . . . . CG-3.4 WED,
CG-5.5 WEDBauer, Benjamin . . . . . . . . . .EE-5a.1 MONBauer, Dominik . . . . . . . . . . CA-P.12 SUN,
CA-P.22 SUN, CA-10.5 THUBauer, Thomas . . . . . . . . . . . .EG-P.1 MON
Bauerschmidt, Sebastian . . . �CD-1.1 SUNBaumgärtner, Stefan . . . . .CB-P.18 MON,
CB-3.4 TUEBaur, Simon . . . . . . . . . . . . . . . EA-2.1 SUNBausá, Luisa . . . . . . . . . . . . . . EH-P.9 WEDBautista, Godofredo . . . . . . . CM-P.5 SUN,
EG-P.11 MON, �CD-P.7 TUEBayn, Igal . . . . . . . . . . . . . . . . JSV-4.4 THUBaynes, Frederick . . . . . . . . . .ED-2.5 MONBaynes, Frederick N. . . . . . ED-1a.3 MONBaz, Assaad . . . CJ-3.5 SUN, CJ-3.6 SUNBazieva, Natalia . . . . . . . . . . CC-5.4 MON,
CC-5.5 MONBeaudoin, Grégoire . . . . . . . . .EF-2.4 SUN,
EF-2.5 SUN, EF-8.1 TUE, CK-10.1 WEDBeaudou, Benoit . . . . . . . . . .CJ-P.49 WEDBeausoleil, Ray . . . . . . . . . . . EA-P.28 THUBecheker, Rezki . . . . . . . . . . . . .CJ-2.4 SUNBecher, Christoph . . . . . . . . . .CE-4.4 SUN,
EA-6.6 TUE, EA-9.1 THU, EA-9.2 THUBéchou, Laurent . . . . . . . . . CB-P.33 MONBeck, Mattias CC-2.1 SUN, CC-2.2 SUN,
CC-2.4 SUN, EH-4.6 WEDBecker, Jonas Nils . . . . . . . . . �CE-4.4 SUNBecker, Nils . . . . . . . . . . . . . . �EE-P.13 SUNBecker, Petra . . . . . . . . . . . . . CD-10.3 TUEBecker, Simon F. . . . . . . . . �EG-P.6 MON,
CK-6.2 MONBednyakova, Anastasia . . . . �EF-3.5 SUN,
CF-P.26 WED, �EF-P.19 THUBeecher, Stephen . . . . . . . . . CE-7.2 MON,
CE-P.3 TUE, CE-P.34 TUE,�CJ-P.3 WEDBeere, Harvey CC-2.3 SUN, CC-2.5 SUN,
CC-P.14 SUN, CB-6.4 WEDBege, Roland . . . . . . . . . . . . . CD-P.35 TUEBeggs, Daryl . . . . . . . . . . . . . EG-P.16 MONBegleris, Ioannis . . . . . . . . . . . . .EI-P.7 TUEBeha, Katja . . . . . . . . . . . . . ED-1a.1 MON,�ED-1a.3 MONBehbood, Naeimeh . . . . . . . . EA-2.3 SUN,
EC-1.4 TUEBehrendt, Andreas . . . . . . . . CA-12.5 THUBeier, Franz . . . . . . . . . . . . . �CJ-10.6 WEDBein, Thomas . . . . . . . . . . . . CE-12.1 WEDBej, Subhajit . . . . . . . . . . . . .�CD-P.16 TUEBek, Alpan . . . . . . . . . . . . . . . . JSI-P.1 TUEBek, Roman �CB-P.18 MON, CB-3.4 TUEBelabas, Nadia . . . . . . . . . . . CK-4a.2 MONBelabas Plougonven, Nadia �CK-7.4 TUEBelardi, Walter . . . . . . . . . . . . CJ-5.1 MONBelardini, Alessandro . . . . �CD-P.21 TUE,
CK-13.5 WED, EH-5.2 THUBelghachem, Nabil . . . . . . . . CA-P.15 SUNBelkin, Mikhail A . . . . . . . . . . �CC-1.1 SUNBell, Alan P. . . . . . . . . . . . . . . . EH-6.6 THUBell, Bryn . . . . . . . . . . . . . . . . JSV-P.8 MONBelli, Federico EE-1.2 SUN, CD-12.3 THUBelshaw, Louise . . . . . . . . . . . CG-6.3 WEDBeltán-Pérez, Georgina . . . �CD-P.26 TUEBelzig, Wolfgang . . . . . . . . . EE-5a.2 MONBen Masaud, Taha . . . . . . . . .�CE-4.3 SUNBen-Youssef, Jamal . . . . . . . . EH-2.6 WEDBenabid, Fetah . . . . . . . . . . . . CH-5.1 TUE,
CG-2.3 TUE, CJ-8.4 WED, CF-5.2 WED
Bendahmane, Abdelkrim . . EE-P.10 SUN,EE-3.2 SUN, �CD-8.3 TUE
Benech, Pierre . . . . . . . . . . . . . CK-7.5 TUEBenedetti, Alessio . . . . . . . �CK-13.5 WED,
EH-5.2 THUBenedetti, Carlo . . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONBenedikter, Julia . . . . . . . . �CK-P.42 MONBengtsson, Samuel N. . . . . . . CG-1.5 TUEBenito, Mónica . . . . . . . . . . . EA-P.20 THUBènnes, Jonathan . . . . . . . . .CH-P.30 THUBennett, Andrew . . . . . . . . .�CE-10.1 WEDBenson, Oliver . . . . . . . . . . . . .CK-2.2 SUN,
CK-P.12 MON, EG-7.4 MON,CK-8.2 TUE
Benson, Trevor . . . . . . . . . . . . CJ-7.2 WED,EH-P.18 WED
Bentivegna, Marco . . . . . . . . EB-5.2 WED,�JSV-3.4 THUBeravat, Ramin . . . . . . . . . . . . �CI-3.3 SUNBercy, Anthony . . . . . . . . . . �ED-3.3 MON,�CH-P.33 THUBerdondini, Luca . . . . . . . . . . . CL-P.6 SUNBerendt, Martin O. . . . . . . . . �CJ-9.2 WEDBeresna, Martynas . . . . . . . �CM-6.3 MON,
CLEO/ECBO-2.3 WED, CJ-P.10 WED,CK-14.4 THU
Berg-Johansen, Stefan . . . . . �EA-1.2 SUNBerg-Sørensen, Kirstine
CLEO/ECBO-2.2 WEDBergé, Luc . . . EE-2.5 SUN, EE-P.1 SUN,
EI-2.6 THU, EI-3a.2 THUBerggren, Karl . . . . . . . . . . . EE-5a.3 MON,
CK-4b.1 MONBergues, Boris . . . . . . . . . . . . . CG-1.3 TUEBéri, Benjamin . . . . . . . . . . . . EH-1.5 WEDBérini, Bruno . . . . . . . . . . . . CK-P.15 MONBernal, M.-P. . . . . . . . . . . . . CK-11.2 WEDBernard, Deconihout . . . . . . CM-7.6 MONBerneschi, Simone . . . . . . . . CH-P.24 THUBernhard, Lamprecht . . . . . . �JSI-2.4 SUNBernhardi, Edward . . . . . . . . CJ-6a.3 MONBerni, Adriano A. . . . . . . . . . CH-P.22 THUBernier, Martin . . . . . . . . . . . . CJ-5.3 MONBerry, Dominic . . . . . . . . . . . . . EA-3.3 SUNBerry, Sam CC-P.13 SUN, EH-P.14 WEDBersch, Christoph . . . . . . . . . . .EF-2.3 SUNBerthelot, Johann . . . . . . . . . EA-10.6 THUBerti, Nicolas . . . . . . . . . . . . CD-P.14 TUE,
CG-P.16 THUBertolotti, Jacopo . . . . . . . . . . CL-4.5 THUBertolotti, Mario . . . . . . . . . . CN-P.1 TUE,
EH-5.2 THUBertone, Elisa . . . . . . . . . . . . .CE-P.24 TUEBertsch, George . . . . . . . . . . CG-P.14 THUBesga, Benjamin . . . . . . . . . . .CL-2.2 THU,
EA-10.6 THUBessing, Robert . . . . . . . . . . . CG-2.1 TUE,
CA-10.1 THUBettiati, Mauro . . . . . . . . . . CB-P.33 MONBettotti, Paolo . . . . . . . . . . . �EA-P.32 THUBetzig, Eric . . . . . . . . . . . . . . . .�PL-1.2 SUNBeugnot, Jean Charles . . . . �CD-1.3 SUN,
CD-6.3 MON, CD-P.23 TUE,CD-P.25 TUE, CD-10.1 TUE
Beveratos, Alexios . . . . . . . . CK-4a.2 MONBhandari, Rakesh . . . . . . . . .�CA-P.43 SUNBhardwaj, Ravi . . . . . . . . . . . . CM-P.2 SUNBhardwaj, Vedula R. . . . . . . CM-P.1 SUN,
CG-6.2 WEDBhattacharya, Arkabrata . . . . CC-4.3 SUNBhattacharya, Pallab . . . . . . �CB-9.1 THUBiadala, Louis . . . . . . . . . . . . . EG-7.5 MONBiagioni, Paolo . . . . . . . . . . . . EH-5.5 THUBiancalana, Fabio . . . . . . . . . . EF-7.4 TUE,
CD-12.3 THU, �CD-13.3 THUBianco, Giuseppe Valerio . . . CK-1.6 SUNBiant, Tristan . . . . . . . . . . . . . . CH-5.3 TUEBiasetti, Demian . . . . . . . . . CK-P.28 MONBibik, Efim . . . . . . . . . . . . . . CK-P.13 MONBiegert, Jens . EE-1.5 SUN, CA-4.3 SUN,
EG-5b.2 MON, CG-3.2 WED,CG-3.4 WED, CF-P.19 WED,CG-5.5 WED, CG-P.5 THU
Bienstman, Peter . . . . . . . . . . . CL-P.8 SUNBigot, Laurent . . . . . . . . . . . . �CE-1.1 SUN,
CJ-3.3 SUN, �CJ-3.5 SUN, CJ-3.6 SUNBijkerk, Fred . . . . . . . . . . . . . CH-P.35 THUBillard, Franck .CJ-2.1 SUN, EF-8.3 TUEBillat, Adrien . . . . . . . . . . . . . . �CD-1.6 SUNBillaud, Antonin . . . . . . . . . �CJ-P.30 WEDBillet, Cyril . . . . . . . . . . . . . . . EF-P.25 THUBinard, Guillaume . . . . . . . . . EH-P.2 WEDBinhammer, Thomas . . . . . . CG-4.3 WED,
CF-P.19 WEDBirindelli, Simone . . . . . . . . . JSV-2.5 THUBirkholz, Simon . . . . . . . . . �EF-4a.1 MON,
EE-5b.2 MON, �CF-5.1 WED,CF-9.4 THU
Birkl, Gerhard .CC-6.6 TUE, EC-P.8 TUEBirks, Tim . . . . . . . . . . . . . . . . . �CJ-3.4 SUNBirtas, Adrian . . . . . . . . . . . . CA-5b.2 MONBisadi, Zahra . . . . . . . . . . . . . EA-P.32 THUBismuto, Alfredo . . . . . . . . . .CB-7.3 WED,�PD-A.3 WEDBisschop, Suzanne . . . . . . . .EG-P.13 MONBiver, Emeric . . . . . . . . . . . . .CM-P.20 SUNBize, Sébastien . . . . . . . . . . . .ED-P.9 MONBlach, Jean-françois . . . . . . . CC-P.17 SUNBlanc, Wilfried . . . . . . . . . . . . CE-P.31 TUEBlanchenet, Anne-Marie . . . . CE-1.1 SUNBlanchet, Valérie . . . . . . . . . .CG-6.1 WED,
CG-6.2 WEDBlanco-Redondo, Andrea . �PD-B.6 WEDBlaser, Stéphane . . . . . . . . . . CB-7.3 WEDBledt, Carlos . . . . . . . . . . . . . .CC-P.14 SUNBloch, Daniel . . . . . . . . . . . . . . EG-4.4 SUNBloch, Jacqueline . . . . . . . . �EB/EG.1 TUEBlock, Erica . . . . . . . . . . . . . . . CM-3.3 SUNBlömer, Dominik . . . . . . . . . . . CC-6.6 TUEBlondy, Jean-Marc . . . . . . . . CJ-P.49 WEDBlum, Christian . . . . . . . . . . . . CL-2.1 THUBlume, Gunnar . . . . . . . . . . . CB-P.9 MON,�CB-P.10 MONBlumenroether, Elias . . . . . . . CL-3.1 THUBlumenstein, Andreas . . . . . CD-P.27 TUEBobkov, Konstantin . . . . . . . . �CJ-3.1 SUNBobrovsky, Alexey . . . . . . . . . CE-P.17 TUEBock, Martin EE-5b.2 MON, CF-1.2 TUEBock, Matthias . . . . . . . . . . . �EA-6.6 TUE,
205
Authors’ Index
EA-9.1 THUBódi, Balázs . . . . . . . . . . . . . . �CG-P.2 THUBoehm, Gerhard . . . . . . . . . . . .CC-1.1 SUNBoerkamp, Martijn . . . . . . . . . CH-4.3 SUNBoes, Andreas . . . . . . . . . . . �CM-6.6 MON,
EH-P.12 WEDBoetti, Nadia Giovanna . . . �CE-P.24 TUEBoge, Robert . . . . . . . . . . . . . .CG-4.1 WEDBogris, Adonis . . . . . . . . . . . . �CI-5.3 MON,
CB-P.23 MON, �CI-P.13 TUEBoguslavskiy, Andrey E. . . . .CG-6.2 WEDBoguslawski, Jakub . . . . . . . �CF-P.5 WEDBoguslawski, M. . . . . . . . . . . . .CD-2.1 SUNBoguslawski, Martin . . . . . CK-P.41 MON,
CK-13.4 WEDBohatý, Ladislav . . . . . . . . . . CD-10.3 TUEBöhm, Florian . . . . . . . . . . . . .EG-P.2 MONBoicea, Niculae . . . . . . . . . . CA-5b.2 MONBoiko, Dmitri . . . . . . . . . . . . .�CB-8.1 THU,
EF-P.10 THUBoitier, Fabien . . . . . . . . . . JSV-P.10 MONBoivinet, Simon . . . . . . . . . . . . �CJ-2.2 SUNBoland, John . . . . . . . . . . . . . . EH-6.6 THUBoller, Klaus . . . . . . . . . . . . .CM-P.19 SUN,
CK-5.4 MON, CJ-12.2 THU,CH-P.35 THU
Boller, Klaus-J. . . . . . . . . . . . . .�CI-4.5 SUNBoltasseva, Alexandra . . . . . . CE-3.2 SUN,
CE-P.30 TUEBomer, Thierry . . . . . . . . . . . . CH-9.2 WEDBonaldi, Michele . . . . . . . . . . . EA-4.5 SUNBonca, Janez . . . . . . . . . . . . . EE-P.17 SUNBongiovanni, Domenico . . . CD-13.5 THUBongs, Kai . . . . . . . . . . . . . . . .ED-P.9 MONBonifacio, Rodolfo . . . . . . . . . .EC-P.6 TUEBonneau, Damien . . . . . . . . . .EA-6.1 TUE,
JSV-1.1 THU, EA-P.28 THUBonsendorf, Dennis . . . . . . . �CB-P.8 MONBonvalet, Adeline . . . . . . . . . . EE-1.3 SUN,
CF-6.5 THUBony, Pierre-Yves . . . . . . . . . . . CI-4.3 SUNBonzon, Christopher . . . . . . . .CK-9.3 TUEBorisov, Pavel . . . . . . . . . . . . . . CC-4.1 SUNBorisov, Sergey . . . . . . . . . . . CH-P.31 THUBorkowski, Mateusz . . . . . . . CH-7.2 WEDBorlolozzo, Umberto . . . . . . . EF-P.5 THUBorrego-Varillas, Rocio . . . . �CF-6.1 THUBorrielli, Antonio . . . . . . . . . . . EA-4.5 SUNBortolozzo, Umberto . . . . . .CH-P.12 THUBorzsonyi, Adam . . . . . . . . . . CF-P.7 WED,
CF-P.21 WEDBosch, Thierry . . . . . . . . . . . . CH-8.1 WEDBoscolo, Sonia . . . . . . . . . . . . . �CI-3.1 SUNBose, Gaurav . . . . . . . . . . . .�CK-P.20 MONBotey, Muriel . . . . . . . . . . . . . CB-P.3 MON,
CB-P.4 MON, �EH-P.16 WEDBottegoni, Federico . . . . . . . JSIV-1.2 SUNBottrill, Kyle . . . . . . . . . . . . . . . �CI-4.4 SUNBouakline, Foudhil . . . . . . . . CG-P.13 THUBouazaoui, Mohamed . . . . . . CJ-1.3 SUN,
CE-1.1 SUN, CE-P.14 TUE,CE-P.15 TUE
Boucaud, Philippe . . . . . . . . . CB-4.3 WEDBoucher, Guillaume . . . . . . .�JSV-2.4 THUBouchon, Patrick . . . . . . . . . .CK-P.6 MON
Bouchoule, Sophie . . . . . . . . CE-11.4 WEDBoudjemaa, Laurent . . . . . . . CA-3.2 SUN,
CF-P.19 WED, CF-P.20 WEDBoudrioua, Azzedine . . . . . �CK-P.27 MONBouhelier, Alexandre . . . . .CK-P.15 MON,
EG-P.8 MONBouillard, Jean-Sebastien . . .EH-4.2 WEDBoulanger, Benoit . . . . . . . . . CE-P.13 TUEBoullet, Johan . . . . . . . . . . . . CJ-11.1 THUBourderionnet, Jérôme . . . . . CJ-1.4 SUN,�CK-7.3 TUEBourdon, Pierre . . . . . . . . . . . CJ-12.5 THUBourgeade, Antoine . . . . . . CM-P.21 SUN,
CM-5a.1 MONBourmpos, Michail . . . . . . . CB-P.31 MONBourquard, Florent . . . . . .CM/LIM.2 TUEBouwmans, Géraud . . . . . . . . .CJ-1.3 SUN,
CE-1.1 SUN, CJ-3.3 SUN, CJ-3.5 SUN,CJ-3.6 SUN, CD-12.2 THU
Bouwmeester, Dirk . . . . . . . EB-P.13 WEDBovino, Fabio Antonio . . . . . �CD-9.3 TUEBowden, Graham . . . . . . . . . EH-P.14 WEDBowen, Patrick . . . . . . . . . . . �EH-P.7 WEDBowen, Patrick G. . . . . . . . �CJ-P.35 WEDBowman, David . . . . . . . . . . . . EC-P.1 TUEBoyd, Robert . . . . . . . . . . . . . PD-A.4 WEDBoyle, Alexis CF-P.25 WED, CG-P.1 THUBrabec, Christoph J. . . . . . . . �JSI-2.1 SUNBrabec, Thomas . . . . . . . . . . CG-P.19 THUBracamontes Rodriguez, Yazmin-Esmeralda
CD-P.26 TUEBradac, Carlo . . . . . . . . . . . . . �CL-2.2 THU,
EA-10.6 THUBradler, Maximilian . . . . . . . . .CF-3.2 TUEBradley, Jonathan D. B. . . CK-12.2 WEDBragheri, Francesca . . . . . . . CM-1.4 SUN,
CL-P.11 SUN, JSII-1a.1 MON,CLEO/ECBO-2.2 WED, CL-1.3 WED
Braglia, Andrea . . . . . . . . . . . CL-P.14 SUNBrainis, Edouard . . . . . . . . . CK-4a.1 MON,�EG-P.13 MONBraive, Rémy . EF-2.5 SUN, EA-4.3 SUN,
CK-4a.2 MON, EF-8.1 TUE,CH-5.3 TUE, CK-10.1 WED
Bramati, Alberto . . . . . . . . CK-P.25 MON,EA-P.4 THU
Brambilla, Enrico . . . . . . . . . �EF-6.3 MON,EA-P.10 THU
Brambilla, Gilberto . . . . . . . . .CE-2.5 SUN,CD-5a.3 MON
Brambilla, Massimo . . . . . . . . EF-1.6 SUN,EE-3.6 SUN, CB-7.4 WED
Branchi, Federico . . . . . . . . . . CF-6.1 THUBranciard, Cyril . . . . . . . . . . EB-2a.1 MONBrandão-Silva, Antônio Carlos
CH-P.9 THUBrandstetter, Martin . . . . . . . .CC-1.4 SUNBrandus, Catalina . . . . . . . . .CA-10.4 THUBrandus, Catalina Alice . . . �CA-P.32 SUNBrasch, Victor . . . . . . . . . . . ED-1a.2 MON,�ED-P.8 MON, CE-9.1 TUEBrauch, Uwe . . . . . . . . . . . . . CB-P.2 MON,
CB-P.16 MONBraud, Alain . . . . . . . . . . . . . . . CE-1.2 SUNBraud, Flavie . . . . . . . . . . . . . . �EE-3.2 SUN
Brauner, Sebastian . . . . . . . . JSV-2.1 THUBravo-Abad, Jorge . . . . . . . . . JSI-1.3 SUNBrazhnikov, Denis . . . . . . . . �EF-P.26 THUBrecht, Benjamin . . . . . . . . �EB-2a.2 MONBrée, Carsten . . . . . . . . . . . . EF-4a.1 MON,
EE-5b.2 MON, EE-5b.3 MON,CF-P.33 WED, CG-P.9 THU
Brekenfeld, Manuel . . . . . . . . EA-P.6 THUBrelet, Yohann . . . . . . . . . . . . . CD-3.5 SUNBrener, Igal . EG-2.2 SUN, CK-6.3 MON,
CC-5.1 MON, EH-5.1 THUBrennecke, Ferdinand . . . . . . . EC-1.2 TUEBrenner, Carsten . . . . . . . . CB-P.21 MON,
CB-10.4 THUBrès, Camille-Sophie . . . . . . . CD-1.6 SUN,
CJ-13.3 THUBresson, Alexandre . . . . . . . .CD-P.36 TUEBretenaker, Fabien . . . . . . . . . CH-5.1 TUEBreuer, Stefan . . . . . . . . . . .CB-P.20 MON,
CC-6.6 TUE, CB-8.4 THU, CB-8.5 THU,CB-9.4 THU, CB-9.5 THU
Breunig, Ingo . . . . . . . . . . . . . .CD-4.4 SUN,CD-10.3 TUE, CD-10.4 TUE,CE-9.4 TUE
Briant, Tristan EA-4.3 SUN, EA-4.4 SUN,EA-P.18 THU
Brida, Daniele . . . . . . . . . . . . . EE-P.7 SUN,EE-P.17 SUN, EE-5a.2 MON,CF-1.1 TUE, EH-5.5 THU, EH-7.3 THU
Briggmann, Dieter . . . . . . . . . . CI-P.6 TUEBrignon, Arnaud . . . . . . . . . . . �CJ-1.4 SUNBrilland, Laurent . . . . . . . . . �CN-1.5 WEDBrimont, Christelle . . . . . . . . .CB-4.3 WEDBrinkmann, Ralf . . . . . . . . . . CA-P.28 SUNBrisset, Jean-Gabriel . . . . . .CD-P.14 TUE,
CD-P.33 TUEBristow, Alan . . . . . . . . . . . . . . CC-4.1 SUNBrito, José . . EA-9.1 THU, �EA-9.2 THUBrizuela, Fernando . . . . . . . . .CG-1.5 TUE,
CG-P.6 THU, CF-8.2 THUBrocklesby, William S . . . . . . .EE-P.6 SUNBroczkowska, Małgorzata . .CE-P.28 TUEBrod, Daniel . . . . . . . . . . . . . . JSV-3.4 THUBrod, Daniel J. . . . . . . . . . . . . EB-5.2 WEDBroderick, Neil G. R. . . . . . . . EF-3.1 SUN,
CJ-P.35 WEDBrongersma, Mark L. . . . . . CK-P.29 MONBronner, Wolfgang . . . . . . . .CB-P.7 MON,
CN-2.2 WEDBrons, Jonathan . . . . . . . . . .CA-P.12 SUN,�CA-P.22 SUN, �CA-P.34 SUN,
CD-8.4 TUE, PD-A.1 WED,CA-10.3 THU, CA-10.5 THU
Brown, Andrew . . . . . . . . . . . CM-7.5 MONBrown, Tom . . . . . . . . . . . . . . CM-7.5 MONBrowning, Colm . . . . . . . . . . . . .CI-2.5 SUNBrox, Olaf CD-P.40 TUE, �CB-11.5 THUBruce, Graham D. . . . . . . . . . . EC-P.1 TUEBrudieu, Barbara . . . . . . . . . CK-14.6 THUBrügmann, Michael . . . . . . . CF-P.34 WEDBrukner, Caslav . . . . . . . . . . . EB-5.4 WEDBrummitt, Pete . . . . . . . . . . CF-P.25 WEDBrun, Mickael . . . . . . . . . . . . . . CH-3.5 SUNBruna, Matteo . . . . . . . . . . . JSIV-1.2 SUN,
JSIV-1.5 SUN
Brune, Michel . . . . . . . . . . . . . .EA-P.2 THUBrunel, Marc EF-2.2 SUN, CA-P.20 SUN,
CN-1.4 WED, EF-P.1 THUBrunner, Daniel . . . . . . . . .�CB-P.34 MON,�CB-7.2 WED, EF-P.11 THU,
EF-P.22 THUBruno, Annalisa . . . . . . . . . . CE-12.3 WEDBruno, Giovanni . . . . . . . . . . . .CK-1.6 SUNBruß, Dagmar . . . . . . . . . . . . . EB-P.9 WEDBryche, Jean-François . . . . . . CL-4.3 THUBuades, Barbara . . . . . . . . . . . . EE-1.5 SUNBubertret, Benoit . . . . . . . . CK-P.15 MONBubnov, Mikhail . . . . . . . . . . . CJ-3.1 SUN,
CJ-8.5 WED, CJ-P.13 WED,CJ-P.48 WED
Buca, Dan . . . . . . . . . . . . . . . . . CB-1.4 TUEBuchegger, Bianca . . . . . . . . CM-6.4 MONBuchler, Ben . . . . . . . . . . . . . . EB-P.2 WEDBuchnev, Oleksandr . . . . . . . CD-7.2 MONBuchs, Gilles . . . . . . . . . . . . . . �CA-9.6 THUBuchvarov, Ivan . . . . . . . . . �CA-P.40 SUN,
CA-4.4 SUN, �CA-11.4 THUBuck, Alexander . . . . . . . . . . . .CG-2.4 TUEBuczyński, Ryszard . . . . . . . . CJ-5.4 MON,
CE-P.33 TUE, CH-P.26 THUBudriunas, Rimantas . . . . . . . �CF-2.5 TUEBudweg, Arne . . . . . . . . . . . . EE-5a.2 MONBuerger, Steven . . . . . . . . . . . CF-5.1 WEDBuettner, Thomas F. S. . . �CD-13.6 THUBugge, Frank . . . . . . . . . . . . . CB-11.2 THUBui, Anastasiya . . . . . . . . . . . . CA-8.5 TUEBuil, Stéphanie . . . . . . . . . �CK-P.15 MON,
EG-P.8 MON, EG-7.5 MONBulanov, Stepan . . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONBuldú, Javier . . . . . . . . . . . . . EF-P.22 THUBuller, Gerald S. . . . . . . . . . . .CN-2.4 WEDBundalo, Ivan-Lazar . . . . . . �CH-P.20 THUBurchardt, Daniel . . . . . . . . �EB-4.3 WED,
EB-P.12 WEDBurgdörfer, Joachim . . . . . . . EE-P.8 SUN,
CG-5.5 WEDBurger, Sven . . . . . . . . . . . . . . EA-8.5 WEDBürgi, René . . . . . . . . . . . . . . CH-P.31 THUBurgy, Frédéric . . . . . . . . . . . . CG-6.1 WEDBurkart, Johannes . . . . . . . . . . CH-2.5 SUNBurr, Geoffrey . . . . . . . . . . . . . . EG-4.6 SUNBurresi, Matteo . . . . . . . . . . . . CK-9.5 TUEBusch, Kurt . . . . . . . . . . . . . . . .CK-8.2 TUEBüse, Alexander . . . . . . . . . . . �EA-1.6 SUNBuse, Karsten . . . . . . . . . . . . . CD-4.4 SUN,
CD-10.3 TUE, CD-10.4 TUE,CE-9.4 TUE
Bustard, Philip . . . . . . . . . . . .EA-10.1 THUButcher, Thomas . . . . . . . . . . �CA-3.6 SUNButkus, Rytis . . . . . . . . . . . . . . EF-6.2 MONButkus, Simas . . . . . . . . . . . . . CM-1.5 SUNButler, Alex �CA-7.5 MON, CJ-P.30 WEDButler, Thomas . . . . . . . . . . . .CB-7.1 WEDButsch, Anna . . . . . . . . . . . . . CD-P.10 TUEButun, Serkan . . . . . . . . . . . .CK-11.4 WEDByer, Robert . . . . . . . . . . . . . . . CD-9.5 TUEBykov, Dmitry . . . . . . . . . . . . PD-A.9 WEDC. Ramirez, Jhonattan . . . . �JSII-P.1 TUECaballero Benitez, Santiago Francisco
EC-P.7 TUECabrera-Granado, Eduardo . . EE-2.5 SUNCacho, Cephise . . . . . . . . . . . . CG-3.3 WEDCadène, Agathe . . . . . . . . . . .EA-P.13 THUCadier, Benoît . . . . . . . . . . . . .CJ-12.5 THUCaer, Charles . . . . . . . . . . . . . CD-P.34 TUECai, Yin . . . . �EB-P.6 WED, EB-P.8 WEDCai, Yixiao . . . . . . . . . . . . . . . . . CL-4.1 THUCai, Ze-Rong . . . . . . . . . . . . . JSIV-1.4 SUNCaillaud, Céline . . . . . . . . . . . .CN-1.5 WEDCaimi, Daniele . . . . . . . . . . . . . CD-P.1 TUECalafell, Irati . . . . . . . . . . . . . . EB-5.4 WEDCalbris, Gaëtan . . . . . . . . . . . . . EG-4.5 SUNCalegari, Francesca . . . . . . . .CG-6.3 WED,
CF-8.4 THUCalendron, Anne-Laure . . . . .CA-4.2 SUN,
CA-10.2 THU, �CF-9.1 THUCalkins, Brice . . . . . . . . . . . . JSV-P.7 MONCallsen, Gordon . . . . . . . . . . CE-5a.2 MONCalmano, Thomas . . . . . . . �CJ-6a.1 MON,
CJ-6a.2 MON, CA-8.2 TUE,CE-P.6 TUE, CJ-P.41 WED,CA-9.5 THU
Calò, Cosimo .CI-2.5 SUN, CB-10.5 THUCalò, Giovanna . . . . . . . . . . .CK-P.31 MONCalvet, Pierre . . . . . . . . . . . . . . .CJ-3.3 SUNCalvez, Stéphane . . . . . . . . . CB-P.17 MONCalvo, Vincent . . . . . . . . . . . . CB-11.1 THUCamara, Abdoulaye . . . . . . . . .EF-9.3 THUCamara, Abdulaye . . . . . . . . . . EC-3.3 TUECamarasa-Gómez, María . . . CI-P.12 TUECambril, Edmond . . . . . . . . . . CK-7.4 TUECamellini, Andrea . . . . . . . . .CE-5a.1 MONCameron, Robert . . . . . . . . . �EC-P.3 TUE,
EF-9.1 THUCamon, Henri . . . . . . . . . . . . . . CK-1.2 SUNCampbell, Geoff . . . . . . . . . . . EB-P.2 WEDCampbell, Joe . . . . . . . . . . . . .ED-2.5 MONCampbell, Russell . . . . . . . . . . EC-P.4 TUECampenhout, Joris V. . . . . . CB-11.3 THUCamper, A . . . . . . . . . . . . . . . . . CF-8.5 THUCampi, Filippo . . . . . . . . . . . . .CG-1.5 TUE,
CG-P.6 THU, CF-8.2 THUCamps, Ivan . . . . . . . . . . . . . . �CE-6.2 MONCamy, Patrice . . . . . . . . . . . . . . CE-1.2 SUNCanalias, Carlota . . . . . . . . . CE-P.32 TUE,
CE-9.2 TUECanals Casals, Josep . . . . . . .CD-6.5 MONCanat, Guillaume . . . . . . . . . �CJ-12.5 THUCanbaz, Ferda . . . . . . . . . . . �CA-12.4 THUCanioni, Lionel . . . . . . . . . . .CM-5a.2 MONCankaya, Huseyin . . . . . . . . . . CA-4.2 SUN,
CA-10.2 THU, CF-9.1 THUCannard, Paul . . . . . . . . . . . . . CC-5.6 MONCanneson, Damien . . . . . . . CK-P.15 MONCanva, Michael . . . . . . . . . . . . .CL-4.3 THUCao, Hui . . . . . . . . . . . . . . . . .ED-1b.2 MONCao, Jianqiu . . . . . . . . . . . . . . . CJ-9.1 WEDCao, Shixun . . . . . . . . . . . . . . . .CC-4.2 SUNCapasso, Federico . . . . . . . . . �PL-2.1 MONCapmany, Jose . . . . . . . . . . . . CH-6.6 WEDCapmany, Juan . . . . . . . . . . . �CD-6.4 MONCapoen, Bruno . . . . . . . . . . . . . CE-1.1 SUNCapone, Massimo . . . . . . . . . EE-P.17 SUNCappelli, Francesco . . . . . . . �CB-6.2 WED
206
Authors’ Index
Caprara Vivoli, Valentina . . .EB-1.4 MONCaracciolo, Etienne . . . . . . . . . CA-2.1 SUNCarbajo, Sergio . . . . . . . . . . . . .CC-3.3 SUNCarbone, Fabrizio . . . . . . . . . . EH-2.3 WEDCarbone, Luigi . . . . . . . . . . . CK-P.25 MONCarbonell-Leal, Miguel . . . . . CL-P.17 SUNCarbonnel, Jérôme . . . . . . . . . CD-3.5 SUNCardenas, Daniel . . . . . . . . . . �CG-2.4 TUECardinal, Thierry . . . . . . . . .CM-5a.2 MONCarlos, Macias-Romero . . . . CL-P.10 SUNCarlos Zilio, Sergio . . . . . . . . . EE-P.5 SUNCarlson, David . . . . . . . . . . . . ED-2.2 MON,
CF-9.5 THUCarman, Robert . . . . . . . . . . . CH-P.7 THUCarminati, Marco . . . . . . . . CK-P.33 MONCarminati, Rémi . . . . . . . . . . . . EG-4.3 SUNCarmody, Neil . . . . . . . . . . . . . CJ-13.2 THUCarmon, Tal . . . . . . . . . . . . . . �CH-1.5 SUNCarolan, Jacques . . . . . . . . . . PD-B.3 WEDCarpeggiani, Paolo . . . . . . . . . .EE-1.4 SUNCarpenter, Lewis G. . . . . . . . . CE-2.5 SUN,�CE-10.4 WEDCarpintero Del Bario, Guillermo
CB-6.3 WEDCarras, Mathieu . . . . . . . . . . . CH-3.5 SUN,
CN-1.5 WED, CB-6.3 WED,CB-11.6 THU
Carré, B . . . . . . . . . . . . . . . . . . . CF-8.5 THUCarretero-Palacios, Sol . . . . �JSI-1.4 SUN,�JSI-2.2 SUN, EG-P.9 MONCarson, Christopher . . . . . . . . EC-P.2 TUECarstens, Henning . . . . . . . .CG-P.12 THU,
CF-9.2 THUCarter, Adrian . . . . . . . . . . . . .CJ-13.2 THUCarter, Richard M. . . . . . . . . . CE-1.5 SUNCaruso, Filippo . . . . . . . . . . . . JSV-3.2 THUCarusotto, Iacopo . . . . . . . . . . .EF-2.1 SUNCarvajal, Joan Josep . . . . . . . EH-P.9 WEDCarvalho, João Carlos de Aquino
EG-4.4 SUNCasagrande, Olivier . . . . . . . �CA-3.2 SUN,
CF-P.19 WED, CF-P.20 WEDCasalboni, Mauro . . . . . . . . . CH-P.10 THUCasanova, Alexis . . . . . . . . . . �CF-6.4 THUCasas-Bedoya, Alvaro . . . . . . CK-5.5 MONCascales, Concepción . . . . . . . CA-2.2 SUNCaspani, Lucia . . . . . . . . . . . . �EA-6.5 TUE,
EF-8.2 TUE, �EA-7.3 TUE,EH-3.4 WED, �PD-B.9 WED
Cassabois, Guillaume . . . . . . CB-4.3 WEDCassan, Eric . . . . . . . . . . . . . . CD-P.34 TUECassataro, Marco . . . . . . . . �CD-P.39 TUECassettari, Donatella . . . . . . .�EC-P.1 TUECassez, Andy CJ-3.3 SUN, CD-12.2 THUCassinerio, Marco . . . . . . . . . ED-2.3 MON,
ED-1b.2 MONCastellano-Hernandez, Elena�CA-2.2 SUNCastelló-Lurbe, David . . . . . . CD-P.9 TUECastiglioni, Luca . . . . . . . . . . .CG-4.5 WEDCastillejo, Marta . . . . . . . . . . �CM-2.2 SUNCastrillo, Antonio . . . . . . . . . ED-2.3 MON,
ED-2.6 MON, ED-P.5 MONCastro, Jarbas . . . . . . . . . . . . . .CL-P.1 SUNCastro-Lopez, Marta . . . . . . . EH-6.3 THU
Cataliotti, Francesco . . . . . . JSIV-2.5 SUNCataliotti, Francesco S. . . . . . EA-4.5 SUNCataluna, Maria Ana . . . . . . CB-10.3 THUCavalcanti, Eric G. . . . . . . . EB-2a.1 MONCeci Ginestrelli, Edoardo . . .CE-P.24 TUECeja-Fdez, Andrea . . . . . . . . . �CL-P.4 SUNCencillo-Abad, Pablo . . . . . .�CK-6.6 MONCenteno, Raymund . . . . . . . .�CB-6.5 WEDCentini, Marco . . . . . . . . . . . CD-P.21 TUE,�EH-5.2 THUCere, Alessandro . . . . . . . . . . . EA-1.4 SUN,�EC-2.2 TUE, �EA-6.2 TUECerullo, Giulio . . . . . . . . . . . . . EE-P.7 SUN,
EE-P.17 SUN, JSIV-1.2 SUN,JSIV-1.3 SUN, JSIV-1.5 SUN,EG-7.6 MON, CE-12.6 WED,CD-11.1 THU, CF-6.1 THU,CG-P.4 THU, CD-13.2 THU,CL-4.2 THU
Cesar, Julijan . . . . . . . . . . . . . . CB-2.3 TUECestari, André . . . . . . . . . . . . . .CL-P.1 SUNCetin, Arif . . . . . . . . . . . . . . .JSII-1a.3 MONCetin, Arif Engin . . . . . . . . . .JSII-2.3 MONChae, Chang Joon . . . . . . . . PD-B.4 WEDChahal, Radwan . . . . . . . . . . . . CE-1.2 SUNChaitanya Kumar, Suddapalli�CD-4.3 SUN, �CD-6.5 MONChalus, Olivier . . . . . . . . . . �CF-P.19 WED,
CF-P.20 WEDChamakou, Nektaria . . . . . . . CM-1.3 SUNChamorovskii, Yuri . . . . . . . . CJ-10.5 WEDChamorovskiy, Alexander . . �CB-7.5 WEDChan, Eng Aik . . . . . . . . . . . . .�EG-2.1 SUNChan, Ho-Yin . . . . . . . . . . . . .CD-P.17 TUEChan, Jaclyn S. . . . . . . . . . . . . .CJ-4.3 SUNChandrappan, Jayakrishnan �CE-1.3 SUNChanéac, Corinne . . . . . . . . . . .CE-1.1 SUNChanelière, Thierry . . . . . . . .EA-5.4 MON,
EA-10.4 THUChang, Darrick E. . . . . . . . . CK-10.3 WEDChang, Huan-Cheng . . . . . . . . CK-2.3 SUNChang, Lantian . . . . . . . . . . �CK-14.1 THUChang, Shu-Wei . . . . . . . . . . CK-14.3 THUChang, Wonkeun . . . . . . . . . . �EF-3.2 SUNChapman, Richard . . . . . . . . . CG-3.3 WEDCharalambidis, Dimitri . . . . . .CG-1.3 TUECharalambidis, Dimitris . . . . . EE-1.4 SUNChardonnet, Christian . . . . . ED-3.3 MON,
CH-P.33 THUCharra, Fabrice . . . . . . . . . . . . EH-P.2 WEDChatterjee, Gourab . . . . . . . . . CA-4.2 SUNChatzipetrou, Marianneza �CM-P.16 SUNChauvet, Mathieu . . . . . . . . . . �EF-7.5 TUEChauviere, Ludivine . . . . . . . .EE-P.17 SUNChaves de Souza Segundo, Pedro
EG-4.4 SUNChe, Huang . . . . . . . . . . . . . . . ED-P.3 MONChécoury, Xavier . . . . . . . . . . CK-7.3 TUE,
CB-4.3 WEDChekalin, Sergey . . . . . . . . . . CD-P.31 TUEChekhlov, Oleg . . . . . . . . . . . . .CA-3.6 SUNChekhova, Maria . . . . . . . . . . CD-9.1 TUE,
EA-7.4 TUEChelnokov, Alexis . . . . . . . . . CB-11.1 THUChembo, Yanne . . . . . . . . . . . . . CI-4.2 SUN
Chembo, Yanne K. . . . . . . . .ED-P.1 MON,CD-10.1 TUE
Chen, Bo-Han . . . . . . . . . . . . . . CF-3.1 TUEChen, Chih-Ying . . . . . . . . . . �CB-8.6 THUChen, Cong . . . . . . . . . . . . . . . . CE-2.1 SUNChen, Deying . . . . . . . . . . . . . . CN-P.2 TUEChen, Edward H. . . . . . . . . . . JSV-4.4 THUChen, Fang-Chung . . . . . . . .CE-12.2 WEDChen, George Y. . . . . . . . . . . . �CJ-4.3 SUNChen, He . . . . . . . . . . . . . . . . . �CJ-P.5 WEDChen, Hong-Yu . . . . . . . . . . . . . CF-3.1 TUEChen, Jinbao . . . . . . . . . . . . . .CJ-11.5 THUChen, Kuan-Yu . . . . . . . . . . . . CE-6.1 MONChen, Kun . . . . . . . . . . . . . . .�CH-P.28 THUChen, Kuo-Ju . . . . . . . . . . . . .�CE-P.9 TUE,
CE-P.10 TUEChen, Min . . . . . . . . . . . . . . . JSIII-1.3 MONChen, Ming-Chang . . . . . . . . . CF-3.1 TUEChen, Mingchen . . . . . . . . . �CJ-P.14 WEDChen, Qingtao . . . . . . . . . . . �CE-P.29 TUEChen, Qun-feng . . . . . . . . . . . ED-2.4 MONChen, Shengping . . . . . . . . . . .CJ-P.5 WEDChen, Shihua . . . . . . . . . . . . . EF-P.20 THUChen, Siming . . . . . . . . . . . . . . CB-9.2 THUChen, Teng-Ming . . . . . . . . . . .CE-P.9 TUEChen, Tzu-Pei . . . . . . . . . . . �CK-14.3 THUChen, Wei Ting . . . . . . . . . . . . . EI-1.4 THUChen, Xiaoshuang . . . . . . . . EG-5a.3 MONChen, Xu . . . . . . . . . . . . . . . . . . EA-4.3 SUNChen, Ya . . . EG-P.11 MON, CD-P.7 TUEChen, Yang-Fang . . . . . . . . . CK-14.3 THUChen, Yaohui CK-3.2 SUN, CB-10.1 THUChen, Yen-Hung . . . . . . . . . . CF-P.17 WEDChen, Yi . . . . . . . . . . . . . . . . . .CA-P.13 SUNChen, Yu-Hui . . . . . . . . . . . . . .EA-5.2 MONChen, Zhaodong . . . . . . . . . . . CN-P.2 TUEChen, Zhigang CD-7.4 MON, EI-1.2 THUChen, Zhighang . . . . . . . . . . .CD-13.5 THUChen, Zilun . . . . . . . . . . . . . . . . CJ-7.5 WEDChenais, Sébastien . . . . . . . .CA-P.27 SUN,�CE-8.2 TUE, CK-12.3 WEDCheng, Chih-Hao . . . . . . . . . . .CB-8.6 THUCheng, Guanghua . . . . . . . . . . CD-P.2 TUECheng, Tonglei . . . . . . . . . . . CD-6.1 MON,
CE-P.12 TUE, CJ-P.43 WED,�CJ-P.45 WEDCheng, Weibo . . . . . . . . . . . . .�CM-3.2 SUNCheng, Wenlong . . . . . . . . . . . EH-2.5 WEDCheng, Xiang’ai . . . . . . . . . . . . . CI-P.9 TUECheng, Yu-Chen . . . . . . . . . . . . CF-3.1 TUECheng, Yu Chieh . . . . . . . . . . CK-1.4 SUN,�CK-1.5 SUN, �CH-P.21 THUCherchi, Matteo . . . . . . . . . . . �CI-P.7 TUE,
CH-6.1 WEDChernysheva, Maria . . . . . . . �CF-P.6 WEDChervinskii, Semen . . . . . . . EH-P.11 WEDChevrollier, Martine . . . . . . . . EG-4.4 SUNChi, Gou-Chung . . . . . . . . . . . . CE-P.9 TUEChia, Shih-Hsuan . . . . . . . . . . CG-P.4 THUChichkov, Boris . . . . . . . . . . �CM-2.1 SUN,
CK-P.22 MONChilds, David T.D. . . . . . . . .CE-11.1 WEDChimier, Benoit . . . . . . . . . . CM-P.21 SUN,
CM-5a.1 MON, CM-5a.2 MON,EI-P.1 TUE
Chin, See Leang . . . . . . . . . . .�EE-4.1 SUN,EI-2.6 THU
Chin, Xin Yu . . . . . . . . . . . . �CE-12.3 WEDChiu, Sheng-Huan . . . . . . . . . . CE-P.9 TUEChng, Brenda . . . . . . . . . . . . . . EA-6.2 TUEChodorow, Urszula . . . . . . . . CC-P.17 SUNChoi, Duk . . . . . . . . . . . . . . . . . CH-3.2 SUNChoi, Duk-yong . . . . . . . . . . . .CD-1.5 SUN,
PD-B.4 WEDChoi, Jae-Hyuck . . . . . . . . . .CK-11.5 WEDChoi, Ju Won . . . . . . . . . . . . . �CE-9.3 TUEChoi, Sun Young . . . . . . . . . . CE-P.6 TUE,
CJ-P.23 WED, CF-4.5 WED,�CA-9.5 THUChojetzki, Christoph . . . . . . . CJ-9.5 WEDChojnowska, Olga . . . . . . . . . CC-P.17 SUNChong, Andy . . . . . . . . . . . . . . . CF-1.6 TUEChong, Harold . . . . . . . . . . . . . .CE-4.3 SUNChong, Harold M.H. . . . . . . . . CE-4.2 SUNChong, Katie . . . . . . . . . . . . . . .EG-2.2 SUNChou, Chun-Hsien . . . . . . . . CE-12.2 WEDChou, Shaoi-wei . . . . . . . . . . . .CG-2.4 TUEChou, Yu-Hsun . . . . . . . . . . �CE-12.2 WEDChoudhary, Amol . . . . . . . . . CE-7.2 MON,
CE-P.3 TUE, CJ-P.3 WEDChow, Weng Wah . . . . . . . . CB-P.29 MONChowdhury, Avishek . . . . . . . . �EF-2.5 SUNChriki, Ronen . . . . . . . . . . . . . . CA-P.4 SUNChristian, James M. . . . . . . . �EI-P.4 TUE,�EI-P.7 TUE, �EF-P.23 THUChristiansen, Silke . . . . . . . . . EG-6.1 MONChristodoulides, Demetrios . EA-1.3 SUN,
EF-2.3 SUN, CD-3.4 SUN, CD-7.4 MON,CB-1.2 TUE
Christodoulides, Demetrios N.CI-1.2 SUN, CE-3.1 SUN, CB-4.4 WED
Christoph, Ulbricht . . . . . . . . . JSI-2.4 SUNChrzanowski, Helen . . . . . . . . EB-3.2 WEDChu, Sai T . CD-P.13 TUE, EA-6.5 TUE,
EF-8.2 TUE, PD-B.9 WEDChu, Sai Tak . . . . . . . . . . . . . . . EA-7.3 TUEChu, Wei-Chun . . . . . . . . . . �CG-P.11 THUChua, Sheon EA-4.4 SUN, �EA-P.18 THUChuchumishev, Danail . . . . .CA-11.4 THUChung, Hung-Ping . . . . . . . .CF-P.17 WEDChung, Il-Sug . . . . . . . . . . . . CB-P.35 MONChung, U-Chan . . . . . . . . . . . .CC-5.1 MONChurkin, Dmitry . . . . . . . . . . . .CJ-4.2 SUN,
CD-P.8 TUE, CJ-P.8 WED,�EF-P.6 THU, EF-P.29 THU,EI-2.1 THU, �EI-2.2 THU
Ciamei, Alessio . . . . . . . . . . . . EB-5.1 WEDCiampini, Donatella . . . . . . . PD-B.5 WEDCiampini, Mario A. . . . . . . . .EA-P.27 THUCiampini, Mario Arnolfo . . �EB-P.9 WED,�JSV-2.2 THUCiappina, Marcelo . . . . . . . EG-5b.2 MON,
CF-P.32 WED, �CG-P.10 THUCibella, Sara . . . . . . . . . . . . . . EH-4.6 WEDCiccacci, Franco . . . . . . . . . . JSIV-1.2 SUNCicchi, Riccardo . . . . . . . . . . . . CC-4.5 SUNCiers, Joachim . . . . . . . . . . . EG-P.13 MONCiesielski, Richard . . . . . . . . CE-12.1 WEDCimek, Jarosław . . . . . . . . . . .CJ-5.4 MON,�CE-P.33 TUE
Ciracì, Cristian . . . . . . . . . . . . �CK-8.6 TUECireasa, Raluca . . . . . . . . . . . . CG-6.2 WEDCirelli, Claudio . . . . . . . . . . . . �CG-4.1 WEDCiret, Charles . . . . . . . . . . . . . . �EF-7.3 TUECiriolo, Anna Gabriella . . . . .JSV-3.2 THUCirmi, Giovanni . . . . . . . . . . . CG-P.4 THU,
CF-9.1 THUCiurana, Alex . . . . . . . . . . . . . .EB-4.4 WEDClark, Alasdair . . . . . . . . . . . . . CK-8.5 TUEClark, Alex . . . . . . . . . . . . . . . CE-12.5 WEDClark, Thomas William . . . . . EC-2.3 TUEClarke, Brendan . . . . . . . . . �EG-5a.3 MONClarkson, Andrew . . . . . . . . . CJ-11.6 THUClarkson, Andy . . . . . . . . . . . CJ-P.10 WEDClarkson, W. Andrew . . . . . CA-7.5 MON,
CJ-P.29 WED, CJ-P.30 WED,CJ-14.3 THU, CJ-14.6 THU
Claudon, Julien . . . . . . . . . . . EE-P.16 SUN,EG-6.5 MON, CD-P.32 TUE
Clausen, Christop . . . . . . . . . . .EA-2.5 SUNClément, Quentin . . . . . . . . . .CN-1.1 WEDClements, Wallace . . . . . . . . EF-P.19 THUClerc, Marcel EF-4a.3 MON, EF-P.2 THUClerc, Marcel Gabriel . . . . . . . EF-8.5 TUE,
EF-P.3 THUClerici, Matteo . . . . . . . . . . . . CC-P.6 SUN,�EE-3.3 SUN, CD-5a.2 MON,�CD-7.4 MON, �CC-6.5 TUE,
EA-6.5 TUE, EA-7.3 TUE, EH-3.4 WEDClewes, Rhea . . . . . . . . . . . . . . CN-2.1 WEDCluzel, Benoît CK-1.2 SUN, CK-8.3 TUE,
CK-11.1 WEDCobb, Stuart . . . . . . . . . . . . . . . CL-3.4 THUCocchi, Eugenio . . . . . . . . . . . . EC-1.2 TUECocker, Tyler L. . . . . . . . . . . . . CF-7.1 THUCodemard, Christophe A. . . . .CJ-4.3 SUNCoen, Stéphane . . . . . . . . . . . �EF-1.1 SUN,
EE-3.5 SUN, ED-P.2 MON,EF-P.18 THU, CD-13.1 THU
Cohadon, Pierre-François . . .EA-4.3 SUN,EA-4.4 SUN, CH-5.3 TUE, EA-P.18 THU
Coillet, Aurelien . . . . . . . . . ED-1a.1 MON,ED-P.1 MON
Cojocaru, Crina . . . . . . . . . . . .CK-1.4 SUN,CK-1.5 SUN, CD-5b.1 MON,CH-P.21 THU
Colakoglu, Tahir . . . . . . . . . . . JSI-P.1 TUEColangelo, Giorgio . . . . . . . . . EA-2.3 SUN,
EC-1.4 TUEColas Des Francs, Gérard CK-P.15 MON,�EG-P.3 MON, EG-P.8 MONColdren, Larry A. . . . . . . . . . EB-P.13 WEDCole, Daniel . . . . . . . . . . . . . .ED-1a.1 MONCole, Daniel C. . . . . . . . . . . . ED-1a.3 MONCole, Garrett D. . . . . . . . . . . . .CF-9.3 THUColet, Pere . . . . . . . . . . . . . . CB-P.27 MON,�ED-P.1 MON, EF-P.28 THUCollier, John CA-3.6 SUN, CF-P.25 WED,
CG-P.1 THUCollins, Matthew . . . . . . . . . . PD-B.4 WEDColombe, Yves . . . . . . . . . . . . PD-B.1 WEDColombier, Jean-Philippe . . . CM-2.4 SUNColuccelli, Nicola . . . . . . . . . ED-2.3 MON,�ED-1b.2 MONColumbo, Lorenzo . . . . . . . . . .EF-1.6 SUN,
207
Authors’ Index
EE-3.6 SUN, CB-7.4 WEDCombrié, Sylvain . . . . . . . . . . .CK-3.4 SUN,
CK-5.1 MON, CD-6.2 MON,CK-7.3 TUE
Comby, Antoine . . . . . . . . . . . CG-6.1 WEDComin, Riccardo . . . . . . . . . . EE-P.17 SUNComoretto, Davide . . . . . . . . EG-P.4 MONConforti, M. . . . . . . . . . . . . . . EF-P.17 THUConforti, Matteo . . . . . . . . . .EE-P.10 SUN,�EE-P.12 SUN, EF-5.5 MON,
EF-4b.2 MON, CD-8.3 TUE,EF-P.20 THU, EI-2.1 THU
Consoli, Antonio . . . . . . . . . . EF-P.12 THUConsolino, Luigi . . . . . . . . . . . . CC-4.5 SUNConti, Claudio . . . . . . . . . . . . .CD-3.3 SUN,
CD-5a.2 MON, CD-7.5 MONContreras, Victor . . . . . . . . �CH-P.11 THUCoolbaugh, Douglas . . . . . . CK-12.2 WEDCoolen, Laurent . . . . . . . . . CK-P.25 MON,
EG-7.5 MON, EH-P.2 WEDCooper, Andrew . . . . . . . . . . . . EF-8.2 TUECooper, Jonathan . . . . . . . . . . CK-8.5 TUECooper, Jonathan M. . . . . .�JSII-2.4 MONCooper, Merlin . . . . . . . . . . . �EA-P.15 THUCooper, Peter A. . . . . . . . . . CE-10.4 WEDCopie, François . . . . . . . . . . . �EF-5.5 MONCoradin, Thibaud . . . . . . . . . . .CL-3.3 THUCorbett, Brian . . . . . . . . . . . CB-P.30 MONCordette, Steevy . . . . . . . . . . . CD-1.6 SUNCorena, Len . . . . . . . . . . . . . . .CJ-13.2 THUCormier, Eric . CA-2.3 SUN, CL-P.5 SUN,
CJ-9.3 WEDCornet, Marion . . . . . . . . . . . �CC-P.9 SUN,�CC-P.10 SUNCorral, Inés . . . . . . . . . . . . . . . CG-P.13 THUCorrielle, Giacomo . . . . . . . . JSV-P.8 MONCorrielli, Giacomo . . . . . . . . �CM-4.4 SUN,
EB-4.1 WED, JSV-2.2 THUCortecchia, Daniele . . . . . . . CE-12.3 WEDCorti, Tommaso . . . . . . . . . . .EF-6.3 MON,
EA-P.10 THUCosci, Alessandro . . . . . . . . . CH-P.24 THUCosi, Franco . . . . . . . . . . . . . .CH-P.24 THUCoskun, Ahmet . . . . . . . . . �JSII-1a.3 MONCossairt, Oliver . . . . . . . . . . . . . . . . . . . . . �JS
SPIE/OM/EQEC.3 MONCosta, Fabio . . . . . . . . . . . . . . .EB-5.4 WEDCotlet, Mircea . . . . . . . . . . . . JSV-4.4 THUCouairon, Arnaud . . . . . . . . . . EE-2.4 SUN,
EE-P.4 SUN, CM-3.1 SUN, EE-3.3 SUN,CM-5a.3 MON, CD-7.4 MON,CD-P.3 TUE
Couceiro, Ramiro . . . . . . . . . CM-P.11 SUNCoudert-Alteirac, Hélène . . .�CG-P.6 THUCoudreau, Thomas . . . . . . . . JSV-2.4 THUCoulibaly, Saliya . . . . . . . . . EF-4a.3 MON,�EF-P.2 THU, EF-P.5 THU, EF-P.7 THUCouris, Stelios . . . . . . . . . . . . CE-P.33 TUECourjal, N. . . . . . . . . . . . . . . . CK-11.2 WEDCourjal, Nadege . . . . . . . . . . . . CK-7.5 TUECourjaud, Antoine . . . . . . . .CD-P.33 TUE,
CF-6.4 THUCourvoisier, Francois . . . . . . �EE-2.4 SUN,
EE-P.3 SUN, CM-7.2 MONCousin, Seth . . . . . . . . . . . . . . .�EE-1.5 SUN
Cousin, Seth L. . . . . . . . . . . �CG-3.2 WED,CG-P.5 THU
Couteau, Christophe . . . . . . . . EG-3.5 SUNCoutts, David CA-1.5 SUN, CB-5.5 WED,
EH-P.12 WEDCoutts, David W . . . . . . . . . . CA-6.5 MONCox, Joel . . . . . . . . . . . . . . . . . �CK-8.4 TUECraig, Chris . . . . . . . . . . . . . . . . CE-2.6 SUNCraig, Christopher . . . . . . . . CD-P.11 TUECrawford, Stephanie . . . . . . . �CJ-4.1 SUN,
CJ-7.3 WEDCreagh, Stephen . . . . . . . . . EH-P.18 WEDCrespi, Andrea . . . . . . . . . . . . CM-4.4 SUN,
EB-4.1 WED, �EB-5.1 WED,EB-5.2 WED, JSV-2.2 THU,�JSV-3.2 THU, JSV-3.4 THU
Crespo, Helder . . . . . . . . . . .CF-P.31 WED,CF-5.3 WED, CG-P.7 THU
Criante, Luigino . . . . . . . . . . . CM-P.9 SUNCrisafi, Francesco . . . . . . . . . CD-13.2 THUCristescu, Simona . . . . . . . . . CH-4.3 SUN,
CF-1.5 TUE, CB-6.5 WEDCristiani, Ilaria . . . . . . . . . . . .CL-P.11 SUN,
JSII-1a.1 MON, CD-6.6 MON,CD-P.4 TUE, CLEO/ECBO-2.2 WED,CL-1.3 WED
Cristiani, Matteo . . . . . . . . . EB/EG.2 TUECrump, Paul . . . . . . . . . . . . . �SH-10.1 SUN,
CB-P.5 MON, CB-5.3 WED,CB-5.4 WED
Cruz, José Luis . . . . . . . . . . . . CL-P.7 SUN,CH-P.27 THU
Ctistis, Georgios . . . . . . . . . . EE-P.16 SUN,EA-3.2 SUN, CD-P.32 TUE
Cui, Bifeng . . . . . . . . . . . . . . . CB-10.3 THUCui, Can . . . . . . . . . . . . . . . . . .CA-P.13 SUNCui, Long . . .CE-2.6 SUN, CD-P.24 TUE,
CI-P.1 TUECumming, Benjamin . . . . . . . . CE-3.4 SUNCurutchet, Arnaud . . . . . . . CB-P.33 MONCvetojevic, Nick . . . . . . . . . . �CH-7.4 WEDCzaplicki, Robert . . . . . . . . EH-P.11 WED,
CE-12.4 WEDCzornomaz, Lukas . . . . . . . . . .CD-P.1 TUEDaan, Lenstra . . . . . . . . . . . . . �CB-8.2 THUDabu, Razvan . . . . . . . . . . . . CF-P.20 WEDDacarro, Giacomo . . . . . . . . . EG-P.4 MOND’Acremont, Quentin . . . . . . .CF-6.4 THUDadalyan, Tigran . . . . . . . . .CK-13.4 WEDDagens, Beatrice . . . . . . . . . �CK-8.3 TUE,
EH-2.6 WEDDahlström, Marcus . . . . . . . . CG-5.1 WEDDahnoun, Naim . . . . . . . . . . . CH-9.4 WEDDai, Tongyu . . . . . . . . . . . . . . �CJ-14.2 THUDainese, Paulo . . . . . . . . . . . CK-P.38 MONDajczgewand, Julian . . . . . . . EA-5.4 MONDal Conte, Stefano . . . . . . �EE-P.17 SUN,�JSIV-1.2 SUN, JSIV-1.3 SUN,
JSIV-1.5 SUNDalacu, Dan . EA-8.2 WED, EA-P.7 THUDamascelli, Andrea . . . . . . . . EE-P.17 SUND’Ambrosio, Vincenzo . . . . . . EA-7.1 TUED’Amico, Ciro . . . . . . . . . . . . . CD-P.2 TUEDamzen, Michael . . . . . . . . . . CA-P.2 SUN,
CA-3.4 SUN, CA-6.4 MON
Danckaert, Jan . . . . . . . . . . CB-P.22 MON,EH-3.3 WED
Dancus, Ioan . . . . . . . . . . . . . CF-P.20 WEDD’Andrea, Cosimo . . . . . . . . JSIV-1.2 SUNDaniault, Louis EE-1.3 SUN, CF-6.5 THUDaniel, Jae . �CJ-11.6 THU, CJ-13.2 THUDaniels, Joost . . . . . . . . . . . .JSIII-1.4 MONDanilevičius, Rokas . . . . . . �CF-P.15 WEDDantelle, Géraldine . . . . . . . .CK-14.6 THUDaran, Emmanuelle . . . . . . CB-P.17 MONDarmo, Juraj �CC-2.4 SUN, CC-P.4 SUN,
EH-P.1 WEDDas, Susanta Kumar . . . . . . EE-5b.2 MONDascalu, Traian . . . . . . . . . . CA-P.29 SUN,
CA-P.32 SUN, CA-5b.2 MON,�CA-10.4 THUDashkevich, Vladimir . . . . . . . CA-8.5 TUEDatta, Animesh . . . . . . . . . . . . EA-6.3 TUEDaubenschüz, Markus . . . �CB-P.14 MONDaveau, Raphaël . . . . . . . . . . PD-B.7 WEDDavidson, Alan . . . . . . . . . . . .CJ-13.2 THUDavidson, Nir . . . . . . . . . . . . . . CA-P.4 SUNDavies, Giles . CC-1.3 SUN, CC-5.6 MONDawes, Judith . . . . . . . . . . . . EH-P.12 WEDDawson, Martin . . . . . . . . . . . CA-1.3 SUN,
CB-3.5 TUEDe Abajo, Javier . . . . . . . . . . . �EI-1.1 THUDe Angelis, Costantino . . . . . EH-7.4 THUDe Angelis, Francesco . . . . . .CL-P.6 SUN,
EG-P.10 MON, EH-5.6 THUde Araujo, Cid . . . . . . . . . . . . . CH-2.2 SUNDE Biévre, S. . . . . . . . . . . . . . EF-P.17 THUDe Boni, Leonardo . . . . . . . CE-P.16 TUE,
CE-9.5 TUE, �CE-9.6 TUEDe Camillis, Simone . . . . . . . CG-6.3 WEDde Ceglia, Domenico . . . . . . . CK-1.6 SUN,�EH-7.4 THUDe Ceuninck, Ward . . . . . . . . . CL-P.8 SUNde Dios, Cristina . . . . . . . . . CB-P.11 MONDe Fazio, Domenico . . . . . . JSIV-1.2 SUN,
JSIV-1.5 SUN, EE-5a.2 MONde Fornel, Frédérique . . . . . CK-11.1 WEDde Groot, Peter . . . . . . . . . . EH-P.14 WEDde Hoogh, Anouk . . . . . . . . . �EG-4.1 SUN,�EF-6.6 MON, �EH-1.3 WEDde Jong, Jakko . . . . . . . . . . . EG-P.12 MONde la Peña, Jose Luis . . . . . . CE-P.27 TUEDe la Rosa, Elder . . . . . . . . . . .CL-P.4 SUNde Lasson, Jakob Rosenkrantz
CK-P.9 MONDe Leseleuc, Sylvain . . . . . . . EB-P.3 WEDDe Marco, Carmela . . . . . . . . CM-1.4 SUNde Mengin, Mikhael . . . . . . . . CK-7.5 TUEde Nalda, Rebeca . . . . . . . . . . CM-2.2 SUNDe Natale, Paolo . . . . . . . . . . CC-4.5 SUN,
CD-8.2 TUE, CH-P.36 THUde Oliveira, C.E.M. . . . . . . . . . EF-7.2 TUEde Paula Siqueira, Jonathas �EE-P.5 SUNde Ridder, René M. . . . . . . . CK-14.1 THUde Riedmatten, Hugues . . . .EA-5.4 MON,
EA-5.5 MON, EB/EG.2 TUEde Roo, Tjaard . . . . . . . . . . . EG-P.14 MONDe Rosa, Maurizio . . . . . . . . �CD-8.2 TUE,
CH-P.36 THUDe Rossi, Alfredo . . . . . . . . . . CK-3.4 SUN,
�CK-5.1 MON, CD-6.2 MON,CK-7.3 TUE
De Sio, Antonietta . . . . . . . . �EG-7.6 MONde Sterke, Carel . . . . . . . . . . �EH-P.8 WEDde Torres, Juan . . . . . . . . . . . �EG-7.3 MONDe Valcárcel, Germán J. . . . .EF-8.6 TUE,
EF-9.4 THU, EA-P.21 THUDe Vault, Clayton . . . . . . . . . CE-P.30 TUEde Vido, Mariastefania . . . . . .CA-3.6 SUNde Vine, Glenn . . . . . . . . . . . . .CH-P.3 THUDe Vittorio, Massimo . . . . . . .CK-1.6 SUNDe Vizia, Maria Domenica . ED-2.6 MONDe Wilde, Yannick . . . . . . . . . .EG-4.3 SUNDean, Julian . . . . . . . . . . . . . . . CH-3.3 SUNDebayle, Arnaud . . . . . . . . . . . EI-3a.2 THUDebord, Benoit . . . . . . . . . . . . CJ-8.4 WEDDebord, Bonoît . . . . . . . . . . . . CH-5.1 TUEDebray, Jérôme . . . . . . . . . . . CE-P.13 TUEDecker, Jonathan . . . . . . . . . CB-5.3 WED,�CB-5.4 WEDDecker, Manuel . . . . . . . . . . . �EG-2.2 SUN,
CK-6.3 MON, EH-5.1 THU,�EH-5.3 THUDecleva, Piero . . . . . . . . . . . . CG-6.3 WED,
CG-P.17 THUDecobert, Jean . . . . . . . . . . . . .CK-7.1 TUEDeconihout, Bernard . . . . . CM-5b.1 MONDeDood, Michiel J.A. . . . . . . .EA-6.4 TUEDeepak, K. L. N. . . . . . . . . . . CM-P.1 SUNDeepak, Kallepalli . . . . . . . . . �CM-P.2 SUNDegasperis, Antonio . . . . . .�EF-4b.3 MONDegen-Knifton, Arthur W . . �EE-P.6 SUNDegert, Jérôme . . . . . . . . . . . . CC-P.9 SUN,
CC-P.10 SUNDegl’Innocenti, Riccardo . . . CC-2.3 SUN,
CC-2.5 SUN, CC-P.14 SUN,�CB-6.4 WEDDekker, Peter . . . . . . . . . . . . .CJ-P.41 WEDDekorsy, Thomas . . . . . . . . . . . CC-P.5 SUNDel Re, Eugenio . . . . . . . . . . . . EF-1.6 SUNDel Re, Lorenzo . . . . . . . . . . . . EA-7.1 TUEDel Vecchio, Pamela . . . . . �CB-P.33 MONDelagnes, Jean Christophe . CA-2.3 SUN,
CL-P.5 SUN, CJ-9.3 WEDDelaporte, Philippe . . . . . . �CM-P.20 SUNDelaye, Philippe . . . . . . . . . . CD-P.34 TUEDeleglise, Samuel . . . . . . . . . . EA-4.3 SUN,
EA-4.4 SUN, CH-5.3 TUE, EA-P.18 THUDélen, Xavier . . . . . . . . . . . . . . CA-9.2 THUDelgado-Pinar, Martina . . .CH-P.27 THU,
CH-P.32 THUDel’Haye, Pascal . . . . . . . . �ED-1a.1 MON,
ED-1a.3 MONDella Valle, Giuseppe . . . . . . EB-5.1 WEDDeloison, Florent . . . . . . . . . . . CL-P.5 SUNDelplace, Karen . . . . . . . . . . . . .CJ-1.3 SUNDelRe, Eugenio . . . . . . . . . . . CD-7.5 MON,
EF-7.2 TUEDematteo Caulier, Ophélie CM-P.21 SUN,
CM-5a.1 MONDemichel, Olivier . . . . . . . . . . . CK-1.2 SUNDEMIRBAS, UMIIT . . . . . . �CA-P.42 SUNDemirbas, Umit . . . . . . . . . . �CF-4.4 WED,
CA-12.4 THUDemircan, Ayhan . . . . . . . . . EE-P.14 SUN,
EF-3.3 SUN, EF-4a.1 MON,EE-5b.2 MON
Demirhan, Yasemin . . . . . . . .CE-P.11 TUEDemmerle, Frederic . . . . . . . . .CC-1.1 SUNDemmler, Stefan . . . . . . . . . .CG-3.1 WED,
CF-8.1 THUDeng, Dinghuan . . . . . . . . . . CD-6.1 MON,
CE-P.12 TUE, CJ-P.43 WED,CJ-P.45 WED
Deng, Ke . . . . . . . . . . . . . . . . . ED-P.3 MONDeninger, Anselm . . . . . . . . . . CC-6.6 TUEDenisov, Alexander . . . . . . . . . CJ-3.1 SUNDenz, Cornelia . . . . . . . . . . . . �CD-2.1 SUN,
CD-2.4 SUN, CK-P.41 MON,CK-13.4 WED, CD-11.2 THU
Depauw, Valérie . . . . . . . . . . . . JSI-1.5 SUNDeppe, Bastian . . . . . . . . . . CJ-6a.2 MON,�CA-7.2 MONDergachev, Alexander A. . . . CN-P.4 TUEDerntl, Christian Georg . . . . �CC-P.4 SUNDeryagin, Anton G. . . . . . . .CB-P.22 MONDerycke, Christophe . . . . . . . CA-3.2 SUN,
CF-P.19 WEDDeSantolo, Anthony . . . . . . . . CJ-4.6 SUNDescamps, Dominique . . . . . CA-2.3 SUN,
CG-6.1 WED, CG-6.2 WEDDescloux, Delphine . . . . . . . . �CD-2.3 SUNDésévédavy, Frederic . . . . . . CD-6.1 MONDesfarges-Berthelemot, Agnès
CJ-1.3 SUN, CJ-1.5 SUNDesgreniers, S. . . . . . . . . . . . . CM-P.1 SUNDeshayes, Yannick . . . . . . . .CB-P.33 MONDetchprohm, Theeradetch . PD-A.2 WEDDetz, Hermann . . . . . . . . . . . . .CC-1.4 SUNDeutsch, Christoph . . . . . . . . . CC-1.4 SUNDevaux, Fabrice . . . . . . . . . . . . EF-7.5 TUEDeveaud, Benoît . . . . . . . . . . EG-P.5 MON,
CD-9.4 TUEDevi, Kavita CD-4.1 SUN, CD-6.5 MON,�CD-10.5 TUEDevillard, Raphael . . . . . . . . . �CL-P.5 SUNDevine, Natasha . . . . . . . . . . . . EI-2.4 THUdeVries, Oliver CJ-8.1 WED, CJ-8.2 WEDDeWolf, Timothy . . . . . . . . . . EG-7.1 MONDhaka, Veer EG-P.11 MON, CD-P.7 TUEDherbecourt, Jean-Baptiste CD-2.3 SUN,
CD-P.36 TUE, �CN-1.1 WEDDhillon, Sukhdeep . . . . . . . . . . CC-1.3 SUNDhingra, Shonali . . . . . . . . . . . CJ-P.3 WEDDholakia, Kishan �CLEO/ECBO-2.4 WEDDi Dio Cafiso, Samuele Davide
CA-2.1 SUNDi Falco, Andrea . . . . . . . . . . EG-4.2 SUN,
CD-P.5 TUE, EH-3.4 WEDDi Lauro, Luigi . . . . . . . . . . . CD-P.13 TUEdi Lieto, Alberto . . . . . . . . . . . CA-4.4 SUNDi Mauro, Louis . . . . . . . . . . . �CG-1.1 TUEDi Mei, Fabrizio . . . . . . . . . �CD-7.5 MON,
EF-7.2 TUEDi Tano, Maira . . . . . . . . . . JSII-1a.1 MONDi Trapani, Paolo . . . . . . . . . . CM-3.1 SUNDiallo, Souleymane . . . . . . . .CD-10.1 TUEDiamanti, Eleni . . . . . . . . . . . EB-P.5 WED,
JSV-4.2 THUDias, Frédéric . . . . . . . . . . . . . EF-P.25 THU
208
Authors’ Index
Dias Ponte, Antonio . . . . . . �CE-P.27 TUEDíaz, Francesc . . . . . . . . . . . CA-P.31 SUN,
CA-4.5 SUN, CA-5a.1 MON,CA-5a.2 MON, CA-5b.3 MON,EH-P.9 WED
Dickinson, Christopher . . . . EF-P.23 THUDickson, Wayne . . . . . . . . . . .EH-4.2 WED,
EH-4.4 WEDDiddams, Scott . . . . . . . . . . ED-1a.1 MON,
ED-2.5 MONDiddams, Scott A. . . . . . . . .ED-1a.3 MONDidier, Marie . . . . . . . . . . . . . . .CL-3.5 THUDidierjean, Julien . . . . . . . . . . CA-9.2 THUDiebel, F. . . . . . . . . . . . . . . . . . .CD-2.1 SUNDiebel, Falco . . . . . . . . . . . . . CK-13.4 WEDDiebold, Andreas . . . . . . . . . . CJ-8.4 WED,
CH-8.2 WED, CF-9.3 THUDiederichs, Carole . . . . . . . . . �EG-3.4 SUNDiels, Jean-Claude . . . . . . . . CH-P.13 THUDierolf, Volkmar . . . . . . . . . CE-5b.2 MON,�CE-P.19 TUEDíez, Antonio . . . . . . . . . . . . . .CL-P.7 SUN,
CH-P.17 THU, �CH-P.27 THU,CH-P.32 THU
DiGiovanni, David . . . . . . . . . . CJ-4.6 SUNDijkstra, Meindert . . . . . . . . CK-14.1 THUDilhaire, Stefan . . . . . . . . . . . . CF-6.4 THUDinani, Hossein . . . . . . . . . . . . �EA-3.3 SUNDinca, Mihai . . . . . . . . . . . . CA-5b.2 MON,
CA-10.4 THUDinesan, Hemanth . . . . . . . . ED-2.6 MON,
ED-P.5 MONDing, He . . . . . . . . . . . . . . . . . . .JSI-1.5 SUNDing, Lei . . . . . . . . . . . . . . . . . CA-P.13 SUNDing, Ying .CK-14.2 THU, CB-10.3 THUDing, Yu . . . . . . . . . . . . . . . . . . �CA-P.5 SUNDipalo, Michele . . . . . . . . . . . . CL-P.6 SUNDisseix, Pierre . . . . . . . . . . . . CE-11.4 WEDDittel, Christoph . . . . . . . . . �JSV-3.5 THUDivya, Sasi . . . . . . . . . . . . . . . CE-12.4 WEDDiziain, Séverine . . . . . . . . . . . CD-8.1 TUEDmochowski, Greg . . . . . . . . . EA-2.6 SUN,
CD-9.2 TUEDocampo, Pablo . . . . . . . . . .CE-12.1 WEDDoeleman, Hugo . . . . . . . . . . EG-6.3 MONDolan, Philip . . . . . . . . . . . . . . . EC-3.2 TUEDolfi, Daniel . . . . . . . . . . . . . .CH-P.12 THUDolores-Calzadilla, Victor . . . CK-3.1 SUNDombi, Péter . . . . . . . . . . . . �CA-P.35 SUN,
CC-3.1 SUN, �EG-5b.2 MON,CG-P.2 THU
Domenico, D’Agostino . . . . . CB-8.2 THUDominec, Filip . . . . . . . . . . . . .CC-5.1 MONDominguez, Jason . . . . . . . . . . EG-2.2 SUNDominguez-Juarez, Jorge Luis�EH-6.5 THUDonaire, Manuel . . . . . . . . . . .EG-P.7 MONDonnet, Christophe . . . . . CM/LIM.2 TUEDöpke, Benjamin . . . . . . . . CB-P.21 MON,�CB-10.4 THUDoran, Nick . . . . . . . . . . . . . . . . CI-P.5 TUED’Orazio, Antonella . . . . . . . . CK-1.6 SUNDoroschenko, Maxim E. . . . CA-P.24 SUNDorrer, Christophe . . . . . . . . CD-11.4 THUDostovalov, Alexandr V. . . . .CM-4.2 SUN
Dotsenko, Igor . . . . . . . . . . . . . EA-P.2 THUDoualan, Jean-Louis . . . . . . . . CE-1.2 SUNDouay, Marc . . . CJ-3.3 SUN, CJ-3.6 SUNDouce, Tom . . . . . . . . . . . . . . JSV-2.4 THUDouillet, Sabine . . . . . . . . . . . CE-P.13 TUEDowd, Emma . . . . . . . . . . . . . .EB-5.4 WEDDowling, Jonathan . . . . . . . . . EA-3.3 SUNDowner, Michael . . . . . . . . �JSIII-1.2 MONDownes, James . . . . . . . . . . .EH-P.12 WEDDoyen, Ioana . . . . . . . . . . . . . . CB-5.3 WEDDrag, Cyril . . . . . . . . . . . . . . . . .CD-2.3 SUNDrampyan, Rafael . . . . . . . �CK-13.4 WEDDrazdys, Ramutis . . . . . . . . . . CK-1.5 SUNDréau, Anaïs . . . . . . . . . . . . . EA-10.3 THUDreisow, Felix . . . . . . . . . . . . . �CM-4.6 SUNDreissen, Laura . . . . . . . . . . . .ED-2.1 MONDresiow, Felix . . . . . . . . . . . . . . EA-1.3 SUNDrevinskas, Rokas . . . . . . . . CM-6.3 MON,�CLEO/ECBO-2.3 WED, �CK-14.4 THUDrewes, Jan . . . . . . . . . . . . . . . .EC-1.2 TUEDrexler, Wolfgang�CLEO/ECBO-1.1 WEDDriad, Rachid . . . . . . . . . . . . . CN-2.2 WEDDriben, Rodislav . . . . . . . . . �EF-6.4 MON,�EF-P.16 THUDrouard, Emmanuel . . . . . . . . JSI-1.5 SUNDruon, Frédéric CJ-1.1 SUN, CJ-1.3 SUN,
CA-2.3 SUN, CG-2.2 TUEDrzewietzki, Lukas . . . . . . .CB-P.20 MON,
CB-8.4 THU, CB-9.4 THU, CB-9.5 THUDszotjan, David . . . . . . . . . . . EG-P.3 MONDu, Pengyuan . . . . . . . . . . . . CA-P.13 SUNDu Preez, Neil . . . . . . . . . . . . CA-12.6 THUDuan, Xiaofeng . . . . . . . . . . . CE-P.29 TUEDuan, Yuwen . . . . . . . . . . . . CJ-P.18 WED,
JSV-1.4 THUDubertret, Benoit . . . . . . . CK-P.25 MON,
EG-P.8 MON, EG-7.5 MONDubietis, Audrius . . . . . . . . CM-5a.3 MONDubrasquet, Romain . . . . . . .CJ-11.1 THUDubreuil, Nicolas . . . . . . . �CD-5a.1 MON,�CD-P.34 TUEDubrovkin, Alexander . . . . . �EH-2.1 WEDDucci, Sara . . . . . . . . . . . . .JSV-P.10 MON,
CD-10.6 TUE, JSV-2.4 THUDuchateau, Guillaume . . . . CM-P.21 SUN,
CM-5a.1 MON, CM-5a.2 MON,EI-P.1 TUE
Duchemin, Ivan . . . . . . . . . . . CB-11.1 THUDuchesne, Constance . . . . . CF-P.30 WEDDucloy, Martial EG-2.1 SUN, EG-4.4 SUNDudelev, Vladislav V. . . . . .CB-P.22 MONDudley, Angela . . . . . . . . . . . . . CH-2.4 SUNDudley, John EE-3.1 SUN, CM-7.2 MON,
EF-P.25 THUDudley, John M. . . . . . . . . . . . EE-2.4 SUN,
EE-P.3 SUN, CF-6.3 THU, CD-13.5 THUDuffus, Ben . . . . . . . . . . . . . . EB-2a.1 MONDuggal, Monty . . . . . . . . . . . .CM-7.5 MONDúill, Seán P. Ó . . . . . . . . . . . . .CI-2.1 SUNDujardin, G. . . . . . . . . . . . . . . EF-P.17 THUDumergue, Mathieu . . . . . . . CG-6.1 WEDDumitrescu, Michael . . . . . . . CB-5.1 WEDDumitrescu, Mihail . . . . . . . CB-P.26 MONDuncan, Cameron . . . . . . . . . EH-P.8 WED
Duparré, Michael . . . . . . . . . . .CH-2.4 SUNDupont-Ferrier, Eva . . . . . . . .EG-1.5 SUN,
CK-2.4 SUNDupont-Nivet, Matthieu . . . �EC-2.4 TUEDupont, Sune . . . . . . . . . . . . . . CH-3.4 SUNDuport, François . . . . . . . . . . . CI-5.1 MONDupuis, Christophe . . . . . . . . . CD-8.6 TUEDupuis, Russell D. . . . . . . . . �PD-A.2 WEDDupuis, Russell Dean . . . . . CE-11.4 WEDDurak, Kadir . . . . . . . . . . . . . . . EC-P.5 TUEDurán-Sánchez, Manuel . . . CD-P.26 TUEDurán, Vicente . . . . . . . . . . . . CF-P.9 WEDDurécu, Anne . . . . . . . . . . . . . CJ-12.5 THUDurfee, Charles . . . . . . . . . . . . CM-3.3 SUNDürr, Stephan . . . . . . . . . . . . . . EA-2.1 SUND’Urso, Brian . . . . . . . . . . . . . .CJ-P.3 WEDDussardier, Bernard . . . . . . .CE-P.31 TUE,�CI-P.4 TUEDutta, Rahul . . . . . . . . . . . . . . . EE-3.1 SUNDuval, Simon . . . . . . . . . . . . . . CJ-5.3 MONDuvochelle, Pierre-Antoine CF-P.20 WEDDvoyrin, Vladislav . . . . . . . . �CJ-7.4 WED,
CJ-P.32 WEDDymshits, Olga . . . . . . . . . . . . CE-P.5 TUEDzipalski, Adrian . . . . . . . . . �CH-9.5 WEDE. Beere, Harvey . . . . . . . . . . PD-B.7 WEDE. Hernandez-Figueroa, Hugo
JSII-P.1 TUEEason, Robert . . . . . . . . . . . . CL-P.16 SUN,
CM-P.17 SUN, CE-7.2 MON,CE-P.3 TUE, CJ-P.3 WED, CL-1.4 WED
Eason, Robert W. . . . . . . . . . CM-7.4 MONEbendorff-Heidepriem, Heike CM-P.8 SUNEberhardt, Ramona . . . . . . . . CJ-4.5 SUN,
CJ-8.2 WED, CJ-P.17 WED,CJ-10.3 WED, CJ-10.6 WED,CJ-11.4 THU
Ebrahim-Zadeh, M. . . . . . . . . .CD-4.3 SUNEbrahim-Zadeh, Majid . . . . .�SH-2.1 SUN,�CD-4.1 SUN, CD-6.5 MON,
CD-10.5 TUEEchternkamp, Katharina E.�EG-5a.1 MON, EG-5a.2 MONEckstein, Andreas . . . . . . . . JSV-P.6 MON,
JSV-2.4 THUEconomou, Eleftherios N. . . . CE-3.3 SUNEder, Bastian . . . . . . . . . . . . �CH-9.6 WED,
CJ-12.3 THUEdwards, Tom . . . . . . . . . . . . CM-7.5 MONEfetov, Dmitri . . . . . . . . . . . . JSIV-2.3 SUNEfremidis, Nikolaos . . . . . . . . �EI-1.2 THU,�EI-1.5 THUEggeling, Christian . . . . . . . . .�SH-3.1 SUNEggleton, Benjamin . . . . . . . CK-5.5 MON,
PD-B.4 WED, PD-B.6 WED,EF-P.24 THU
Eggleton, Benjamin J. . . . . CD-13.6 THUEibl, Matthias . . . . . . . . . . . . CD-P.19 TUEEich, Pascal . EA-9.1 THU, EA-9.2 THU,�EA-9.3 THUEichelkraut, Toni . . . . . . . . . . . CH-2.4 SUNEichhammer, Emanuel . . . . �EA-5.3 MONEichhorn, Marc . . . . . . . . . . . CA-P.39 SUNEidam, Tino CJ-1.2 SUN, CG-P.12 THU,
CF-9.2 THU
Eikema, Kjeld . . . . . . . . . . . . . ED-2.1 MONEikema, Kjeld SE . . . . . . . . . . .CH-1.4 SUNEilanlou, Abdolreza Amani . CG-6.4 WEDEilenberger, Falk . . . . . . . . . . EE-P.13 SUNEisaki, Hiroshi . . . . . . . . . . . . .EE-P.17 SUNEisele, Max . . . . . . . . . . . . . . . . CF-7.1 THUEl-Amraoui, Mohammed . . CJ-P.34 WEDEl-Ganainy, Ramy . . . . . . . . . �CB-1.2 TUE,�EI-P.6 TUEEl Gmili, Youssef . . . . . . . . . CE-11.4 WEDEl Hamzaoui, Hicham . . . . . . CJ-1.3 SUN,
CE-1.1 SUN, CE-P.14 TUE,CE-P.15 TUE
El Taher, Atalla . . . . . . . . . . . . .CJ-4.2 SUNElahi, Parviz . . . . . . . . . . . . . . . .CJ-2.6 SUNElahi, Perviz . . . . . . . . . . . . . .CJ-P.19 WEDElena P., Silaeva . . . . . . . . . . CM-7.6 MONElesin, Yuriy . . . . . . . . . . . . . . . CK-9.1 TUEElezzabi, Abdulhakem . . . . EG-5b.2 MONElissalde, Cathy . . . . . . . . . . . CC-5.1 MONEllinas, Kosmas . . . . . . . . . . .CM-P.16 SUNEllis, Andrew . . �CI-1.3 SUN, CI-3.4 SUNElman, Vladimir . . . . . . . . . . . EA-P.3 THUEloi, Fabien . . . . . . . . . . . . . CK-P.15 MON,�EG-P.8 MONElsaesser, Thomas . . . . . . . EE-5b.2 MON,
CF-1.2 TUEElsäßer, Wolfgang . . . . . . . CB-P.13 MON,
CC-6.6 TUE, CB-8.4 THU, CB-9.4 THU,EA-P.16 THU, EA-P.17 THU
Emaury, Florian . . . . . . . . . . �CJ-8.4 WED,�CH-8.2 WED, �CF-9.3 THUEmons, Moritz . . . . . . . . . . . . . CA-3.5 SUNEmsia, Ali . . . . . . . . . . . . . . . . . . CI-P.6 TUEEndo, Akira . . . . . . . . . . . . . . .CA-P.30 SUNEndo, Mamoru . . . . . . . . . . . . �CF-4.2 WEDEngelsen, Søren Balling . . . . .CH-3.4 SUNEngland, Duncan . . . . . . . . . EA-10.1 THUEnglund, Dirk . . . . . . . . . . . �JSIV-2.3 SUN,�CK-4b.1 MON, EB-3.4 WED,
JSV-1.2 THU, JSV-4.4 THUEppich, Bernd . . . . . . . . . . . . CB-P.6 MON,
CB-P.10 MONEpping, Jörn . . . . . . . . . . . . . �CK-5.4 MONErattupuzha, Sonia . . . . . . . . EE-P.8 SUN,
EE-4.3 SUN, CG-6.5 WED,�CG-6.6 WEDErbert, Goetz . . . . . . . . . . . . . CB-5.3 WEDErbert, Götz CB-P.5 MON, CB-P.6 MON,
CB-P.12 MON, CB-P.19 MON,CD-P.40 TUE, CB-5.4 WED,CB-10.4 THU, CB-11.2 THU,CB-11.5 THU
Ercolani, Daniele . . . . . . . . . . . CF-7.1 THUErgecen, Emre . . . . . . . . . . . . . CJ-2.6 SUN,
CM-P.18 SUN, �CK-P.3 MONErkintalo, Miro EF-1.1 SUN, EF-3.1 SUN,
EE-3.4 SUN, �EE-3.5 SUN,EF-P.18 THU, EF-P.25 THU,�CD-13.1 THU
Ermolov, Alexey . . . . . . . . . . . �EE-1.1 SUNErneux, Thomas . . . . . . . . . CB-P.22 MON,
EF-P.1 THU, EF-P.28 THUErni, Daniel . . . . . . . . . . . . . . . . JSI-2.3 SUNErni, Rolf . . . . . . . . . . . . . . . . . .CD-P.1 TUE
Ernsting, Ingo . . . . . . . . . . . . ED-2.4 MON,ED-3.4 MON
Ertel, Klaus . . . . . . . . . . . . . . . . CA-3.6 SUNErven, Chris . . . . . . . . . . . . . . JSV-4.5 THUEs, F . . . . . . . . . . . . . . . . . . . . . . JSI-P.1 TUEEsarey, Eric . . . . . . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONEscaff, Daniel . . . . . . . . . . . . . . EF-P.3 THUEscalante, Jose . . . . . . . . . . . CB-11.1 THUEschner, Juergen . . . . . . . . . . . EA-9.3 THUEschner, Jürgen . . . . . . . . . . . EA-9.1 THU,
EA-9.2 THUEsfandyarpour, Majid . . . . .CK-P.29 MONEsmann, Martin . . . . . . . . . . EG-P.6 MON,
CK-6.2 MONEsposito, Marco . . . . . . . . . . CK-13.5 WEDEsquivias, Ignacio . . . . . . . . . CB-5.2 WED,
CB-7.6 WED, EF-P.12 THUEsser, Dominik . . . . . . . . . . �CE-10.3 WEDEsteban-Martin, Adolfo . . . . CD-4.1 SUN,
EF-8.6 TUEEsteso, Victoria . . . . . . . . . . . �EG-P.9 MONEtezadi, Dordaneh . . . . . . JSII-1a.3 MON,�JSII-2.3 MONEttoumi, Wahb . . . . . . . . . . �CD-P.38 TUEEuser, Tijmen . . . . . . . . . . . . .PD-A.9 WEDEverett, Jesse . . . . . . . . . . . . . EB-P.2 WEDF. de Sá, Gilberto . . . . . . . . CK-P.19 MONFabian, Matthias . . . . . . . . . . .CH-P.6 THUFabian, Simone . . . . . . . . . . . . CJ-8.2 WEDFabre, Baptiste . . . . . . . . . . . CG-6.1 WED,
CG-6.2 WEDFABRE, Claude . . . . . . . . . . . . EA-1.1 SUN,
ED-P.4 MON, ED-1b.3 MON,EB-P.6 WED, EB-P.8 WED
Fabris, Davide . . . . . . . . . . . . �CG-1.2 TUE,�CF-5.3 WEDFaccio, Daniele EF-2.1 SUN, EE-3.3 SUN,
CD-7.4 MON, CF-3.5 TUE,�EH-3.4 WED, �CN-2.4 WEDFade, Julien . . . . . . . . . . . . . . . .CL-3.2 THUFaez, Sanli . . . . . . . . . . . . . . . . . EG-3.2 SUNFaggiani, Rémi . . . . . . . . . . . CK-11.1 WEDFairfield, Jessamyn A. . . . . . . EH-6.6 THUFaist, Jérôme .CC-2.1 SUN, CC-2.2 SUN,
CC-2.4 SUN, CB-1.4 TUE, CK-9.3 TUE,CB-6.2 WED, EH-4.6 WED,PD-B.8 WED, CB-11.1 THU
Falcao-Filho, Edilson . . . . . . �CH-2.2 SUNFalkner, Matthias . . . . . . . . . . EG-2.2 SUNFalkovich, Gregory . . . . . . . . . . EI-2.2 THUFallnich, Carsten . . . . . . . . . . CK-5.4 MONFan, Dengfeng . . . . . . . . . . . . .CF-P.1 WEDFan, Fan . . . . . . . . . . . . . . . . . . CB-4.1 WEDFan, Guangyu CF-2.1 TUE, CG-2.3 TUE,�CF-5.2 WEDFan, Rongwei . . . . . . . . . . . . . . CN-P.2 TUEFan, Shanhui . . . . . . . . . . . . . . �JSI-1.1 SUNFan, Shuzhen . . . . . . . . . . . . . . CC-P.7 SUNFan, Youwen . . . . . . . . . . . . . �CJ-12.2 THUFang, Chao . . . . . . . . . . . . . . . .EH-4.1 WEDFang, Fengzhou . . . . . . . . . . . EH-1.5 WEDFang, Shaobo . . . . . . . . . . . . . �CG-P.4 THUFang, Wenjing . . . . . . . . . . . . CE-P.29 TUEFang, Xu . . . . . . . . . . . . . . . . . . �EG-2.3 SUN
209
Authors’ Index
Fanjoux, Gil . . . . . . . . . . . . . . �CD-6.3 MONFaoro, Riccardo . . . . . . . . . . . PD-B.5 WEDFarahi, Salma . CL-5.3 THU, CL-5.5 THUFarinello, Paolo . . . . . . . . . . . . CA-1.4 SUNFarkas, Balázs . . . . . . . . . . . . . CG-P.6 THUFarkas, Gyözö . . . . . . . . . . . . . . CC-3.1 SUNFarley, Kevin . . . . . . . . . . . . . . CJ-13.2 THUFarnesi, Daniele . . . . . . . . . . CH-P.24 THUFarrell, Carl . . . . . . . . . . . . . . CD-11.4 THUFarrera, Pau . . . . . . . . . . . . . EB/EG.2 TUEFarries, M. . . . . . . . . . . . . . . . . .CJ-7.2 WEDFarsari, Maria .CM-1.3 SUN, CE-3.3 SUNFasci, Eugenio . . . . . . . . . . . . ED-2.3 MON,
ED-2.6 MON, �ED-P.5 MONFatome, Julien . . . . . . . . . . . . . CI-4.3 SUN,
EF-4b.2 MONFattahi, Hanieh . . . . . . . . . . . �CF-1.3 TUE,
CG-P.3 THUFattakhova, Zukhra T. . . . . CE-P.25 TUEFaucon, Marc . . . . . . . . . . . . . . TF-2.1 TUEFaugeron, Mickael . . . . . . . . . CB-5.2 WEDFaure, Basile . . . . . . . . . . . . . . CN-1.1 WEDFaure, Benoit . . . . . . . . . . . . . �CH-9.2 WEDFavero, Ivan . . . . . . . . . . . . JSV-P.10 MON,
CD-10.6 TUE, JSV-2.4 THUFedder, Helmut . . . . . . . . . . . . CK-2.3 SUNFedorov, Nikita . . . . . . . . . . . . . EI-P.1 TUEFedorov, Vladimir Yu. . . . . . . CC-P.8 SUNFedorova, Ksenia . . . . . . . . . . CB-3.2 TUE,
CF-P.2 WEDFedorova, Ksenia A. . . . . . �CD-P.28 TUE,
CE-11.3 WEDFedoruk, Mikhail . . . . . . . . . CF-P.26 WED,
CJ-P.40 WED, EF-P.19 THUFedotov, Andrei B. . . . . . . . . . CF-3.4 TUEFedotov, Ilya . . . . . . . . . . . . . . �CL-5.6 THUFedotov, Sergey . . . . . . . . . . .CM-6.3 MONFedotov, Vassili A. . . . . . . . . . . EI-1.4 THUFedotova, Olga . . . . . . . . . . .�EF-P.15 THUFedrizzi, Alessandro . . . . . . �EB-1.1 MON,
EB-2a.1 MONFehrembach, Anne-Laure . CK-11.3 WEDFehrenbacher, David . . . . . . �ED-P.7 MONFei, Jiarui . . . . . . . . . . . . . . . . .CE-P.29 TUEFeinaeugle, Matthias . . . . . CM-P.17 SUN,�CM-7.4 MONFeise, David CB-P.9 MON, CB-P.10 MONFeist, Armin . . . . . . . . . . . . . .EG-5a.1 MONFeizpour, Amir . . . . . . . . . . . . �EA-2.6 SUN,
CD-9.2 TUEFejer, Martin . . . . . . . . . . . . . . .CD-9.5 TUEFekete, Júlia . . . . . . . . . . . . . EG-5b.2 MONFélix, Corinne . . . . . . . . . . . . . CE-P.13 TUEFeng, Chengyong . . . . . . . . . CH-P.13 THUFeng, Fang . . . . . . . . . . . . . . . . . CI-4.2 SUNFeng, Xinliang . . . . . . . . . . . . JSIV-1.3 SUNFeng, Yan . . . . . . . . . . . . . . . . CJ-P.11 WEDFeng, Ying . . . . . . . . . . . . . . . . .CJ-9.1 WEDFeng, Zhenhua . . . . . . . . . . . . . . CI-2.3 SUNFennel, Thomas . . . . . . . . . . EG-5b.1 MONFenollosa, Roberto . . . . . . . . . �JSI-1.2 SUNFerenczi, Gergely . . . . . . . . . �EA-P.24 THUFermann, Martin . . . . . . . . ED-1b.1 MON,�TF-1.2 TUEFermann, Martin E. . . . . . . . CH-7.2 WED,
�CH-9.1 WEDFernández, Alma . . . . . . . . . . . �CJ-2.5 SUNFernandez Gonzalvo, Xavier�EA-5.2 MONFerrante, Carino . . . . . . . . . . CE-12.6 WEDFerrari, Andrea . . . . . . . . . . . JSIV-1.2 SUN,
JSIV-1.5 SUN, EE-5a.2 MONFerrari, Andrea Carlo . . . . . . . CJ-9.6 WEDFerré, Amélie CG-6.1 WED, CG-6.2 WEDFerre, Simon . . . . . . . . . . . . . .CN-1.5 WED,�CB-11.6 THUFerrera, Marcello . . . . . . . . . . �CE-3.2 SUN,
CE-P.30 TUE, EA-6.5 TUE,EF-8.2 TUE, EA-7.3 TUE
Ferrier, Alban EA-2.4 SUN, EA-P.31 THUFerrini, Gabriele . . . . . . . . . . . EE-P.17 SUNFeugnet, Gilles . . . . . . . . . . . . . CH-5.1 TUEFeurer, Thomas . . . . . . . . . . CF-P.34 WEDFévrier, Sébastien . . . . . . . . . . CJ-8.5 WEDFibrich, Martin . . . . . . . . . . . .CA-P.24 SUNFigueiredo, Jose . . . . . . . . . . . . CI-5.2 MONFilippov, Valery . . . . . . . . . . .CE-P.13 TUE,�CJ-10.5 WEDFill, Ernst . . . . . . . . . . . . . . . . CG-P.12 THUFinazzi, Marco . . . . . . . . . . . . JSIV-1.2 SUNFinger, Martin . . . . . . . . . . . . .�CD-9.1 TUEFinot, Christophe . . . . . . . . . . . CI-3.1 SUN,
CI-4.2 SUN, �EF-P.27 THUFiore, Andrea CK-3.1 SUN, EA-6.4 TUE,
JSV-2.5 THUFirth, William . . . . . . . . . . . . . .EF-1.5 SUN,
CB-P.15 MON, EC-P.6 TUE,EC-3.3 TUE, EF-9.3 THU
Fischer, Ingo . . . . . . . . . . . . CB-P.27 MON,CB-P.34 MON, CB-7.2 WED,EF-P.11 THU, EF-P.22 THU
Fischer, Julian . . . . . . . . . . . . . CB-1.1 TUEFischer, Marc . . . . . . . . . . . . . .CB-6.1 WEDFischer, Marco . . . . . . . . . . . . . EH-7.3 THUFischer, Marco P. . . . . . . . . . �EH-5.5 THUFischer, Martin . . . . . . . . . . . . EA-P.1 THU,�EA-P.3 THU, EA-P.11 THUFischer, Peter . . . . . . . . . . . . . EG-P.2 MONFischer, Ulrich . . . . . . . . . . . . . .EG-4.6 SUNFisher, Kent . . . . . . . . . . . . . . EA-10.1 THUFitzpatrick, Casey . . . . . . . . EB-P.11 WEDFlamini, Fulvio . . . . . . . . . . . . EB-5.2 WED,
JSV-3.4 THUFlammini, Mariano . . . . . . . . . EF-7.2 TUEFlanagan, Aiden . . . . . . . . . . . CM-2.3 SUNFlatae, Assegid . . . . . . . . . . . . .CK-9.5 TUEFlavio, Mor . . . . . . . . . . . . . . . CK-14.5 THUFleddermann, Roland . . . . . . CH-P.3 THUFleming, Simon . . . . . . . . . . EH-P.13 WEDFloery, Tobias . . . . . . . . . . . . . . CF-2.1 TUEFlores-Arias, Maria Teresa CM-P.11 SUN,
CM-P.12 SUNFlorescu, Marian . . . . . . . . . CK-P.14 MONFlorez, Omar . . . . . . . . . . . . �CK-P.38 MONFlöry, Tobias . . . . . . . . . . . . . . �CD-4.5 SUNFoerster, Alexander . . . . . . . . CB-4.2 WEDFollman, David . . . . . . . . . . . . .CF-9.3 THUFompeyrine, Jean . . . . . . . . . . CD-P.1 TUEFonseca, Ruben . . . . . . . . . . . . CE-9.5 TUEFontana, Giorgio . . . . . . . . . . EA-P.32 THU
Forberich, Karen . . . . . . . . . . . JSI-2.1 SUNForbes, Andrew . . . . . . . . . . . . CH-2.4 SUNForchel, Alfred . . . . . . . . . . . . . CB-1.1 TUEForeman, Matthew . . . . . . . . . CH-4.2 SUNFörg, Benjamin . . . . . . . . . . . . CG-4.4 WEDForget, Nicolas CF-2.4 TUE, CF-3.5 TUE,
CF-P.27 WEDForget, Sébastien . . . . . . . . �CA-P.27 SUN,
CE-8.2 TUE, CK-12.3 WEDForrest, Adam . . . . . . . . . . . �CB-10.3 THUForrester, Alan . . . . . . . . . . �CK-P.18 MONForsberg, Pontus . . . . . . . . . . . CL-4.1 THUFörster, Michael . . . . . . . . . . . CG-4.4 WEDFortier, Tara . . . . . . . . . . . . . .�ED-2.5 MONFortier, Tara M. . . . . . . . . . . ED-1a.3 MONFortin, Vincent . . . . . . . . . . . . CJ-5.3 MONFörtsch, Michael . . . . . . . . . . EB-3.1 WED,
EA-P.11 THUFoster, Peta . . . . . . . . . . . . . . CF-P.25 WEDFotakis, Costas . . . . . . . . . . . CM-P.3 SUN,
CM-7.3 MONFotiadi, Andrei . . . . . . . . . . . . . CJ-2.2 SUN,
CJ-P.16 WED, �CJ-P.28 WEDFouché, Mathilde . . . . . . . . . EA-P.13 THUFourcade-Dutin, Coralie . . . . CG-2.3 TUE,
CF-5.2 WEDFournier, Maryse . . . . . . . . . . . . CI-P.8 TUEFowler, David . . . . . . . . . . . . .CB-11.1 THUFragkos, Alexandros . . . . . . CB-P.31 MONFrancis, Matthew . . . . . . . . . . CJ-7.2 WEDFranke-Arnold, Sonja . . . . . . . EC-2.3 TUEFranzl, Gerald . . . . . . . . . . . . . EB-4.5 WEDFrassetto, Fabio . . . . . . . . . . .CG-6.3 WED,�CF-8.4 THUFratalocchi, Andrea . . . . . . . . EG-4.2 SUN,
CD-P.5 TUE, EH-7.1 THU, EH-7.2 THUFrederich, Hugo . . . . . . . . . CK-P.15 MON,
EG-7.5 MON, EH-P.2 WEDFreegarde, Tim . . . . . . . . . . .CK-P.18 MONFreeman, Joshua . . . . . . . . . . CC-5.6 MONFreysz, Eric . .CC-P.9 SUN, CC-P.10 SUNFriberg, Ari . . . . . . . . . . . . . . . . EE-3.1 SUNFriberg, Ari T. . . . . . . . . . . . . . CF-6.3 THUFrick, Stefan . . . . . . . . . . . . . . EB-4.2 WEDFricke, Jörg CB-5.4 WED, CB-11.2 THU,
CB-11.5 THUFriedrich, Franziska . . . . . . �EA-P.16 THU,
EA-P.17 THUFriesem, Asher A. . . . . . . . . . . CA-P.4 SUNFrigerio, Jacopo . . . . . . . . . . . .EH-5.5 THUFrisquet, Benoit . . . . . . . . . �EF-4b.2 MONFritsche, Haro . . . . . . . . . . . . CJ-P.17 WEDFroehly, Luc . . . . . . . . . . . . . . . .EE-P.3 SUNFrolova, Lidiya . . . . . . . . . . . .CD-P.31 TUEFromherz, Thomas . . . . . . . . .CC-2.6 SUN,
CK-P.5 MONFrost, Thomas . . . . . . . . . . . . . CB-9.1 THUFrosz, Michael Henoch . . . . . . CI-3.3 SUNFsaifes, Ihsan . . . . . . . . . . . . . .�CH-5.1 TUEFu, Chien-Chung . . . . . . . . . . CE-P.10 TUEFu, Songnian . . . . . . . . . . . . . . . .CI-2.3 SUNFuchs, Frank . . . . . . . . . . . . . �CN-2.2 WEDFuchs, Lukas . . . . . . . . . . . . . . EB-4.1 WEDFuerbach, Alex . . . . . . . . . . . . CH-P.6 THUFuerbach, Alexander . . . . . . . CM-4.3 SUN
Fuerst, Josef Urban . . . . . . . . CD-4.4 SUNFuhrberg, Peter . . . . . . . . . . .CB-P.7 MON,
CJ-7.2 WEDFuji, Takao . . . . . . . . . . . . . . �CF-P.30 WEDFujii, Leo . . . . . . . . . . . . . . . . CF-P.16 WEDFujii, Takuro . . . . . . . . . . . . . . . CK-3.3 SUNFujimoto, Yasushi . . . . . . . . �CJ-P.9 WED,
CJ-P.38 WED, CJ-P.47 WEDFujisawa, Takeshi . . . . . . . . . .CK-P.7 MONFujiwara, Honami . . . . . . . . . . CM-3.4 SUNFujiwara, Masazumi . . . . . . CK-P.12 MONFujiwara, Mikio . . . . . . . . . . EA-P.25 THU,
EA-P.28 THU, JSV-4.1 THU,JSV-4.5 THU
Fujiwara, Takehisa . . . . . . . . .EE-P.18 SUNFujiwara, Yasufumi . . . . . . . . CE-P.19 TUEFukumi, Kouhei . . . . . . . . . . CK-P.17 MONFülöp, Attila . . . . . . . . . . . . . . �CD-P.9 TUEFülöp, József A. . . . . . . . . . . . .CA-3.3 SUNFülöp, József András . . . . . . �CC-3.1 SUN,�CC-3.5 SUNFung, Yin Hsien . . . . . . . . . . . �EC-1.5 TUEFurfaro, Luca EE-P.3 SUN, CD-6.3 MON,
CM-7.2 MONFürst, Josef U. . . . . . . . . . . . �CD-10.3 TUEFurukawa, Yusuke . . . . . . . . . CG-6.4 WED,
CG-P.18 THUFurusawa, Akira . . . . . . . . . . . EA-1.5 SUN,
EB-P.3 WEDFurutani, Yuji . . . . . . . . . . . . CF-P.30 WEDFushimi, Akihiro . . . . . . . . . . . CK-9.2 TUE,
CK-9.4 TUEFuwa, Maria . . . . . . . . . . . . . . �EB-P.3 WEDGaafar, Mahmoud . . . . . . . . . . CB-3.2 TUEGacemi, Djamal . . . . . . . . . . . . CC-2.2 SUNGacoin, Thierry . . . . . . . . . . . CK-14.6 THUGadalla, Kamal . . . . . . . . . . . . .CL-3.4 THUGadonas, Roaldas . . . . . . . . CK-P.10 MONGadret, Gregory . . . . . . . . . . . CD-6.1 MONGaertner, Tom . . . . . . . . . . . . . CK-7.1 TUEGaeta, Alexander L. . . . . . . . CH-8.6 WED,
PD-A.5 WEDGafney, Harry D. . . . . . . . . . . . EH-6.5 THUGaggero, Alessandro . . . . . . . . EA-6.4 TUEGai, Xin . . . . . . CD-1.5 SUN, CH-3.2 SUNGaida, Christian . . . . . . . . . . . CJ-5.5 MON,
CJ-13.1 THU, �CJ-13.4 THU,CJ-13.5 THU
Gailevicius, Darius . . . . . . . .CK-P.10 MONGaio, Michele . . . . . . . . . . . . . �EH-6.3 THUGaižauskas, Eugenijus . . . . . EF-P.15 THUGalarreta, Betty . . . . . . . . . JSII-1a.3 MONGalimberti, Marco . . . . . . . �CF-P.25 WED,
CG-P.1 THUGalisteo-López, Juan F. . . �CK-P.24 MONGallais, Laurent . . . . . . . . . . . CA-P.35 SUNGalland, Christophe . . . . . . . . EG-1.4 SUN,
EA-7.6 TUE, JSV-1.2 THU,JSV-4.2 THU
Gallet, Valentin . . . . . . . . . . . .CH-8.4 WEDGalli, Matteo . . . . . . . . . . . . . EG-P.4 MON,
JSV-P.3 MON, EA-7.6 TUE,JSV-1.2 THU
Gallmann, Lukas . . . . . . . . . . . EE-4.2 SUN,CF-2.3 TUE, CG-4.1 WED,
CG-4.5 WED, CG-5.3 WEDGallo, Katia . . . . . . . . . . . . . . . CK-5.3 MONGallot, Guilhem . . . . . . . . . . . . CC-P.1 SUNGaltier, Sandrine . . . . . . . . . . ED-2.1 MONGalvão, Ernesto . . . . . . . . . . . JSV-3.4 THUGalvao, Ernesto F. . . . . . . . . . EB-5.2 WEDGalzerano, Gianluca . . . . . . �ED-2.3 MON,
ED-2.6 MON, ED-1b.2 MONGamaly, Eugene . . . . . . . . . . . .CM-1.2 SUNGambetta, Alessio . . . . . . . . . ED-2.3 MONGao, Chunqing . . . . . . . . . . . �CA-P.18 SUNGao, Mingwei . . . . . . . . . . . . . CA-P.18 SUNGao, Wenlong . . . . . . . . . . . . �EH-1.5 WEDGao, Yuanda . . . . . . . . . . . . . JSIV-2.3 SUNGaponov, Dmitry . . . . . . . . . . . CJ-2.4 SUNGarbat, Katarzyna . . . . . . . . .CC-P.17 SUNGarbin, Bruno . . . . . . . . . . . . . �EF-1.4 SUNGarces, Ignacio . . . . . . . . . . . . . .CI-2.4 SUNGarcés, Rafael . . . . . . . . . . . �EA-P.19 THU,�EA-P.21 THUGarcía-Blanco, Sonia . . . . . . .CE-7.3 MONGarcía de Abajo, F. Javier . .CK-8.4 TUE,
EH-2.4 WEDGarcía de Abajo, Francisco Javier
JSIV-2.2 SUNGarcia de Abajo, Javier . . . . CL-P.15 SUNGarcia, Gustavo A. . . . . . . . . CG-6.1 WEDGarcia-Lechuga, Mario . . �CM-5b.3 MONGarcía-Ojalvo, Jordi . . . . . . . EF-P.22 THUGarcia-Parajo, Maria . . . . . . . EG-4.6 SUN,
EH-6.1 THUGarcia-Pomar, Juan Luis . �EH-P.17 WEDGarcia-Sucerquia, Jorge . . . .CL-P.17 SUNGardes, Frederic Y. . . . . . . . . . CK-7.2 TUEGariepy, Genevieve . . . . . . . . .CN-2.4 WEDGarín, Moises . . . . . . . . . . . . . . JSI-1.2 SUNGarnier, Josselin . . . . . . . . . . . . EI-2.1 THUGarnov, Sergey . . . . . . . . . . . CA-11.1 THUGarrelie, Florence . . . . . . �CM/LIM.2 TUEGarthoff, Robert . . . . . . . . . . EB-4.3 WED,
EB-P.12 WEDGassenq, Alban . . . . . . . . . . �CB-11.1 THUGassino, Riccardo . . . . . . . . . CL-P.14 SUNGateau, Julien . . . . . . . . . . . . CG-P.16 THUGates, James . . . . . . . . . . . . . JSV-3.1 THUGates, James C. . . . . . . . . . . . CE-2.3 SUN,
CE-2.5 SUN, JSV-P.6 MON,JSV-P.7 MON, CE-10.4 WED,CE-10.5 WED, JSV-1.3 THU
Gatti, Alessandra . . . . . . . . . .EF-6.3 MON,�EA-P.10 THUGatti, Davide . . . . . . . . . . . . . ED-2.3 MON,�ED-3.5 MONGaudio, Rosalinda . . . . . . . . . . EA-6.4 TUEGaudreau, Louis . . . . . . . . . . JSIV-2.5 SUNGaur, Ankita . . . . . . . . . . . . . . . .CI-P.4 TUEGauthier, Jean-Christophe . . CJ-5.3 MONGauthier-lafaye, Olivier . . . . .CK-1.2 SUN,�CB-P.17 MON, CK-P.31 MON,
CK-11.3 WEDGauthier-manuel, Ludovic . . . EF-7.5 TUEGawith, Corin B.E. . . . . . . . . .CE-2.5 SUN,
CE-10.4 WEDGawlik, Wojciech . . . . . . . . . CH-P.18 THUGayral, Bruno . . . . . . . . . . . . . CB-4.3 WED
210
Authors’ Index
Gazzetto, Michela . . . . . . . . . CD-6.6 MONGbadebo, Adenowo . . . . . . . . �CE-1.4 SUNGe, Li . . . . . . CB-1.2 TUE, EH-P.15 WEDGebhardt, Martin . . . . . . . . . �CJ-5.5 MON,
CJ-13.1 THU, CJ-13.4 THU,�CJ-13.5 THUGecevičius, Mindaugas
CLEO/ECBO-2.3 WED, CK-14.4 THUGeddes, Cameron . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONGeen, Matthew . . . . . . . . . . . . .CB-2.4 TUEGehring, Tobias . . . . . . . . . . �CH-P.22 THUGeiger, Randall . . . . . . . . . . . CB-11.1 THUGeiger, Richard CB-1.4 TUE, CK-9.3 TUEGeiregat, Pieter . . . . . . . . . .EG-P.13 MON,�CK-11.6 WEDGeiselmann, Michael . . . . . . ED-P.8 MON,
CE-9.1 TUEGeiss, Reinhard . . . . . . . . . . . . CD-2.2 SUNGelens, Lendert . . . . . . . . . . . ED-P.2 MONGelfand, Ryan EG-7.1 MON, CL-2.4 THUGeller, Tzahi . . . . . . . . . . . . . . . EA-7.5 TUEGéneaux, R . . . . . . . . . . . . . . . . CF-8.5 THUGéneaux, Romain . . . . . . . . . �CG-6.1 WEDGenest, Jérôme . . . . . . . . . . . . CJ-7.1 WEDGenet, Cyriaque . . . . . . . . . . �EH-1.1 WEDGeng, Xiaotao . . . . . . . . . . . . . CG-P.3 THUGenoud, Guillaume . . . . . . . . . CH-3.3 SUNGentner, Jean-Louis . . . . . . . . CK-7.1 TUEGenty, Frédéric . . . . . . . . . . . CE-11.4 WEDGenty, Goëry . CD-1.2 SUN, EE-3.1 SUN,
CF-6.3 THU, CH-P.16 THU,EF-P.25 THU
Geoffroy, Ghita . . . . . . . . . . . . . .EI-P.1 TUEGeorges, Patrick . . . . . . . . . . . CJ-1.1 SUN,
CJ-1.3 SUN, CB-5.3 WED,CF-P.27 WED, CA-9.2 THU
Georgiou, Giorgos . . . . . . . . . . CC-4.3 SUNGérard, Bruno CD-4.2 SUN, CN-1.1 WEDGérard, Jean-Michel . . . . . . EE-P.16 SUN,
EG-6.4 MON, EG-6.5 MON,CD-P.32 TUE, EA-9.6 THU
Geremia, Riccardo . . . . . . . . . CM-4.4 SUNGerhardt, Ilja . . . . . . . . . . . . . . �EG-3.3 SUNGerhardt, Nils C. . . . . . . . . . . CB-2.1 TUE,
CB-2.2 TUEGericke, Fabian . . . . . . . . . . . �EA-8.3 WEDGerke, Stefan . . . . . . . . . . . . . �EB-P.8 WEDGerke, Tim . . . . . . . . . . . . . . . . �TF-1.1 TUEGerlach, Philipp . . . . . . . . . CB-P.14 MON,
CB-2.6 TUEGerlich, Stefan . . . . . . . . . . . . . EA-P.2 THUGermino, Jose . . . . . . . . . . . . .CE-P.16 TUEGérôme, Frédéric . . . . . . . . . . CH-5.1 TUE,
CG-2.3 TUE, CJ-8.4 WED, CF-5.2 WEDGerrits, Thomas . . . . . . . . . CK-4a.2 MON,
JSV-P.7 MON, EA-6.3 TUE,JSV-1.5 THU
Gerth, Daniel . . . . . . . . . . . . . . CF-5.1 WEDGeskus, Dimitri . . . . . . . . . . . . CA-1.2 SUN,
CH-1.3 SUN, �CA-P.9 SUN,�CJ-6a.3 MONGeßler, Jonas . . . . . . . . . . . . . . EA-P.5 THUGeuzebroek, Douwe . . . . . . . CJ-12.2 THUGhadimi, Amir . . . . . . . . . . . . . EA-4.2 SUN
Ghalbouni, Joe . . . . . . . . . . . . EB-P.5 WEDGhatrehsamani, Sajad . . . .CK-P.39 MON,
CE-P.20 TUEGhazal, Omar M.S. . . . . . . �CE-11.1 WEDGhenuche, Petru . . . . . . . . . . .EG-7.3 MONGheorghe, Lucian . . . . . . . . . CA-P.32 SUNGholipour, Behrad . . . . . . . . �CE-2.6 SUN,�CD-P.11 TUE, CD-P.24 TUE,�EH-3.2 WEDGiacobino, Elisabeth . . . . . . . EA-1.2 SUN,�EC-3.1 TUE, EA-P.4 THU, EI-3a.3 THUGiakoumaki, Argyro N. . . . . . CM-1.3 SUNGianfrani, Livio . . . . . . . . . . . ED-2.3 MON,
ED-2.6 MON, ED-P.5 MONGiannetti, Ambra . . . . . . . . . CL-P.13 SUN,
CH-P.24 THUGiannetti, Claudio . . . . . . . . . EE-P.17 SUNGibson, Christopher . . . . . . . �EF-5.3 MONGibson, Ursula CH-4.4 SUN, CE-P.8 TUEGiden, Ibrahim . . . . . . . . . . . EH-P.16 WEDGierl, Christian . . . . . . . . . . . . . CB-2.3 TUEGies, Christopher . . . . . . . . . .CB-4.2 WED,
EA-8.3 WEDGiesbrecht, Nadja . . . . . . . . .CE-12.1 WEDGiessen, Harald . . . . . . . . . . . . CD-4.3 SUN,
CD-4.6 SUN, EH-1.2 WED,CD-11.1 THU, CL-4.2 THU
Gil Villalba, Abel . . . . . . . . . �CM-7.2 MONGilardi, Giovanni . . . . . . . . . . . . CI-2.6 SUNGilchrist, Alexei . . . . . . . . . . . .EB-1.1 MONGill, Patrick . . . . . . . . . . . . . . . ED-P.9 MONGilles, Clément . . . . . . . . . . . CN-1.5 WED,�CB-6.3 WEDGilles, Marin . . . . . . . . . . . . . . . �CI-4.3 SUNGillespie, William . . . . . . . . . .CM-3.5 SUN,
CD-P.30 TUE, CE-P.1 TUEGillibert, Raymond . . . . . . . . . CL-4.3 THUGinat, Ran . . . . . . . . . . . . . . . . CN-1.3 WEDGini, Emilio . . . . . . . . . . . . . . . .CF-4.1 WEDGinis, Vincent . . . . . . . . . . . . �EH-3.3 WEDGioannini, Mariangela . . . . . . CB-9.4 THUGisin, Nicolas EA-2.4 SUN, EA-P.31 THUGisselbrecht, Mathieu . . . . . �CG-5.1 WEDGissibl, Timo . . . . . . . . . . . . . . .CD-4.6 SUNGitzinger, Gregory . . . . . . . . . CF-2.4 TUE,
CF-3.5 TUEGiudici, Massimo . . . . . . . . . . �EF-1.2 SUN,
CB-2.5 TUE, CD-13.4 THUGiuliani, Guido .CC-6.6 TUE, CI-P.8 TUEGiusfredi, Giovanni . . . . . . . .CH-P.36 THUGiust, Remo . . EE-2.4 SUN, EE-P.3 SUN,
CM-7.2 MONGladkovskaya, Olga . . . . . . . . CM-2.3 SUNGlaser, Martin . . . . . . . . . . . . .CK-P.5 MONGlazunov, Ilya . . . . . . . . . . . . . . CE-P.5 TUEGleyzes, Sébastien . . . . . . . . . EA-P.2 THUGlöckner, Rosa . . . . . . . . . . . . �EC-2.5 TUEGloppe, Arnaud . . . . . . . . . . . �EG-1.5 SUN,
CK-2.4 SUNGmeiner, Benjamin . . . . . . . . . EG-3.1 SUNGnilitskyi, Iaroslav . . . . . . . . �CM-2.5 SUN,
JSI-P.1 TUEGobert, Olivier . . . . . . . . . . . . CH-8.4 WEDGodard, Antoine . . . . . . . . . . .CD-2.3 SUN,
CD-P.36 TUE, CN-1.1 WED
Godfrey, Mark . . . . . . . . . . . . JSV-4.5 THUGodin, Thomas . . . . . . . . . . . . CJ-2.4 SUN,�EF-4b.1 MON, EF-P.25 THUGoebel, Thorsten A. . . . . . . . �CM-4.1 SUNGogolides, Evangelos . . . . . .CM-P.16 SUNGolant, Konstantin . . . . . . . .CJ-10.5 WEDGold, Peter . . . . . . . . . . . . . . . .EA-8.3 WEDGoldenberg, Leonid . . . . . . . .CE-P.17 TUEGoldner, Philippe . . . . . . . . . . EA-2.4 SUN,
EA-P.31 THUGolez, Denis . . . . . . . . . . . . . . EE-P.17 SUNGolling, Matthias . . . . . . . . . .CF-4.1 WED,
CH-8.3 WED, CF-9.3 THUGolunski, Mikolaj . . . . . . . . . CH-P.18 THUGomes, Jean-Thomas . . . . . .�CA-9.2 THUGomes, Maria . . . . . . . . . . . . . CH-P.9 THUGomes, Pedro . . . . . . . . . . . . . . EC-3.3 TUEGomez Aranzadi, Mikel . . . . CE-P.27 TUEGomez, Carmen . . . . . . . . . . .CD-P.20 TUEGomez Rivas, Jaime . . . . . . . �CC-4.3 SUNGomez-Varela, Ana Isabel . CM-P.12 SUNGomila, Damià . . . . . . . . . . . ED-P.1 MON,
ED-P.2 MONGonçalves, Cledson . . . . . . . CF-P.31 WEDGonsalves, Anthony . . . . . �JSIII-1.4 MONGonzalez-Acevedo, Bastian . .JSI-1.5 SUNGonzalez de Alaiza Martinez, Pedro�EE-2.5 SUN, �EI-3a.2 THUGonzález-Herráez, Miguel . CH-P.17 THUGonzalez, Jaime . . . . . . . . . . JSIV-2.4 SUNGonzález, Jesús González . . .CM-2.2 SUNGonzález-Vázquez, Jesús . . CG-P.13 THUGoorden, Sebastianus . . . . . �EB-4.6 WEDGopal, Amrutha . . . . . . . . . .CM-5a.3 MONGorbach, Andrey . . . . . . . . . . . .EF-3.4 SUNGörblich, Markus . . . . . . . . . . . CB-2.3 TUEGorceix, Olivier . . . . . . . . . . . . �EC-1.3 TUEGordienko, Vjacheslav . . . . . . EE-P.2 SUNGordienko, Vyacheslav . . . . CF-P.13 WEDGordon, Neil . . . . . . . . . . . . . CM-P.15 SUNGordon, Reuven . . . . . . . . . . �EG-7.1 MON,�CL-2.4 THUGorjan, Martin . . . . . . . . . . . . CA-P.1 SUN,
CA-10.1 THUGorman, Philip M. . . . . . . . . . . CJ-4.3 SUNGorodetsky, Andrei . . . . . . . .CC-5.4 MON,�CC-5.5 MONGorodetsky, Michael L. . . . . ED-P.8 MONGorza, Marie-Pascale . . . . . . EG-P.7 MONGorza, Simon-Pierre . . . . . . . . EF-7.3 TUEGotti, Riccardo . . . . . . . . . . . . ED-3.5 MONGötzinger, Stephan . . . . . . . . EG-3.1 SUN,
EG-3.2 SUN, �EG-6.1 MON,EA-5.3 MON
Gouhier, Benoit . . . . . . . . . . �CH-P.19 THUGoulding, David . . . . . . . . . CB-P.24 MON,�CB-7.1 WEDGoulielmakis, Eleftherios . . . .CG-P.2 THUGouraud, Baptiste . . . . . . . �EB/EG.3 TUEGouriou, Pierre . . . . . . . . . . . . �CJ-3.3 SUNGow, Paul . . . . . . . . . . . . . . . �CC-P.13 SUNGoykhman, Ilya . . . . . . . . . . . JSIV-1.5 SUNGozhyk, Iryna . . . . . . . . . . . �CK-12.3 WED,
CK-14.6 THUGrabka, Michal . . . . . . . . . . . CH-P.18 THU
Gradoni, Gabriele . . . . . . . . . EH-P.18 WEDGraf, Christina . . . . . . . . . . . EG-5b.1 MONGraf, Thomas . . . . . . . . . . . . CB-P.2 MON,
CB-P.16 MON, CA-7.3 MON,CA-9.2 THU
Gräfe, Markus . . . . . . . . . . . . �EA-1.3 SUN,CD-P.12 TUE, EB-3.3 WED,�EB-P.1 WED, EA-P.9 THU,JSV-3.3 THU
Graham, Chris . . . . . . . . . . . . .CC-5.6 MONGrajales, Daniel . . . . . . . . . �JSII-1a.2 MONGrande, Marco . . . . . . . . . . . . CK-1.6 SUN,
CK-P.31 MONGrandi, Samuele . . . . . . . . . . CE-12.5 WEDGrandjean, Nicolas . . . . . . . . . CB-8.1 THUGranet, Gérard . . . . . . . . . . . . . . . . . . . . . . �JS
SPIE/OM/EQEC.1 MONGrange, Rachel . . . . . . . . . . . . .CD-2.2 SUNGrange, Thomas . . . . . . . . . . �CC-1.5 SUN,�EA-9.6 THUGranger, Geoffroy . . . . . . . . �CJ-P.49 WEDGrangier, Philippe . . . . . . . . . JSV-4.2 THUGrant-Jacob, James . . . . . . CM-P.17 SUN,
CE-7.2 MON, �CE-P.3 TUE,CJ-P.3 WED
Grant-Jacob, James A. . . . . CM-7.4 MONGrant, Stephen . . . . . . . . . . .�CD-P.30 TUEGrassani, Davide . . . . . . . . . JSV-P.3 MON,
EA-7.6 TUE, JSV-1.2 THUGrasso, Marco . . . . . . . . . . . . . CD-P.7 TUEGrattan, Kenneth . . . . . . . . . . CH-P.6 THUGravina, Stefania . . . . . . . . . . ED-P.5 MONGrazioso, Fabio . . . . . . . . . . . PD-B.9 WEDGrech, David . . . . . . . . . . . . . . . CE-4.2 SUNGreenhalgh, Justin . . . . . . . . . CA-3.6 SUNGreenwood, Jason B. . . . . . . CG-6.3 WEDGregersen, Niels . . . . . . . . . . �EG-6.5 MON,
CK-P.9 MONGrégoire, Beaudoin . . . . . . CB-P.32 MON,
CB-1.3 TUEGreif, Michael . . . . . . . . . . . . . CG-4.5 WEDGreiner, Marcel . . . . . . . . . . CB-P.10 MONGrelu, Philippe CJ-2.1 SUN, EI-P.3 TUE,
EI-P.5 TUE, EF-8.3 TUE, CJ-P.7 WED,EF-P.20 THU
Gremillet, Laurent . . . . . . . . . EI-3a.2 THUGretzinger, Thomas . . . . . . . . CM-P.8 SUNGreven, Martin . . . . . . . . . . . . EE-P.17 SUNGriebner, Uwe . . . . . . . . . . . . CA-P.31 SUN,
CA-4.4 SUN, CA-4.5 SUN,CA-5a.1 MON, CA-5a.2 MON,CA-5b.3 MON, CF-1.2 TUE
Gries, Wolfgang . . . . . . . . . . CJ-P.17 WEDGriffin, Paul . . .EC-P.2 TUE, EC-3.3 TUEGrigore, Oana . . . . . . . . . . . . CA-10.4 THUGrigoriev, Victor . . . . . . . . . . . EG-7.3 MONGrillanda, Stefano . . . . . . . . CK-13.3 WEDGrimm, Stephan . . . . . . . . . . CA-P.21 SUNGris-Sánchez, Itandehui . . . . . CJ-3.4 SUNGrisard, Arnaud . . . . . . . . . . . CD-4.2 SUN,
CN-1.1 WEDGrishin, Michail . . . . . . . . . . . CA-P.26 SUNGrishina, Diana . . . . . . . . . . . . �CE-2.2 SUNGroenen, Rik . . . . . . . . . . . . . CM-P.19 SUNGrognot, Marianne . . . . . . . . �CC-P.1 SUN
Grohe, Andreas . . . . . . . . . . . CJ-P.17 WEDGrojean, T. . . . . . . . . . . . . . . CK-11.2 WEDGroom, Kristian M. . . . . . . . CE-11.1 WEDGroß, Petra . . . . . . . . . . . . . . . EG-P.6 MONGrosjean, Thierry . . . . . . . . . . . EG-4.6 SUNGross, Elad . . . . . . . . . . . . . . . .CN-1.3 WEDGross, Simon �CI-1.5 SUN, �CM-P.7 SUN,�CM-P.8 SUN, CJ-7.1 WED,�CB-5.5 WED, CH-7.4 WED,
CJ-P.41 WEDGrosso, Gabriele . . . . . . . . . . . �CD-9.4 TUEGrote, Norbert . . . . . . . . . . . . . CK-7.1 TUEGrüner, Christoph . . . . . . . . . . CH-4.5 SUNGrüner-Nielsen, Lars . . . . . . . . CJ-2.5 SUNGrunwald, Rüdiger . . . . . . . . EE-5b.2 MONGrupp, Alexander . . . . . . . . �EE-5a.2 MONGruson, V . . . . . . . . . . . . . . . . . CF-8.5 THUGrützmacher, Detlev . . . . . . . CC-2.6 SUN,
CB-1.4 TUEGschrey, Manuel . . . . . . . . . . . EA-8.5 WEDGstalter, Marion . . . . . . . . . �CF-P.21 WEDGu, Erdan . . . . . . . . . . . . . . . . . CA-1.3 SUNGu, Min . . . . . . . . . . . . . . . . . . . .CE-3.4 SUNGu, Wen-ju . . . . . . . . . . . . . . . . EA-9.5 THUGuandalini, Annalisa . . . . . . . .CA-2.1 SUNGuanghui, Yuan . . . . . . . . . . . EH-3.2 WEDGuasoni, Massimiliano . . . . . . . CI-4.3 SUNGubaydullin, Azat . . . . . . . . . .CG-5.4 WEDGuduru, Surya SK . . . . . . . . �CM-P.9 SUNGüell, Frank . . . . . . . . . . . . . �CE-5a.2 MONGuellati-Khelifa, Saida . . . . CH-P.33 THUGuénot, Diégo . . . . . . . . . . . . .CG-5.1 WEDGuérin, Stéphane . . . . . . . . . . EG-P.3 MONGuérnot, Diego . . . . . . . . . . . . .CG-1.5 TUEGuerout, Romain . . . . . . . . . . EG-P.7 MONGuerreiro, Thiago . . . . . . . . . .EB-1.4 MONGuéry-Odelin, David . . . . . . .EA-10.4 THUGuggenmos, Alexander . . . . . CF-8.1 THUGühlke, Marina . . . . . . . . . . . . EH-6.4 THUGuichard, Florent . . . . . . . . . . CJ-1.1 SUN,
CJ-1.3 SUN, CF-P.27 WEDGuilet, Stéphane . . . . . . . . . . . CK-7.4 TUEGuille, Antoine . . . . . . . . . . CK-4a.1 MON,
EG-P.13 MONGuillemot, François . . . . . . . CK-14.6 THUGuillet, Thierry . . . . . . . . . . . �CB-4.3 WEDGuillot, Emmanuel . . . . . . . . CA-11.6 THUGuilloy, Kevin . . . . . . . . . . . . .CB-11.1 THUGuina, Mircea . . . . . . . . . . . . CB-P.1 MON,
CA-5b.1 MON, CB-3.1 TUE,CB-4.5 WED, CB-5.1 WED,CB-11.4 THU
Guiraud, Germain . . . . . . . . . �CJ-11.1 THUGuizzetti, Giorgio . . . . . . . . . . EG-P.4 MONGumenyuk, Regina . . . . . . . . CE-P.35 TUEGündogan, Mustafa . . . . . . . .EA-5.5 MONGünther, Axel . . . . . . . . . . . . . �CE-8.3 TUEGünthner, Thomas . . . . . . . . . EA-P.5 THUGuo, Chen . . . . . . . . . . . . . . . . . CF-6.2 THUGuo, Hairun �EE-P.11 SUN, EF-3.6 SUN,�CF-P.17 WEDGuo, Rui . . . . . EH-5.1 THU, EH-5.3 THUGuo, Shaofeng CI-P.9 TUE, CJ-11.5 THUGuo, Surong . . . . . . . . . . . . . .�CK-6.2 MONGuo, Wei . . . . . . . . . . . . . . . . . . CD-1.5 SUN
211
Authors’ Index
Guo, Weiming . . . . . . . . . . . . CB-11.3 THUGuo, Yi . . . . . . . . . . . . . . . . . . CF-P.22 WEDGupta, Manish . . . . . . . . . . . . . EA-3.3 SUNGupta, Mohit . . . . . . . . . . . . . . . . . . . . . . . . JS
SPIE/OM/EQEC.3 MONGupta, Urvashi . . . . . . . . . . . EG-P.12 MONGürel, Kutan . . . . . . . . . . . . . �CA-6.1 MONGuretsky, Sergei . . . . . . . . . . .CE-P.13 TUEGurevich, Sergey A. . . . . . . . CK-P.1 MONGurevich, Svetlana . . . . . . . . . EF-P.4 THUGuryanov, Aleksei . . . . . . . . . CJ-8.5 WED,
CJ-P.48 WEDGuryanov, Alexei . . . . . . . . . .CJ-P.13 WEDGuryanov, Alexey . . . . . . . . . . . CJ-3.1 SUNGusachenko, Ivan . . . . . . . . . CL-P.12 SUN,
CL-3.3 THUGustave, François . . . . . . . . . �EE-3.6 SUN,�CB-7.4 WEDGustavsson, Johan S. . . . . . . . CB-2.4 TUEGüther, Reiner . . . . . . . . . . . . CB-P.6 MONGutiérrez, Jose M. . . . . . . . . EF-P.11 THUGüttinger, Johannes . . . . . . CK-10.3 WEDGutty, François . . . . . . . . . . . . �CD-4.2 SUNGuyon, Olivier . . . . . . . . . . . . . CH-7.4 WEDH.A. Ras, Robin . . . . . . . . . . . CM-P.5 SUNH. Gabrielli, Lucas . . . . . . . . . JSII-P.1 TUEHaag, Johannes . . . . . . . . . . . PD-B.1 WEDHaakh, Harald R. . . . . . . . . . . EG-3.2 SUN,
EA-10.5 THUHaarlammert, Nicoletta . . . . .CJ-4.5 SUN,�CJ-P.17 WED, �CJ-10.3 WED,
CJ-10.6 WEDHaase, Johannes . . . . . . . . . .EE-5a.1 MONHabib, Md. Selim . . . . . . . . �CJ-P.1 WED,�CJ-P.12 WED, �CJ-P.22 WEDHaboucha, Adil . . . . . . . . . . . . CJ-5.3 MONHackl, Florian . . . . . . . . . . . . �CK-P.5 MONHaddadi, Samir . . . . . . . . . . . . .EF-2.4 SUNHadfield, Robert . . . . . . . . . . JSV-4.5 THUHadfield, Robert H. . . . . . . EA-P.28 THU,
JSV-4.1 THUHadji, Emmanuel . . . . . . . . . . .CK-8.3 TUEHadjiantoniou, Sebastian . . . CM-P.2 SUNHädrich, Steffen . . . . . . . . . . .CJ-5.5 MON,�CG-2.5 TUE, CG-3.1 WED,�CJ-8.2 WED, CJ-13.5 THU,
CF-8.1 THUHaefner, Matthias . . . . . . . . . . CG-2.1 TUEHaelterman, Marc . . . . . . . . . . CI-5.1 MONHaenen, Ken . . . . . . . . . . . . . . . CL-P.8 SUNHaessler, Stefan . . . . . . . . . . . . CG-2.3 TUEHäfner, Matthias . . . . . . . . . .CA-10.1 THUHagedorn Frandsen, Lars . . . �CK-9.1 TUEHaglund, Emanuel P. . . . . . . . CB-2.4 TUEHaglund, Erik . . . . . . . . . . . . . �CB-2.4 TUEHaïdar, Riad .CK-P.6 MON, CD-8.6 TUEHakobyan, Sargis . . . . . . . . . . CA-6.1 MONHalagacka, Lukas . . . . . . . . . . EH-2.6 WEDHald, Jan . . . . . . . . . . . . . . . . . . CH-5.4 TUEHalfmann, Thomas . . . . . . . �EA-5.1 MONHalioua, Yacine . . . . . . . . . JSV-P.10 MONHallaji, Matin EA-2.6 SUN, �CD-9.2 TUEHamazaki, Junichi . . . . . . . . �CC-P.11 SUNHamel, Deny . . . . . . . . . . . . . . EB-5.4 WEDHamel, Deny R. . . . . . . . . . . . EB-1.5 MON
Hamel, Philippe . . . . . . . . . . . . EF-2.4 SUNHamilton, Craig S. . . . . . . . . JSV-2.1 THUHamo, Hilla Ben . . . . . . . . . . . CH-4.5 SUNHan, Hau-Vei . . . . . . . . . . . . . CE-P.10 TUEHan, Songhee . . . . . . . . . . . . . . CG-1.4 TUEHan, Xiumei . . . . . . . . . . . . . . . CA-2.2 SUNHan, Yu . . . . . . . . . . . . . . . . . . . EH-7.2 THUHan, Zheng . . . . . . . . . . . . . . . . CK-7.3 TUEHanaizumi, Osamu . . . . . . . . . CE-P.4 TUEHand, Duncan P. . . . . . . . . . . . CE-1.5 SUNHändchen, Vitus . . . . . . . . . . CH-P.22 THUHandelman, Amir . . . . . . . . . . �CL-P.9 SUNHandloser, Matthias . . . . . . CE-12.1 WEDHandong, Sun . . . . . . . . . . . . . .CF-9.6 THUHandschin, Charles . . . . . . . . CG-6.1 WEDHangauer, Andreas . . . . . . . �CH-8.5 WEDHanisch, Julia . . . . . . . . . . . . CD-11.2 THUHanna, Marc �CJ-1.1 SUN, �CJ-1.3 SUN,
CD-P.34 TUE, CG-2.2 TUE,CB-5.3 WED, CF-P.27 WED
Hänsch, Theodor W. . . . . . . .CH-1.2 SUN,CK-2.3 SUN, EG-6.2 MON,CK-P.42 MON, �PL-3.1 MON
Hänsel, Wolfgang . . . . . . . . . . .CC-2.2 SUNHansen, Michael . . . . . . . . . . .ED-2.4 MONHansson, Tobias . . . . . . . . . .CD-P.20 TUE,�EI-2.5 THUHanusch, Fabian . . . . . . . . . .CE-12.1 WEDHaq, A F M Saniul . . . . . . . . PD-A.2 WEDHarabuchi, Yu . . . . . . . . . . . . .EE-P.18 SUNHarbord, Edmund . . . . . . . . . .EA-8.4 WEDHarder, Georg . . . . . . . . . . . . . JSV-1.5 THUHarjanne, Mikko . . . . . . . . . . . .CI-P.7 TUE,
CH-6.1 WEDHärkönen, Antti . . . . . . . . . . CA-5b.1 MONHaroche, Serge . . . . . . . . . . . .�PL-4.1 TUE,
EA-P.2 THUHarouri, Abdelmounaim . . . . .JSI-1.5 SUNHarper, Paul . . . . . . . . . . . . . . . . CI-P.5 TUEHarren, Frans CH-4.3 SUN, CF-1.5 TUE,
CB-6.5 WEDHarrington, James . . . . . . . . .CC-P.14 SUNHarris, Nicholas . . . . . . . . . CK-4b.1 MON,
EA-7.6 TUE, JSV-1.2 THU,JSV-4.2 THU
Harrold, Chris . . . . . . . . . . . . .PD-B.3 WEDHarte, Tiffany . . . . . . . . . . . . . . EC-P.1 TUEHarteveld, Cornelis . . . . . . . . . CE-2.2 SUNHarth, Anne . . . . . . . . . . . . . . . CF-6.2 THUHartl, Christian . . . . . . . . . . . .EH-P.1 WEDHartl, Ingmar . CA-4.2 SUN, CF-1.6 TUEHartmann, Florian . . . . . . . . CM-6.4 MONHartmann, Jean-Michel . . . . CB-1.4 TUE,
CB-11.1 THUHartmann, Paul . . . . . . . . . . . .EI-3a.1 THUHartmann, Sébastien . . . . .CB-P.13 MON,
EA-P.16 THU, �EA-P.17 THUHartschuh, Achim . . . . . . . . CE-12.1 WEDHartung, Alexander . . . . . . . CD-P.18 TUEHasan, Tawfique . . . . . . . . . . .CF-P.6 WEDHasanuzzaman, G.K.M. . . . . CJ-P.1 WEDHashimoto, Toshikazu . . . . . PD-B.3 WEDHashimoto, Yosuke . . . . . . . . . EA-1.5 SUNHasman, Erez . . . . . . . . . . . . . �EG-2.4 SUNHasse, Kore . . . . . . . . . . . . . . �CJ-6a.2 MON
Hassinen, Jukka . . . . . . . . . . . CM-P.5 SUNHässler, Stefan . . . . . . . . . . . . CF-5.2 WEDHasson, Victor . . . . . . . . . . . CF-P.23 WEDHatem, Osama . . . . . . . . . . . . CC-5.6 MONHati, Archita . . . . . . . . . . . . . . ED-2.5 MONHatzopoulos, Zacharias . . . . . EF-9.2 THUHaub, John . CJ-11.6 THU, CJ-13.2 THUHaula, Elena V. . . . . . . . . . . . CE-P.25 TUEHauri, Christoph . . . . . . . . . .CC-P.16 SUN,
CC-3.4 SUNHauri, Christoph P. . . . . . . . . CC-P.2 SUN,
CC-3.2 SUN, CC-3.6 SUNHaus, Joseph . . . . . . . . . . . . . . EH-7.4 THUHause, Alexander . . . . . . . . �CF-P.29 WEDHausmann, Katharina . . . . . CJ-P.42 WEDHawkes, Steve . . . . . . . . . . . .CF-P.25 WEDHawkins, Thomas . . . . . . . . . .CH-4.4 SUN,
CE-P.8 TUEHayashi, Daisuke . . . . . . . . . . . CI-5.4 MONHayashi, Juliano G. . . . . . . �EH-P.13 WEDHayashi, Masumi . . . . . . . . . CD-11.3 THUHayashi, Shin’ichiro . . . . . . . . CC-P.7 SUNHayat, Alex . . . . . . . . . . . . . . . EB-1.2 MONHayes, John . . . . . . . . . . . . . . . CA-7.5 MONHazari, Arnab . . . . . . . . . . . . . .CB-9.1 THUHe, Peijun . . �CL-P.16 SUN, CL-1.4 WEDHe, Qiong . . . . . . . . . . . . . . . . . .CE-3.5 SUNHe, Wei . . . . . . . . . . . . . . . . . . ED-P.9 MONHe, Wenbin . . . . . . . . . . . . . . �CJ-12.4 THUHe, Yunrui . . . . . . . . . . . . . . . �CE-P.18 TUEHeadley, Clifford . . . . . . . . . . . . CJ-4.6 SUNHealy, Noel . . CH-4.4 SUN, CE-P.8 TUE,
CH-6.5 WEDHeath, Daniel . . . . . . . . . . . .�CM-P.17 SUNHeath, Daniel J. . . . . . . . . . . CM-7.4 MONHeathcote, Robert . . . . . . . . CF-P.25 WEDHebling, János CC-3.1 SUN, CC-3.5 SUNHefner, Timo . . . . . . . . . . . . . . .EE-P.7 SUNHegarty, Stephen P. . . . . . .CB-P.24 MON,
CB-7.1 WEDHeideman, René . . . . . . . . . . . CK-5.4 MONHeidmann, Antoine . . . . . . . . EA-4.3 SUN,
EA-4.4 SUN, CH-5.3 TUE, EA-P.18 THUHeidmann, Samuel . . . . . . . . . CK-7.5 TUEHeilmann, René . . . . . . . . . . . .EA-1.3 SUN,�CK-4a.3 MON, CK-4a.3 MON,
CK-4a.3 MON, �EB-3.3 WED,EB-P.1 WED, EA-P.9 THU,JSV-3.3 THU
Hein, Alexander . . . . . . . . . . �CB-P.2 MONHeindel, Tobias . . . . . . . . . . . . EA-8.5 WEDHeiner, Zsuzsanna . . . . . . . . . �EH-6.4 THUHeinrich, Matthias . . . . . . . . . EA-1.3 SUN,�CI-1.2 SUN, �CE-3.1 SUN,�CD-3.4 SUN, �CB-4.4 WEDHeinrichs, Niko . . . . . . . . . . . . EG-P.2 MONHeinz, Tony F. . . . . . . . . . . . �JSIV-1.1 SUNHeinze, Georg . . . . . . . . . . . �EB/EG.2 TUEHeinzig, Matthias . . . . . . . . . CJ-10.6 WEDHeiss, Dominik . . . . . . . . . . . . �CK-3.1 SUNHelbers, Andrew . . . . . . . . . �CE-5b.2 MONHell, Stefan W. . . . . . . . . . . . . �PL-1.1 SUNHellwig, Tim . . . . . . . . . . . . . . CK-5.4 MONHelml, Wolfram . . . . . . . . . . . . CG-1.3 TUEHelt, Lukas G. EA-1.6 SUN, JSV-1.4 THU
Hemmer, Michael . . . . . . . . . . EE-1.5 SUN,�CA-4.3 SUN, CG-3.2 WED,CG-3.4 WED, CG-5.5 WED,CA-10.2 THU, CG-P.5 THU
Hemming, Alexander . . . . . .CJ-11.6 THU,�CJ-13.2 THUHemsley, Elizabeth . . . . . . . . .EA-6.1 TUE,�EA-P.28 THUHenderson, Matthew . . . . . . . CH-5.6 TUEHenderson, Robert . . . . . . . . .CN-2.4 WEDHenderson, Victoria . . . . . . . . �EC-P.2 TUEHendrikx, Ruud . . . . . . . . . . . .EG-6.3 MONHengsberger, Matthias . . . . . CG-4.5 WEDHenkel, Jost . . . . . . . . . . . . . . . CG-1.2 TUEHennrich, Markus . . . . . . . . . PD-B.1 WEDHenrot, Fabien . . . . . . . . . . . . . EF-7.5 TUEHens, Zeger . . . . . . . . . . . . . CK-4a.1 MON,
EG-P.13 MON, CK-11.6 WEDHentschel, Michael . . . . . . . . �EB-P.4 WEDHepp, Christian . . . . . . . . . . . . CE-4.4 SUNHeras, Carmen . . . . . . . . . . . . EH-P.9 WEDHerink, Georg . . . . . . . . . . . . EG-5a.2 MONHermelin, Sylvain . . . . . . . . . CG-P.16 THUHermier, Jean-Pierre . . . . .CK-P.15 MON,
EG-P.8 MON, �EG-7.5 MONHernández-García, Carlos . . . CG-P.7 THUHernandez-Gomez, Cristina .CA-3.6 SUN,
CF-P.25 WED, CG-P.1 THUHernández, José Antonio Pérez
EG-5b.2 MONHernandez, Yves . . . . . . . . . . . . CJ-2.2 SUNHernangómez-Pérez, Daniel CI-P.12 TUEHéron, Sébastien . . . . . . . . . �CK-P.6 MONHerr, Tobias ED-1a.2 MON, ED-P.8 MONHerrero, Ramon . . . . . . . . . . CB-P.3 MON,
CB-P.4 MON, EH-P.16 WEDHerriot, Sandrine . . . . . . . . . CF-P.20 WEDHerrmann, Harald . . . . . . . . JSV-P.4 MONHerrmann, Jens . . . . . . . . . . . CG-5.3 WEDHerrmann, Joachim . . . . . . . . . EE-2.5 SUNHertel, Tobias . . . . . . . . . . . . . . EE-P.7 SUNHertz, Edouard CJ-2.1 SUN, EF-8.3 TUEHeshmat, Barmak . . . . . . . . . CN-2.4 WEDHétet, Gabriel . . . . . . . . . . . �EA-10.3 THU,�EA-10.4 THUHeuck, Mikkel . . . . . . . . . . . .�EB-3.4 WED,
CB-10.1 THUHeuer, Alexander . . . . . . . . . .CE-P.22 TUEHeuer, Axel . . . . . . . . . . . . . . . . EA-3.4 SUNHeugel, Simon EA-P.1 THU, EA-P.3 THUHeuser, Sebastian . . . . . . . . . .CG-4.1 WEDHewak, Dan CE-2.6 SUN, CD-P.11 TUE,
CH-6.5 WEDHeyes, Abi S. . . . . . . . . . . . . . EF-P.23 THUHeyl, Christoph M. . . . . . . . .�CG-1.5 TUE,
CG-P.6 THU, CF-8.2 THUHideki, Hatano . . . . . . . . . . . CD-P.37 TUEHideur, Ammar . . . . . . . . . . . .�CJ-2.4 SUN,�CM-5b.1 MON, EF-4b.1 MON,
CJ-8.5 WEDHiemstra, Thomas . . . . . . �JSV-P.6 MON,
EA-6.3 TUEHigashi, Yuki . . . . . . . . . . . . . . �CA-2.4 SUNHigginbottom, Daniel . . . . . . EB-P.2 WEDHiggins, Gerard . . . . . . . . . . �PD-B.1 WED
Higuchi, Takuya . . . . . . . . . . . .CC-6.3 TUEHiguera-Rodriguez, Aura . . . .CK-3.1 SUNHiguet, Julien . . . . . . . . . . . . . CG-6.2 WEDHilico, Adèle . . . . . . . . . . . . . . . EA-2.2 SUNHill, Kelly . . . . . . . . . . . . . . . . . .CH-4.1 SUNHillenbrand, Rainer . . . . . . . �JSIV-2.1 SUNHiltunen, Jussi . . . . . . . . . . . .JSII-2.2 MONHinds, Edward . . . . . . . . . . . .CE-12.5 WEDHinkley, Nathan . . . . . . . . . . . ED-2.5 MONHinz, Christopher . . . . . . . �EE-5a.1 MON,
EG-P.14 MONHipp, Florian . . . . . . . . . . . . . . EB-4.5 WEDHirabayashi, Takuma . . . . . EH-P.10 WEDHiramatsu, Kotaro . . . . . . . . .CH-7.3 WEDHirosawa, Kenichi . . . . . . . . CA-P.23 SUN,
CA-6.2 MON, CK-6.1 MON,CA-8.1 TUE, CF-P.16 WED,EA-P.12 THU
Hnatovsky, Cyril . . . . . . . . . . . .CL-2.5 THUHo, Chih-Hua . . . . . . . . . . . . . �CK-1.4 SUNHo, Sze-Phing . . . . . . . . . . . . . .CC-6.5 TUEHo, Victor . . . . . . . . . . . . . . . . . .EF-8.2 TUEHoang, Thang B. . . . . . . . . . . EH-4.1 WEDHobbs, Richard . . . . . . . . . . . EE-5a.3 MONHobson, Peter A. . . . . . . . . . . .CD-8.5 TUEHochberg, Michael . . . . . . .CK-4b.1 MON,
EA-7.6 TUE, JSV-1.2 THUHodaei, Hossein . . . . . . . . . . . CB-4.4 WEDHoekman, Marcel . . . . . . . . . . .CI-4.5 SUN,
CK-5.4 MONHoff, Ulrich . . . . . . . . . . . . . . JSV-P.6 MONHoffmann, Armin . . . . . . . . . . CG-2.5 TUE,
CJ-8.2 WEDHoffmann, Axel . . . . . . . . . . .CE-5a.2 MONHoffmann, Björn . . . . . . . . . . .EG-6.1 MONHoffmann, Hans-Dieter . . . CE-10.3 WEDHoffmann, Martin . . . . . . . . .CA-6.1 MON,
CF-9.3 THUHoffmann, Michael . . . . . . . EE-5b.2 MONHoffmann, Norbert . . . . . . . . . . EI-2.4 THUHoffmann, Thomas . . . . . . .CB-P.19 MONHöfling, Sven . . . . . . . . . . . . . �CB-1.1 TUE,
CB-6.1 WED, EA-8.3 WED,EA-8.4 WED, EA-P.5 THU
Hofmann, Bernd . . . . . . . . . . . CF-5.1 WEDHofmann, Julian . . . . . . . . . . �CB-P.9 MONHofmann, Luisa . . . . . . . . . . . CG-1.3 TUE,
CG-2.4 TUEHofmann, Martin R. . . . . . CB-P.21 MON,
CB-2.1 TUE, CB-2.2 TUE, CB-10.4 THUHofmann, Matthias S. . . . . . EG-6.2 MONHofmann, Michael . . . . . . . EE-5b.2 MON,�EE-5b.3 MON, �CF-P.33 WEDHofmann, Peter . . . . . . . . . . . . CA-9.1 THUHöfner, Kathrin . . . . . . . . . . . . CK-8.2 TUEHogan-Lamarre, Pascal . . . �CG-P.19 THUHögele, Alexander . . . . . . . . . EG-6.2 MONHogg, Richard A. . . . . . . . . . CE-11.1 WEDHolgado, Warein . . . . . . . . . . CF-5.3 WED,�CG-P.7 THUHoll, Peter . . . . . . . . . . . . . . . �CB-P.7 MONHolleville, David . . . . . . . . . . .ED-P.9 MONHollinger, Richard . . . . . . . . . . CD-P.6 TUEHolmes, Chris . . . . . . . . . . . . . . CE-2.3 SUNHolmes, Christopher . . . . . . .�CE-2.5 SUN,
212
Authors’ Index
CE-10.4 WEDHolzberger, Simon . . . . . . . . .CJ-8.1 WED,�CG-P.12 THU, CF-9.2 THUHolzinger, Steffen . . . . . . . . . .EA-8.3 WEDHolzwarth, Ronald . . . . . . . . . CC-2.2 SUN,
CJ-14.1 THUHommelhoff, Peter . . . . . . . . CG-4.4 WEDHone, James . . . . . . . . . . . . . JSIV-2.3 SUNHong, Kuo-Bin . . . . . . . . . . . CE-12.2 WEDHong, Seungsoo . . . . . . . . . .CK-P.26 MONHönninger, Clemens . . . . . . CM-P.21 SUN,
CM-5a.1 MONHoogland, Heinar . . . . . . . . . �CJ-14.1 THUHooker, Chris . . . . . . . . . . . . CF-P.25 WEDHopkins, John-Mark . . . . . . . . CB-3.5 TUEHorackova, Lucie . . . . . . . . . . . CA-P.6 SUNHorak, Peter EE-P.6 SUN, CK-10.2 WED,
CE-10.5 WED, EH-P.3 WEDHori, Hirokazu . . . . . . . . . . . EG-P.15 MONHornecker, Gaston . . . . . . . . . EA-9.6 THUHorstmann, Marcel . . . . . . . . EB-4.6 WEDHosaka, Aruto . . . . . . . . . . . . CA-6.2 MON,�EA-P.12 THUHosako, Iwao . . . . . . . . . . . . .CC-P.11 SUN,
CF-P.10 WEDHosseini, Ehsan S. . . . . . . . .CK-12.2 WEDHou, Jing . . . . CJ-7.5 WED, CJ-P.5 WEDHouard, Aurélien . . . . . . . . . . .EE-P.4 SUN,
CD-3.5 SUN, CD-P.3 TUE, CG-1.5 TUE,CF-8.2 THU
Houard, Jonathan . . . . . . . .CM-5b.1 MONHoutepen, Arjan . . . . . . . . . CK-11.6 WEDHouver, Sarah . . . . . . . . . . . . . .CC-1.3 SUNHowe, Richard . . . . . . . . . . . . .CF-P.6 WEDHowle, Christopher . . . . . . . . CN-2.1 WEDHrelescu, Calin . . . . . . . . . . . . EH-P.5 WEDHrnecek, Erich . . . . . . . . . . . . CN-2.3 WEDHsu, Chia-Chen . . . . . . . . . . . . CF-3.1 TUEHsu, Wei-Chi . . . . . . . . . . . . . CK-14.3 THUHu, Guohua . . . . . . . . . . . . . . . CF-P.6 WEDHu, Haiyang . . . . . . . . . . . . . . CE-P.18 TUEHu, Jinmeng . . . . . . . . . . . . . .CJ-P.11 WEDHu, Minglie . . . . . . . . . . . . . . . . CF-1.4 TUEHu, Qi . . . . . . . . . . . . . . . . . . �CH-P.34 THUHu, Tomonori �CJ-5.2 MON, CJ-7.3 WEDHu, Wenchao . . . . . . . . . . . . . . �CI-P.2 TUEHu, Yi . . . . . CD-7.4 MON, CD-13.5 THUHu, Youfang . . . . . . . . . . . . . . . CK-7.2 TUEHua, Li . . . . . . . . . . . . . . . . . . . �CC-2.2 SUNHua, Ping . . . CE-7.2 MON, CE-P.3 TUE,
CJ-P.3 WEDHuang, Chung Che . . . . . . . . CH-6.5 WEDHuang, Jhih-Kai . . . . . . . . . . CK-14.3 THUHuang, Jianfeng . . . . . . . . . . . EH-7.2 THUHuang, Jiong-Fu . . . . . . . . . .CE-12.2 WEDHuang, Jungang . . . . . . . . . . . . EI-P.7 TUEHUANG, Kun . . . . . . . . . . . . . . EA-1.1 SUNHuang, Liangjin . . . . . . . . . . . . �CI-P.9 TUEHuang, Pei-Chi . . . . . . . . . . . . . CF-3.1 TUEHuang, Wenqian . . . . . . . . . . . CC-3.3 SUNHuang, Xiaojun . . . . . . . . . . .CF-P.22 WEDHuang, Yongqing . . . . . . . . . CE-P.18 TUE,
CE-P.29 TUEHübel, Hannes . . . . . . . . . . . . .EB-1.5 MONHuber, Andreas . . . . . . . . . . . �CC-5.2 MON
Huber, Günter . . . . . . . . . . . CJ-6a.1 MON,CA-7.2 MON, CA-8.2 TUE,CA-8.3 TUE, CE-P.6 TUE,CJ-P.41 WED, CA-9.5 THU
Huber, Markus A. . . . . . . . . . �CF-7.1 THUHuber, Robert . . . . . . . . . . . CD-P.19 TUE,
CJ-9.4 WEDHuber, Rupert . . . . . . . . . . . . . CF-7.1 THUHuber, Tobias . . . . . . . . . . . . EA-8.2 WED,�EA-P.7 THU, EA-P.8 THUHudson, Darren . . . . . . . . . . . CJ-5.2 MON,
CJ-7.3 WEDHudson, Darren D. . . . . . . . . . CJ-4.1 SUN,
CD-13.6 THUHugall, James T. . . . . . . . . . . . EG-4.5 SUNHugentobler, Urs . . . . . . . . . .CH-9.6 WED,
CJ-12.3 THUHugger, Stefan . . . . . . . . . . . . CN-2.2 WEDHughes, Josh . . . . . . . . . . . . . .ED-P.9 MONHughes, Mark . . . . . . . . . . . . . CJ-13.2 THUHugi, Andreas . . . . . . . . . . . . . CB-6.2 WEDHugonnot, Emmanuel . . . . . . . CJ-3.3 SUNHuhtio, Teppo . . . . . . . . . . .EG-P.11 MON,
CD-P.7 TUEHuignard, Jean-Pierre . . . . . CH-P.12 THUHuisman, Simon R. . . . . . . . . . EA-3.2 SUNHuisman, Thomas J. . . . . . . . EA-3.2 SUNHulst, Niek F. van . . . . . . . . . . EG-4.5 SUNHumbert, Georges . . . . . . . . . . CH-5.1 TUEHümmer, Thomas . . . . . . . . �EG-6.2 MON,
CK-P.42 MONHumphreys, Peter . . . . . . . .JSV-P.6 MON,
JSV-3.1 THUHumphreys, Peter C . . . . . . .�EA-6.3 TUE,
JSV-1.3 THUHumphries, Peter C. . . . . . . JSV-P.7 MONHunger, David CH-1.2 SUN, CK-2.3 SUN,
EG-6.2 MON, CK-P.42 MON,EA-9.6 THU
Hurtado, Antonio . . . . . . . . . . �EF-1.3 SUNHusakou, Anton . . . . . . . . . . . . EE-2.5 SUNHusko, Chad . . . . . . . . . . . . . . PD-B.6 WEDHussain, Syed . . . . . . . . . . . . .CM-7.5 MONHutchinson, Mark . . . . . . . . . CH-5.6 TUE,
CL-5.4 THUHuth, Florian . . . . . . . . . . . . . .CC-5.2 MONHutterer, Martin . . . . . . . . . . .CH-9.6 WEDHuttunen, Mikko J. . . . . . . . . CD-P.7 TUEHuub, Ambrosius . . . . . . . . . . .CB-8.2 THUHuyet, Guillaume . . . . . . . . CB-P.24 MON,
CB-7.1 WEDHwang, Jaesuk . . . . . . . . . . . CE-12.5 WEDHwang, Min-Soo . . . . . . . . �CK-11.5 WEDHyvärinen, Heikki J . . . . . . CK-P.20 MONHyyti, Janne . . . . . . . . . . . . .�EE-5b.2 MONIbarra-Escamilla, Baldemar CD-P.26 TUEIbrügger, Martin . . . . . . . . . . . . EC-2.5 TUEIbsen, Morten . . . . . . . . . . . . . . CH-5.5 TUEIchikawa, Satoshi . . . . . . . . . CE-11.5 WEDIegorov, Roman . . . . . . . . . . . . �CJ-2.3 SUNIhantola, Sakari . . . . . . . . . . . .CN-2.3 WEDIijima, Kodai CA-P.23 SUN, �CA-8.1 TUEIikubo, Ryo . . . . . . . . . . . . . . . EE-P.18 SUNIkesue, Akio . . . . . . . . . . . . . . . CE-7.4 MONIkonic, Zoran . . . . . . . . . . . . . . .CB-1.4 TUE
Ikuta, Rikizo . . . . . . . . . . . . . .EA-P.25 THUIlday, F. Oemer . . . . . . . . . . . . CJ-2.6 SUN,�TF-2.2 TUEIlday, Fatih . . . . . . . . . . . . . . . CJ-P.26 WEDIlday, Fatih Omer . . . . . . . . . .CM-2.5 SUN,
CM-P.18 SUN, CM-4.5 SUN,CK-P.3 MON, CK-P.34 MON,CJ-P.19 WED, CJ-P.31 WED,CL-5.1 THU
Ilday, Omer . . . CJ-2.3 SUN, JSI-P.1 TUEIlday, Serim . . . . . . . . . . . . . . . .CM-2.5 SUNIliev, Hristo CA-P.40 SUN, CA-11.4 THUImamoglu, Atac . . . . . . . . . . .EA-P.30 THUImamura, Takeshi . . . . . . . . .CH-P.29 THUImbrock, Jörg CD-2.4 SUN, CD-11.2 THUImoto, Nobuyuki . . . . . . . . . . EA-P.25 THUImran, Muhammad . . . . . . . . .CI-P.10 TUEInácio, Patricia Loren . . . . . .CE-P.13 TUEInoue, Shuichiro . . . . . . . . . . EA-P.22 THUInoue, Tatsuki . . . . . . . . . . . . CJ-P.37 WEDIonescu, Alina . . . . . . . . . . . . CA-10.4 THUIonin, Andrey A. . . . . . . . . . . . CN-P.4 TUEIqbal, Muhammad . . . . . . . . . . CK-3.4 SUNIreland, Michael . . . . . . . . . . . CM-P.7 SUNIreland, Mike . . . . . . . . . . . . . . CM-P.8 SUNIreland, Philip . . . . . . . . . . . . . . EC-P.1 TUEIronside, Charles . . . . . . . . . . CK-14.2 THUIsa, Fumihiro . . . . . . . . . . . . �CF-P.16 WEDIsabelle, Sagnes . . . . . . . . . .CB-P.32 MON,
CB-1.3 TUEIsella, Giovanni . . . . . . . . . . . . .EH-5.5 THUIshibashi, Shigeo . . . . . . . . . . �CA-6.6 MONIshibashi, Tadao . . . . . . . . . . . ED-2.5 MONIshigaki, Naoya . . . . . . . . . . . .CA-P.43 SUNIshii, Nobuhisa . . . . . . . . . . . . .�CF-2.2 TUEIshii, Osamu CJ-P.9 WED, CJ-P.38 WEDIshikawa, Kenichi . . . . . . . . . CG-P.15 THUIskhakov, Timur . . . . . . . . . . . .CD-9.1 TUEIsmaeel, Rand . . . . . . . . . . . �CD-5a.3 MONIsobe, Keisuke . . . . . . . . . . . . . .CL-4.6 THUIsrael, Yonatan . . . . . . . . . . . CD-11.5 THUItakura, Ryuji . . . . . . . . . . . . . �CF-8.3 THUItatani, Jiro . . . . . . . . . . . . . . . . CF-2.2 TUEItina, Tatiana . . . . . . . . . . . . . . .EE-2.4 SUNItobe, Hiroki . . . . . . . . . . . . . . �CK-9.6 TUEItoh, Mikitaka . . . . . . . . . . . . .PD-B.3 WEDIvanov, Igor . . . . . . . . . . . . . . . CG-4.2 WEDIvanov, Misha . . . . . . . . . . . . .CG-4.2 WED,
CG-5.4 WED, CG-P.13 THUIvleva, Lyudmila . . . . . . . . . . .CA-P.41 SUNJ. Spence, David . . . . . . . . . . CA-1.1 SUN,
CA-P.9 SUNJabczynski, Jan K. . . . . . . . . CA-P.25 SUNJacak, Jaroslaw . . . . . . . . . . . CM-6.4 MONJacassi, Andrea . . . . . . . . . . EG-P.10 MONJackson, Stuart . . . . . . . . . . . CJ-5.2 MON,�CJ-7.3 WEDJackson, Stuart D. . . . . . . . . . . CJ-4.1 SUNJacqmin, Hermance . . . . . . . .�CG-2.2 TUEJacqmin, Thibaut . . . . . . . . . . EA-4.3 SUN,
EA-4.4 SUN, CH-5.3 TUEJacques, Vincent . . . . . . . . . . EA-10.3 THUJaeck, Julien . . . . . . . . . . . . . . .CD-8.6 TUEJäger, Matthias . . . . . . . . . . . �CJ-9.5 WEDJahnke, Frank CB-4.2 WED, EA-8.3 WED
Jain, Chhavi . . . . . . . . . . . . . . PD-A.8 WEDJain, Deepak . . . . . . . . . . . . . . �CJ-3.2 SUN,
CJ-P.30 WED, CJ-14.3 THUJain, Saurabh . . . . . . . . . . . . CJ-P.33 WED,
CJ-12.1 THUJakutis-Neto, Jonas . . . . . . . . CA-P.9 SUNJalali, Mandana . . . . . . . . . . . �JSI-2.3 SUNJambunathan, Venkatesan . �CA-P.6 SUN,
CA-P.30 SUN, CA-P.31 SUN,CA-4.5 SUN, CA-5b.3 MON
Jamier, Raphael . . . . . . . . . . CJ-P.49 WEDJamonneau, Pierre . . . . . . . . EA-10.3 THUJandieri, Kakhaber . . . . . . . .CE-11.6 WEDJang, Hoon . . . . . . . . . . . . . . . . CK-3.5 SUNJang, Jae . . . . . . . . . . . . . . . . . EF-P.18 THUJang, Jae K. . . EF-1.1 SUN, EE-3.5 SUN,
CD-13.1 THUJanicot, Sylvie . . . . . . . . . . . . .CB-5.3 WEDJanner, Davide . . . . . . . . . . . . . CL-P.2 SUNJannesari, Reyhaneh . . . . . . . CK-P.5 MONJansen, Florian . . . . . . . . . . . . . CJ-1.2 SUNJansen, GS Matthijs . . . . . . . �CH-1.4 SUNJarnac, Amelie . . . . . . . . . . . . CG-1.5 TUE,�CF-8.2 THUJarschel, Paulo . . . . . . . . . . . CK-P.38 MONJärvinen, Samu . . . . . . . . . . . . CH-7.5 WEDJarvis, Jan . . . . . . . . . . . . . . . . CN-2.2 WEDJauregui, Cesar . . . . . . . . . . . .CJ-5.5 MON,
CJ-10.1 WED, �CJ-10.2 WED,CJ-13.1 THU, CJ-13.5 THU
Jauregui-Misas, Cesar . . . . . .CJ-13.4 THUJaurigue, Lina . . . . . . . . . . . . . CB-9.5 THUJauslin, Hans . . . . . . . . . . . . . .EG-P.3 MONJavaloyes, Julien . . . . . . . . . . . EF-1.2 SUN,
EF-1.3 SUN, EF-1.4 SUN, CI-5.2 MON,�EI-P.2 TUE, �CB-2.5 TUE,CB-7.6 WED, CD-13.4 THU
Javaux, Clémentine . . . . . .CM-5a.1 MON,CK-P.15 MON, CK-P.25 MON,EG-7.5 MON
Javaux Léger, Clémentine . CM-P.21 SUNJaverzac-Galy, Clément . . . .CB-10.6 THUJavůrek, Dalibor . . . . . . . . .�CK-P.32 MONJaworski, Piotr . . . . . . . . . . . . �CE-1.5 SUNJazbinsek, Mojca . . . . . . . . . . . CC-3.6 SUNJedrkiewicz, Ottavia . . . . . . . CM-3.1 SUNJedrzejczyk, Daniel . . . . . . . . CB-P.9 MONJelínek, Michal . . . . . . . . . . . CA-P.30 SUN,�CA-P.37 SUN, �CA-P.41 SUN,
CA-4.3 SUNJelinkova, Helena . . . . . . . . .CA-P.24 SUN,
CA-P.25 SUN, CA-P.37 SUN,CA-P.41 SUN, CA-4.3 SUN
Jendrzejewski, Maik . . . . . . CB-P.10 MONJennewein, Thomas . . . . . . . �EB-1.5 MONJenson, Adam . . . . . . . . . . . . CF-P.25 WEDJeong, Hwanseong . . . . . . . CJ-P.23 WED,�CF-4.5 WEDJeong, Kwang-Yong . . . . . . CK-11.5 WEDJeong, Tae Moon . . . . . . . . JSIII-1.1 MONJeong, Yoonchan . . . . . . . . . CK-P.26 MONJEONG, Youn-Chang . . . . . . . EA-1.1 SUNJepsen, Peter . . . . . . . . . . . . . CE-P.20 TUEJessop, David CC-2.3 SUN, CC-2.5 SUN,
CC-P.14 SUN, CB-6.4 WED
Jestin, Yoann . . . . . . . . . . . . . . EA-7.3 TUEJetter, Michael . . . . . . . . . . CB-P.16 MON,
CB-P.18 MON, CB-3.4 TUEJex, Igor . . . . . . . . . . . . . . . . . . JSV-2.1 THUJha, Animesh . . . . . . . . . . . . CM-6.5 MON,�CM-7.5 MONJhajj, Nihal . . . . . . . . . . . . . . . . EE-2.1 SUNJian, Pu . . . . . . . . . . . . . . . . . . ED-P.4 MONJiang, Aiting . . . . . . . . . . . . . . . CC-1.1 SUNJiang, Hua . EG-P.11 MON, CD-P.7 TUEJiang, Huawei . . . . . . . . . . . . CJ-P.11 WEDJiang, Jie . . ED-1b.1 MON, TF-1.2 TUE,
CH-9.1 WEDJiang, Junjie . . . . . . . . . . . . . . . CC-4.2 SUNJiang, Qi . . . . . . . . . . . . . . . . . . CB-9.2 THUJiang, Yifan . . . . . . . . . . . . . . . . CC-1.1 SUNJiang, Zongfu . . . . . . . . . . . . . .CJ-P.5 WEDJiménez-Galán, Alvaro . . . . �CG-5.2 WEDJimenez, Jesus . . . . . . . . . . . . . EF-1.5 SUN,�CB-P.15 MONJiménez-Solano, Alberto . . CK-P.24 MONJimenez Villar, Ernesto . . �CK-P.19 MONJin, Aijun . . . . . . . . . . . . . . . . . .CJ-7.5 WEDJin, Jing . . . . . . . . . . . . . . . . . CH-P.14 THUJin, Lei . . . . . . . . . . . . . . . . . . . �CJ-P.4 WEDJin, Yuwei . . . . . . . . . . . . . . . . . �CF-1.5 TUEJin, Zuanming . . . . . . . . . . . . . .CC-4.2 SUNJinzenji, Taka-aki . . . . . . . . . . .CE-8.5 TUEJipa, Florin . . . . . . . . . . . . . . . CA-P.29 SUNJirauschek, Christian . . . . . . �CC-1.2 SUN,�CJ-9.4 WEDJobez, Pierre �EA-2.4 SUN, EA-P.31 THUJobin, Frederic . . . . . . . . . . . . .CJ-5.3 MONJocher, Christoph . . . . . . . . . . CF-9.2 THUJochim, Selim . . . . . . . . . . . . . �EC-1.1 TUEJoel, Andrew . . . . . . . . . . . . . . .CB-2.4 TUEJoffre, Manuel . . . . . . . . . . . . �EE-1.3 SUN,�CF-6.5 THUJofre, Marc . . . . . . . . . . . . . . . . CL-1.2 WEDJohnson, Adrea R. . . . . . . . . CH-8.6 WED,
PD-A.5 WEDJohnson, Allan S. . . . . . . . . . . CG-3.3 WEDJohnson, Sam . . . . . . . . . . . . . . EC-3.2 TUEJohnson, Trent . . . . . . . . . . . . . CC-4.1 SUNJohnsson, Per CG-1.5 TUE, CG-P.6 THU,
CF-8.2 THUJoly, Alexandre . . . . . . . . . . . . .CD-4.2 SUNJoly, Nicolas .CD-9.1 TUE, PD-B.2 WEDJoly, Simon . . . . . . . . . . . . . . CB-P.33 MONJonavicius, Tomas . . . . . . . . . CM-1.2 SUNJones, Max . . . CH-4.4 SUN, CE-P.8 TUEJones, R. Jason . . . . . . . . . . �ED-2.2 MON,�CF-9.5 THUJonuscheit, Joachim . . . . . . . CC-5.2 MONJose, Gin . . . . CE-1.3 SUN, CM-6.5 MONJost, John . �ED-1a.2 MON, CE-9.1 TUEJost, John D. . . . . . . . . . . . . . CB-10.6 THUJovanovic, Nemanja . . . . . . . CM-P.7 SUN,
CH-7.4 WEDJu, YouLun . . CA-P.5 SUN, CJ-14.2 THUJuan, Mathieu . . . . . . . . . . . . . CL-2.2 THU,�EA-10.6 THUJuan, Mathieu L. . . . . . . . . . . . EA-1.6 SUNJuergen, Kreuzer . . . . . . . . . . CM-7.6 MONJukna, Tomas . . . . . . . . . . . . CH-P.21 THU
213
Authors’ Index
Jukna, Vytautas . . . . . . . . . . . EE-2.4 SUN,CM-3.1 SUN, CD-P.3 TUE
Jules, Jean-Charles . . . . . . . . CD-6.1 MONJuliá, Enrique . . . . . . . . . . . . . .CM-P.4 SUNJullien, Aurélie . . . . . . . . . . . . . CG-2.2 TUEJullien, Ludovic . .CLEO/ECBO-1.2 WEDJumpertz, Louise . . . . . . . . . . CN-1.5 WEDJung, Markus . . . . . . . . . . . . . CJ-10.3 WEDJung, Seungyong . . . . . . . . . . . CC-1.1 SUNJung, Yongmin . . . . . . . . . . . . .CJ-3.2 SUN,
CJ-12.1 THUJunge, Christian . . . . . . . . . . . . EA-2.2 SUNJüngling, Thomas . . . . . . . . . EF-P.22 THUJuodkazis, Saulius . . . . . . . . . CM-1.2 SUN,
CM-1.5 SUNJupé, Marco . . . . . . . . . . . . . .EE-5b.2 MONJuska, Gediminas . . . . . . . . . �JSV-2.6 THUJusza, Anna . . . . . . . . . . . . . . . CH-6.3 WEDKabakova, Irina V. . . . . . . . . CD-13.6 THUKabeya, David . . . . . . . . . . . . . �CJ-1.5 SUNKablukov, Sergey . . . . . . . . . CJ-P.16 WEDKaczmarek, Malgosia . . . . . .CC-P.17 SUNKaenders, Wilhelm . . . . . . . . ED-P.9 MONKaertner, Franz . . . . . . . . . . . . CC-3.3 SUNKafenda, Kim . . . . . . . . . . . . . . EG-3.3 SUNKafesaki, Maria . . . . . . . . . . . . CE-3.3 SUNkahaly, subhendu . . . . . . . . . . . CG-2.6 TUEKahle, Hermann . . . . . . . . . CB-P.16 MON,
CB-P.18 MON, �CB-3.4 TUEKaierle, Stefan . . . . . . . . . �CM/LIM.1 TUEKailasnath, Madanan . . . . . CE-12.4 WEDKaipurath, Rishad K. . . . . . . EH-3.4 WEDKaiser, Robin . EC-3.3 TUE, EF-9.3 THUKajikawa, Eiji . . . . . . . . . . . . �CJ-14.4 THUKajikawa, Shota . . . . . . . . . �CJ-P.38 WEDKakarla, Ravikiran . . . . . . . . . . .CI-4.4 SUNKakavelakis, George . . . . . . . CM-7.3 MONKakenov, Nurbek . . . . . . . . . CC-P.18 SUN,
CA-12.4 THUKakinuma, Yasuhiro . . . . . . . . CK-9.6 TUEKaksis, Edgar . . . . . . . . . . . . . . CA-3.3 SUNKalaee, Mahmoud . . . . . . . . . . EG-1.1 SUNKalashnikov, Mikhail . . . . . �CF-P.18 WEDKalashnikov, Vladimir . . . . .CA-P.22 SUN,
PD-A.1 WED, CA-10.5 THUKalaycioglu, Hamit . . . . . . �CJ-P.19 WED,
CJ-P.31 WED, CL-5.1 THUKaldvee, Kaarel . . . . . . . . . . . . CL-P.3 SUNKalkandjiev, Todor . . . . . . . CD-P.30 TUE,
EC-P.8 TUEKalt, Heinz . . . . . . . . . . . . . . . . CK-9.5 TUEKaltenbach, André . . . . . . . �CD-P.35 TUEKambayashi, Yuta . . . . . . . . �CJ-P.37 WEDKamboj, Varun . . . . . . . . . . . . .CC-2.3 SUNKamioka, Syunya . . . . . . . . .CK-P.12 MONKamp, Martin . . . . . . . . . . . . . CB-1.1 TUE,�CB-6.1 WED, EA-8.3 WED,
EA-8.4 WED, EA-P.5 THUKamynin, Vladimir . . . . . . . �CJ-P.44 WEDKanai, Teruto . . . . . . . . . . . . . . CF-2.2 TUEKanai, Tsuneto . . . . . . . . . . . . CF-2.1 TUE,�CF-2.4 TUEKanda, Natsuki . . . . . . . . . . . . CC-6.3 TUEKandidov, Valery P. . . . . . . . . CN-P.4 TUEKane, Deb . . �CE-P.2 TUE, �CH-P.7 THU
Kanemitsu, Yoshihiko . . . . . . .CF-7.4 THUKaneshima, Keisuke . . . . . . . . CF-2.2 TUEKang, Bong Joo . . . . . . . . . . . �CC-P.3 SUNKang, Qionque . . . . . . . . . . . . CJ-12.1 THUKanger, Hans . . . . . . . . . . . . .CK-14.1 THUKannari, Fumihiko . . . . . . . . CA-P.23 SUN,
CA-6.2 MON, CK-6.1 MON,CA-8.1 TUE, CF-P.16 WED,EA-P.12 THU, CL-4.6 THU
Kanno, Atsushi �CI-2.2 SUN, CI-3.6 SUN,CI-5.6 MON
Kantola, Emmi . . . . . . . . . . . CB-P.1 MON,�CB-3.1 TUEKao, Tsung Sheng . . . . . . . CE-12.2 WED,
CK-14.3 THUKao, Tsung-Ting . . . . . . . . . . PD-A.2 WEDKapulainen, Markku . . . . . . . . CI-P.7 TUE,
CH-6.1 WEDKaraman, Jasmin . . . . . . . . . . EH-P.1 WEDKarbasi, Salman . . . . . . . . . . . .CD-3.3 SUNKardaś, Tomasz . . . . . . . . . . . CF-P.8 WEDKarioja, Pentti . . . . . . . . . . . �JSII-2.2 MONKariyama, Ryosuke . . . . . . �CA-P.23 SUN,
CA-6.2 MON, CA-8.1 TUEKarjalainen, Hertta . . . . . . . . CB-4.5 WEDKarlsson, Mikael . . . . . . . . . . . .CL-4.1 THUKarnadi, Indra . . . . . . . . . . . . . �CK-3.5 SUNKarpf, Andreas . . . . . . . . . . . . CN-2.5 WEDKarpf, Sebastian . . . . . . . . . �CD-P.19 TUEKarpierz, Mirosław . . . . . . . . . EF-8.4 TUEKarpinski, Michal . . . . . . . �JSV-P.2 MON,
EA-P.15 THUKarpowicz, Nicholas . . . . . . . .CF-1.3 TUE,
CF-7.5 THU, CG-P.3 THUKartashov, Daniil . . . . . . . . . . EE-4.3 SUN,
CD-P.6 TUE, CF-3.5 TUE, CG-6.5 WEDKärtner, Franz . . . . . . . . . . . EE-5a.3 MON,�CF-5.4 WEDKärtner, Franz. X. . . . . . . . . . CA-4.2 SUN,
CA-10.2 THU, CG-P.4 THU,CF-9.1 THU
Karvonen, Lasse . . . . . . . . . EG-P.11 MON,CD-P.7 TUE
Karvounis, Artemios . . . . . . �EH-3.5 WEDKasamatsu, Akifumi . . . . . . CC-P.11 SUN,
CF-P.10 WEDKasatani, Atsushi . . . . . . . . .�CC-P.12 SUNKashyap, Raman . . . . . . . . . . . CJ-9.6 WEDKaskow, Mateusz . . . . . . . . .�CA-P.25 SUNKasmi, Lamia . . . . . . . . . . . . �CG-4.5 WED,
CG-5.3 WEDKaspar, Sebastian . . . . . . . . . CB-P.7 MONKasparian, Jérôme . . . . . . . .CD-P.14 TUE,
CD-P.33 TUE, CD-P.38 TUE,CF-P.24 WED, CG-P.16 THU
Kasper, Susane . . . . . . . . . . . . CG-5.1 WEDKassal, Ivan . . . . . . . . . . . . . . EA-P.14 THUKassi, Samir . . . . . . . . . . . . . . . CH-2.5 SUNKaszlikowski, Dagomir . . . . . . EA-1.4 SUNKasztelanic, Rafał . . . . . . . . . .CJ-5.4 MONKatano, Yutaro . . . . . . . . . . . . . CI-3.5 SUNKataura, Hiromichi . . . . . . . . . CJ-4.4 SUN,
CJ-P.4 WEDKatayama, Takeo . . . . . . . . . . �CI-5.4 MONKatis, Ioannis . . . . . . . . . . . . .CL-P.16 SUN,
�CL-1.4 WEDKatori, Hidetoshi . . . . . . . . . . ED-3.2 MONKaufmann, Thomas . . . . . . . EA-P.26 THUKaupp, Hanno . . . . . . . . . . . . .�CK-2.3 SUNKaur Gulati, Gurpreet . . . . . . EC-2.2 TUE,
EA-6.2 TUEKauranen, Martti . . . . . . . . EG-P.11 MON,
CD-P.7 TUE, EH-P.11 WED,CE-12.4 WED
Kaushal, Jivesh . . . . . . . . . . . . CG-4.2 WEDKauten, Thomas . . . . . . . . �EA-P.26 THU,
JSV-3.5 THUKawagishi, Masahiko . . . . . . CD-11.3 THUKawagoe, Hiroyuki . . . . . . . . .�CL-5.2 THUKawaguchi, Hitoshi . . . . . . . . . CI-5.4 MONKawanishi, Tetsuya . . . . . . . . . CI-2.2 SUN,
CI-3.6 SUN, CI-5.6 MON, CI-P.11 TUE,CF-P.10 WED
Kawano, Hiroyuki . . . . . . . . . . CL-4.6 THUKawata, Yoshimasa . . . . . . . . CE-8.4 TUE,
EH-P.10 WEDKayanuma, Yosuke . . . . . . . . EE-P.18 SUNKazanskii, Andrey . . . . . . . . .CK-14.4 THUKazansky, Peter . . . . . . . . . . CM-6.3 MON,
CLEO/ECBO-2.3 WED, CJ-P.10 WED,CK-14.4 THU
Kazasidis, Orestis . . . . . . . . . �CE-7.5 MONKbashi, Hani . . . . . . . . . . . . . CM-P.15 SUNKedenburg, Stefan . . . . . . . . .�CD-4.6 SUNKeeling, Jonathan . . . . . . . . . . EC-P.1 TUEKeiber, Sabine . . . . . . . . . . . . �CF-7.5 THU,
CG-P.3 THUKeiding, Søren Rud . . . . . . . . .CH-3.4 SUNKeil, Robert EA-1.3 SUN, EA-P.26 THU,
JSV-3.5 THU, JSV-4.6 THUKeilmann, Fritz . . . . . . . . . . . CC-5.2 MON,�CF-7.2 THUKelkar, Hrishikesh . . . . . . . . . EG-6.1 MONKelleher, Bryan . . . . . . . . . �CB-P.24 MON,
CB-7.1 WED, CB-7.4 WEDKelleher, Edmund . . . . . . . . . . CD-1.4 SUNKelleher, Edmund John Railton�EF-5.4 MON, CJ-9.6 WEDKeller, Janine . . . . . . . . . . . . . EH-4.6 WEDKeller, Ursula .CD-2.5 SUN, EE-4.2 SUN,
CA-7.1 MON, CF-2.3 TUE,CJ-8.4 WED, CG-4.1 WED,CG-4.5 WED, CF-4.1 WED,CH-8.2 WED, CH-8.3 WED,CH-8.6 WED, CG-5.3 WED,PD-A.5 WED, CF-9.3 THU
Kellert, Martin . . . . . . . . . . . . �CA-3.5 SUNKellou, Abdelhamid . . . . . . . . CJ-P.7 WEDKemlin, Vincent . . . . . . . . . . . . EE-1.3 SUNKemnitzer, Matthias . . . . . . . .CA-2.1 SUNKemp, Alan . . .CA-1.3 SUN, CA-8.4 TUEKen, Olga S. . . . . . . . . . . . . . . CK-P.1 MONKenanakis, George . . . . . . . . . .CE-3.3 SUNKenji, Kitamura . . . . . . . . . . .CD-P.37 TUEKenyon, Anthony . . . . . . . . .CK-10.2 WEDKermène, Vincent . . . . . . . . . . CJ-1.3 SUN,
CJ-1.5 SUNKern, Pierre . . . . . . . . . . . . . . . .CK-7.5 TUEKerouredan, Olivia . . . . . . . . . .CL-P.5 SUNKerridge-Johns, William . . . .CA-6.4 MON
Kerse, Can . . CJ-P.19 WED, CL-5.1 THUKersteen, Grizelda . . . . . . . .CB-P.18 MONKesim, Denizhan Koray . . .CJ-P.19 WED,
CJ-P.31 WED, �CL-5.1 THUKeskinen, Jorma . . . . . . . . . . .CH-7.5 WEDKessel, Alexander . . . . . . . . .EG-5b.1 MONKewes, Günter . . . . . . . . . . . . �CK-8.2 TUEKhajavikhan, Mercedeh . . . . CD-3.4 SUN,
CB-4.4 WEDKhaled, Federico . . . . . . . . . . .CE-7.4 MONKhan, Khouler . . . . . . . . . . . . . CE-2.6 SUN,
CD-P.11 TUEKharenko, Denis . . . . . . . . . �CF-P.26 WEDKharitonov, Artem . . . . . . . . . CE-P.5 TUEKharitonov, Svyatoslav . . . . �CJ-13.3 THUKhasanov, Oleg . . . . . . . . . . . EF-P.15 THUKheifets, Anatoli . . . . . . . . . . CG-4.2 WED,
CG-5.1 WEDKhenkin, Mark . . . . . . . . . . . .CK-14.4 THUKho, Kiang Wei . . . . . . . . . . CE-12.5 WEDKhodakovskiy, Nikita . . . . . CF-P.18 WEDKhokhar, Ali Z. . . . . . . . . . . . . CK-7.2 TUEKhokhlova, Margarita . . . . . �CG-P.8 THUKhoshnegar, Milad . . . . . . . . EA-8.2 WED,
EA-P.7 THUKhripunov, Sergey . . . . . . . . CA-11.3 THUKhromova, Irina . . . . . . . . . . . CC-5.1 MONKianirad, Hoda . . . . . . . . . . . �CE-P.32 TUEKibler, Bertrand . . . . . . . . . . CD-6.1 MON,
EF-4b.2 MONKicas, Simonas . . . . . . . . . . . . .CK-1.5 SUNKido, Ladislav . . . . . . . . . . . . . . CJ-4.5 SUNKienberger, Reinhard . . . . . . CG-2.1 TUE,
CH-9.6 WED, CJ-12.3 THUKienel, Marco CJ-1.2 SUN, CJ-13.4 THUKienle, Florian . . . . . . . . . . . . . CA-2.1 SUNKikas, Jaak . . . . . . . . . . . . . . . . CL-P.3 SUNKildishev, Alexander . . . . . . . CE-3.2 SUN,
CE-P.30 TUEKim, Byunghoon . . . . . . . . . . CG-1.5 TUE,
CG-P.6 THU, CF-8.2 THUKim, Dai-Sik . . . . . . . . . . . . . . .EH-5.4 THUKim, Dong-Eon . . . . . . . . . . EG-5b.1 MON,
CG-P.3 THUKim, Dongeon . . . . . . . . . . . . .CG-4.4 WEDKim, Dongjun . . . . . . . . . . . . . �CA-P.3 SUNKim, Hwi . . . . . . . . . . . . . . . . CK-P.23 MONKim, Hyung Taek . . . . . . . �JSIII-1.1 MONKim, Hyuntai . . . . . . . . . . . �CK-P.26 MONKim, I Jong . . . . . . . . . . . . . . JSIII-1.1 MONKim, Ji Won . . . . . . . . . . . . . . . CA-P.3 SUNKim, Jinseob . . . . . . . . . . . . .CK-P.26 MONKim, Jongbum . . . . . . . . . . . . CE-P.30 TUEKim, Joonsoo . . . . . . . . . . . . CK-P.23 MONKim, Ju-Young . . . . . . . . . . . . . CK-3.5 SUNKim, Mi Hye . . . . . . . . . . . . . �CE-P.6 TUE,
CJ-P.23 WED, CF-4.5 WED,CA-9.5 THU
Kim, Na Young . . . . . . . . . . . . CB-1.1 TUEKim, Seung-Hyun . . . . . . . . . . EH-5.4 THUKim, Song-Ju . . . . . . . . . . . . EG-P.15 MONKim, Won Tae . . . . . . . . . . . . . CC-P.3 SUNKing, Gary . . . . . . . . . . . . . . . .CA-12.6 THUKinoshita, Nobuhiro . . . . . . . . . CI-3.5 SUNKinsey, Nathaniel . . . . . . . . . . CE-3.2 SUN,
�CE-P.30 TUEKintaka, Yuji . . . . . . . . . . . . . . .CA-2.4 SUNKioseoglou, George . . . . . . . .CM-7.3 MONKippenberg, Tobias . . . . . . . . EG-1.4 SUN,
EA-4.2 SUN, ED-1a.2 MON,CE-9.1 TUE
Kippenberg, Tobias J. . . . . .ED-P.8 MON,CB-10.6 THU
Kisel, Viktor .CA-P.38 SUN, CA-9.3 THUKitaeva, Galiya . . . . . . . . . . . .CC-P.19 SUNKitajima, Shotaro . . . . . . . . . .�CA-2.5 SUNKitamura, Kyoko . . . . . . . . �CK-13.6 WEDKitzerow, Heinz . . . . . . . . . �CK-P.16 MONKitzerow, Heinz-Siegfried . . . CE-P.7 TUEKitzler, Markus . . . . . . . . . . . . EE-P.8 SUN,
EE-4.3 SUN, �CG-6.5 WED,CG-6.6 WED
Kitzler, Ondrej . . . . . . . . . . . . CA-6.5 MONKivshar, Yuri EG-2.2 SUN, CK-6.3 MON,
EH-3.1 WED, EH-5.1 THU, EH-5.3 THUKivshar, Yuri S. . . . . . . . . . . . . EH-7.1 THUKlar, Thomas . . . . . . . . . . . . . CM-6.4 MONKlar, Thomas A. . . . . . . . . . . EH-P.5 WEDKlatt, Gregor . . . . . . . . . . . . . . .CC-P.5 SUNKlehr, Andreas . . . . . . . . . .�CB-P.19 MON,
CB-8.4 THU, CB-10.4 THU,CB-11.5 THU
Klein, Nico . . . . . . . . . . . . . . . . EB-1.3 MONKlein, Thomas . . . . . . . . . . . . CD-P.19 TUEKleineberg, Ulf . . . . . . . . . . . . . CF-8.1 THUKlenke, Arno .�CJ-1.2 SUN, CG-2.5 TUE,
CG-3.1 WED, CJ-13.4 THUKlenner, Alexander . . . . . . . . CD-2.5 SUN,�CA-7.1 MON, CH-8.2 WED,
CH-8.3 WED, CH-8.6 WED,�PD-A.5 WEDKlier, Jens . . . . . . . . . . . . . . . . CC-5.2 MONKlimant, Ingo . . . . . . . . . . . . CH-P.31 THUKlimczak, Mariusz . . . . . . . . . CJ-5.4 MONKlimentov, Dmitry . . . . . . . �CJ-P.32 WEDKlimont, Adam . . . . . . . . . . . . CC-2.3 SUN,�CC-2.5 SUN, CC-P.14 SUNKliner, Dahv . . . . . . . . . . . . . �CJ-11.2 THUKling, Matthias . . . . . . . . . . EG-5b.1 MON,�CG-4.4 WEDKling, Rainer . . . . . . . . . . . . CM-P.21 SUN,
CM-5a.1 MON, �TF-2.1 TUEKlingebiel, Sandro . . . . . . . . �CA-10.1 THUKliuiev, Pavel . . . . . . . . . . . . . CG-4.5 WEDKneipp, Janina . . . . . . . . . . . . .EH-6.4 THUKnigge, Steffen . . . . . . . . . . . .CB-P.5 MONKnight, Jonathan C. . . . . . . . . CE-1.5 SUNKnips, Lukas . . . . . . . . . . . . . �EB-1.3 MONKnittel, Vanessa . . . . . . . . . . . �EH-7.3 THUKo, Do-Kyeong . . . . . . . . . . . . .CE-9.3 TUEKo, Min Jae . . . . . . . . . . . . . . . JSI-1.4 SUNKoashi, Masato . . . . . . . . . . . EA-P.25 THUKobayashi, Ryo . . . . . . . . . . �EA-P.22 THUKobayashi, Toshiki . . . . . . . �EA-P.25 THUKobayashi, Yohei . . . . . . . . . . .CF-4.2 WEDKobtsev, Sergey . . . . . . . . . . CA-11.3 THUKocabaş, Coşkun . . . . . . . . . CC-P.18 SUN,
CA-12.4 THUKocer, Hasan . . . . . . . . . . . . �CK-11.4 WEDKoch, Martin CB-3.2 TUE, CE-11.6 WED
214
Authors’ Index
Koch, Ralf . . . . . . . . . . . . . . . CJ-P.17 WEDKocharovskaya, Ekaterina . .EF-P.13 THUKocharovsky, Vitaly . . . . . . . EF-P.13 THUKocharovsky, Vladimir . . . . �EF-P.13 THUKock, Ole . . . . . . . . . . . . . . . . .ED-P.9 MONKoduru Joshi, Siddarth . . . . . EA-1.4 SUNKoeckelberghs, Guy . . . . . . . . .CE-9.6 TUEKoehler, Christian . . . . . . . . . . EE-2.5 SUNKoehler, Johannes R. . . . . . �CD-P.10 TUEKoenderink, Femius . . . . . . . .EG-6.3 MONKoeth, Johannes . . . . . . . . . . .CB-6.1 WEDKögel, Benjamin . . . . . . . . . . . CB-2.3 TUEKohfeldt, Anja . . . . . . . . . . �CB-P.12 MONKöhl, Michael . . . . . . . . . . . . . . EC-1.2 TUEKohnle, Verena . . . . . . . . . . . . EG-P.5 MONKohno, Kenta . . . . . . . . . . . . . CJ-14.4 THUKoke, Sebastian . . . . . . . . . . . CF-5.1 WEDKolesik, Miroslav . . . . . . . . . . . EE-2.2 SUNKolkowski, Radoslaw . . . . . . . CK-8.1 TUEKollmann, Heiko . . . . . . . . . . .EG-P.6 MONKolokolov, Igor . . . . . . . . . . . . . .EI-2.2 THUKolpakov, Stanislav . . . . . . �CM-P.15 SUNKolthammer, Steven . . . . . JSV-P.6 MON,
JSV-3.1 THUKolthammer, W. Steven . . JSV-P.7 MON,
EA-6.3 TUE, JSV-1.3 THUKolykhalova, Ekaterina D. CB-P.22 MONKompanets, Victor . . . . . . . . CD-P.31 TUEKonios, Dimitris . . . . . . . . . . .CM-7.3 MONKonishi, Kuniaki . . . . . . . . . . . .CC-6.3 TUEKonkov, Oleg . . . . . . . . . . . . . CK-14.4 THUKonotop, Vladimir . . . . . . . . . EF-6.4 MONKonstantaki, Mary . . . . . . . . .CL-P.14 SUNKontturi, Ville . . . . . . . . . . . . JSII-2.2 MONKonyashkin, Aleksey . . . . . �CE-P.21 TUE,
CE-P.23 TUEKonyushkin, Vasilii A. . . . . . CA-P.24 SUNKopczynski, Krzysztof . . . . . CA-P.15 SUNKoppens, Frank . . . . . . . . . . . JSIV-2.5 SUNKoppens, Frank H. L. . . . . . JSIV-2.2 SUNKopylov, Dmitrii . . . . . . . . . . CD-P.31 TUEKorchak, Vladimir N. . . . . . . CE-P.25 TUEKordts, Arne . . . . . . . . . . . . . . . CE-9.1 TUEKores, Cristine . . . . . . . . . . . . . CA-1.2 SUNKornienko, Vladimir . . . . . . �CC-P.19 SUNKorovin, Alexander . . . . . . . . EH-P.6 WEDKorpijärvi, Ville-Markus . . . CB-P.1 MON,
CA-5b.1 MON, CB-4.5 WED,�CB-11.4 THUKosareva, Olga . . . . . . . . . . . . . �EI-2.6 THUKoschorreck, Marco . . . . . . . . �EC-1.2 TUEKosen, Sandoko . . . . . . . . . . . . EC-2.2 TUEKoshino, Kazuki . . . . . . . . . . . EB-P.7 WEDKoshkinbayeva, Ainur . . . . . . �CH-3.5 SUNKositsyn, Roman . . . . . . . . . .CA-12.2 THUKoskinen, Kalle . . . . . . . . . �EH-P.11 WED,
CE-12.4 WEDKoster, Gertjan . . . . . . . . . . . CM-P.19 SUNKosters, Dolfine . . . . . . . . . . . EH-1.3 WEDKostin, Yuri . . . . . . . . . . . . . . . CB-7.5 WEDKotas, Dariusz . . . . . . . . . . . .CH-P.18 THUKotnala, Abhay . . . . . . . . . . . EG-7.1 MON,
CL-2.4 THUKotov, Leonid . . . . . . . . . . . . �CJ-8.5 WED,�CJ-P.48 WED
Köttig, Felix . . . . . . . . . . . . . �PD-A.7 WEDKotur, Marija CG-1.5 TUE, CG-5.1 WED,
CF-6.2 THUKoulouklidis, Anastasios D. �CC-P.8 SUNKouznetsov, Mikhail S. . . . . CE-P.25 TUEKovačev, Miltin . . . . . . . . . . . .CG-4.3 WEDKovacev, Milutin . . . . . . . . . CD-P.27 TUE,
CG-P.9 THUKovács, Katalin . . . . . . . . . . . . CG-1.4 TUEKovalev, Anton . . . . . . . . . . �CA-P.14 SUNKowa, Maya . . . . . . . . . . . . . . . CA-3.1 SUNKowalczuk, Laura . . . . . . . . . . CL-3.3 THUKowalczyk, Maciej . . . . . . . . . CF-P.5 WEDKowzan, Grzegorz . . . . . . . . .CH-7.2 WED,
CH-9.1 WEDKozhevnikov, Igor . . . . . . . . .CH-P.35 THUKozyreff, Gregory . . . . . . . . . . �JSI-1.3 SUNKrachmalnicoff, Valentina . . .EG-4.3 SUNKracht, Dietmar . . . . . . . . . . . CE-2.4 SUN,
CA-4.1 SUN, CJ-P.25 WED,CJ-P.42 WED
Krakowski, Michel . . . . . . . . �CB-5.2 WEDKrall, Michael . . . . . . . . . . . . . . CC-1.4 SUNKrämer, Ria G. . . . . . . . . . . CM-P.10 SUN,
CM-4.1 SUN, CJ-11.3 THUKränkel, Christian . . . . . . . . CJ-6a.1 MON,
CJ-6a.2 MON, CA-7.2 MON,CA-8.2 TUE, CA-8.3 TUE, CE-P.6 TUE,CE-P.22 TUE, CJ-P.41 WED,CA-12.1 THU
Kränkel, Cristian . . . . . . . . . . . CA-9.5 THUKrapick, Stephan . . . . . . . . . JSV-P.4 MONKrasavin, Alexey . . . . . . . . . . .EH-4.2 WEDKrasnokutska, Inna . . . . . . . . �EA-4.3 SUNKrauss, Nico . . . . . . . . . . . . . . . CC-P.5 SUNKrauss, Thomas . . . . . . . . . . . EG-4.2 SUN,
CD-P.5 TUE, CK-11.1 WEDKrauss, Thomas F. . . . . . . . . CK-1.1 SUN,
PD-B.6 WEDKrausz, Ferenc . . . . . . . . . . . . CA-P.1 SUN,
CA-P.12 SUN, CA-P.22 SUN,CA-P.34 SUN, CD-8.4 TUE,CF-1.3 TUE, CD-P.18 TUE,CG-1.3 TUE, CG-2.4 TUE, CJ-8.1 WED,CG-4.4 WED, CF-P.32 WED,PD-A.1 WED, CF-7.5 THU,CA-10.1 THU, CA-10.5 THU,CG-P.3 THU, CG-P.10 THU,CG-P.12 THU, CF-9.2 THU,CA-12.3 THU
Krauth, J. . . . . . . . . . . . . . . . . . CD-4.3 SUNKravets, Nina . . . . . . . . . . . . . CD-7.2 MONKrebs, Manuel . . . . . . . . . . . . .CG-2.5 TUE,
CJ-8.2 WED, CF-8.1 THUKremp, Tristan . . . . . . . . . . . . . CJ-4.6 SUNKresic, Ivor . . . . . . . . . . . . . . . . �EC-3.3 TUEKress, Florian . . . . . . . . . . . . . PD-B.1 WEDKretschmar, Martin . . . . . . . CG-4.3 WED,�CG-P.9 THUKrishnan, Ananth . . . . . . . . . .EH-P.4 WEDKroesen, Sebastian . . . . . . . . . CD-2.4 SUNKroetz, Peter . . . . . . . . . . . . . .�CA-4.2 SUNKrolikowski, Wieslaw . . . . .CD-5b.1 MON,
CL-2.5 THUKroon, David CG-1.5 TUE, CG-5.1 WED
Krstajic, Nikola . . . . . . . . . . . .CN-2.4 WEDKruchinin, Stanislav . . . . . . CF-P.32 WEDKrückel, Clemens . . . . . . . . . . CD-P.9 TUEKrüger, Michael . . . . . . . . . . . CG-4.4 WEDKruschke, Bastian . . . . . . . . CJ-P.17 WEDKruse, Kai . . . . . . . . . . . . . . . . . CA-3.5 SUNKruse, Regina . . . . . . . . . . . . �JSV-2.1 THUKryzhanovskaya, Natalia . . �CB-4.5 WEDKubeček, Václav . . . . . . . . . CA-P.30 SUN,
CA-P.37 SUN, CA-P.41 SUN,CA-4.3 SUN
Küber, Johannes . . . . . . . . . . . EC-P.8 TUEKübler, Harald . . . . . . . . . . . JSV-P.9 MONKucera, Stephan . . . . . . . . . . .EA-9.1 THU,
EA-9.2 THU, EA-9.3 THUKuchinskii, Vladimir I. . . . . CB-P.22 MONKudashova, Yulia . . . . . . . . . . CB-4.5 WEDKudlinski, Alexandre . . . . . . EE-P.10 SUN,
EE-P.12 SUN, EE-3.2 SUN,EF-5.5 MON, CD-8.3 TUE,CD-P.25 TUE
Kueppers, Franko . . . . . . . . . . . CI-P.6 TUEKuerbis, Christian . . . . . . . . CB-P.28 MONKues, Michael EA-6.5 TUE, EA-7.3 TUE,
PD-B.9 WED, CD-13.5 THUKuhlicke, Alexander . . . . . . . . CK-8.2 TUEKuhlmey, Boris . . . . . . . . . . . . EH-P.8 WEDKuhlmey, Boris T. . . . . . . . . EH-P.13 WEDKuhn, Aurelien CK-2.4 SUN, EA-4.4 SUNKuhn, Stefan . . . . . . . . . . . . . . . CJ-4.5 SUNKuipers, Kobus . . . . . . . . . . . . EG-4.1 SUN,
EG-4.2 SUN, EF-6.6 MON, CD-P.5 TUE,EH-1.3 WED
Kukharenko, Oleksii . . . . . . . . CC-P.5 SUNKukushkin, Vladimir . . . . . . .EF-P.13 THUKulagina, Marina . . . . . . . . . . CB-4.5 WEDKulakovskii, Vladimir . . . . . . . CB-1.1 TUEKuleshov, Nikolai . . . . . . . . CA-5a.1 MON,
CA-5a.2 MON, CA-8.5 TUEKuleshov, Nikolay . . . . . . . . CA-P.38 SUN,
CA-9.3 THUKumada, Takayuki . . . . . . . . . CF-8.3 THUKumagai, Akiko . . . . . . . . . . . . CL-4.6 THUKumar, Arunandan . . . . . . . . EG-P.8 MONKumar, Arununndan . . . . . .CK-P.15 MONKumar, S. Chaitanya . . . . . . . CD-4.1 SUNKumar, Shubham . . . . . . . . . �CB-P.4 MONKumar, Vikas . . . . . . . . . . . . CD-11.1 THU,
CD-13.2 THU, CL-4.2 THUKumarasinghe, Chathurangi�EG-5b.3 MONKundermann, Stefan . . . . �CF-P.12 WED,
CA-9.6 THU, CH-P.30 THUKung, A. H. . . . . . . . . . . . . . . . .CF-3.1 TUEkunwar, Puskal . . . . . . . . . . . �CM-P.5 SUNKuo, Hao-Chung . . . . . . . . . . CE-P.9 TUE,
CE-P.10 TUE, CK-14.3 THUKüpper, Jochen . . . . . . . . . . . CA-7.2 MONKüppers, Franko . . . . . . . . . . . CB-2.3 TUEKuretake, Satoshi . . . . . . . . . . CA-2.4 SUNKurilchik, Sergey . . . . . . . . . �CA-P.38 SUNKurkov, Andrei . . . . . . . . . . . . .CJ-7.4 WEDKurkov, Andrey . . . . . . . . . . .CJ-P.44 WEDKurt, Hamza . . . . . . . . . . . . . EH-P.16 WEDKurt, Metin . . . . . . . . . . . . . . .CE-P.11 TUE
Kurtsiefer, Christian . . . . . . . .EA-1.4 SUN,EC-P.5 TUE, EC-2.2 TUE, EA-6.2 TUE
Kurz, Heiko . . . . . . . . . . . . . . . . EE-P.1 SUNKurz, Heiko G. . . . . . . . . . . . �CG-4.3 WED,
CG-P.9 THUKurzynski, Pawel . . . . . . . . . . �EA-1.4 SUNKuse, Naoya �ED-1b.1 MON, TF-1.2 TUEKushmaro, Ariel . . . . . . . . . . . .CH-4.5 SUNKuszelewicz, Robert . . . . . . . . EF-8.1 TUEKutluer, Kutlu . . . . . . . . . . . �EA-5.4 MON,
EA-5.5 MONKuwata-Gonokami, Makoto . CC-6.3 TUEKuykens, Bart . . . . . . . . . . . . . . EF-7.3 TUEKuzel, Petr . . . . . . . . . . . . . . . .CC-5.1 MONKuzin, Evgene . . . . . . . . . . . . CD-P.26 TUEKuznetsov, Aleksey . . . . . . . CJ-P.24 WEDKuznetsov, Ivan . . . . . . . . . . .CA-P.33 SUNKuznetsov, Maxim . . . . . . . . CJ-10.4 WEDKwaśny, Michał . . . . . . . . . . . .�EF-8.4 TUEKwek, Leong Chuan . . . . . . . . EA-7.1 TUEKwon, Hyounghan . . . . . . . �CK-P.23 MONKwon, O-Pil . . CC-P.3 SUN, CC-3.6 SUNKwon, Soon-Hong . . . . . . . . CK-11.5 WEDKymakis, Emmanuel . . . . . . .CM-P.3 SUN,
CM-7.3 MONL. Vos, Willem . . . . . . . . . . . .CD-P.32 TUELa Rocca, Rosanna . . . . . . . . . CL-P.6 SUNLabat, Damien . . . . . . . . . . . . . .CJ-1.3 SUNLaberdesque, Romain . . . . . . �CK-1.2 SUNLabeye, Pierre . . . . . . . . . . . . . .CH-3.5 SUNLabeyrie, Guillaume . . . . . . . . EC-3.3 TUE,
EF-9.3 THULaburthe-Tolra, Bruno . . . . . . EC-1.3 TUELacava, Cosimo . . . . . . . . . . �CD-P.4 TUE,
CI-P.8 TUELacroix, Simon . . . . . . . . . . . . CH-9.3 WEDLadislav, Kuna . . . . . . . . . . . . . JSI-2.4 SUNLadugin, Maxim . . . . . . . . . . . CB-7.5 WEDLaegsgaard, Jesper . . . . . . . . . CH-5.4 TUELafargue, Clément . . . . . . . . . �CK-8.1 TUELaffaille, Pierre . . . . . . . . . . . . . CC-2.2 SUNLagarde, Delphine . . . . . . . . CE-11.4 WEDLagatsky, Alexander . . . . . . . . CB-3.5 TUELagendijk, Ad . . . . . . . . . . . CK-13.2 WED,
CL-4.5 THULagoudakis, Pavlos . . . . . . . . . EF-9.2 THULaguta, Oleksii . . . . . . . . . . �CE-P.14 TUE,�CE-P.15 TUELahini, Yoav . . . . . . . . . . . . . CK-4b.1 MONLai, Yi-Chun . . . . . . . . . . . . . . . CE-P.9 TUELai, Yinchieh . . . . . . . . . . . . . CF-P.11 WEDLaiho, Kaisa . . . . . . . . . . . . . . . EA-P.5 THULaing, Anthony . . . . . . . . . . �PD-B.3 WEDLalanne, Philippe . . . . . . . . . CK-11.1 WEDLaliotis, Athanasios . . . . . . . . �EG-4.4 SUNLalkens, Birka CL-P.18 SUN, EH-6.2 THULallier, Eric . . . CJ-1.4 SUN, CD-4.2 SUN,
CN-1.1 WEDLalouat, Loïc . . . . . . . . . . . . . �JSI-1.5 SUN,
CK-11.1 WEDLam, Ping Koy . . . . . . . . . . . . EB-P.2 WEDLambrecht, Astrid . . . . . . . . . EG-P.7 MONLamont, Michael R.E. . . . . . CH-8.6 WED,
PD-A.5 WEDLamrini, Samir . . . . . . . . . . . CB-P.7 MON,
�CJ-7.2 WEDLamy de la Chapelle, Marc . .CL-4.3 THULancaster, David . . . . . . . . . . �CJ-7.1 WEDLancaster, David G . . . . . . .�CJ-P.18 WEDLancis, Jesús �CL-P.17 SUN, CM-P.4 SUNLandsman, Alexandra . . . . . CG-5.3 WED,
CG-P.10 THULang, Ben . . . . . . . . . . . . . . . �EG-P.16 MONLangbein, Wolfgang . . . . . . . EG-6.6 MONLange, Robert . . . . . . . . . . . . CA-12.3 THULange, Sven . . . . . . . . . . . . . . . .CL-P.3 SUNLangner, Andreas . . . . . . . . . CA-P.21 SUNLangrock, Carsten . . . . . . . . . .CD-9.5 TUELanin, Aleksandr A. . . . . . . . . �CF-3.4 TUELanzani, Guglielmo . . . . . . . . . EE-P.7 SUNLapine, Mikhail . . . . . . . . . . . .EH-P.8 WEDLaplane, Cyril . . . . . . . . . . . . . .EA-2.4 SUN,�EA-P.31 THULaporta, Paolo . . . . . . . . . . . .ED-2.3 MON,
ED-2.6 MON, ED-1b.2 MON,ED-3.5 MON
Laptev, Alexander . . . . . . . . . . CJ-3.1 SUNLarat, Christian CJ-1.4 SUN, CD-4.2 SUNLarciprete, Maria Cristina . . .EH-5.2 THULarimian, Seyedreza . . . . . . . �EE-P.8 SUN,�EE-4.3 SUN, CG-6.5 WED,
CG-6.6 WEDLarin, Sergey . . . . . . . . . . . . . CA-12.2 THULarsen, Esben . . . . . . . . . . . . . CG-5.1 WEDLarssen, Esben W. . . . . . . . . . .CG-1.5 TUELarsson, Anders . . . . . . . . . . . . CB-2.4 TUELaruelle, François . . . . . . . . CB-P.33 MONLassonde, Philippe . . . . . . . . .CD-7.4 MONLászló, Forró . . . . . . . . . . . . . CK-14.5 THULatmiral, Ludovico . . . . . . . . JSV-3.4 THULatour, Gaël . CL-P.12 SUN, CL-3.3 THULaude, Vincent . . . . . . . . . . . . .CD-1.3 SUNLaudyn, Urszula . . . . . . . . . . . . EF-8.4 TUELAURAT, Julien . . . . . . . . . . . EA-1.1 SUN,
EB/EG.3 TUELaurell, Fredrik . . . . . . . . . . .CD-P.41 TUE,
CE-P.32 TUE, CE-9.2 TUE,CJ-P.15 WED, CL-4.1 THU,CJ-14.5 THU
Laurent, Arnoldi . . . . . . . . . . CM-7.6 MONLaurent, Philippe . . . . . . . . . . CH-9.2 WEDLausecker, Elisabeth . . . . . . . CK-P.5 MONLausten, Rune . . . . . . . . . . . . EA-10.1 THULaux, Sébastien . . . . . . . . . . . .CA-3.2 SUN,
CF-P.19 WED, CF-P.20 WEDLaverdant, Julien . . . . . . . . .CK-P.25 MONLavery, Domanic . . . . . . . . . . . . CI-3.2 SUNLavrinenko, Andrei V. . . . . CK-P.40 MONLawrence, Jon . . . . . . . . . . . . CM-P.7 SUN,
CH-7.4 WEDLawrence, Mark . . . . . . . . . . . EH-1.5 WEDLazaro, Jose A. . . . . . . . . . . �JSIV-2.4 SUNLazaro, Jose Antonio . . . . . . . . CI-2.4 SUNLazoul, Mohamed . . . . . . . . CK-P.27 MONLe, Anh Thu . . . . . . . . . . . . . . CG-3.4 WEDLe Bris, Arthur . . . . . . . . . . . CK-14.6 THULe Coarer, Etienne . . . . . . . . . CK-7.5 TUELe Gac, Gaëlle . . . . . . . . . . . �CE-11.4 WEDLe Goëc, Jean-Pierre . . . . . . .CB-5.2 WEDLe Gouët, Julien . . . . . . . . . . .CJ-12.5 THU
215
Authors’ Index
LE JEANNIC, Hanna . . . . . . . EA-1.1 SUNLe, Quang Trung . . . . . . . . . . . .CI-P.6 TUELe Roux, Xavier . . . . . . . . . . CD-P.34 TUELe, Son . . . . . . . . . . . . . . . . . . . . . CI-3.2 SUNLe Targat, Rudolphe . . . . . . .ED-P.9 MONLeach, Jonathan . . . . . . . . . . .CN-2.4 WEDLeahu, Grigore . . . . . . . . . . . .�CN-P.1 TUE,
CK-13.5 WEDLeake, Gerard . . . . . . . . . . . . CK-12.2 WEDLebedev, Vladimir . . . . . . . . . . .EI-2.2 THULebental, Melanie . . . . . . . . CK-12.3 WEDleblanc, adrien . . . . . . . . . . . . .�CG-2.6 TUELebreton, Armand . . . . . . . . .�CC-1.3 SUN,�CK-4a.2 MONLebugle, Maxim . . . . . . . . . . . JSV-4.6 THULebugle, Maxime . . . . . . . . CM-5b.2 MON,
EA-P.9 THU, JSV-3.3 THU,JSV-3.5 THU
Lecaplain, Caroline . . . . . . .ED-1a.2 MON,CE-9.1 TUE, �CB-10.6 THU
Lechuga, Laura M. . . . . . . .JSII-1a.2 MONLecomte, André . . . . . . . . . . .CJ-P.49 WEDLecomte, Steve . . . . . . . . . . CF-P.12 WED,
CA-9.6 THU, CH-P.30 THULecourt, Jean-Bernard . . . . . . CJ-2.2 SUNLeder, Norbert . . . . . . . . . . . . . CC-2.4 SUNLederer, Max . . . . . . . . . . . . . . .CA-3.5 SUNLederman, David . . . . . . . . . . . CC-4.1 SUNLedingham, Patrick M. . . . . .EA-5.5 MONLee, Andrew �CA-6.3 MON, CA-7.4 MONLee, Byoungho . . . . . . . . . . . CK-P.23 MONLee, Chao-Kuei . . . . . . . . . . �CA-P.16 SUN,�CA-P.19 SUNLee, Chien-Chung . . . . . . . .ED-1b.1 MON,
CH-9.1 WEDLee, Chris . . . . . . . . . . . . . . . . .CK-5.4 MONLee, Dongyeul . . . . . . . . . . . .CK-P.26 MONLee, Hansuek . . . . . . . . . . . . ED-1a.1 MONLee, Ka-Lun . . . . . . . . . . . . . . CH-P.19 THULee, Kevin . . . . . . . . . . . . . . . . . TF-1.2 TUELee, Kevin F. CH-7.2 WED, CH-9.1 WEDLee, Kwanil . . . . . . . . . . . . . . . .CF-4.5 WEDLee, Po-Tsung . . . . . . . . . . . . . CE-P.9 TUELee, S-H . . . . . . . . . . . . . . . . . . . CC-3.6 SUNLee, Sang Bae . . . . . . . . . . . . . CF-4.5 WEDLee, Seong Ku . . . . . . . . . . . JSIII-1.1 MONLee, Seung Heon . . . . . . . . . . . CC-P.3 SUNLee, Seungwoo . . . . . . . . . . . . . CK-3.5 SUNLee, Stephen . . . . . . . . . . . . . . CN-2.1 WEDLee, Timothy . . . . . . . . . . . . CD-5a.3 MONLee, Yong-Hee . . . . . . . . . . . . . CK-3.5 SUNLeemans, Wim . . . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONLégaré, François . . . . . . . . . . . EE-3.3 SUN,
CD-7.4 MON, CG-6.2 WEDLeger, James R. . . . . . . . . . . . �SH-4.1 SUNLéger, Yoan . . . . . . . . . . . . . . . EG-P.5 MONLegratiet, Luc . . . . . . . . . . . . . .CK-7.4 TUELehoucq, Gaelle . . . . . . . . . . . CK-3.4 SUN,
CD-6.2 MONLei, Bing . . . . . . . . . . . . . . . . . .�CJ-9.1 WEDLeidinger, Markus . . . . . . . . . .�CE-9.4 TUELeijssen, Rick . . . . . . . . . . . .�CK-10.5 WEDLein, Manfred CG-1.2 TUE, CG-4.3 WEDLeiner, Claude . . . . . . . . . . . . . EI-3a.1 THU
Leino, Iiro . . . . . . . . . . . . . . . .CA-5b.1 MONLeinonen, Tomi . . . . . . . . . . . CB-P.1 MON,
CB-3.1 TUE, CB-5.1 WEDLeinse, Arne CK-5.4 MON, CJ-12.2 THULeite, Ana B. . . . . . . . . . . . . . EF-P.23 THULeite, Ivo . . . . . . . . . . . . . . . . . .CC-5.4 MONLeite, Ivo T. . . . . . . . . . . . . . . .CC-5.5 MONLeitenstorfer, Alfred . . . . . . EE-5a.1 MON,
EE-5a.2 MON, ED-P.7 MON,EG-P.14 MON, CF-1.1 TUE,CF-4.4 WED, EH-5.5 THU, EH-7.3 THU
Lelarge, François . . . . . . . . . . . CI-2.5 SUN,CB-10.5 THU
Lelii, Francesca . . . . . . . . . . . . CL-1.3 WEDLelit, Marcin . . . . . . . . . . . . . . CH-6.3 WEDLemaître, Aristide . . . . . . .JSV-P.10 MON,
CD-8.6 TUE, CD-P.20 TUE,CD-10.6 TUE
Lemarchand, Fabien . . . . . . CK-11.3 WEDLemell, Christoph . . . . . . . . . . EE-P.8 SUN,
CG-5.5 WEDLemke, Norbert . . . . . . . . . . . CJ-12.3 THULempel, Alexa . . . . . . . . . . . . . EH-6.5 THULeng, Jinyong CI-P.9 TUE, CJ-11.5 THULenhard, Andreas . . . . . . . . . . EA-6.6 TUE,�EA-9.1 THU, EA-9.2 THULenzner, Matthias . . . . . . . .�CH-P.13 THULeo, François .ED-P.2 MON, EF-7.3 TUELeo, Giuseppe . . . . . . . . . . JSV-P.10 MON,
CD-P.20 TUE, CD-10.6 TUE,JSV-2.4 THU
Leon-Montiel, Roberto . . . . EA-P.14 THULeonardon, Jeremie . . . . . . . . .CC-2.2 SUNLeonetti, Marco . . . . . . . . . . . �CD-3.3 SUNLeong, Philip . . . . . . . . . . . . . PD-B.4 WEDLeong, Victor . . . . . . . . . . . . . . EC-2.2 TUELeoni, Roberto EA-6.4 TUE, EH-4.6 WEDLepage, Guy . . . . . . . . . . . . . . . . CJ-1.4 SUNLerch, Stefan . . . . . . . . . . . . . . �EA-7.2 TUELerin, Adolfo . . . . . . . . . . . . . JSIV-2.4 SUNLermer, Matthias . . . . . . . . . . .CB-1.1 TUELesparre, Fabien . . . . . . . . . . . CA-9.2 THULethiec, Clotilde . . . . . . . . . CK-P.25 MON,
EH-P.2 WEDLeuchs, Gerd EA-1.2 SUN, �SH-5.1 SUN,
EB-2a.3 MON, EA-7.4 TUE,EB-3.1 WED, PD-B.2 WED,CH-P.23 THU, EA-P.1 THU,EA-P.3 THU, EA-P.4 THU,EA-P.11 THU, EI-3a.3 THU
Levchenko, Andrey . . . . . . . . . .CJ-3.1 SUNLevenson, Ariel . . . . . . . . . . . . . EF-2.4 SUNLeveque, Thomas . . . . . . . . . .CH-9.2 WEDLewandowski, Jarosław . . . . CH-6.3 WEDLewenstein, Maciej . . . . . . . .CG-P.10 THULewty, Nick . . . . . . . . . . . . . . . . EC-P.5 TUELeyman, Ross . . . . . . . . . . . . . CC-5.4 MONLeymann, Heinrich A. M. . .�CB-4.2 WEDLeymarie, Joël . . . . . . . . . . . .CE-11.4 WEDLhermite, Jérôme . . . . . . . . . �CJ-9.3 WEDL’Huillier, Anne . . . . . . . . . . . .CG-1.5 TUE,
CG-5.1 WED, CF-6.2 THU,CG-P.6 THU, CF-8.2 THU
Li, Borui . . . . . . . . . . . . . . . . . . . �CI-2.3 SUNLi, Chunyong . . . . . . . . . . . . . .CN-2.4 WED
Li, Gaoxing . . . . . . . . . . . . . . . . EA-9.5 THULi, Guanhai . . . . . . . . . . . . . . EG-5a.3 MONLi, Jensen . . . . . . . . . . . . . . . . . EH-1.5 WEDLi, Jie-Ru . . . . . . . . . . . . . . . . . CE-P.10 TUELi, Jin . . . . . �CD-P.13 TUE, �EF-8.2 TUELi, Junshuai . . . . . . . . . . . . . . CE-5a.3 MONLi, Lei . . . . . . . . . . . . . . . . . . . . . CJ-7.5 WEDLi, Lianhe . . . CC-1.3 SUN, JSV-2.5 THULi, Luozhou . . . . . . . . . . . . . . . JSV-4.4 THULi, Ming . . . . . . . . . . . . . . . . . . . . CI-4.1 SUNLi, Peng . . . . . . . . . . . . . . . . . . . CF-1.6 TUELi, Qing . . . . . . . . . . . . . . . . . .CF-P.22 WEDLi, Ran . . . . . . . . . . . . . . . . . . . �CA-7.4 MONLi, Sensen . . . . . . . . . . . . . . . �CA-P.13 SUNLi Voti, Roberto . . . . . . . . . . . CN-P.1 TUE,
CK-13.5 WED, EH-5.2 THULi, Wenxue . CJ-P.6 WED, CJ-P.46 WEDLi, Xin . . . . . . . . . . . . . . . . . . . CE-11.4 WEDLi, Xiuling . . . . . . . . . . . . . . . . . CE-P.9 TUELi, Yahua . . . . . . . . . . . . . . . . .CJ-P.18 WEDLi, Yan . . . . . . . . . . . . . . . . . . .CH-P.28 THULi, Ying . . . . . . . . . . . . . . . . . . . .EA-7.1 TUELi, YingYi . . . . . . . . . . . . . . . . . CA-P.5 SUNLi, Yuelong . . . . . . . . . . . . . . . . JSI-1.4 SUNLi, Zhibo . . . . . . . . . . . . . . . . . .�CK-8.5 TUELi, Zhihong . . . . . . . . . . . . . . . CJ-12.1 THULiang, Dawei . . . . . . . . . . . . . CE-P.26 TUE,
CA-11.6 THULiang, Qijun . . . . . . . . . . . . . . .�CC-P.5 SUNLiaros, Nikos . . . . . . . . . . . . . . CE-P.33 TUELiebermeister, Lars . . . . . . . . EG-P.2 MONLiebertz, Josef . . . . . . . . . . . . CD-10.3 TUELieger, Roland . . . . . . . . . . . . .EB-P.4 WEDLiem, Andreas . . . . . . . . . . . . .�CJ-4.5 SUN,
CJ-8.2 WED, CJ-P.17 WED,CJ-10.3 WED, CJ-11.3 THU,CJ-11.4 THU
Lien, Yu-Hung . . . . . . . . . . . .CE-12.5 WEDLienau, Christoph . . . . . . . . . EG-P.6 MON,
EG-7.6 MON, CK-6.2 MONLiero, Armin . . . . . . . . . . . . . CB-P.19 MONLiesner, Thomas . . . . . . . . . .CF-P.24 WEDLiew, Tim . . . . . . . . . . . . . . . . . .EF-9.2 THULifschitz, Agustin . . . . . . . . JSIII-1.1 MONLihachev, Grigoriy . . . . . . . . . ED-P.8 MONLikhachev, Mikhail . . . . . . . . . CJ-3.1 SUN,
CJ-8.5 WED, �CJ-P.13 WED,CJ-P.48 WED
Lilienfein, Nikolai . . . . . . . . . CA-P.12 SUN,CG-P.12 THU, �CF-9.2 THU
Lim, Christina . . . . . . . . . . . . CH-P.19 THULim, Yah Leng . . . . . . . . . . . . CH-8.1 WEDLimpert, Jens CJ-1.2 SUN, CJ-5.5 MON,
CG-2.5 TUE, CG-3.1 WED,CJ-8.1 WED, CJ-8.2 WED,�CJ-8.3 WED, CJ-10.1 WED,CJ-10.2 WED, CG-P.12 THU,CJ-13.1 THU, CJ-13.4 THU,CJ-13.5 THU, CF-8.1 THU, CF-9.2 THU
Lin, Bin-Cheng . . . . . . . . . . . . . CE-P.9 TUELin, Chien-Chung . . . . . . . . . . CE-P.9 TUE,
CE-P.10 TUELin, Chii Dong . . . . . . . . . . . . .CG-3.4 WEDLin, Ching-Fuh . . . . . . . . . . . �CE-6.1 MONLin, Da-Wei . . . . . . . . . . . . . . CK-14.3 THU
Lin, Di . . . . CA-7.5 MON, �CJ-P.10 WEDLin, Fan-Yi . . . . . . . . . . . . . . . . CB-8.6 THULin, Guoping . . . . . . . . . . . . . �CD-10.1 TUELin, Jipeng . CA-1.1 SUN, EH-P.12 WEDLin, N . . . . . . . . . . . . . . . . . . . . . CF-8.5 THULinares-Vallejo, Erick . . . . . . .EB-4.2 WEDLindberg, Robert . . . . . . . . . �CJ-P.15 WEDLindemann, Markus . . . . . . . �CB-2.1 TUE,
CB-2.2 TUELindgren, Gustav . . . . . . . . . . CE-P.32 TUELindinger, Albrecht . . . . . . . CG-P.16 THULindroth, Eva . . . . . . . . . . . . . CG-5.1 WEDLinfield, Edmund . . . . . . . . . . CC-1.3 SUN,
CC-5.6 MON, JSV-2.5 THULingnau, Benjamin . . . . . . . . . CB-9.3 THULink, Sandro M. . . . . . . . . . . .CF-4.1 WED,�CH-8.3 WEDLipatiev, Aleksey . . . . . . . . . . CM-6.3 MONLipatov, Denis . . . . . . . . . . . . .CJ-8.5 WED,
CJ-P.13 WED, CJ-P.48 WEDLipiński, Stanisław . . . . . . . . CE-P.28 TUELipovskii, Andrey . . . . . . . . . CB-4.5 WED,
EH-P.11 WEDLipsanen, Harri . . . . . . . . . . EG-P.11 MON,
CD-P.7 TUELipson, Michal . . . . . . . . . . . . CH-8.6 WED,
PD-A.5 WED, JSV-4.4 THULisak, Daniel . . . . . . . . . . . . . . CH-7.2 WEDLiscidini, Marco . . . . . . . . . . . EB-1.2 MON,
EG-P.4 MON, JSV-P.3 MON,EA-7.6 TUE
Lisdat, Christian . . . . . . . . . . .ED-P.9 MONLisinetskii, Victor . . . . . . . . . .CE-P.17 TUELisitsky, Igor S. . . . . . . . . . . . CE-P.25 TUELita, Adriana . . . . . . . . . . . . . .JSV-1.5 THULita, Adriana E. . . . . . . . . . .JSV-P.7 MON,
EA-6.3 TUELittle, Brent . CD-P.13 TUE, EF-8.2 TUELittle, Brent E. . . . . . . . . . . . . EA-6.5 TUE,
EA-7.3 TUE, PD-B.9 WEDLittle, Douglas CE-P.2 TUE, CH-P.7 THULittlejohns, Callum G. . . . . . . CK-7.2 TUELiu, Changxu EG-4.2 SUN, �CD-P.5 TUE,�EH-7.2 THULiu, Chen . . . . . . . . . . . . . . . . . CJ-13.6 THULiu, Fu . . . . . . . . . . . . . . . . . . . .EH-1.5 WEDLiu, Hangyu . . . . . . . . . . . . . . . .CA-1.3 SUNLiu, Huiyun .CK-10.2 WED, CB-9.2 THULiu, Jiang . . . . . . . . . . . . . . . . �CJ-13.6 THULIU, Jianli . . . . . . . . . . . . . . . . . EA-1.1 SUNLiu, Lai . . . . . . . . . . . . . . . . . . .CE-P.12 TUELiu, Meng . . . . . . . . . . . . . . . . JSIV-1.4 SUNLiu, Peter Q. . . . . . . . . . . . . . �PD-B.8 WEDLiu, Qingcao . . . . . . . . . . . . . EG-5b.1 MONLiu, Quan . . . . . . . . . . . . . . . . . . JSI-2.5 SUNLiu, Shuang . . . . . . . . . . . . . . . . .CI-2.3 SUNLiu, Wei . . . . .CJ-9.1 WED, CJ-11.5 THULiu, Xing . . . .EE-P.11 SUN, �EF-3.6 SUNLiu, Yang . . . ED-P.3 MON, CJ-P.6 WED,
CJ-P.46 WEDLiu, Yu . . . . . . . . . . . . . . . . . . .�CL-P.14 SUNLiu, Yuh-Shiuan . . . . . . . . . . .PD-A.2 WEDLiu, Zhaohong . . . . . . . . . . . . CA-P.13 SUNLiu, Zheng . . . . . . . . . . . . . . . . . EF-P.2 THULiu, Zhenyu . . . . . . . . . . . . . . .PD-B.4 WED
Liu, Zhicheng . . . . . . . . . . . . . CB-4.1 WEDLivshits, Daniil A. . . . . . . . . .CD-P.28 TUELobach, Ivan . . . . . . . . . . . . �CJ-P.16 WED,
CJ-P.28 WEDLobintsov, Andrei . . . . . . . . . .CB-7.5 WEDLocatelli, Andrea . . . . . . . . . . .EH-7.4 THULocatelli, Massimiliano . . . . . .CC-4.5 SUNLodahl, Peter . . . . . . . . . . . . . PD-B.7 WEDLodewyck, Jèrôme . . . . . . . . .ED-P.9 MONLoeser, Markus . . . . . . . . . . . CA-P.21 SUN,�CA-9.4 THULöffler, Wolfgang . . . . . . . . . EB-P.13 WEDLoghmari, Zayneb . . . . . . . . EF-4a.3 MONLoiko, Pavel CA-P.31 SUN, CA-4.5 SUN,
CA-5a.1 MON, �CA-5a.2 MON,�CA-5b.3 MON, �CA-8.5 TUE,CE-P.5 TUE, �CE-P.13 TUE
Loiko, Pavel A. . . . . . . . . . . . CE-P.25 TUELoiko, Yurii . . . . . . . . . . . . . . . �CA-P.7 SUNLoiko, Yury . . . EC-P.8 TUE, CL-2.5 THULoir, Anne-Sophie . . . . . . .CM/LIM.2 TUELoiseau, Pascal . . . . . . . . . . . �CE-7.4 MONLojewska, Joanna . . . . . . . . . . CC-P.6 SUNLombard, Laurent . . . . . . . . . . CJ-1.3 SUN,
CJ-12.5 THULombardo, Antonio . . . . . . .JSIV-1.2 SUN,
EE-5a.2 MONLombosi, Csaba . . . . . . . . . . . .CC-3.1 SUN,
CC-3.5 SUNLong, Shengya . . . . . . . . . . . . . . CI-2.3 SUNLongdell, Jevon . . . . . . . . . . . .EA-5.2 MONLonghi, Stefano . . . . . . . . . . . . EF-7.4 TUE,
EB-5.1 WEDLonnqvist, Jan . . . . . . . . . . . .CH-P.11 THULopez, John . . . . . . . . . . . . . CM-P.21 SUN,
CM-5a.1 MONLópez-López, Rafael . . . . . . CM-P.11 SUNLópez-Luke, Tzarara . . . . . . . . CL-P.4 SUNLopez-Martens, Rodrigo . . . . CG-2.2 TUELopez, Olivier . . . . . . . . . . . . ED-3.3 MON,
CH-P.33 THULoranger, Sébastien . . . . . . . . CJ-9.6 WEDLoschenov, Victor . . . . . . . . . . CL-P.3 SUNLoscher, André . . . . . . . . . . . . .CA-9.2 THULotarev, Sergey . . . . . . . . . . . CM-6.3 MONLoterie, Damien . . . . . . . . . . . �CL-5.3 THULötscher, Lauryna . . . . . . . . .CD-P.18 TUELötstedt, Erik EE-4.3 SUN, CG-6.5 WEDLoudon, Rodney . . . . . . . . . . . .EF-9.1 THULouis, Hélène . . . . . . . . . . . . . .�EF-P.9 THULouisy, Maité . . . . . . . . . . . . . . CG-1.5 TUELouvergneaux, Eric . . . . . . . . EF-P.5 THU,
EF-P.9 THULove, Adrian . . . . . . . . . . . . . . .CJ-5.1 MONLove, John D. . . . . . . . . . . . . . . .CI-1.5 SUNLöw, Robert . . . . . . . . . . . . . �JSV-P.9 MONLowndes, David . . . . . . . . . . . �EB-4.2 WEDLoza-Alvarez, Pablo . . . . . . . . CL-P.7 SUNLozes-Dupuy, Françoise . . .CK-P.31 MONLu, Chao . . . . . . . . . . . . . . . . . . CE-6.3 MONLu, Chih-Hsuan . . . . . . . . . . . . �CF-3.1 TUELu, Guo-Wei . . . . . . . . . . . . . . �CI-P.11 TUELü, Haibin . . . . . . . . . . . . . . . . . . CI-P.9 TUELu, Ming . . . . . . . . . . . . . . . . . JSV-4.4 THULu, Tien-Chang . . . . . . . . . . .CE-12.2 WED
216
Authors’ Index
Lu, Wei . . . . . . . . . . . . . . . . . . EG-5a.3 MONLu, Yongfeng . . . . . . . . . . . . . . �TF-2.3 TUELu, Zehuang . . . . . . . . . . . . . �ED-P.3 MONLu, Zhiwei . . . . . . . . . . . . . . . . CA-P.13 SUNLubeigt, Walter . . . . . . . . . . . CA-7.4 MONLuc, Legratiet . . . . . . . . . . . . . . CB-1.3 TUELucas, Erwan . . . . . . . . . . . . ED-1a.2 MON,
CB-10.6 THULucas-Leclin, Gaëlle . . . . . . . �CB-5.3 WEDLucchini, Matteo . . . . . . . . . .CG-4.1 WED,
CG-4.5 WED, �CG-5.3 WEDLucero, Adrian . . . . . . . . . . . CF-P.23 WEDLucianetti, Antonio . . . . . . . . CA-P.6 SUN,
CA-P.31 SUNLücking, Fabian . . . . . . . . . . . CJ-8.1 WED,
CA-10.3 THU, CG-P.12 THULudbrook, Bart . . . . . . . . . . . .EE-P.17 SUNLudewig, Peter . . . . . . . . . . . CE-11.6 WEDLudewigt, Klaus . . . . . . . . . . CJ-10.3 WEDLüdge, Kathy .CB-9.3 THU, CB-9.5 THULudin, Wsevolod V . . . . . . . CE-11.2 WEDLudlow, Andrew . . . . . . . . . . . ED-2.5 MONLudwig, André . . . . . . . . . . . . �EE-4.2 SUN,
CG-4.5 WED, CG-5.3 WEDLugli, Paolo . . . . . . . . . . . . . . . . CC-1.2 SUNLuke, Kevin .CH-8.6 WED, PD-A.5 WEDLumer, Yaakov . . . . . . . . . . . JSIV-P.1 TUE,
CK-13.1 WEDLummen, Tom T.A. . . . . . . . �EH-2.3 WEDLundin, Wsevolod . . . . . . . . CE-11.3 WEDLundquist, Ted . . . . . . . . . . . CD-11.4 THULunin, Vladimir . . . . . . . . . . . CA-11.3 THULuo, Ai-Ping . . . . . . . . . . . . . .JSIV-1.4 SUNLuo, Cheng-Jhih . . . . . . . . . .CF-P.11 WEDLuo, Daping . . . . . . . . . . . . . . . CJ-P.6 WEDLuo, Kai-Hong . . . . . . . . . . . JSV-P.1 MON,
JSV-P.4 MONLuo, Kathy . . . EF-1.1 SUN, EE-3.4 SUN,
EE-3.5 SUN, EF-P.18 THU,CD-13.1 THU
Luo, Weijie . . . . . . . . . . . . . . . . �CE-3.5 SUNLuo, Zhi-Chao . . . . . . . . . . . �JSIV-1.4 SUNLupi, Jean-François . . . . . . . �CE-P.31 TUELupi, Stefano . . . . . . . . . . . . . EE-P.17 SUNLureau, François . . . . . . . . . . . CA-3.2 SUN,
CF-P.19 WED, �CF-P.20 WEDLuther-Davies, Barry . . . . . . .CD-1.5 SUN,
CH-3.2 SUNLuvsandamdin, Erdenetsetseg
CB-P.28 MONLuxmoore, Isaac J. . . . . . . . . PD-B.8 WEDLwin, Richard . . . . . . . . . . . . EH-P.13 WEDLyngsø, Jens Kristian . . . . . . .CH-5.4 TUEM. García-Blanco, Sonia . . CJ-6a.3 MONM. Lechuga, Laura . . . . . . . . JSII-P.1 TUEM. Pask, Helen . . . . . . . . . . . . CA-P.9 SUNM. Rasel, Ernst . . . . . . . . . . . ED-P.9 MONM Tino, Guglielmo . . . . . . . . ED-P.9 MONMa, Guo-Hong . . . . . . . . . . . . �CC-4.2 SUNMa, Pan . . . . . . . . . . . . . . . . . . . CH-3.2 SUNMa, Shaojie . . . . . . . . . . . . . . . . CE-3.5 SUNMaaßdorf, Andre . . . . . . . . . .CB-P.5 MON,
CD-P.40 TUE, CB-5.4 WED,CB-11.5 THU
Mac Suibhne, Naoise . . . . . . . . CI-1.3 SUN
Macchiavello, Chiara . . . . . . .EB-P.9 WEDMacDonald, Kevin F. . . . . . . EG-2.3 SUN,
EG-5a.3 MON, CK-6.5 MON,CD-8.5 TUE, CH-7.3 WED,EH-3.5 WED
Macedo, Zélia . . . . . . . . . . . . . CH-P.9 THUMacGregor, Calum . . . . . . . . CK-14.2 THUMacias-Romero, Carlos . . . . . CL-3.5 THUMackenzie, Jacob . . . . . . . . . CE-7.2 MON,
CE-P.3 TUE, CE-P.34 TUE, CJ-P.3 WEDMacLean, Jean-Philippe . . �EA-10.1 THUMaclot, Sylvain . . . . . . . . . . . . CG-P.6 THUMaddaloni, Pasquale . . . . . . .CD-8.2 TUE,
CH-P.36 THUMadden, Steve . . . . . . . . . . . . CD-1.5 SUN,�CH-3.2 SUN, CE-7.1 MON,�CJ-P.2 WEDMader, Matthias . . . . . . . . . . �CH-1.2 SUN,
CK-P.42 MONMaeda, Yasuhiro . . . . . . . . . . �CL-4.4 THUMaestre, Haroldo . . . . . . . . . . CD-6.4 MONMaestroni, Valerio . . . . . . . . . . CE-9.2 TUEMafi, Arash . . . . . . . . . . . . . . . . CD-3.3 SUNMagden, Emir Salih . . . . . . CK-12.2 WEDMaglione, Mario . . . . . . . . . . . CC-5.1 MONMagno, Giovanni . . . . . . . . �CK-P.31 MONMagoulakis, Evangelos . . . . . ED-2.4 MONMahendra, Andri . . . . . . . . . . PD-B.4 WEDMahler, Dylan . . . . . . . . . . . . . EB-1.2 MONMaidment, Luke . . . . . . . . . . . CN-2.1 WEDMaier, Christine . . . . . . . . . . .PD-B.1 WEDMaigyte, Lina . . . . . . . . . . . . . CK-1.4 SUN,
CK-P.10 MONMailis, Sakellaris . . . . . . . . . . �CE-4.2 SUN,
CM-6.6 MONMaillart, Emmanuel . . . . . . . . CL-4.3 THUMaillotte, Herve . . . . . . . . . . . CD-1.3 SUN,
CD-P.25 TUEMainz, Roland . . . . . . . . . . . . . CG-P.4 THUMairesse, Yann . . . . . . . . . . . CG-6.1 WED,
CG-6.2 WEDMaisons, Grégory . . . . . . . . . . CB-6.3 WEDMaissen, Curdin . . . . . . . . . . . EH-4.6 WEDMaitre, Agnès . . . . . . . . . . . . . EG-4.3 SUN,�CK-P.25 MON, �EH-P.2 WEDMaiuri, Margherita . . . . . . . . .EG-7.6 MONMaiwald, Martin . . . . . . . . . . CB-P.6 MON,
CB-11.2 THUMajedi, Hamed . . . . . . . . . . . EA-8.2 WED,
EA-P.7 THUMajor, Arkady . . . . . . . . . . . . �CF-P.2 WEDMajor, Balázs . . . . . . . . . . . . . . CG-1.4 TUEMajor, Kyle . . . . . . . . . . . . . . CE-12.5 WEDMajor, Zsuzsanna . . . . . . . . . .CA-P.1 SUN,
CA-10.1 THU, CA-12.3 THUMajus, Donatas . . . . . . . . . . CM-5a.3 MONMak, Ka Fai .EE-1.1 SUN, CG-P.11 THUMakara, Mariusz . . . . . . . . . . . . CI-1.4 SUNMäkelä, Jaakko . . . . . . . . . . . .CB-5.1 WEDMakino, Kenzo . . . . . . . . . . . . �EA-1.5 SUNMakino, Shuntaro . . . . . . . . �CK-P.7 MONMäkitalo, Jouni . . . . . . . . . . . . CD-P.7 TUEMakles, Kevin EA-4.3 SUN, �CH-5.3 TUEMakris, Konstantinos . . . . �EH-P.15 WEDMaksimenka, Raman . . . . . . . CF-2.4 TUE,
CF-3.5 TUEMalekizandi, Mohammadreza�CI-P.6 TUEMalerba, Mario . . . . . . . . . . EG-P.10 MON,
EH-5.6 THUMalevich, Pavel . . . . . . . . . . . .CD-4.5 SUN,
CF-2.1 TUE, CF-2.4 TUE, CF-3.5 TUEMalinauskas, Mangirdas . . .�CM-1.2 SUN,�CM-1.5 SUN, CM-P.13 SUN,
CK-P.10 MON, CH-P.21 THUMalinowski, Marina . . . . . . . CM-7.5 MONMalka, Victor . . . . . . . . . . . . JSIII-1.1 MONMalmström, Mikael . . . . . . .CJ-P.15 WED,�CL-4.1 THU, CJ-14.5 THUMaluckov, Aleksandra . . . . . . CH-P.8 THUMalyarevich, Alexander . . . . . CE-P.5 TUEMammez, Dominique . . . . . �CD-P.36 TUEManceau, Mathieu . . . . . . . . . EA-P.4 THUMandon, Julien . . . . . . . . . . . . CH-4.3 SUN,
CF-1.5 TUE, CB-6.5 WEDMangold, Mario . . . . . . . . . . �CF-4.1 WED,
CH-8.3 WED, CF-9.3 THUMannella, Riccardo . . . . . . . .PD-B.5 WEDMannelli, Ilaria . . . . . . . . . . . . �CL-P.2 SUNManninen, Aki . . .CLEO/ECBO-1.3 WEDManninen, Albert . . . . . . . . . . �CH-3.3 SUNMans, Torsten . . . . . . . . . . . . . .CA-3.5 SUNManschwetus, B . . . . . . . . . . . CF-8.5 THUManschwetus, Bastian . . . . . .CG-P.6 THUMånsson, Erik . . . . . . . . . . . . . CG-5.1 WEDMantel, Klaus . . . . . . . . . . . . . .EA-P.1 THUMantilla-Perez, Paola . . . . . . . JSI-2.5 SUNMantl, Siegfried . . . . . . . . . . . . CB-1.4 TUEMantsyzov, Boris . . . . . . . . .�CD-P.31 TUEManzoni, Cristian . . . . . . . . JSIV-1.3 SUN,
JSIV-1.5 SUN, CF-6.1 THU,CG-P.4 THU
Mao, Hann-Shin . . . . . . . . . JSIII-1.4 MONMaple, Lewis . . . . . . . . . . . . �EH-P.14 WEDMaragkou, Maria . . . . . . . . . . . EG-3.4 SUNMaram, Reza . . . . . . . . . . . . . . . CI-4.1 SUNMarandi, Alireza . . . . . . . . . . .�CD-9.5 TUEMarangoni, Marco . . . . . . . . . CH-2.5 SUN,
ED-2.3 MON, ED-3.5 MON,CD-11.1 THU, CD-13.2 THU,CL-4.2 THU
Marangos, Jon . . . . . . . . . . . . . CG-1.2 TUEMarangos, Jon P. . . . . . . . . . . CG-3.3 WEDMarceau, Vincent . . . . . . . . . CG-P.19 THUMarchenko, Denys . . . . . . . . . CH-4.3 SUN,
CB-6.5 WEDMarchetti, Riccardo . . . . . . . CD-P.4 TUE,�CI-P.8 TUEMarchiori, Chiara . . . . . . . . . . CD-P.1 TUEMarconi, Lorenzo . . . . . . . . . . . EA-4.5 SUNMarconi, Mathias . . . . . . . . . . EF-1.2 SUN,
CB-2.5 TUE, �CD-13.4 THUMarcus, Gilad . . . . . . . . . . . . . . CG-1.3 TUEMaréchal, Etienne . . . . . . . . . . EC-1.3 TUEMareev, Evgeniy . . . . . . . . . . . EE-P.2 SUN,
CF-P.13 WEDMargulis, Walter . . . . . . . . . . CD-6.3 MONMariani, Silvia . . . . . . . . . . . . CD-10.6 TUEMariano, Marina . . . . . . . . . . . JSI-1.3 SUNMarie, Didier . . . . . . . . . . . . . �CL-P.10 SUN
Marin, Esteban . . . . . . . . . . . . �CK-9.3 TUEMarin, Francesco . . . . . . . . . . �EA-4.5 SUNMarini, Andrea . . . . . . . . . . .�CL-P.15 SUN,
JSIV-1.5 SUN, �EF-7.4 TUE,CD-12.3 THU
Marino, Francesco . . . . . . . . . EF-2.1 SUN,EA-4.5 SUN
Mario, Tonin . . . . . . . . . . . . . �CK-14.5 THUMariscal, Antonio . . . . . . . . . .CE-6.2 MONMarkham, Matthew . . . . . . . . CE-4.4 SUNMarkham, Matthew L. . . . . .JSV-4.4 THUMarkos, Christos . . . . . . . . CK-P.39 MON,
CH-P.25 THUMarkovic, Vesna . . . . . . . . . . �CA-9.1 THUMarks, Robert S. . . . . . . . . . . . CH-4.5 SUNMarkus, Karahka . . . . . . . . . .CM-7.6 MONMarmalyuk, Alexander . . . . . CB-7.5 WEDMarpaung, David . . . . . . . . . . CK-5.5 MONMarquardt, Christoph . . . . . . EA-1.2 SUN,
EB-3.1 WED, PD-B.2 WED,EA-P.11 THU, EI-3a.3 THU
Marquez, D. T. . . . . . . . . . . . . CM-P.1 SUNMarquez, Daniela . . . . . . . . . . CM-P.2 SUNMarris-Morini, Delphine . . . JSV-4.2 THUMarrucci, Lorenzo . . . . . . . . . . EA-7.1 TUEMarsal, Lluís . . . . . . . . . . . . . . . JSI-1.2 SUNMarsal, Nicolas . . . . . . . . . . . . EF-6.1 MONMarshall, Graham D. . . . . . . .EA-6.1 TUE,
PD-B.3 WEDMarshall, Kenneth . . . . . . . . CD-11.4 THUMarsili, Francesco . . . . . . . .CK-4a.2 MON,
EB-1.5 MONMarsili, Margherita . . . . . . . .JSIV-1.5 SUNMartens, Daan . . . . . . . . . . . . . CL-P.8 SUNMartial, Igor . . . . . . . . . . . . . . . CA-9.2 THUMartin, Anthony . . . . . . . . . . .EB-1.4 MONMartin, Aude . . . . . . . . . . . . . �CD-6.2 MONMartin-Cano, Diego . . . . . . �EA-10.5 THUMartin Ciurana, Ferran . . . . . EA-2.3 SUN,
EC-1.4 TUEMartin, Fernando . . . . . . . . . . EE-1.4 SUN,
CG-5.2 WED, CG-5.4 WED,CG-6.3 WED, CG-P.13 THU,�CG-P.17 THU
Martin, Guillermo . . . . . . . . . �CK-7.5 TUEMartín-López, Enrique . . . . . EA-6.1 TUE,
PD-B.3 WEDMartin, Vicente . . . . . . . . . . . .EB-4.4 WEDMartinache, Franz . . . . . . . . . CH-7.4 WEDMartinenghi, Romain . . . . . . CD-10.1 TUEMartinez, Anthony . . . . . . . . . .CI-2.5 SUN,
CB-10.5 THUMartínez Calderón, Miguel .CE-P.27 TUEMartínez-Fernández, Lara . CG-P.13 THUMartinez-Jimenez, Gregorio . CE-4.2 SUNMartinez-Llinas, Jade . . . . CB-P.27 MON,�EF-P.28 THUMartínez-Lorente, Rubén . . �EF-1.6 SUN,�EF-8.6 TUEMartinez-Mateo, Jesus . . . . . EB-4.4 WEDMartinez-Otero, Alberto . . . . JSI-2.5 SUNMartinez, Pedro . . . . . . . . . . . CL-1.2 WEDMartínez Saavedra, José Ramón�EH-2.4 WEDMartinez Vazquez, Rebeca CL-P.11 SUN,
CM-P.9 SUN, JSII-1a.1 MON,CL-1.3 WED
Martini, Carla . . . . . . . . . . . . . .CM-2.5 SUNMartins, Renato Juliano . . .CM-P.14 SUNMárton, István . . . . . . . . . . . . . CC-3.1 SUNMartorell, Jordi JSI-1.3 SUN, JSI-2.5 SUNMaruyama, Momoko . . . . . . . .CC-6.4 TUEMarzahl, Daniel-Timo . . . . . �CA-8.2 TUE,
CA-8.3 TUEMasaki, Yuta . . . . . . . . . . . . . �CK-6.1 MONMasala, Silvia . . . . . . . . . . . . . . EH-7.2 THUMasella, Guido . . . . . . . . . . . . PD-B.5 WEDMaser, Andreas . . . . . . . . . . . . �EG-3.1 SUNMashanovich, Goran . . . . . . . . CE-4.3 SUNMashanovich, Goran Z. . . . CM-7.4 MON,
CK-7.2 TUEMashiko, Yutaka . . . . . . . . . . CA-12.1 THUMashkovich, Eugene . . . . . . �CC-6.1 TUE,
CC-6.2 TUEMasini, Luca . . . . . . . . . . . . . . CB-6.4 WEDMaslov, Alexey . . . . . . . . . . . �CK-P.4 MONMaslowski, Piotr . . . . . . . . . �CH-7.2 WED,
CH-9.1 WEDMasoller, Cristina . . . . . . . . �EF-4a.2 MONMason, Paul . . . . . . . . . . . . . . . CA-3.6 SUNMassar, Serge . . . . . . . . . . . . . . CI-5.1 MONMassonnet, Didier . . . . . . . . . CH-9.2 WEDMasuda, Masaya . . . . . . . . . . CJ-P.47 WEDMatalla, Mathias . . . . . . . . . .CB-11.5 THUMataloni, Paolo . . . . . . . . . . . CM-4.4 SUN,
EB-P.9 WED, EB-5.1 WED,EB-5.2 WED, JSV-2.2 THU,JSV-3.4 THU
Mateman, Richard . . . . . . . . .CK-5.4 MONMateo, Cherry May . . . . . . �CB-P.16 MONMateos, Xavier . . . . . . . . . . . CA-P.31 SUN,
CA-4.4 SUN, CA-4.5 SUN,�CA-5a.1 MON, CA-5a.2 MON,CA-5b.3 MON, CE-P.13 TUE
Mathieson, Robert . . . . . . . . CM-7.5 MONMatia-Hernando, Paloma . . .CG-1.2 TUE,
CG-3.3 WEDMatras, Guillaume . . . . . . . . CF-P.20 WEDMatrosov, Vladimir . . . . . . . . .CA-9.3 THUMatsubara, Eiichi . . . . . . . . .�CC-P.15 SUNMatsuda, Nathan . . . . . . . . . . . . . . . . . . . . JS
SPIE/OM/EQEC.3 MONMatsuda, Nobuyuki . . . . . . . PD-B.3 WEDMatsui, Tatsuya . . . . . . . . . . . . CE-8.4 TUEMatsumoto, Morio . . . . . . . . CJ-P.45 WEDMatsuo, Shinji . . . . . . . . . . . . .�CK-3.3 SUNMatthew, Mary . . . . . . . . . . �CF-P.24 WEDMatthew, White . . . . . . . . . . . .JSI-2.4 SUNMatthews, Jonathan C. F. . PD-B.3 WEDMatthews, Mary . . . . . . . . . .CD-P.33 TUE,�CG-P.16 THUMattioli, Francesco . . . . . . . . . EA-6.4 TUEMatzdorf, Christian . . . . . . . . .CJ-4.5 SUN,
CJ-P.17 WEDMauclair, Cyril . . . . . . . . . . . . �CM-2.4 SUNMaulini, Richard . . . . . . . . . . . CB-7.3 WEDMaurer, Jochen . . . . . . . . . . . . .EE-4.2 SUNMaurer, Raffael EE-P.8 SUN, EE-4.3 SUNMaurin, Isabelle . . . . . . . . . . . . EG-4.4 SUNMauritsson, Johan . . . . . . . . . CG-5.1 WED
217
Authors’ Index
Mauritsson, Johann . . . . . . . . CG-1.5 TUEMaury, Axel . . . . . . . . . . . . . . �EG-P.7 MONMavrona, Elena . . . . . . . . . . �CC-P.17 SUNMaweza, Loyiso . . . . . . . . . . �CA-12.6 THUMaxein, Dominik . . . . . . . . . EB/EG.3 TUEMaximov, Mikhail . . . . . . . . . CB-4.5 WEDMaximov, Mikhail V. . . . . . CB-P.22 MONMayer, Aline . . . . . . . . . . . . . . . CD-2.5 SUNMayer, Aline S. . . . . . . . . . . �CH-8.6 WED,
PD-A.5 WEDMayer, Benedikt W. . . . . . . . .EE-4.2 SUN,�CF-2.3 TUEMazhorova, Anna . . . . . . . . . . CC-6.5 TUEMazurenka, Mikhail . . . . . . . . �CL-3.1 THUMazzamuto, Giacomo . . . . �JSIV-2.5 SUNMazzera, Margherita . . . . . . EA-5.4 MON,�EA-5.5 MONMazzucchi, Gabriel . . . . . . . . �EC-P.7 TUEMback, Christian Blaise Landry
EI-P.3 TUE, EI-P.5 TUEMcBryde, Duncan . . . . . . . . . CC-P.13 SUNMcCarthy, Eoin . . . . . . . . . . . . EH-6.6 THUMcCarthy, Mary . . . . . . . . . . . . .CI-1.3 SUNMcClelland, David . . . . . . . . . CH-P.3 THUMcCloskey, David . . . . . . . . . �EH-6.6 THUMcConnell, Gail . . . . . . . . . . . CA-1.1 SUN,
CL-3.4 THUMcCracken, Richard . . . . . . . PD-A.6 WEDMcCracken, Richard A. . . . . ED-P.6 MONMcCutcheon, William . . . . �JSV-P.8 MONMcDaniel, Clare . . . . . . . . . . . �CM-2.3 SUNMcDonald, Graham S. . . . . . . EI-P.4 TUE,
EI-P.7 TUE, EF-P.23 THUMcGregor, Scot . . . . . . . . . . . CH-9.3 WEDMcKay, Aaron . . . . . . . . . . . . �CA-1.5 SUN,�CA-1.6 SUNMcKnight, Loyd . . . . . . . . . . . �CB-3.5 TUEMcMillan, Alex . . . . . . . . . . . JSV-P.8 MONMcPolin, Cillian . . . . . . . . . . .�EH-4.2 WEDMéchin, David . . . . . . . . . . . . .CN-1.5 WEDMecking, Stefan . . . . . . . . . .EG-P.14 MONMedisauskas, Lukas . . . . . . . . CG-5.4 WEDMedvedkov, Oleg . . . . . . . . . CJ-P.13 WEDMégret, Partice . . . . . . . . . . . . . CJ-2.2 SUNMégret, Patrice . . . . . . . . . . . CJ-P.28 WEDMegy, Robert . . . . . . . . . . . . . . CK-8.3 TUEMehta, Karan . . . . . . . . . . . . . PD-A.2 WEDMeier, Torsten . . . . . . . . . . . . . EF-6.4 MONMeinhardt-Wollweber, Merve CL-3.1 THUMeint, Smit . . . . . . . . . . . . . . . CB-8.2 THUMeisenheimer, Sarah-Katharina�CD-4.4 SUNMeissner, Karl . . . . . . . . . . . . . .CL-P.2 SUNMeissner, Peter . . . . . . . . . . CB-P.11 MONMejia-Cortes, Cristian . . . . EH-P.17 WEDMekhov, Igor . . . . . . . . . . . . . . .EC-P.7 TUEMelanen, Petri . . . . . . . . . . . . CB-5.3 WEDMelati, Daniele . . . . . . . . . . .CK-P.33 MONMélen, Gwenaelle . . . . . . . . . �EB-4.1 WEDMelkonian, Jean-Michel . . . . CD-2.3 SUN,
CD-P.36 TUE, CN-1.1 WEDMelloni, Andrea . . . . . . . . . CK-P.11 MON,
CK-P.33 MON, CK-13.3 WED,EH-7.5 THU
Melzer, Jeffrey . . . . . . . . . . . . CC-P.14 SUN
Ménard, Jean-Michel . . . . . . �EF-6.5 MONMendonca, Cleber . . . . . . . �CE-P.16 TUE,
CE-9.5 TUEMendonça, Cleber R. . . . . . . CE-6.3 MON,
CE-9.6 TUEMendonça, Cleber Renato .CM-P.14 SUNMendoza, Gabriel J. . . . . . . . �EA-6.1 TUEMendoza-Yero, Omel . . . . . .CL-P.17 SUN,
CM-P.4 SUNMeneghetti, Alessio . . . . . . . EA-P.32 THUMenezo, Sylvie . . . . . . . . . . . . . .CI-P.8 TUEMeng, Hsin-Fei . . . . . . . . . . . . .CE-P.9 TUEMeng, PeiBei . . . . . . . . . . . . �CA-P.17 SUNMennea, Paolo L. . . . . . . . . . . CE-2.3 SUN,
JSV-P.6 MON, �JSV-P.7 MON,CE-10.5 WED, JSV-1.3 THU
Menzel, Ralf . . . . . . . . . . . . . . .�EA-3.4 SUNMenzel, Susanne . . . . . . . . . . CB-P.2 MONMerceron, Loïc . . . . . . . . . . . . CG-6.1 WEDMercier, Brigitte . . . . . . . . . . . CG-2.2 TUEMercier De Lépinay, Laure . .EG-1.5 SUN,�CK-2.4 SUNMerckling, Clement . . . . . . . CB-11.3 THUMeredith, Win . . . . . . . . . . . .CE-11.3 WEDMerghem, Kamel . . . . . . . . . . . CI-2.5 SUN,�CB-10.5 THUMergo, Pawel . . CE-1.6 SUN, CI-1.4 SUNMeriggi, Laura . . . . . . . . . . . �CK-14.2 THUMerimaa, Mikko . . . . . . . . . . . .CH-3.3 SUNMerino, David . . . . . . . . . . . . . �CL-P.7 SUNMerlone, Andrea . . . . . . . . . . ED-2.6 MONMero, Mark . �CF-4.3 WED, CF-9.4 THUMesaritakis, Charis . . . . . . �CB-P.23 MONMessaddeq, Younès . . . . . . . CJ-P.34 WEDMessaoudene, Sonia . . . . . . . . .CI-P.8 TUEMessina, Gabriele C. . . . . . . . . CL-P.6 SUNMessner, Leon . . . . . . . . . . . . . EA-8.3 WEDMestre, Valdeci . . . . . . . . . . CK-P.19 MONMetcalf, Ben . . . . . . . . . . . . . . JSV-3.1 THUMetcalf, Benjamin . . . . . . . . JSV-P.6 MONMetcalf, Benjamin J. . . . . . JSV-P.7 MON,
EA-6.3 TUE, �JSV-1.3 THUMetz, Philip Werner . . . . . . . CA-8.2 TUE,�CA-8.3 TUEMetzendorf, Simon . . . . . . . �CA-12.5 THUMetzger, Klaus . . . . . . . . . . . CM-7.5 MONMetzger, Thomas . . . . . . . . . .CA-P.1 SUN,
CF-1.3 TUE, CG-2.1 TUE,CA-10.1 THU, CA-12.3 THU
Mével, Eric . . . . . . . . . . . . . . . .CG-6.1 WEDMexis, Meletios . . . . . . . . . . . .CB-4.3 WEDMhibik, Oussama . . . . . . . . .CA-P.27 SUN,
CE-8.2 TUEMi, Junping . . . . . . . . . . . . . . CB-10.3 THUMichael, Stephan . . . . . . . . �CB-P.29 MONMichailovas, Andrejus . . . . .CA-P.26 SUN,
CF-P.15 WED, CA-11.2 THUMichailovas, Kirilas . . . . . . .�CA-11.2 THUMichalska, Maria . . . . . . . . . . CF-P.8 WEDMichalzik, Rainer . . . . . . . . CB-P.14 MON,
CB-2.1 TUE, CB-2.2 TUE, CB-2.6 TUEMichaud-Belleau, Vincent . . CJ-7.1 WEDMichel, Knut CG-2.1 TUE, CA-10.1 THUMichieletto, Mattia . . . . . . . . .CH-5.4 TUEMichiels, Luc . . . . . . . . . . . . . . . CL-P.8 SUN
Michler, Peter . . . . . . . . . . . CB-P.16 MON,CB-P.18 MON, CB-3.4 TUE
Micklethwaite, Stuart . . . . . CM-6.5 MONMidolo, Leonardo . . . . . . . . . JSV-2.5 THUMidorikawa, Katsumi . . . CM/LIM.3 TUE,
CG-6.4 WED, CG-6.5 WED,CG-P.18 THU, CL-4.6 THU
Mierzejewski, Maciej . . . . . . EE-P.17 SUNMigal, Ekaterina . . . . . . . . . .CF-P.13 WEDMíguez, Hernán . . . . . . . . . . . JSI-1.4 SUN,
JSI-2.2 SUN, CK-P.24 MON,EG-P.9 MON
Miguez, Maria . . . . . . . . . . .CD-5b.2 MON,�CD-P.15 TUEMikhaël, Myara . . . . . . . . . .CB-P.32 MON,
CB-1.3 TUEMikhailov, Sergey A. . . . . . . PD-B.8 WEDMiki, Shigehito . . . . . . . . . . .EA-P.25 THU,
EA-P.28 THU, JSV-4.1 THU,JSV-4.5 THU
Mikkelsen, Maiken H. . . . . . . EH-4.1 WEDMikutis, Mindaugas . . . . . . . CE-P.35 TUEMilanese, Daniel . . . . . . . . . . CE-P.24 TUEMilanović, Vitomir . . . . . . . . EF-P.10 THUMilburn, Gerard J. . . . . . . . . EA-P.19 THUMilchberg, Howard . . . . . . . . . �EE-2.1 SUNMildren, Richard . . . . . . . . . . .CA-1.5 SUN,
CA-1.6 SUNMilian, Carles .EE-2.4 SUN, EE-P.4 SUN,�EF-3.4 SUN, CM-5a.3 MON,
CD-7.4 MON, �CD-P.3 TUEMiller, Aaron J. . . . . . . . . . . . .EB-1.5 MONMiller, Luke . . . . . . . . . . . . . . . . EC-1.2 TUEMiller, R.J. Dwayne . . . . . . . . CA-4.2 SUN,�CF-7.3 THUMillot, Guy EF-4b.2 MON, �CH-7.1 WEDMills, Benjamin . . . . . . . . . . CM-P.17 SUN,
CM-7.4 MONMills, Shaun . . . . . . . . . . . . . . . EH-6.6 THUMilman, Perola . . . . . . . . . . . JSV-2.4 THUMin, Bumki . . . . . . . . . . . . . . . . CK-3.5 SUNMinaeva, Olga . . . . . . . . . . . EB-P.11 WEDMinamide, Hiroaki . . . . . . . . . .CC-P.7 SUNMinardi, Stefano . . . . . . . . . �CM-3.1 SUN,�CM-5a.3 MON, �CD-P.2 TUEMinassian, Ara . . . . . . . . . . . . CA-P.2 SUN,
CA-6.4 MONMincuzzi, Girolamo . . . . . . . . . TF-2.1 TUEMink, Jan . . . . . . . . . . . . . . . . . .CH-4.3 SUNMinkov, Momchil . . . . . . . �CK-P.36 MON,�CK-P.37 MONMinkovich, Vladimir . . . . . . . . CH-5.2 TUEMinot, Christophe . . . . . . . . . . CK-7.4 TUEMinowa, Yosuke . . . . . . . . . . CE-11.5 WEDMinzioni, Paolo . . . . . . . . . . .CL-P.11 SUN,
JSII-1a.1 MON, CD-6.6 MON,CD-P.4 TUE, CI-P.8 TUE,CLEO/ECBO-2.2 WED, CL-1.3 WED
Miranda, Miguel . . . . . . . . . . . CG-1.5 TUE,CF-P.31 WED, �CF-6.2 THU,CG-P.6 THU, CG-P.7 THU
Mirasso, Claudio R. . . . . . . . EF-P.11 THUMiri, Mohammad-Ali . . . . . . . .CI-1.2 SUN,
EF-2.3 SUN, CE-3.1 SUN, CD-3.4 SUN,CB-4.4 WED
Mirin, Richard P. . . . . . . . . . . EB-1.5 MONMirnaziry, Sayyed Reza . . . �EF-P.24 THUMironov, Evgeniy . . . . . . . . . . CE-7.6 MONMiroshnichenko, Andrey . . . . EH-5.1 THUMiroshnichenko, Andrey E. . EH-7.1 THUMisawa, Kazuhiko . . . . . . . . CD-11.3 THUMishchik, Konstantin . . . . �CM-P.21 SUN,�CM-5a.1 MONMisiti, Maria . . . . . . . . . . . . . . . CC-P.6 SUNMisoguti, Lino . . . . . . . . . . . . . EE-P.5 SUN,�CD-5b.2 MON, CD-P.15 TUE,
CE-9.5 TUEMissori, Mauro . . . . . . . . . . . . �CC-P.6 SUNMitchell, Arnan . . . . . . . . . . CM-6.6 MON,
EH-P.12 WEDMitchell, Brandon . . . . . . . .CE-5b.2 MON,
CE-P.19 TUEMitchell, Colin J. . . . . . . . . . . .CK-7.2 TUEMitchell, Morgan W. . . . . . . . EA-2.3 SUN,
EC-1.4 TUE, JSV-4.3 THUMitrofanov, Oleg . . . . . . . . . CC-P.14 SUN,�CC-5.1 MON, �CC-5.6 MONMitschke, Fedor . . . . . . . . . . CF-P.29 WEDMittelberger, Daniel . . . . . . JSIII-1.4 MONMittleman, Daniel M. . . . . . . �SH-9.1 SUNMiura, Kenta . . . . . . . . . . . . . . �CE-P.4 TUEMiura, Kiyotaka . . . . . . . . . . .CM-6.1 MONMiura, Taisuke . . . . . . . . . . . . CA-P.30 SUNMivelle, Mathieu . . . . . . . . . . �EG-4.6 SUN,�EH-6.1 THUMiyabe, Shungo . . . . . . . . . . . CG-6.4 WEDMiyake, Yoshihiko . . . . . . . . . . CC-P.7 SUNMiyamoto, Katsuhiko . . . . . .CM-3.4 SUN,
CA-3.1 SUN, CA-7.6 MONMiyanaga, Noriaki . . . . . . . . CJ-P.47 WEDMiyawaki, Atsushi . . . . . . . . . . CL-4.6 THUMizeikis, Vygantas . . . . . . . . CM-1.2 SUN,
CM-P.13 SUNMlynczak, Jaroslaw . . . . . . . �CA-P.15 SUNMocek, Tomas . . . . . . . . . . . . CA-P.6 SUN,
CA-P.30 SUN, CA-P.31 SUNModi, Kavan . . . . . . . . . . . . . . EB-1.1 MONModsching, Norbert . . . . . . . CJ-10.1 WEDMohamed. Seghir, Seghilani�CB-P.32 MON, �CB-1.3 TUEMohamed, Sellahi . . . . . . . . . . CB-1.3 TUEMohr, Christian . . . . . . . . . .ED-1b.1 MON,
TF-1.2 TUE, CH-9.1 WEDMohr, Till . CB-P.13 MON, �CC-6.6 TUEMöhrle, Martin . . . . . . . . . . . . .CK-7.1 TUEMoiseev, Eduard . . . . . . . . . . .CB-4.5 WEDMoison, Jean-Marie . . . . . . . . CK-7.4 TUEMokhov, Sergiy . . . . . . . . . . . �CH-P.4 THUMokrousova, Daria V. . . . . . . CN-P.4 TUEMolenaar, Robert . . . . . . . . . . .CL-2.1 THUMølgaard Pedersen, Jens Kristian�CH-P.25 THUMolin, Stéphanie . . . . . . . . . CH-P.12 THUMolina, Mario I. . . . . . . . . . . EH-P.17 WEDMolina, Pablo . . . . . . . . . . . . . EH-P.9 WEDMolina-Terriza, Gabriel . . . . . EA-1.6 SUN,
CL-2.2 THU, EA-10.6 THUMolinari, Elisa . . . . . . . . . . . . . EG-7.6 MONMolitor, Andreas . . . . . . . . �CB-P.13 MON,
EA-P.17 THU
Møller Israelsen, Stine . . . . . . .CJ-2.5 SUNMoloney, Jerome V. . . . . . . . �EE-2.2 SUN,�SH-6.1 SUNMolter, Daniel . . . . . . . . . . . . .CC-5.2 MONMompart, Jordi . . . . . . . . . . . .CA-P.7 SUN,
EC-P.8 TUE, CL-2.5 THUmonchoce, sylvain . . . . . . . . . . CG-2.6 TUEMoncorgé, Richard . . . . . . . . . CE-1.2 SUNMondello, Chiara . . . . . . . . . CL-P.11 SUN,
JSII-1a.1 MON, CL-1.3 WEDMondes, Valerie . . . . . . . . . . EG-5b.1 MONMondragón, Rosa . . . . . . . . . . CM-P.4 SUNMongin, Denis . . . . . . . . . . . �CD-P.14 TUEMonmayrant, Antoine . . . . . .CK-1.2 SUN,
CB-P.17 MON, CK-P.31 MON,CK-11.3 WED, �CH-9.3 WED
Monnier, Paul . . . . . . . . . . . . . . EF-2.4 SUNMonoszlai, Balazs . . . . . . . . . . CC-3.6 SUNMonro, Tanya CH-4.1 SUN, CH-5.6 TUE,
CL-5.4 THUMonro, Tanya M . . . . . . . . . .CJ-P.18 WEDMonteiro, Fernando . . . . . . . �EB-1.4 MONMontes Bajo, Miguel . . . . . . �JSI-2.5 SUNMonzón-Hernández, David . CH-6.2 WEDMoocarme, Matthew . . . . . . . EH-6.5 THUMoodie, Dave . . . . . . . . . . . . . CC-5.6 MONMoore, Merritt . . . . . . . . . . . . JSV-1.3 THUMoparthi, Satish B. . . . . . . . .EG-7.3 MONMoqanaki, Amir . . . . . . . . . . . EB-5.4 WEDMorais, Natália . . . . . . . . . . �CD-P.20 TUE,�CD-10.6 TUEMorales Delgado, Edgar Emilio�CL-5.5 THUMorales, Felipe . . . . . . . . . . . CG-4.2 WED,�CG-5.4 WED, CG-P.13 THUMorand, Alain . . . . . . . . . . . . . CK-7.5 TUEMorandi, Vittorio . . . . . . . . . CE-5a.1 MONMorandotti, Roberto . . . . . . . CC-P.6 SUN,
EE-3.3 SUN, CD-5a.2 MON,CD-7.4 MON, CC-6.5 TUE,CD-P.13 TUE, EA-6.5 TUE,EF-8.2 TUE, EA-7.3 TUE,PD-B.9 WED, CD-13.5 THU
Morante, Joan Ramon . . . . CE-5a.2 MONMoreau, Julien . . . . . . . . . . . . . CL-4.3 THUMoreno-Hernández, Carlos �CH-6.2 WEDMoretti, Luigi . . . . . . . . . . . . �ED-2.6 MONMorgenweg, Jonas . . . . . . . . . .CA-3.5 SUNMorgner, Uwe . . . . . . . . . . . . . EE-2.5 SUN,
EE-P.14 SUN, EF-3.3 SUN, CA-4.1 SUN,CK-P.22 MON, EE-5b.2 MON,CD-P.27 TUE, CG-4.3 WED,CG-P.9 THU
Morichetti, Francesco . . . . CK-P.11 MON,�CK-P.33 MON, �CK-13.3 WEDMorier-Genoud, François . . . .CD-9.4 TUEMorimoto, Shohei . . . . . . . . . EE-P.15 SUNMorimoto, Tomohide . . . . . . CC-P.15 SUNMORIN, Olivier . . . . . . . . . . . �EA-1.1 SUN,
EB/EG.3 TUEMorin, Philippe . . . . . . . . . . . . . CI-4.2 SUN,
EF-4b.2 MONMorioka, Toshio . . . . . . . . . . . CI-P.10 TUEMorita, Ryuji EE-P.9 SUN, EE-P.15 SUN,
CM-3.4 SUN, CF-P.28 WED
218
Authors’ Index
Mork, Jesper CK-3.2 SUN, EG-6.5 MON,CB-P.35 MON, CK-P.9 MON,�CB-10.1 THU
Morlanes, Tomás . . . . . . . . . . CE-P.27 TUEMorohashi, Isao . . . . . . . . . . �CF-P.10 WEDMorrison, Blair . . . . . . . . . . . �CK-5.5 MONMorrissey, Padraic . . . . . . . . CB-P.30 MONMorsch, Oliver . . . . . . . . . . . �PD-B.5 WEDMortensen, N. Asger . . . . . . . . . . . . . . . . �JS
SPIE/OM/EQEC.2 MONMosca Conte, Adriiano . . . . . CC-P.6 SUNMosca, Simona . . . . . . . . . . . . CD-8.2 TUE,
CH-P.36 THUMoser, Christophe . . . . . . . . . CL-5.3 THU,
CL-5.5 THUMoshammer, Robert . . . . . . CG-3.4 WED,
CG-5.5 WEDMosk, Allard EB-4.6 WED, CK-13.2 WEDMosk, Allard P. EA-3.2 SUN, CL-4.5 THUMoskalenko, Valentina . . . .�CB-10.2 THUMoss, Daniel . . . . . . . . . . . . . . . EE-3.3 SUNMoss, David J . . . . . . . . . . . CD-P.13 TUE,
EA-6.5 TUE, EF-8.2 TUE, EA-7.3 TUE,PD-B.9 WED
Mota, Alessandro . . . . . . . . . . �CL-P.1 SUNMottay, Eric . . . . . . . . . . . . . . . �TF-1.3 TUEMou, Chengbo . . . . . . . . . . . . CF-P.6 WEDMoubissi, Alain Brice . . . . . . . . EI-P.5 TUEMoudakir, Tarik . . . . . . . . . . CE-11.4 WEDMounaix, Patrick . . . . . . . . . . CC-5.1 MONMouradian, Sara . . . . . . . . . . JSV-4.4 THUMoutrie, Michael . . . . . . . . . . CH-9.5 WEDMower, Jacob . . . . . . . . . . . . CK-4b.1 MONMoya-Cessa, Hector . . . . . . . . EA-P.9 THUMücke, Oliver D. . . . . . . . . . . CG-P.4 THUMueckstein, Raimund . . . . . . CC-5.6 MONMuellen, Klaus . . . . . . . . . . . .JSIV-1.3 SUNMueller, Philipp . . . . . . . . . . . . EA-9.3 THUMühlenbernd, Holger . . . . . CK-P.16 MONMuhr, Alexander . . . . . . . . . .CE-10.2 WEDMukhin, Ivan . . . . . . . . . . . . . CA-P.33 SUNMuldarisnur, Mulda . . . . . . CK-P.16 MONMüller, André . . . . . . . . . . . . CB-P.6 MON,
CB-11.2 THUMuller, Harm Geert . . . . . . . . CG-4.2 WEDMüller, Michael . . . . . . . . . . . . CJ-1.2 SUN,
CJ-13.4 THUMüller, Philipp EA-9.1 THU, EA-9.2 THUMüller, Timo . . . . . . . . . . . . . . ED-3.4 MONMunns, Jack . . . . . . . . . . . . . . . EA-6.1 TUEMurari, Krishna . . . . . . . . . . . . CA-4.2 SUNMurata, Hiroshi . . . . . . . . . . . . CI-5.6 MONMurayama, Koji . . . . . . . . . . . . CA-2.4 SUNMurdoch, Stuart . . . . . . . . . . �EE-3.4 SUN,�EF-P.18 THUMurdoch, Stuart G. . . . . . . . . EF-1.1 SUN,
EE-3.5 SUN, CD-13.1 THUMurib, Mohammed Sharif . . �CL-P.8 SUNMuroi, Tetsuhiko . . . . . . . . . . . �CI-3.5 SUNMurooka, Yoshie . . . . . . . . . . .EH-2.3 WEDMurr, Karim . . . . . . . . . . . . . . EA-10.5 THUMurray, Matthew . . . . . . . . . . CE-1.3 SUN,�CM-6.5 MONMurray, Robert . . . . . . . . . . . . .CD-1.4 SUNMurtagh, Michelle . . . . . . . . . �CA-1.1 SUN
Murzina, Tatiana . . . . . . . . . CD-P.31 TUEMuschet, Alexander . . . . . . . . CG-1.3 TUEMusgrave, Ian . . . . . . . . . . . CF-P.25 WED,
CG-P.1 THUMusha, Mitsuru . . . . . . . . . . . CJ-14.4 THUMusolino, Stefan . . . . . . . . . . . CL-5.4 THUMussler, Gregor . . . . . . . . . . . .CC-2.6 SUN,
CB-1.4 TUEMussot, A. . . . . . . . . . . . . . . . �EF-P.17 THUMussot, Arnaud . . . . . . . . . . EE-P.10 SUN,
EE-P.12 SUN, CJ-3.3 SUN, EE-3.2 SUN,EF-5.5 MON, CD-8.3 TUE
Mužík, Jiří . . . . . . . . . . . . . . . �CA-P.30 SUNMysyrowicz, André . . . . . . . . .EE-P.4 SUN,
CD-3.5 SUN, CD-P.3 TUE, CF-8.2 THUN. Christodoulides, Demetrios
EA-P.9 THUNabekawa, Yasuo . . . . . . . . . CG-6.4 WED,�CG-P.18 THUNadgaran, Hamid . . . . . . . . . . JSI-2.3 SUNNafa, Malik . . . . . . . . . . . . . . .CA-P.27 SUNNagai, Masaya . . . . . . . . . . . . CC-P.15 SUNNagasaka, Kenshiro . . . . . . . CJ-P.43 WEDNagashima, Keisuke . . . . . . . . CC-6.4 TUENagele, Stefan . . . . . . . . . . . . . EE-P.8 SUNNagy, Benedek J. . . . . . . . . . CA-P.35 SUNNagy, Tamas . . . . . . . . . . . . EE-5b.2 MON,�CD-P.27 TUE, CG-4.3 WED,
CG-P.9 THUNagymihaly, Roland S. . . . . �CF-P.7 WEDNähle, Lars . . . . . . . . . . . . . . . .CB-6.1 WEDNahon, Laurent . . . . . . . . . . . .CG-6.1 WEDNaimi, Sepideh Tayeb . . . . . . .�CI-2.1 SUNNajafi, Faraz . . . . . . . . . . . . . CK-4b.1 MONNakagawa, Ken’ichi . . . . . . . .CJ-14.4 THUNakagawa, Yosuke . . . . . . . . . CK-9.6 TUENakajim, Shota . . . . . . . . . . .CF-P.28 WEDNakamura, Kei . . . . . . . . . . . JSIII-1.4 MONNakano, Hitoshi . . . . . . . . . . CJ-P.47 WEDNakano, Motoyoshi . . . . . . . . . CF-8.3 THUNakao, Hiroaki . . . . . . . . . . . . . CA-2.5 SUNNakao, Kazuya . . . . . . . . . . . . . CI-5.4 MONNakjima, Kazuhisa . . . . . . . JSIII-1.1 MONNalawade, Bhiku . . . . . . . . . .EF-4a.2 MONNalla, Venkatram . . . . . . . . . . �CF-9.6 THUNam, Chang Hee . . . . . . . . .JSIII-1.1 MONNam, Sae Woo . . . . . . . . . . CK-4a.2 MON,
EB-1.5 MON, JSV-P.7 MON,EA-6.3 TUE, JSV-1.5 THU
Nambiar, Siddharth . . . . . . . .CK-P.2 MONNamekata, Naoto . . . . . . . . . EA-P.22 THUNamiq, Medya . . . . . . . . . . . . �CH-5.5 TUENanot, Sebastien . . . . . . . . . JSIV-2.2 SUNNapier, Bruce . . . . . . . . . . . . . . CJ-7.2 WEDNapierala, Marek . . . . . . . . . . CE-1.6 SUN,
CI-1.4 SUNNapolitano, Mario . . . . . . . . . . EA-2.3 SUNNärhi, Mikko �CD-1.2 SUN, �EE-3.1 SUNNarita, Akimitsu . . . . . . . . . . JSIV-1.3 SUNNarmontas, Andrius . . . . . . . .EF-6.2 MONNaruse, Makoto . . . . . . . . . �EG-P.15 MONNash, Geoffrey R. . . . . . . . . . PD-B.8 WEDNasilowski, Michel . . . . . . . CK-P.15 MON,
EG-P.8 MON, EG-7.5 MONNasilowski, Tomasz . . . . . . . . CE-1.6 SUN,
CI-1.4 SUN, CE-P.28 TUENasir, Mazhar . . . . . . . . . . . . . EH-4.4 WEDNatarajan, Chandra . . . . . . . JSV-4.5 THUNatarajan, Chandra M. . . . EA-P.28 THU,
JSV-4.1 THUNatrella, Michele . . . . . . . . . . CC-5.6 MONNaughton, Thomas
CLEO/ECBO-1.3 WEDNava, Giovanni . . . . . . . . . . �CL-P.11 SUN,
JSII-1a.1 MON, �CD-6.6 MON,�CLEO/ECBO-2.2 WED, CL-1.3 WEDNavarrete-Benlloch, Carlos �EA-P.20 THUNavarrete-f, Carlos . . . . . . . . . EF-9.4 THUNavas, David . . . . . . . . . . . . �CF-P.31 WEDNavickaite, Gabriele . . . . . . JSIV-2.2 SUN,
JSIV-2.5 SUNNavratil, Petr . . . . . . . . . . . . . . CA-P.6 SUNNawata, Kouji . . . . . . . . . . . . . .CC-P.7 SUNNaylor, Bruno . . . . . . . . . . . . . . EC-1.3 TUENazabal, Virginie . . . . . . . . . . . CE-1.2 SUNNdao, A . . . . . . . . . . . . . . . . . CK-11.2 WEDNeale, Steven N. . . . . . . . . . .JSII-2.4 MONNebel, Christoph . . . . . . . . . . EG-P.2 MONNebioglu, Mehmet Ali . . . . . CE-P.11 TUENedeljkovic, Milos . . . . . . . . . . CK-7.2 TUENeethling, Pieter . . . . . . . . . CF-P.34 WEDNegel, Jan-Philipp . . . . . . . . . CA-9.2 THUNegru, Razvan . . . . . . . . . . . . . CK-7.4 TUENeira, Andres . . . . . . . . . . . . . CD-7.3 MONNemec, Michal . . . . . . . . . . . CA-P.24 SUN,
CA-P.25 SUNNemitz, Wolfgang . . . . . . . . . �EI-3a.1 THUNemoto, Natsuki . . . . . . . . . . �CC-6.3 TUENesher, Ofer . . . . . . . . . . . . . .�CN-1.3 WEDNeshev, Dragomir . . . . . . . . . .EG-2.2 SUN,
CK-6.3 MON, EH-5.1 THU, EH-5.3 THUNeshev, Dragomir N. . . . . . . JSV-2.3 THUNessling, Hauke . . . . . . . . . . . . . CI-P.6 TUENesterov, Maxim . . . . . . . . . �EH-1.2 WEDNeugebauer, Martin . . . . . . .�EG-P.1 MONNeuhaus, Leonhard . . . . . . . .�EA-4.4 SUN,
EA-P.18 THUNeumann, Jörg . . . . . . . . . . . . CE-2.4 SUN,
CA-4.1 SUN, CJ-P.25 WED,CJ-P.42 WED
Neumeyr, Christian . . . . . . . . . CB-2.3 TUENevas, Saulius . . . . . . . . . . . . . CH-2.1 SUNNevsky, Alexander . . . . . . . . . ED-3.4 MONNg, Vincent . . . . . . . . . . . . . �EH-P.12 WEDNg, Wing . . . . . . . . . . . . . . . . CK-10.2 WEDNguimdo, Romain Modeste �CB-8.3 THUNguyen, Duc-Minh . . . . . . �CD-P.24 TUE,�CI-P.1 TUENguyen, Huan . . . . . . . . . . . . . �EC-P.5 TUENguyen, Linh . . . . . . . . . . . . . . �CH-4.1 SUNNibbering, Erik . . . . . . . . . . . EF-4a.1 MONNicholl, Adrian . . . . . . . . . . . . CN-2.3 WEDNicholson, Jeffrey . . . . . . . . . . �CJ-4.6 SUNNicolas, Adrien . . . . . . . . . . .EB/EG.3 TUENicolas, Descharmes . . . . . . CK-14.5 THUNielsen, Bo M. . . . . . . . . . . . CH-P.22 THUNielsen, Kristian . . . . . . . . . CH-P.20 THU,
CH-P.25 THUNiemi, Tapio . . . . . . . . . . . . . . CB-4.5 WEDNieto, Daniel . . . . . . . . . . . �CM-P.11 SUN,
�CM-P.12 SUNNiguès, Antoine . . . . . . . . . . . . EC-3.4 TUENihashi, Shunsuke . . . . . . . . EH-P.10 WEDNikas, Thomas . . . . . . . . . . . . . CI-5.3 MONNikiforov, Oleg . . . . . . . . . . . . �CB-9.5 THUNikkinen, Jari . . . . . . . . . . . �CA-5b.1 MONNikolaev, Andrey . . . . . . . . . CE-11.3 WEDNikolajeff, Fredrik . . . . . . . . . . CL-4.1 THUNikolave, Andrey . . . . . . . . . CE-11.2 WEDNilsson, Johan . . . . . . . . . . . . CJ-P.36 WEDNing, Cun-Zheng . . . . . . . . . �CB-4.1 WEDNiquet, Yann Michel . . . . . . CB-11.1 THUNirmalathas, Ampalavanapillai
CH-P.19 THUNishii, Junji . . . . . . . . . . . . . .CK-P.17 MONNishimoto, Yusuke . . . . . . . . . CL-4.4 THUNishizawa, Norihiko . . . . . . . .�CJ-4.4 SUN,
CJ-P.4 WED, CL-5.2 THUNisoli, Mauro CG-6.3 WED, CF-8.4 THUNocentini, Sara . . . . . . . . . . . .�CK-9.5 TUENock, Richard . . . . . . . . . . . . EB-4.2 WED,
CH-9.4 WEDNoda, Susumu . . . . . . . . . . . CK-13.6 WEDNoe, Jonathan . . . . . . . . . . . . EG-6.2 MONNoel, Healy . . . . . . . . . . . . . . . . CE-4.2 SUNNold, Johannes . . . . . . . . . . . . CJ-4.5 SUN,
CJ-10.3 WED, CJ-10.6 WED,�CJ-11.4 THUNolte, Stefan . .EA-1.3 SUN, CI-1.2 SUN,
CM-P.10 SUN, CE-3.1 SUN,CM-4.1 SUN, CM-4.6 SUN,CM-6.2 MON, JSIV-P.1 TUE,EB-3.3 WED, EB-P.1 WED,CJ-11.3 THU, EA-P.9 THU,JSV-3.3 THU
Nomura, Yoshitaka . . . . . . . . . .CJ-4.4 SUNNonobe, Kazuki . . . . . . . . . . . .CJ-P.4 WEDNorris, Barnaby . . . . . . . . . . . .CH-7.4 WEDNoskov, Roman E. . . . . . . . . CD-P.10 TUENotake, Takashi . . . . . . . . . . . . CC-P.7 SUNNouchi, Pascale . . . . . . . . . . CH-P.12 THUNoury, Adrien . . . . . . . . . . . . CK-10.3 WEDNovikov, Anton . . . . . . . . . . . CA-12.2 THUNovikov, Innokenty I. . . . . . CB-P.22 MONNovikov, Vladimir . . . . . . . . .CD-P.31 TUENovoa, David CD-1.1 SUN, CD-P.39 TUENubbemeyer, Thomas . . . . . �CA-P.1 SUNNukulin, Maxim . . . . . . . . . . . . .EI-2.2 THUNunn, Joshua . . . . . . . . . . . . . . EA-6.3 TUENuño, Javier . . . . . . . . . . . . . �CJ-P.21 WEDNunzi Conti, Gualtiero . . . . CH-P.24 THUObara, Yuki . . . . . . . . . . . . . �CD-11.3 THUOberbeckmann, Daniel . . . . . CN-P.3 TUEObermaier, Johannes . . . . . . CJ-12.3 THUObraztsov, Peter . . . . . . . . . . CA-11.1 THUObraztsova, Elena . . . . . . . . .CA-11.1 THUO’Brien, Jeremy . . . . . . . . . . EB-5.5 WED,
JSV-4.5 THUO’Brien, Jeremy L. . . . . . . . . EA-6.1 TUE,
PD-B.3 WED, JSV-1.1 THU,EA-P.28 THU, JSV-4.1 THU
O’Brien, Peter . . . . . . . . . . . . . . CJ-1.4 SUNObronov, Ivan . . . . . . . . . . . . CA-12.2 THUOchi, Yoshihiro . . . . . . . . . . . . .CC-6.4 TUEO’Connor, Daniel . . . . . . . . . . EH-4.2 WED
O’Connor, Gerard . . . . . . . . . . CM-2.3 SUNOden, Jérémy . . . . . . . . . . . . .CD-P.34 TUEOdent, Vincent . . . . . . . . . . . �EF-8.5 TUE,�EF-P.3 THU, �EF-P.5 THUOe, Yasuko . . . . . . . . . . . . . �CK-P.12 MONO’Faolain, Liam . . . . . . . . . . . . CK-1.3 SUNOffrein, Bert J. . . . . . . . . . . . . CD-P.1 TUEOguchi, Kenichi . . . . . . . . . . . CC-P.12 SUNOguma, Manabu . . . . . . . . . . PD-B.3 WEDOhadi, Hamid . . . . . . . . . . . . . . EF-9.2 THUOhdan, Hideaki . . . . . . . . . . . . EA-1.5 SUNOhishi, Yasutake . . . . . . . . . .CD-6.1 MON,
CE-P.12 TUE, �CJ-P.43 WED,CJ-P.45 WED
Ohmae, Noriaki . . . . . . . . . . .�ED-3.2 MONOhtsu, Motoichi . . . . . . . . . .EG-P.15 MONOjambati, Oluwafemi . . . . �CK-13.2 WEDOka, Kazuhiko . . . . . . . . . . . . . EE-P.9 SUNOkamoto, Shinya . . . . . . . . . CE-11.5 WEDOkamoto, Tetushi . . . . . . . . CH-P.29 THUOkamura, Yasuyuki . . . . . . . . . CI-5.6 MONOkawachi, Yoshitomo . . . . . CH-8.6 WED,
PD-A.5 WEDOkeil, Hesham . . . . . . . . . . . . . CC-1.2 SUNOkell, William . . . . . . . . . . . . . .CG-1.2 TUEOkhotnikov, Oleg . . . . . . . . .CE-P.35 TUE,
CJ-10.5 WEDOkhrimchuk, Andrey . . . . . �CA-11.1 THUOki, Yuji . . . . . . . . . . . . . . . . . . . CE-2.1 SUNOkino, Tomoya . . . . . . . . . . �CG-6.4 WED,
CG-P.18 THUOkuyama, Yohei . . . . . . . . . �CA-11.5 THUOladeji, Ayodele . . . . . . . . . . . CJ-7.2 WEDOlaizola, Santiago Miguel . .CE-P.27 TUEOlarte, Omar . . . . . . . . . . . . . . .CL-P.7 SUNOldenbeuving, Ruud . . . . . . . CJ-12.2 THUOleg, Louchev . . . . . . . . . . . �CD-P.37 TUEOliveira, Pedro . . . . . . . . . . . . .CG-P.1 THUOliver, Neus . . . . . . . . . . . . . �EF-P.22 THUOlivéro, Aurore . . . . . . . . . . . . �CL-4.3 THUOlivier, Nicolas . . . . . . . . . . . . EH-4.2 WEDOllmann, Zoltán . . . . . . . . . . . CC-3.1 SUN,
CC-3.5 SUNOmatsu, Takashige . . . . . . . . CM-3.4 SUN,
CA-3.1 SUN, CA-6.3 MON, CA-7.6 MONOmoda, Emiko CJ-4.4 SUN, CJ-P.4 WEDOnda, Tomomi . . . . . . . . . . . CA-11.5 THUOng, Junn Yaw . . . . . . . . . . . CD-P.11 TUEOno, Atsushi . . . . . . . . . . . . . EH-P.10 WEDOnur, Alexander . . . . . . . . . EG-P.12 MON,
EA-10.2 THUOoka, Yuta . . �CK-9.2 TUE, CK-9.4 TUEOpheij, Aron . . . . . . . . . . . . . . EF-6.6 MONOppo, Gian-Luca . . . . . . . . . . .EF-1.1 SUN,�EF-1.5 SUN, EF-5.3 MON,
CB-P.15 MON, �EC-P.4 TUE,EC-P.6 TUE, EC-3.3 TUE, EF-9.3 THU,CL-3.4 THU
Orazi, Leonardo . . . . . . . . . . . .CM-2.5 SUNOrbe, Luis Jorge . . . . . . . . . . .CB-6.3 WEDO’Regan, Bryan . . . . . . . . . . CK-11.1 WEDOreshkov, Bozhidar . . . . . . . �CA-4.4 SUN,
CA-11.4 THUOriá, Marcos . . . . . . . . . . . . . . . EG-4.4 SUNOriana, Aurelio . . . . . . . . . . . . .CF-6.1 THU
219
Authors’ Index
Orieux, Adeline . . . . . . . . . . . EB-P.9 WED,JSV-2.2 THU
Origlia, Stefano . . . . . . . . . . . ED-P.9 MONOrlandi, André . . . . . . . . . . . . . CL-P.1 SUNOrlov, Oleg . . . . . . . . . . . . . . . CA-P.14 SUNOrlovich, Valentin . . . . . . . . . . CA-8.5 TUEOrlovskii, Yurii . . . . . . . . . . . . �CL-P.3 SUNOrnigotti, Marco . . . . . . . . . . .EA-1.2 SUN,
CH-2.4 SUNOrobtchouk, Régis . . . . . . . . . JSI-1.5 SUN,
CH-3.5 SUNOrsel, Kasper . . . . . . . . . . . . �CM-P.19 SUNOrsila, Lasse . . . . . . . . . . . . . . . CD-1.2 SUNOrtega-Quijano, Noé . . . . . . �CL-3.2 THUOrtega, Tiago . . . . . . . . . . . . . . CL-P.1 SUNOrtegel, Norbert . . . . . . . . . . EB-4.3 WED,
EB-P.12 WEDOrtïn, Silvia . . . . . . . . . . . . . . EF-P.11 THUOrtsiefer, Markus . . . . . . . . CB-P.11 MON,
CB-2.3 TUEOsawa, Takumi . . . . . . . . . . . . CE-P.4 TUEOsellame, Roberto . . . . . . . . .CM-1.4 SUN,
CL-P.11 SUN, CM-4.4 SUN,JSII-1a.1 MON, JSV-P.8 MON,EB-4.1 WED, CLEO/ECBO-2.2 WED,EB-5.1 WED, EB-5.2 WED,CL-1.3 WED, JSV-2.2 THU,JSV-3.2 THU, JSV-3.4 THU
Osewski, Pawel . . . . . . . . . . . CD-P.21 TUEO’Shaughnessy, Ben . . . . . . . CB-7.1 WEDO’Shea, Danny . . . . . . . . . �EG-P.12 MON,�EA-10.2 THUOsiko, Vyacheslav V. . . . . . . CA-P.24 SUNOstendorf, Ralf . . . . . . . . . . . . CD-4.2 SUN,
CN-2.2 WEDØsterkryger, Andreas Dyhl �CK-P.9 MONOstermann, Laurin . . . . . . . . . EA-P.8 THUOsterwalder, Jürg . . . . . . . . . .CG-4.5 WEDOstrowski, Lukasz . . . . . . . . . . CI-1.4 SUN,
CE-P.28 TUEOsuch, Tomasz . . . . . . . . . . . .CH-6.3 WEDOsvaldo Dias, Guilherme . . CB-11.1 THUOsvay, Karoly . . . . . . . . . . . . . CF-P.7 WED,
CF-P.21 WEDOszetzky, Dániel . . . . . . . . . . CA-P.35 SUNOtobe, Tomohito . . . . . . . . �CG-P.14 THUOttaviano, Luisa . . . . . . . . . . .CK-3.2 SUN,
CK-5.2 MONOtte, Maya . . . . . . . . . . . . . . . . CL-3.1 THUOttenhues, Christoph . . . . .�CJ-P.42 WEDOttevaere, Heidi . . . . . . . . . . CH-P.26 THUOtto, Hans-Jürgen . . . . . . . . . CJ-1.2 SUN,�CJ-10.1 WED, CJ-10.2 WEDOtuka, Adriano José Galvani
CM-P.14 SUNOu, Jun-Yu .CK-6.6 MON, �EH-4.5 WEDOuadghiri Idrissi, Ismail . . . . �EE-P.3 SUNOudar, Jean-Louis . . . . . . . . . . CJ-2.4 SUNOugazzaden, Abdallah . . . . CE-11.4 WEDOujja, Mohamed . . . . . . . . . . .CM-2.2 SUNOulton, Ruth . . . . . . . . . . . . EG-P.16 MON,
EA-8.4 WEDOvchinnikov, Andrey . . . . . . . .CC-3.2 SUNOvermeyer, Ludger . . . . . . . . . CE-2.4 SUNOzcan, Aydogan . . . . . . . . JSII-1a.3 MON,
�CL-1.1 WEDÖzkan, Vedat Ali . . . . . . . . . .CC-P.18 SUNÖzsoy Keskinbora, Cigdem . EH-2.2 WEDOzyuzer, Lutfu . . . . . . . . . . . . CE-P.11 TUEP Barwood, Geoffrey . . . . . . ED-P.9 MONPadilla Michel, Yazmin . . . �CH-P.10 THUPae, Ki Hong . . . . . . . . . . . . JSIII-1.1 MONPagliano, Francesco Maria . JSV-2.5 THUPaiè, Petra . . . . . . . . . . . . . . . CL-P.11 SUN,
JSII-1a.1 MON, CL-1.3 WEDPainter, Oskar . . . . . . . . . . . . . EG-1.1 SUN,
CK-10.4 WEDPal, Atasi . . . . . . . . . . . . . . . . . CH-P.6 THUPal, Vishwa . . . . . . . . . . . . . . . �CA-P.4 SUNPalacios, Alicia . . . . . . . . . . . . EE-1.4 SUN,
CG-6.3 WED, CG-P.17 THUPalashov, Oleg . . . . . . . . . . . CA-P.33 SUN,
CE-7.6 MONPalastro, John . . . . . . . . . . . . . .EE-2.1 SUNPálfalvi, László . . . . . . . . . . . . . CC-3.5 SUNPallmann, Wolfgang . . . . . . . CA-9.1 THU,
CA-9.2 THUPalmer, Guido . . . . . . . . . . . . . .CA-3.5 SUNPalomba, Stefano . . . . . . . . . EH-P.8 WEDPaltoglou, Vassilis . . . . . . . . . . EI-1.2 THU,
EI-1.5 THUPan, Jiaoqing . . . . . . . . . . . . .CB-10.3 THUPanagiotopoulos, Paris . . . . . . EE-2.2 SUNPanajotov, Krassimir . . . . . . CB-8.5 THU,
EF-P.14 THUPanapakkam, Vivek . . . . . . . . .CI-2.5 SUN,
CB-10.5 THUPandraud, Gregory . . . . . . . . . EA-4.5 SUNPang, Fufei . . . . . . . . . . . . . . . .CF-P.1 WEDPang, Meng . . . . . . . . . . . . . . .CJ-12.4 THUPannell, Chris . . . . . . . . . . . . . CJ-14.6 THUPanov, Nikolay . . . . . . . . . . . . . .EI-2.6 THUPant, Mihir . EB-3.4 WED, JSV-1.2 THUPantouvaki, Marianna . . . . . CB-11.3 THUPapadopoulos, Dimitrios . . . . CG-2.2 TUEPapadopoulos, Ioannis . . . . . . CL-5.5 THUPapaioannou, Maria . . . . . . . . �CI-1.1 SUNPape, Alexander . . . . . . . . . . EE-P.14 SUN,
EF-3.3 SUNPapernyi, Serguei . . . . . . . . . EF-P.19 THUPapillon, Dominique . . . . . . . . CD-4.2 SUNPapp, Scott . . . . . . . . . . . . . . ED-1a.1 MONPapp, Scott B. . . . . . . . . . . . ED-1a.3 MONPapsimakis, Nikitas . . . . . . . . . EI-1.4 THUPapukutty Rajan, Rajitha . . �CD-3.1 SUNParadissanos, Ioannis . . . . . . CM-7.3 MONParadowska, Magdalena . . . .CH-7.2 WEDParaiso, Taofiq . . . . . . . . . . . .�EG-1.1 SUN,
CK-10.4 WEDPardo, Fabrice . . . . . . . . . . . . CK-P.6 MON,
CD-8.6 TUEPariente, Gustave . . . . . . . . . �CH-8.4 WEDParigi, Valentina . . . . . . . . . . . �EG-4.3 SUNParillaud, Olivier . . . . . . . . . . .CB-5.2 WEDParis, Matteo G.A. . . . . . . . .CH-P.22 THUParisi, Maria CD-8.2 TUE, CH-P.36 THUParisini, Andrea . . . . . . . . . . CE-5a.1 MONPark, Hong-Gyu . . . . . . . . . . CK-11.5 WEDPark, Ji-Yong . . . . . . . . . . . . .CJ-P.23 WEDPark, Kyoungyoon . . . . . . . .CK-P.26 MON
Park, Nam Hun . . . . . . . . . . .CJ-P.23 WEDPark, NamKyoo . . . . . . . . . . . EG-P.6 MONPark, Sae June . . . . . . . . . . . . �CC-4.4 SUNParka, Janusz . . . . . . . . . . . . . CC-P.17 SUNParker, Richard . . . . . . . . . . . .CJ-14.3 THUParmeggiani, Camilla . . . . . . . CK-9.5 TUEParmigiani, Francesca . . . . . . . CI-4.4 SUNParnet, François . . . . . . . . . . . .CL-3.2 THUParra, Albert . . . . . . . . . . . . .CD-5b.1 MONParra-Rivas, Pedro . . . . . . . . �ED-P.2 MONParravicini, Jacopo . . . . . . . .CD-7.5 MON,
EF-7.2 TUEParrivicini, Jacopo . . . . . . . . . . EF-1.6 SUNParry, Bryn . . . . . . . . . . . . . . .CF-P.25 WEDParsonage, Tina . . . . . . . . . . �CE-7.2 MON,
CE-P.3 TUE, CJ-P.3 WEDParvitte, Bertrand . . . . . . . . . �CH-P.2 THUPascal, Jourdain . . . . . . . . . . .CL-P.10 SUNPaschke, Katrin . . . . . . . . . . .SH-10.1 SUN,
CB-P.9 MON, CB-P.10 MON,CD-P.35 TUE
Pascual-Winter, Maria FlorenciaEA-5.4 MON
Pasiskevicius, Valdas . . . . . CD-P.41 TUE,CE-9.2 TUE, CJ-P.15 WED,CJ-14.5 THU
Pask, Helen . CA-1.2 SUN, CA-6.3 MON,CA-7.4 MON, CH-7.6 WED
Pasquazi, Alessia . . . . . . . �CD-5a.2 MON,CC-6.5 TUE, CD-P.13 TUE,EA-6.5 TUE, EF-8.2 TUE, EA-7.3 TUE
Passaseo, Adriana . . . . . . . . CK-13.5 WEDPassenberg, Wolfgang . . . . . . CK-7.1 TUEPastor, Daniel . . . . . . . . . . . . . CH-P.5 THUPastouret, Alain . . . . . . . . . . . . CE-1.1 SUNPatas, Alex . . . . . . . . . . . . . . . CG-P.16 THUPatchkovskii, Serguei . . . . . .CG-6.2 WED,
CG-P.13 THUPatel, Sanketkumar . . . . . . . . .CC-6.6 TUEPatera, Giuseppe . . . . . . . . . . . EF-9.4 THUPathak, Vishwa Bandhu . . JSIII-1.1 MONPati, Aseem Prakash . . . . . . .CG-4.6 WEDPatimisco, Pietro . . . . . . . . . . .CH-3.1 SUNPatriarche, Gilles . . . . . . . . . CE-11.4 WEDPatrini, Maddalena . . . . . . . . EG-P.4 MONPattathil, Rajeev . . . . . . . . . CF-P.25 WEDPätzold, Welm . . . . . . . . . . �CK-P.22 MONPauc, Nicolas . . . . . . . . . . . . . CB-11.1 THUPaul, Douglas J. . . . . . . . . . . . EH-5.5 THUPaul, Sujoy . . . . . . . . . . . . . . . .�CB-2.3 TUEPaulus, Gerhard . . . . . . . . . . . . CG-2.3 TUEPavel, Nicolaie . . . . . . . . . . . CA-P.29 SUN,�CA-5b.2 MON, CA-10.4 THUPavesi, Lorenzo . . . . . . . . . . . EA-P.32 THUPavlov, Artem . . . . . . . . . . . . . CH-P.1 THUPavlov, Ihor CM-2.5 SUN, CM-P.18 SUN,
CM-4.5 SUN, CK-P.3 MON,CK-P.34 MON, �JSI-P.1 TUE
Pavlyuk, Anatoly . . . . . . . . . . . CA-8.5 TUEPavone, Francesco . . . . . . . . . .CC-4.5 SUNPawlak, Dorota A. . . . . . . . . CD-P.21 TUEPawlus, Robert . . . . . . . . . . . . �CB-9.4 THUPazzagli, Sofia . . . . . . . . . . . . JSIV-2.5 SUNPeacock, Anna . . . . . . . . . . . . CH-4.4 SUN,
CE-P.8 TUE, CH-6.5 WED
Peacock, Anna C. . . . . . . . . . . CE-4.2 SUNPeaudecerf, Bruno . . . . . . . . . EA-P.2 THUPeccianti, Marco . . . . . . . . . . .CC-P.6 SUN,
CD-5a.2 MON, CC-6.5 TUE,EA-6.5 TUE, EF-8.2 TUE, EA-7.3 TUE
Peckus, Martynas . . . . . . . . . . CK-1.5 SUN,CK-P.10 MON
Pedersen, Christian . . . . . . .CH-P.15 THU,CH-P.34 THU
Pedrosa, Laura . . . . . . . . . . . CH-9.6 WED,CJ-12.3 THU
Pe’er, Avi . �EE-5b.1 MON, �EA-7.5 TUEPeev, Momtchil . . . . . . . . . . . EB-4.4 WED,
EB-P.4 WEDPeharz, Gerhard . . . . . . . . . . . .EI-3a.1 THUPeigné, Arnaud . . . . . . . . . . �CH-P.12 THUPeinke, Emanuel . . . . . . . . . . CD-P.32 TUEPelc, Jason . . . . . . . . . . . . . . . EA-P.28 THUPelé, Anne-Laure . . . . . . . . . . �CE-1.2 SUNPeli, Simone . . . . . . . . . . . . . . EE-P.17 SUNPellegrina, Alain . . . . . . . . . . CF-P.19 WEDPellegrino, Mario . . . . . . . . . . CL-P.13 SUNPelli, Stefano . . . . . . . . . . . . �CH-P.24 THUPelling, Andrew . . . . . . . . . . . .CM-P.2 SUNPelouard, Jean-Luc . . . . . . . CK-P.6 MON,
CD-8.6 TUEPeña, Alexandra . . . . . . . . . . CE-P.13 TUEPenasa, Mariane . . . . . . . . . . �EA-P.2 THUPenciu, Raluca-Sorina . . . . . . . EI-1.5 THUPeng, Cheng . . . . . . . . . . . . . .JSIV-2.3 SUNPeng, Junsong . . . . . . . . . . . .�CJ-14.5 THUPeng, Lung Han . . . . . . . . . .CK-P.27 MONPengji, Ding . . . . . . . . . . . . . . . �EE-2.3 SUNPénillard, Anne . . . . . . . . . . . . .CK-7.4 TUEPenin, Alexander . . . . . . . . . . CC-P.19 SUNPennetta, Riccardo . . . . . . . . PD-A.9 WEDPenttinen, Jussi-Pekka . . . �CB-P.1 MON,
CB-3.1 TUEPeräjärvi, Kari . . . . . . . . . . . . .CN-2.3 WEDPerchoux, Julien . . . . . . . . . . .CH-8.1 WEDPéré-Laperne, Nicolas . . . . . . CD-8.6 TUEPerentos, Andreas . . . . . . . . . . . CI-3.4 SUNPerevezentsev, Evgeny . . . . �CA-P.33 SUNPerez, Angela . . . . . . . . . . . . . . EA-7.4 TUEPérez-Hernández, Jose Antonio
CG-P.10 THUPerez, Juan M. . . . . . . . . . . . �CL-1.2 WEDPerez-Leija, Armando . . . . . . EA-1.3 SUN,
CK-4b.2 MON, �EA-P.9 THU,JSV-3.3 THU, JSV-3.5 THU,JSV-4.6 THU
Pérez, Pablo . . . . . . . . . . . . . . EF-P.12 THUPérez, Pere . . . . . . . . . . . . . . . . .CL-P.7 SUNPerez-Serrano, Antonio . . . . . EI-P.2 TUE,
CB-5.2 WED, �CB-7.6 WEDPerez-Vizcaino, Jorge . . . . . . . CE-2.2 SUNPergament, Mikhail . . . . . . . . .CA-3.5 SUNPeřina, Jan . . . . . . . . . . . . . . CK-P.32 MONPerret, Leopoldine . . . . . . . . . EH-P.8 WEDPerrone, Guido . . . . . . . . . . . . CL-P.14 SUNPerrone, Sandro . . . . . . . . . . EF-4a.2 MONPerros, Elodie . . . . . . . . . . . . . . EG-4.3 SUNPersechino, Mauro . . . . . . . .�JSV-4.2 THUPertot, Daniel . . . . . . . . . . . . . . EC-1.2 TUEPertsch, Thomas . . . . . . . . . . .EG-2.2 SUN,
CD-2.2 SUN, EE-P.13 SUN,CM-5a.3 MON, CK-P.8 MON,JSV-P.5 MON, CD-8.1 TUE,�EF-7.1 TUE, CF-P.17 WED,JSV-2.3 THU, EF-P.21 THU
Peruch, Silvia . . . . . . . . . . . . �CD-7.3 MONPerumal, Dharanipathy . . . .CK-14.5 THUPervak, Vladimir . . . . . . . . . CA-P.12 SUN,
CA-P.22 SUN, CA-P.34 SUN,CD-8.4 TUE, CG-1.3 TUE,PD-A.1 WED, CA-10.3 THU,CA-10.5 THU, CG-P.12 THU
Pervak, Volodymyr . . . . . . . . . CF-7.5 THUPeschel, Ulf EF-2.3 SUN, CK-P.35 MON,
EH-P.6 WEDPesquera, Luis . . . . . . . . . . . �EF-P.11 THU,
EF-P.12 THU, EF-P.14 THUPetelin, Jaka . . . . . . . . . . . . . CJ-P.20 WEDPeter, Weßels . . . . . . . . . . . . .CJ-P.25 WEDPetermann, Ann Britt . . . . . . CE-8.3 TUEPeters, Achim . . . . . . . . . . . . CB-P.12 MONPeters, Frank . . . . . . . . . . . . CB-P.30 MONPeters, Luke . . . . . . . . . . . . . . . CC-P.6 SUNPetev, Mihail . . . . . . . . . . . . . . . EE-3.3 SUNPetit, Marlène . . . . . . . . . . . . . .CK-1.2 SUNPetit, Stephane . . . . . . . . . . . . CL-P.5 SUN,
CG-6.1 WED, CG-6.2 WEDPetit, Yannick . . . . . . . . . . . CM-5a.2 MONPetkelis, Juozas . . . . . . . . . . .CJ-P.39 WEDPetkovšek, Rok . . . . . . . . . . �CJ-P.20 WEDPetra, Rafidah . . . . . . . . . . . . . .CE-4.3 SUNPetridis, Costas . . . . . . . . . . . CM-P.3 SUN,
CM-7.3 MONPetrik, Peter . . . . . . . . . . . . . . . CE-1.3 SUNPetronijevic, Emilija . . . . . . .CD-P.21 TUEPetropoulos, Periklis . . . . . . . . .CI-4.4 SUNPetrov, Valentin . . . . . . . . . . . CA-1.4 SUN,
CA-P.31 SUN, CA-4.4 SUN,CA-4.5 SUN, CA-5a.1 MON,CA-5a.2 MON, CA-5b.3 MON
Petrovic, Jovana . . . . . . . . . . . CH-P.8 THUPetruzzella, Maurangelo . . �JSV-2.5 THUPetruzzelli, Vincenzo . . . . . . .CK-1.6 SUN,
CK-P.31 MONPetti, Lucia . . . . . . . . . . . . . . . . CK-8.1 TUEPezzè, Luca . . . . . . . . . . . . . . EA-P.27 THUPfau, Tilman . . . . . . . . . . . . . JSV-P.9 MONPfeifer, Hannes . . . . . . . . . . . . EG-1.1 SUN,�CK-10.4 WEDPfeiffer, Adrian Nikolaus . . �CG-4.6 WEDPfeiffer, Martin . . . . . . . . . . ED-1a.2 MON,�CE-9.1 TUEPfeiffer, Martin H.P. . . . . . . .ED-P.8 MONPhan Huy, Kien . . . . . . . . . . �CD-P.23 TUEPhang, Sendy . . . . . . . . . . . �EH-P.18 WEDPhilippe, Lalanne . . . . . . . . . . .CB-1.3 TUEPhillips, Christopher . . . . . . . �CD-2.5 SUNPhillips, Christopher R. . . . . . EE-4.2 SUN,
CF-2.3 TUEPhillips, Hilary . . . . . . . . . . . . . CH-3.3 SUNPhillips, Ian . . . . . . . . . . . . . . . . .CI-P.5 TUEPhillips, Jonathan . . . . . . . . . .CA-3.6 SUN,
CF-P.25 WEDPiazza, Luca . . . . . . . . . . . . . . EH-2.3 WEDPibiri, Enrico CL-P.18 SUN, EH-6.2 THU
220
Authors’ Index
Picard, Emmanuel . . . . . . . . . .CK-8.3 TUEPiccardi, Armando . . . . . . . . �CD-7.2 MONPiccirillo, Bruno . . . . . . . . . . . . EC-2.3 TUEPiché, Michel . . . . . . . . . . . . .CG-P.19 THUPicot-Clemente, Jeremy . . . �CD-6.1 MONPicozzi, Antonio CI-4.3 SUN, EI-2.1 THUPicqué, Nathalie . . . . . . . . . . .CH-7.1 WEDPiehler, Stefan . . . . . . . . . . . . CA-7.3 MONPiekarek, Mateusz . . . . . . . . . . EA-6.1 TUEPierangeli, Davide . . . . . . . . CD-7.5 MON,�EF-7.2 TUEPierre, Magistretti . . . . . . . . . CL-P.10 SUNPierre, Marquet . . . . . . . . . . . CL-P.10 SUNPierrot, Simonette . . . . . . . . . CA-9.1 THUPietra, Alice . . . . . . . . . . . . . . CL-P.11 SUNPietrzyk, Monika . . . . . . . . . . EH-3.4 WEDPigeau, Benjamin . . . . . . . . . . EG-1.5 SUN,
CK-2.4 SUNPilipavicius, Jurgis . . . . . . . . CE-P.35 TUEPilny, Rouven H. . . . . . . . . �CB-P.21 MON,
CB-10.4 THUPin, Christophe . . . . . . . . . . . . CK-8.3 TUEPingault, Benjamin . . . . . . . . . CE-4.4 SUNPinkal, Kevin . . . . . . . . . . . . . . .EA-3.4 SUNPinkse, Pepijn . . . . . . . . . . . . . EB-4.6 WEDPinkse, Pepijn W.H. . . . . . . . EA-3.2 SUN,
EH-P.3 WEDPiramidowicz, Ryszard . . . . . CH-6.3 WEDPiro, Nicolas . . EG-1.4 SUN, EA-4.2 SUNPirotta, Stefano . . . . . . . . . . EG-P.4 MON,
EA-7.6 TUEPirzio, Federico . . . . . . . . . . . �CA-1.4 SUN,
CA-2.1 SUNPisanello, Ferrucio . . . . . . . .CK-P.25 MONPiskarskas, Algis . . . . . . . . . . . EF-6.2 MONPissadakis, Stavros . . . . . . . .CL-P.14 SUN,
CH-P.26 THUPistora, Jaromir . . . . . . . . . . . EH-2.6 WEDPitanti, Alessandro . . . . . . . . CB-6.4 WEDPitkäaho, Tomi . �CLEO/ECBO-1.3 WEDPitois, Stéphane . . . . . . . . . . . CH-7.1 WEDPlaja, Luis . . . . . . . . . . . . . . . . .CG-P.7 THUPlankl, Markus . . . . . . . . . . . . . CF-7.1 THUPlech, Anton . . . . . . . . . . . . . CM-6.2 MONPlenge, Jürgen . . . . . . . . . . . EG-5b.1 MONPleshakov, Ivan . . . . . . . . . . CK-P.13 MONPleyer, Tobias . . . . . . . . . . . . CA-12.3 THUPlötner, Marco . . . . . . . . . . . . CJ-8.1 WED,
CJ-8.2 WEDPlotnik, Yonatan . . . . . . . . . JSIV-P.1 TUE,
CK-13.1 WEDPlum, Eric . . . CI-1.1 SUN, CK-6.6 MON,�EH-1.4 WED, �CH-7.3 WED,
EH-4.5 WEDPlus, Stéphane . . . . . . . . . . . . . CE-1.1 SUNPodivilov, Eugeny . . . . . . . . . . . EI-2.2 THUPodivilov, Evgeniy . . . . . . . CF-P.26 WED,
CJ-P.16 WED, CJ-P.24 WEDPodobnik, Boštjan . . . . . . . . CJ-P.20 WEDPodoliak, Nina . . . . . . . . . . �CK-10.2 WED,
CE-10.5 WED, �EH-P.3 WEDPodshivalov, Alexey . . . . . . . . EE-P.2 SUN,
CF-P.13 WEDPogna, Eva . . . . . . . . . . . . . . . JSIV-1.2 SUNPogna, Eva Arianna Aurelia
�JSIV-1.5 SUN, CE-12.6 WEDPogoretskii, Vadim . . . . . . . . . CK-3.1 SUNPoh, Hou Shun . . . . . . . . . . . . .EA-1.4 SUNPohl, Johannes . . . . . . . . . . .CB-P.10 MONPoint, Guillaume . . . . . . . . . . �EE-P.4 SUN,�CD-3.5 SUNPoitras, Carl B. . . . . . . . . . . . JSV-4.4 THUPoizat, Jean-Philippe . . . . . . . EA-9.6 THUPokorny, Fabian . . . . . . . . . . .PD-B.1 WEDPoletto, Luca CG-6.3 WED, CF-8.4 THUPoli, Nicola . . . . . . . . . . . . . . . ED-P.9 MONPolisseni, Claudio . . . . . . . . �CE-12.5 WEDPolli, Dario . . . . . . . . . . . . . . �CD-13.2 THUPollnau, Markus . . . . . . . . . �CA-P.39 SUN,
CJ-6a.3 MON, CE-7.3 MON,�CK-12.1 WEDPolo, Juan . . . . . . . . . . . . . . . . . EC-P.8 TUEPolónyi, Gyula CA-3.3 SUN, CC-3.5 SUNPolyakov, Vadim . . . . . . . . . �CA-P.11 SUN,
CA-P.14 SUNPolynkin, Pavel . . . . . . . . . . . �EE-P.1 SUN,
CM-3.2 SUN, �PD-A.4 WEDPomel, Francis . . . . . . . . . . . CF-P.24 WEDPonce, Fernando . . . . . . . . . . PD-A.2 WEDPons, Antonio Javier . . . . . . EF-P.22 THUPons, Bernard . . . . . . . . . . . . CG-6.1 WED,
CG-6.2 WEDPontin, Antonio . . . . . . . . . . . . EA-4.5 SUNPoole, Philip J. . . . . . . . . . . . EA-8.2 WED,
EA-P.7 THUPopa, Daniel . . . . . . . . . . . . . . .CJ-9.6 WEDPopov, Sergei . . . . . . . . . . . . . . CD-1.4 SUNPopov, Sergei Vitalyerich . . . CJ-9.6 WEDPopp, Juergen . . . . . . . . . . . �JSII-2.1 MONPoppe, Andreas . . . . . . . . . . �EB-4.4 WED,�EB-4.5 WED, EB-P.4 WEDPorte, Xavier . . . . . . . . . . . �CB-P.27 MON,
CB-7.2 WEDPortella-Oberli, Marcia . . . . EG-P.5 MON,
CD-9.4 TUEPortier, Benjamin . . . . . . . . . �CD-8.6 TUEPortuondo-Campa, Erwin . . CA-9.6 THU,�CH-P.30 THUPosner, Matthew T. . . . . . .JSV-P.7 MON,�CE-10.5 WEDPostava, Kamil . . . . . . . . . . . . EH-2.6 WEDPotemkin, Fedor . . . . . . . . . . �EE-P.2 SUN,�CF-P.13 WEDPotenz, Marco . . . . . . . . . . . . PD-A.8 WEDPoti, Luca . . . . . . . . . . . . . . . . . CI-P.10 TUEPotocek, Vaclav . . . . . . . . . . EA-P.24 THU,�EA-P.33 THUPottage, John . . . . . . . . . . . . . CH-9.5 WEDPottie, Paul-Eric . . . . . . . . . . ED-3.3 MON,
CH-P.33 THUPoturaj, Krzysztof . . . . . . . . . . .CI-1.4 SUNPoulton, Christopher . . . . . . EF-P.24 THUPoulton, Christopher G. . . CK-P.21 MONPouysegur, Julien . . . . . . . . . . . CJ-1.3 SUNPowell, David . . . . . . . . . . . . . . EH-5.1 THUPrangsma, Jord C. . . . . . . . . EH-P.3 WED,�CL-2.1 THUPrati, Franco . EE-3.6 SUN, CB-7.4 WEDPratti, Franco . . . . . . . . . . . . . . EF-1.6 SUNPredojevic, Ana . . . . . . . . . . �EA-8.2 WED,
EA-P.7 THU, EA-P.8 THUPrehn, Alexander . . . . . . . . . . . EC-2.5 TUEPremaratne, Malin . . . . . . . EG-5b.3 MON,
EH-2.5 WEDPressl, Benedikt . . . . . . . . . . �EA-P.5 THU,
EA-P.26 THUPrevedelli, Marco . . . . . . . . . . ED-3.5 MONPrévost, Florian . . . . . . . . . . . . .CJ-1.3 SUNPrévôt, André . . . . . . . . . . . . CD-P.14 TUEPrezzi, Deborah . . . . . . . . . . JSIV-1.5 SUNPriebe, Gerd . . . . . . . . . . . . . . . CA-3.5 SUNPrilepsky, Jaroslaw . . . . . . . . . �CI-3.2 SUNPrilmüller, Max . . . . . . . . . . . �EA-P.8 THUPrimiani, Peppino . . . . . . . . . CB-5.2 WEDPrinz, Stephan . . . . . . . . . . . . CG-2.1 TUE,
CA-10.1 THUPrior, Estefania . . . . . . . . . .�CB-P.11 MONProchnow, Oliver . . . . . . . . . CF-P.19 WEDProcopio, Lorenzo . . . . . . . . . EB-5.4 WEDProdi, Giovanni A. . . . . . . . . . .EA-4.5 SUNPronin, Oleg . . . . . . . . . . . . . CA-P.12 SUN,
CA-P.22 SUN, CA-P.34 SUN,CD-8.4 TUE, PD-A.1 WED,CA-10.3 THU, �CA-10.5 THU
Proux, Raphaël . . . . . . . . . . . . .EG-3.4 SUNProvino, Laurent . . . . . . . . . . CN-1.5 WEDPruneri, Valerio . . . . . . . . . . . . CL-P.2 SUN,
CH-6.6 WED, EH-4.3 WED,CL-1.2 WED, JSV-4.3 THU
Pryde, Geoff . . . . . . . . . . . . . . .EB-3.2 WEDPrziwarka, Thomas . . . . . . . CB-P.19 MONPsaltis, Demetri . . . . . . . . . . . CL-5.3 THU,
CL-5.5 THUPu, Minhao . . . . . . . . . . . . . . �CK-5.2 MONPuchkova, Anastasiya . . . . �CL-P.18 SUN,
EH-6.2 THUPucker, Georg . . . . . . . . . . . . EA-P.32 THUPuerto, Daniel . . . . . . . . . . . .CM-P.20 SUNPugliese, Diego . . . . . . . . . . . CE-P.24 TUEPugžlys, Audrius . . . . . . . . . . .CA-3.3 SUN,
CD-4.5 SUN, CF-2.1 TUE, CF-2.4 TUE,CF-3.5 TUE
Pujol, Maria Cinta . . . . . . . . CE-P.13 TUEPulci, Olivia . . . . . . . . . . . . . . . .CC-P.6 SUNPullen, Michael . . . . . . . . . . . �CG-3.4 WEDPullen, Michael G. . . . . . . . . CG-3.2 WED,
CG-5.5 WEDPupeza, Ioachim . . . . . . . . . . CJ-8.1 WED,
CG-P.12 THU, CF-9.2 THUPurlys, Vytautas . . . . . . . . .�CK-P.10 MONPurnawirman, Purnawirman�CK-12.2 WEDPusch, Tobias CB-2.1 TUE, �CB-2.2 TUEPusino, Vincenzo . . . . . . . . . . .CD-P.4 TUEPustelny, Szymon . . . . . . . . . CH-P.18 THUPutnam, William . . . . . . . . .�EE-5a.3 MONPutzer, Philipp . . . . . . . . . . . CH-9.6 WED,
CJ-12.3 THUPuust, Laurits . . . . . . . . . . . . . . CL-P.3 SUNPuzyrev, Dmitry . . . . . . . . . . . EF-P.4 THUPyragaite, Viktorija . . . . . . . �EF-6.2 MONPyrkov, Yurii . . . . . . . . . . . . . . CH-P.1 THUPysz, Dariusz . . . . . . . . . . . . . CJ-5.4 MON,
CH-P.26 THUQi, Sisheng . . . . . . . . . . . . . . . . CD-1.5 SUN
Qiang, Xiaogang . . . . . . . . . . �EB-5.5 WEDQin, Peng . . . . . . . . . . . . . . . . . . CF-1.4 TUEQiu, W. . . . . . . . . . . . . . . . . . �CK-11.2 WEDQuarterman, Adrian . . . . . . . �CB-3.3 TUE,
CB-3.6 TUEQuélin, Xavier . . . . . . . . . . . CK-P.15 MON,
EG-P.8 MON, EG-7.5 MONQuerasser, Edwin . . . . . . . . . . EB-P.4 WEDQuercioli, Franco . . . . . . . . . CH-P.24 THUquere, fabien . CG-2.6 TUE, CH-8.4 WEDQuidant, Romain . . . . . . . . . .EH-4.3 WED,
EA-10.6 THUQuinlan, Franklin . . . . . . . . . ED-1a.3 MONQuinlan, Franklyn . . . . . . . . . ED-2.5 MONQuiñonez, Erik . . . . . . . . . . . . EH-2.3 WEDQuintero-Bermudez, Rafael �CK-P.8 MONQuiquempois, Yves . . . . . . . . . CJ-3.3 SUN,
CJ-3.5 SUN, CJ-3.6 SUN, CD-12.2 THUQuirce, Ana EF-P.12 THU, EF-P.14 THUR Hill, Ian . . . . . . . . . . . . . . . . ED-P.9 MONR. Petersen, Sidsel . . . . . . . . CJ-P.14 WEDR. Vistas, Cláudia . . . . . . . . �CE-P.26 TUERaabe, Nils . .CF-4.3 WED, �CF-9.4 THURabbani, Hadi . . . . . . . . . . . .CK-12.3 WEDRačiukaitis, Gediminas . . . . .CF-P.4 WED,
CJ-P.39 WEDRácz, Péter CA-P.35 SUN, EG-5b.2 MONRadhakrishnan, Padmanabhan
CE-12.4 WEDRadier, Christophe . . . . . . . . CF-P.20 WEDRading, Linnea . . . . . . . . . . . . CG-1.5 TUE,
CG-P.6 THU, CF-8.2 THURadnatarov, Daba . . . . . . . . �CA-11.3 THURadovanović, Jelena . . . . . . .EF-P.10 THURadwell, Neal . . . . . . . . . . . . . �EC-2.3 TUERadzewicz, Czesław . . . . . . . .CF-P.8 WEDRadziunas, Mindaugas . . . .�CB-P.3 MON,�CB-P.28 MONRafailov, Edik . . . . . . . . . . . . . CA-P.7 SUN,
CM-P.15 SUN, �CC-5.4 MON,CB-3.2 TUE, CF-P.2 WED
Rafailov, Edik U. . . . . . . . . CB-P.22 MON,CC-5.5 MON, CD-P.28 TUE,CE-11.2 WED, CE-11.3 WED
Rahimi-Iman, Arash . . . . . . . .CB-1.1 TUE,CB-3.2 TUE
Rahlves, Maik .CE-8.3 TUE, CL-3.1 THURaicevic, Nevena . . . . . . . . . . �CH-P.8 THURaimond, Jean-Michel . . . . . .EA-P.2 THURaineri, Fabrice . . . . . . . . . . . . EF-2.4 SUN,
CK-10.1 WEDRaj, Rama . . . . . . . . . . . . . . . CK-10.1 WEDRaj, Shasidran . . . . . . . . . . . . . CH-P.3 THURaja, Ahmad . . . . . . . . . . . . . . .CD-1.3 SUNRakić, Aleksandar . . . . . . . . . CH-8.1 WEDRamaiah-Badarla, Venkata . .CD-4.1 SUNRamdane, Abderrahim . . . . . . CI-2.5 SUN,
CB-10.5 THURamirez, Lourdes Patricia . . . CJ-1.3 SUNRamírez, Mariola . . . . . . . . . . EH-P.9 WEDRamirez, Patricia . . . . . . . . . . CB-5.3 WEDRamos, Philippe . . . . . . . . . . . .CA-3.2 SUNRamponi, Roberta . . . . . . . . .CM-P.9 SUN,
CM-4.4 SUN, EB-5.1 WED,EB-5.2 WED, JSV-3.4 THU
Ramsay, Jacob . . . . . . . . . . . . �CH-3.4 SUNRandoux, Stéphane . . . . . . . . EF-5.2 MONRanta, Sanna . . . . . . . . . . . . . . CB-3.1 TUERao, Gottipaty . . . . . . . . . . . .�CN-2.5 WEDRarity, John . . . . . . . . . . . . . EG-P.16 MON,
JSV-P.8 MON, EB-4.2 WED,�EA-8.4 WED, CH-9.4 WEDRaserbat-Plantey, Antoine . JSIV-2.5 SUNRaskar, Ramesh . . . . . . . . . . . CN-2.4 WEDRastogi, Vipul . . . . . . . . . . . . . . CI-P.4 TUERattunde, Marcel . . . . . . . . . .CB-P.7 MONRau, Markus . . . . . . . . . . . . . . EB-4.1 WEDRauch, Simon . . . . . . . . . . . . .CB-5.6 WED,�CB-8.4 THURausch, Stefan . . . . . . . . . . . CF-P.19 WEDRauschenbach, Bernd . . . . . . .CH-4.5 SUNRauschenbeutel, Arno . . . . . . EA-2.2 SUN,
EA-2.5 SUN, �CH-2.3 SUNRauter, Patrick . . . . . . . . . . . . �CC-2.6 SUNRavaro, Marco . . . . . . . . . . . . .�CC-4.5 SUNRavi, Koustuban . . . . . . . . . . . �CC-3.3 SUNRaya, Angel . . . . . CLEO/ECBO-1.2 WEDRaybaut, Myriam . . . . . . . . . . CD-2.3 SUN,
CD-P.36 TUE, CN-1.1 WEDRaybould, Tim A. . . . . . . . . . . �EI-1.4 THURaymer, Michael G. . . . . . . .EB-2a.2 MONRazdobreev, Igor . . . . . . . . . .CE-P.14 TUE,
CE-P.15 TUERazskazovskaya, Olga . . . . . . CG-1.3 TUE,
CF-7.5 THU, CG-P.3 THURazzari, Luca CD-7.4 MON, CC-6.5 TUE,
EA-6.5 TUEReboud, Julien . . . . . . . . . . . JSII-2.4 MONReboud, Vincent . . . . . . . . . . CB-11.1 THURechtsman, Mikael . . . . . . . JSIV-P.1 TUERechtsman, Mikael C. . . . . CK-13.1 WEDRedding, Brandon . . . . . . . . ED-1b.2 MONReddy, Dileep V. . . . . . . . . . EB-2a.2 MONRedeker, Kai . . . . . . . . . . . . . . EB-4.3 WED,�EB-P.12 WEDRedondo, Javier . . . . . . . . . . CH-P.21 THUReed, Bryan W. . . . . . . . . . . . EH-2.3 WEDReed, Graham . . . . . . . . . . . . . . CE-4.3 SUNRegelskis, Kestutis . . . . . . . �CF-P.4 WED,
CJ-P.39 WEDRegensburger, Alois . . . . . . . . .EF-2.3 SUNRehault, Julien . . . . . . . . . . . .EG-7.6 MON,
CD-13.2 THUReichel, Jakob . . . . . . . . . . . . . CH-1.2 SUNReichel, Volker . . . . . . . . . . . . . CJ-4.5 SUNReichert, Fabian . . . . . . . . . . . CA-8.2 TUE,�CA-10.2 THUReichert, Moritz . . . . . . . . . . EA-P.17 THUReid, Derryck . . . . . . . . . . . . �CN-2.1 WED,
PD-A.6 WED, CD-11.4 THUReid, Derryck T. . . . . . . . . . . ED-P.6 MONReigue, Antoine . . . . . . . . . . . . EC-1.3 TUEReijn, Saara-Maarit . . . . . . . . �CH-1.3 SUNReilly, Sean . . �CA-1.3 SUN, CA-8.4 TUEReimer, Christian . . . . . . . . . . EA-6.5 TUE,
EA-7.3 TUE, PD-B.9 WEDReinhardt, Carsten . . . . . . . CK-P.22 MONReinlein, Claudia . . . . . . . . . . .CM-4.1 SUNReitzenstein, Stephan . . . . . . CB-1.1 TUE,
EA-8.3 WED, EA-8.5 WED
221
Authors’ Index
Rekstyte, Sima . . . . . . . . . . . . CM-1.2 SUN,CM-1.5 SUN, �CM-P.13 SUN
Rempe, Gerhard . . . . . . . . . . . EA-2.1 SUN,EC-2.5 TUE, EA-P.6 THU
Ren, Xiaomin . . . . . . . . . . . . CE-5a.3 MON,CE-6.4 MON, CE-P.18 TUE,CE-P.29 TUE
Ren, Yuan . . . .CC-2.3 SUN, CC-2.5 SUN,CC-P.14 SUN, CB-6.4 WED
Renard, William . . . . . . . . . . . CJ-12.5 THURenato Mendonça, Cleber . . .EE-P.5 SUNRenaud, Cyril . . . . . . . . . . . . . .CC-5.6 MONRenaudat Saint-Jean, Margaux
CC-1.3 SUNRenema, Jelmer J. . . . . . . . . . .EA-6.4 TUERenger, Jan . .EH-4.3 WED, EH-6.3 THUReno, John . . . . . . . . . . . . . . . .CC-5.1 MONRenversez, Gilles . . . . . . . . . . �EF-P.8 THURenz, Günther . . . . . . . . . . . . �CN-P.3 TUEReparaz, Juan Sebastian . . CE-5a.2 MONResan, Bojan CA-6.1 MON, CA-9.1 THU,
CA-9.2 THUResch, Kevin . . . . . . . . . . . . . .EA-10.1 THUResch, Kevin J. . . . . . . . . . . . .EB-1.5 MONResidori, Stefania . . . . . . . . CH-P.12 THU,
EF-P.5 THURessel, Peter . . . . . . . . . . . . . .CB-11.2 THURestoin, Christine . . . . . . . . . CJ-P.49 WEDReuter, Dirk . . . . . . . . . . . . . EG-P.12 MONRéveret, François . . . . . . . . . CE-11.4 WEDRezai, Mohammed . . . . . . . . . .EG-3.3 SUNRezem, Maher . . . . . . . . . . . . . .CE-8.3 TUERicciardi, Iolanda . . . . . . . . . . CD-8.2 TUE,�CH-P.36 THURichardson, David . . . . . . . . CD-P.17 TUE,�CJ-12.1 THURichardson, David J. . . . . . . . CJ-9.2 WEDRichter, Daniel . . . . . . . . . . �CM-P.10 SUNRichter, Maria . . . . . . . . . . . . CG-5.4 WED,�CG-P.13 THURichter, Sören . . . . . . . . . . . . CM-6.2 MONRicken, Raimund . . . . . . . . .JSV-P.4 MON,
JSV-2.1 THURico, María L. . . . . . . . . . . . . .CD-6.4 MONRico, Mauricio . . . . . . . . . . . . . CA-2.2 SUNRiede, Andrea . . . . . . . . . . . . CA-12.5 THURiedi, Sabine . . . . . . . . . . . . . . CB-6.2 WEDRiedl, Thomas . . . . . . . . . . . . . �CE-8.1 TUERiedle, Eberhard . . . . . . . . . . . .CF-3.2 TUERiesen, Hans . . . . . . . . . . . . . . . CD-3.1 SUNRiesen, Nicolas . . . . . . . . . . . . . .CI-1.5 SUNRieutors, Francois . . . . . . . . .CB-11.1 THURigaud, Philippe . . . . . . . . . . . . CJ-1.3 SUNRighini, Giancarlo . . . . . . . . .CH-P.24 THURiis, Erling . . . . . . . . . . . . . . . . . EC-P.2 TUERijnders, Guus . . . . . . . . . . . .CM-P.19 SUNRingbauer, Martin . . . . . . . . EB-1.1 MON,�EB-2a.1 MONRingsted, Tine . . . . . . . . . . . . . CH-3.4 SUNRisser, Christophe . . . . . . . . . .CH-P.2 THURistau, Detlev . . . . . . . . . . . EE-5b.2 MON,
CG-4.3 WEDRitchie, David CC-2.3 SUN, CC-2.5 SUN,
CC-P.14 SUN, CB-6.4 WEDRitsch, Helmut . . . . . . . . . . . . .EA-P.8 THU
Ritsch-Marte, Monika�CLEO/ECBO-2.1 WEDRitter, Stephan . . . . . . . . . . . . EA-P.6 THURivas, Daniel . . . . . . . . . . . . . . �CG-1.3 TUERivère, Alice . . . . . . . . . . . . . . EA-P.13 THURivière, Paula . . . . . . . . . . . . . CG-5.4 WEDRizaoglu, Anil . . . . . . . . . . . . . CK-P.3 MONRizvi, Sahrish . . . . . . . . . . . . . JSIV-2.5 SUNRizza, Carlo . . . . . . . . . . . . . . . . EF-1.6 SUNRizzelli, Giuseppe . . . . . . . . . �CI-P.12 TUERizzo, Carlo . . . . . . . . . . . . . . EA-P.13 THURo, Jung Hoon . . . . . . . . . . . . . CE-9.3 TUERobb, Gillian . . . . . . . . . . . . . . . CL-3.4 THURobb, Gordon �EC-P.6 TUE, EC-3.3 TUE,
EF-9.3 THURobert-Philip, Isabelle . . . . . . EF-2.5 SUN,
EA-4.3 SUN, CK-4a.2 MON,CH-5.3 TUE, CK-10.1 WED
Robert, Yannick . . . . . . . . . . . CB-5.2 WEDRoberts, Lyle . . . . . . . . . . . . . �CH-P.3 THURobertson, Mike . . . . . . . . . . .CC-5.6 MONRobin, Thierry . . . . . . . . . . . . CJ-12.5 THURoch, Jean-François . . . . . . .EA-10.3 THURochat, Michel . . . . . . . . . . . . CB-7.3 WEDRochette, Martin . . . . . . . . . . CD-1.3 SUN,
CJ-P.34 WEDRochev, Yury . . . . . . . . . . . . . . CM-2.3 SUNRöder, Robert . . . . . . . . . . . . . CD-P.6 TUERodin, Aleksej . . . . . . . . . . . �CA-P.26 SUNRodrigo, Peter John . . . . . �CH-P.15 THU,
CH-P.34 THURodrigues, José . . . . . . . . . . . .�CE-9.5 TUERodrigues Jr., José Joatan . CH-P.9 THURodrigues, Natercia . . . . . . .CF-P.25 WEDRodriguez, Ainara . . . . . . . . . CE-P.27 TUERodriguez, Alejandro . . . . . . . EF-P.8 THURodriguez-Oliveros, Rogelio . CK-8.2 TUERodriguez, Pedro . . . . . . . . .CB-P.15 MONRodt, Sven . . . . . . . . . . . . . . . . EA-8.5 WEDRoelkens, Gunther . . . . . . . . . CK-7.2 TUE,
EF-7.3 TUERoelli, Philippe . . . . . . . . . . . . �EG-1.4 SUNRoeloffzen, Chris G.H. . . . . . . . CI-4.5 SUNRoesch, Markus . . . . . . . . . . . . CC-2.2 SUNRoeser, Fabian . . . . . . . . . . �CA-P.21 SUN,
CA-9.4 THURoger, Thomas . . . . . . . . . . . . . EF-2.1 SUNRoger, Tom . . . . . . . . . . . . . . . EH-3.4 WEDRogers, Adam . . . . . . . . . . . . CF-P.25 WEDRogers, Edward . . . . . . . . . . . .EH-3.2 WEDRogers, Edward T. F. . . . . . . . CI-1.1 SUN,
EG-3.5 SUNRogge, Sven . . . . . . . . . . . . . . .EA-5.2 MONRohde, Ingo . . . . . . . . . . . . . . �CA-P.28 SUNRöhm, André . . . . . . . . . . . . . �CB-9.3 THURohr, Sven . . . . . . . . . . . . . . . . .CK-2.4 SUNRohrbacher, Andreas . . . . . . CA-6.1 MON,
CA-9.1 THURohwer, Erich . . . . . . . . . . . . CF-P.34 WEDRoither, Stefan . . . . . . . . . . . . EE-4.3 SUN,
CG-6.5 WEDRoke, Sylvie . . . . . . . . . . . . . . . �CL-3.5 THURoland, Iannis . . . . . . . . . . . . . CB-4.3 WEDRoldán, Eugenio . . . . . . . . . . . EF-8.6 TUE,
EF-9.4 THU
Rolland, Antoine . . . . . . . . .ED-1a.3 MON,ED-2.5 MON
Romanelli, Marco . . . . . . . . . �EF-2.2 SUN,�CA-P.20 SUN, �CI-5.5 MON,�CN-1.4 WED, �EF-P.1 THURomanini, Daniele . . . . . . . . . .CH-2.5 SUNRomanov, Alexey N. . . . . . . .CE-P.25 TUERomanov, Sergei . . . . . . . . CK-P.35 MON,�EH-P.6 WEDRomanova, Alexandra . . . . CK-P.35 MONRomeira, Bruno . . . . . . . . . . . �CI-5.2 MONRomuald, Houdré . . . . . . . . . CK-14.5 THURonning, Carsten . . . . . . . . . . CD-P.6 TUERonzani, Alberto . . . . . . . . . . CB-6.4 WEDRopers, Claus . . . . . . . . . . . .EG-5a.1 MON,
EG-5a.2 MONRoque, Pablo M. de . . . . . . . . EG-4.5 SUNRosa, Tiago . . . . . . . . . . . . . . . . CL-P.1 SUNRosales, Jose Luis . . . . . . . . . EB-4.4 WEDRösch, Markus �CC-2.1 SUN, CC-2.4 SUNRose, P. . . . . . . . . . . . . . . . . . . . CD-2.1 SUNRosei, Federico . . . . . . . . . . . CE-5a.1 MONRoselló-Mechó, Xavier . . . . CH-P.32 THURosen, Shamir . . . . . . . . . . . . CD-11.5 THURosencher, Emmanuel . . . . . . CD-8.6 TUERosenfeld, Wenjamin . . . . . . EB-4.3 WED,
EB-P.12 WEDRosenman, Gil . . . . . . . . . . . . . .CL-P.9 SUNRosenthal, Eric . . . . . . . . . . . . . EE-2.1 SUNRoslund, Jonathan . . . . . . . . ED-P.4 MON,�ED-1b.3 MON, EB-P.6 WED,
EB-P.8 WEDRoso, Luis . . . . . . . . . . . . . . . .CG-P.10 THURoss, Ian . . . . . . . . . . . . . . . . . . CG-P.1 THURossell, Marta D. . . . . . . . . . . CD-P.1 TUERossi, Giuliano . . . . . . . . . . . . . CL-P.1 SUNRossi, Giulio Maria . . . . . . . . . CG-P.4 THURossi, Matteo . . . . . . . . . . . . . EB-P.9 WEDRosskopf, Jürgen . . . . . . . . . . . CB-2.3 TUERota Nodari, S. . . . . . . . . . . . EF-P.17 THURotenberg, Nir EG-3.2 SUN, EG-4.1 SUN,
EG-4.2 SUN, EF-6.6 MON, CD-P.5 TUE,EH-1.3 WED
Rotermund, Fabian . . . . . . . . CC-P.3 SUN,CE-P.6 TUE, CJ-P.23 WED,CF-4.5 WED, CA-9.5 THU
Roth, Bernhard CE-8.3 TUE, CL-3.1 THURothhadt, Jan . . . . . . . . . . . . . CG-2.5 TUERothhardt, Jan . . . . . . . . . . . �CG-3.1 WED,
CF-8.1 THURothhardt, Manfred . . . . . . . . CJ-9.5 WEDRotter, Stefan . . . . . . . . . . . .EH-P.15 WEDRottwitt, Karsten . . . . . . . . . . . CJ-2.5 SUNRotundo, Fabio . . . . . . . . . . . . CM-2.5 SUNRouchon, Denis . . . . . . . . . . . CB-11.1 THURougier, Sébastien . . . . . . . . CJ-P.49 WEDRousseaux, Benjamin . . . . . . EG-P.3 MONRoussignol, Philippe . . . . . . . . EG-3.4 SUNRouzée, Arnaud . . . . . . . . . . . . CG-1.4 TUERoy, Philippe . . . . . . . . . . . . . CJ-P.49 WEDRoy, Tapashree . . . . . . . . . . . . EH-3.2 WEDRoyon, Romain . . . . . . . . . . . . CJ-9.3 WEDRózanowski, Krzysztof . . . . . CH-6.3 WEDRozema, Lee . . . . . . . . . . . . . �EB-1.2 MON,�EB-5.4 WED
Rozhin, Alex . . . . . . . . . . . . . . CF-P.6 WEDRoztocki, Piotr . . . . . . . . . . . . EA-7.3 TUE,
PD-B.9 WEDRozzi, Carlo Andrea . . . . . . . EG-7.6 MONRUAUDEL, Josselin . . . . . . . . EA-1.1 SUNRubino, Eleonora . . . . . . . . . . . EE-3.3 SUNRuchon, T . . . . . . . . . . . . . . . . . CF-8.5 THURuchon, Thierry . . . . . . . . . . . CG-6.1 WEDRudawski, Piotr . . . . . . . . . . . CG-1.5 TUE,
CF-6.2 THU, CG-P.6 THU, CF-8.2 THURudé, Miquel . . . . . . . . . . . . . �EH-4.3 WEDRudenkov, Alexander . . . . . . �CA-9.3 THURudner, Mark S. . . . . . . . . . CK-13.1 WEDRuehl, Axel . . . CA-4.2 SUN, CF-1.6 TUERuesink, Freek . . . . . . . . . . . . �EG-6.3 MONRuf, Hartmut . . . . . . . . . . . . . .CG-6.2 WEDRühl, Eckart . . . . . . . . . . . . . EG-5b.1 MONRuhnke, Norman . . . . . . . . . �CB-P.6 MONRuitenbeek, Thomas . . . . . .EB-P.13 WEDRuiz-Rivas, Joaquín . . . . . . . . EF-8.6 TUE,�EF-9.4 THURumpel, Martin . . . . . . . . . . .�CA-7.3 MONRuncorn, Tim Howard . . . . . . CJ-9.6 WEDRuncorn, Timothy . . . . . . . . . �CD-1.4 SUNRunge, Antoine F. J . . . . . . . �EF-3.1 SUN,
CJ-P.35 WEDRupp, Philipp . . . . . . . . . . . . EG-5b.1 MONRusak, Evgenia . . . . . . . . . . . CK-6.3 MON,
EH-5.1 THURußbüldt, Peter . . . . . . . . . . CE-10.3 WEDRusetsky, Grigory . . . . . . . . . EF-P.15 THURussell, Nicholas J. . . . . . . . .PD-B.3 WEDRussell, Philip CD-1.1 SUN, EE-1.2 SUN,
CD-9.1 TUE, PD-A.9 WED,PD-B.2 WED, �CD-12.1 THU,CG-P.11 THU
Russell, Philip St. J. . . . . . . . EE-1.1 SUN,EF-6.5 MON, CD-P.10 TUE,CD-P.39 TUE, PD-A.7 WED
Russell, Phillip St.J . . . . . . . . . .CI-3.3 SUNRusteika, Nerijus . . . . . . . . . CE-P.35 TUE,
CF-P.15 WEDRusu, Spiridon . . . . . . . . . . . CB-P.25 MONRutkauskas, Marius . . . . . . �CD-11.4 THURutkowska, Katarzyna . . . . . . EF-8.4 TUERütz, Helge . . . . . . . . . . . . . �JSV-P.1 MONRyabchun, Alexandr . . . . . . �CE-P.17 TUERyabova, Anastasiya . . . . . . . . CL-P.3 SUNRyabushkin, Oleg . . . . . . . . . CE-P.21 TUE,
CE-P.23 TUERybarczyk, Théo . . . . . . . . . . . EA-P.2 THURybin, Maxim . . . . . . . . . . . . CA-11.1 THURyczkowski, Piotr . . . . . . . . . . CF-6.3 THURygula, Anna . . . . . . . . . . . . .CH-P.18 THURytz, Daniel . . . . . . . . . . . . . . CE-P.13 TUERyu, Soichiro . . . . . . . . . . . . . . �CE-2.1 SUNSaari, Sampo . . . . . . . . . . . . . .CH-7.5 WEDSabah, Cumali . . . . . . . . . . . . CE-P.11 TUESabbar, Mazyar . . . . . . . . . . . .CG-4.1 WEDSacher, Joachim . . . . . . . . . �CB-5.6 WED,
CB-8.4 THUSada, Cinzia . . . . . . . . . . . . . . CD-6.6 MONSadot, Dan . . . . . . . . . . . . . . . . CI-P.15 TUESadzak, Nikola . . . . . . . . . . . .�EG-7.4 MONSagnes, Isabelle . . . . . . . . . . . . EF-2.4 SUN,
CK-4a.2 MON, EF-8.1 TUESahin, Döndü . . . . . . . . . . . . . . EA-6.4 TUESahin, Ramazan . . . . . . . . . . CM-7.1 MONSahm, Alexander . . . . . . . . . . CB-P.9 MONSahu, Jayanta . . . . . . . . . . . . . .CJ-3.2 SUN,
CJ-P.29 WED, CJ-P.30 WED,CJ-P.33 WED, CJ-12.1 THU,CJ-14.3 THU
Sahu, Jayanta Kumar . . . . . . CJ-9.2 WEDSaito, Mitsunori . . . . . . . . . . CK-P.17 MONSaito, Nobuo . . . . . . . . . . . . . . . .CI-3.5 SUNSaito, Norihito . . . . . . . . . . . . CA-P.36 SUNSaitoh, Kunimasa . . . . . . . . . CK-P.7 MONSaitzek, Sebastien . . . . . . . . . CC-P.17 SUNSakaguchi, Yuki . . . . . . . . . . �CJ-P.47 WEDSakaidani, Takahide . . . . . . . EA-P.22 THUSakakibara, Youichi . . . . . . . . CJ-4.4 SUN,
CJ-P.4 WEDSakakura, Masaaki . . . . . . . . CM-6.1 MONSakamoto, Takahide . . . . . . . �CI-P.3 TUE,
CI-P.11 TUE, CF-P.10 WEDSakat, Emilie . . . . . . . . . . . . . . EH-5.5 THUSakharov, Aleksey . . . . . . . . CE-11.3 WEDSakharov, Alexey V . . . . . . . CE-11.2 WEDSala, Filip . . . . . . . . . . . . . . . . . . EF-8.4 TUESala, Massimiliano . . . . . . . . EA-P.32 THUSala, Tommaso . . . . . . . . . . . �CH-2.5 SUN,
ED-3.5 MONSalakhutdinov, Vsevolod . . . �EA-P.4 THUSalamu, Gabriela . . . . . . . . �CA-P.29 SUN,
CA-5b.2 MON, CA-10.4 THUSalazar-Serrano, Luis Jose . �CH-6.6 WEDSaleh, Khaldoun . . . . . . . . . . CD-10.1 TUESaleh, Mohammed . . . . . . . �CD-12.3 THUSalem, Abdallah . . . . . . . . . . . .CL-5.4 THUSales, Salvador . . . . . . . . . . . . CH-6.6 WEDSalffner, Katharina . . . . . . . . �CH-2.1 SUNSalières, P . . . . . . . . . . . . . . . . �CF-8.5 THUSalmi, Joel . . . . . . . . . . . . . . .CB-P.26 MONSalomon, Christophe . . . . . . .CH-9.2 WEDSalut, R. . . . . . . . . . . . . . . . . . CK-11.2 WEDSalut, Roland . . . . . . . . . . . . . CM-7.2 MONSalvestrini, Jean-Paul . . . . . CE-11.4 WEDSamarelli, Antonio . . . . . . . . .EH-5.5 THU,
CK-14.2 THUSampaolo, Angelo . . . . . . . . . . CH-3.1 SUNSamsonova, Elena . . . . . . . . . . CL-P.3 SUNSamsonova, Zhanna . . . . . . . �CD-P.6 TUESan-Martín, Daniel . . . . . . . . EF-P.11 THUSanchez Bautista, Enrique . CD-6.5 MONSánchez, Daniel . . . . . . . . . . . CA-4.3 SUN,
CF-P.19 WEDSánchez-García, Laura . . . . �EH-P.9 WEDSánchez Muñoz, Carlos . . . .EA-P.20 THUSand, Johan CD-1.2 SUN, �CN-2.3 WEDSandoghdar, Vahid . . . . . . . . .EG-3.1 SUN,
EG-3.2 SUN, EG-6.1 MON, EA-5.3 MONSanduta, Ana . . . . . . . . . . . . CB-P.25 MONSangalli, Davide . . . . . . . . . . JSIV-1.5 SUNSanghera, Jas . . . . . . . . . . . . . CM-P.8 SUNSangouard, Nicolas . . . . . . . . EB-1.4 MONSanhedrai, Hillel . . . . . . . . . . . .EA-7.5 TUESanner, Nicolas . . . . . . . . . . CM-5b.2 MONSansone, Giuseppe . . . . . . . �CG-3.5 WED,
CF-8.4 THU
222
Authors’ Index
Sansoni, Linda . . . . . . . . . . . . CM-4.4 SUN,�JSV-P.4 MON, EB-5.1 WED,JSV-2.1 THU
Santagati, Raffaele . . . . . . . . .EA-6.1 TUE,JSV-1.1 THU, �JSV-4.1 THU
Santamaria, Luigi . . . . . . . . . .CD-8.2 TUE,CH-P.36 THU
Santarelli, Giorgio . . . . . . . . . .CC-2.2 SUN,CJ-9.3 WED, CF-6.4 THU,CH-P.33 THU
Santerelli, Giorgio . . . . . . . . . CJ-11.1 THUSantinelli, Andrea . . . . . . . . . . CM-4.4 SUNSantos, Francisco . . . . . . . . . . .CE-9.5 TUESapienza, Riccardo . . . . . . . . . EH-6.3 THUSaraceno, Clara . . . . . . . . . . . CJ-8.4 WED,
CH-8.2 WEDSaraceno, Clara J. . . . . . . . . . . CF-9.3 THUSaraceno, Clara Jody . . . . . . CA-6.1 MONSaravi, Sina .CK-P.8 MON, �CD-8.1 TUESarkar, Mitradeep . . . . . . . . . . CL-4.3 THUSartorius, Thomas . . . . . . . . CE-10.3 WEDSasaki, Masahide . . . . . . . . . EA-P.25 THU,
EA-P.28 THU, JSV-4.1 THU,JSV-4.5 THU
Sassermann, Mathias . . . . . �EG-6.6 MONSassi, Ugo . . . . . . . . . . . . . . . .EE-5a.2 MONSato, Atsushi . . . . . . . . . . . . . . CC-P.7 SUNSato, Hidetoshi . . . . . . . . . . . . .CL-4.4 THUSato, Shunsuke . . . . . . . . . . . CG-P.14 THUSato, Takeshi . . . . . . . . . . . . . CG-P.15 THUSato, Tomonari . . . . . . . . . . . . CK-3.3 SUNSato, Yasuaki . . . . . . . . . . . . . . CE-8.4 TUESato, Yoichi . . . . . . . . . . . . . . . �CA-P.8 SUNSatoshi, Wada . . . . . . . . . . . . CD-P.37 TUESattler, Bettina . . . . . . . . . . . CJ-10.3 WEDSaule, Tobias . . . . . . . . . . . . . �CJ-8.1 WED,
CG-P.12 THUSauter, Fabian . . . . . . . . . . .CB-P.18 MON,
CB-3.4 TUESautter, Juergen . . . . . . . . . . CK-6.3 MON,
EH-5.1 THUSauvan, Christophe . . . . . . . CD-P.34 TUESavel’ev, Andrei . . . . . . . . . . . . .EI-2.6 THUSavelii, Inna . . . . . . . . . . . . . . . . CE-1.1 SUNSavenko, Ivan . . . . . . . . . . . . . . CB-1.1 TUESavinov, Vassili . . . . . . . . . . �EA-P.23 THUSavitski, Vasili CA-1.3 SUN, �CA-8.4 TUESavona, Vincenzo . . . . . . . .CK-P.36 MON,
CK-P.37 MONSavostianova, Nadja A. . . . .PD-B.8 WEDSavva, Kyriaki . . . . . . . . . . . . CM-7.3 MONSavvidis, Pavlos . . . . . . . . . . . . EF-9.2 THUSawada, Ryohto . . . . . . . . . .�CG-P.15 THUSawada, Ryota . . . . . . . . . . . .CA-6.2 MON,
EA-P.12 THUSayinc, Hakan . . . . . . . . . . . . . CE-2.4 SUN,
CJ-P.42 WEDSayrin, Clément . . . . . . . . . . . . EA-2.5 SUNScaiano, Tito . . . . . . . . . . . . . . CM-P.2 SUNScalari, Giacomo . . . . . . . . . . .CC-2.1 SUN,
CC-2.2 SUN, CC-2.4 SUN, �EH-4.6 WEDScalora, Michael . . . . . . . . . . . CK-1.6 SUN,
CK-8.6 TUE, EH-7.4 THUScamarcio, Gaetano . . . . . . . . CH-3.1 SUNScarcella, Carmello . . . . . . . . . .CJ-1.4 SUN
Schädler, Kevin . . . . . . . . . . . . �EG-1.2 SUNSchaedler, Kevin . . . . . . . . . . JSIV-2.5 SUNSchäfer, Michael . . . . . . . . . . . CJ-7.2 WEDSchäfer, Sascha . . . . . . . . . . EG-5a.1 MONSchäferling, Martin . . . . . . . . EH-1.2 WEDSchäffler, Friedrich . . . . . . . . CK-P.5 MONSchanne-Klein, Marie-Claire�CL-P.12 SUN, �CL-3.3 THUSchartner, Erik . . . . . . . . . . . . CH-5.6 TUE,�CL-5.4 THUSchaub, Emmanuel . . . . . . . . . CL-3.2 THUSchauss, Jakob . . . . . . . . . . . EG-5a.1 MONSchell, Andreas . . . . . . . . . . CK-P.12 MONSchell, Andreas W. . . . . . . . . CK-2.2 SUN,
EG-7.4 MONSchemme, Thomas . . . . . . �CK-P.41 MONScheucher, Michael . . . . . . . . . EA-2.2 SUNScheuermann, Julian . . . . . . . CB-6.1 WEDSchibli, Thomas R . . . . . . . ED-1b.1 MON,
CH-9.1 WEDSchiek, Roland . . . . . . . . . . . JSV-2.3 THU,
EF-P.21 THUSchiemangk, Max . . . . . . . . CB-P.12 MONSchiller, Stephan . . . . . . . . . �ED-2.4 MON,
ED-P.9 MON, �ED-3.4 MONSchilling, Christian . . . . . . . . .CN-2.2 WEDSchilling, Ryan . . . . . . . . . . . . . EA-4.2 SUNSchilt, Stéphane . . . . . . . . . . CA-6.1 MON,
CH-8.2 WED, �CB-7.3 WEDSchimmel, Guillaume . . . . . . CB-5.3 WEDSchimpf, Damian . . . . . . . . . . . CC-3.3 SUNSchlederer, Benedikt . . . . . . . .CK-2.3 SUNSchlosser, Malte . . . . . . . . . . . .CC-6.6 TUESchlosser, Peter . . . . . . . . . . . . CB-3.5 TUESchmaltz, Felix . . . . . . . . . . . . .EC-P.8 TUESchmeissner, Roman . . . . . .ED-1b.3 MONSchmid, Karl . . . . . . . . . . . . . . . CG-2.4 TUESchmidt, Bruno E. . . . . . . . . .CG-6.2 WEDSchmidt, Christian . . . . . . . . . EH-5.5 THUSchmidt, Frank . . . . . . . . . . . . EA-8.5 WEDSchmidt, Markus . . . . . . . . . . PD-A.8 WEDSchmidt, Ronny . . . . . . . . . . . EA-8.5 WEDSchmitt, Annika . . . . . . . . . . CM-6.2 MONSchmitt-Sody, Andreas . . . . . EE-P.1 SUN,�CF-P.23 WEDSchmool, David . . . . . . . . . . CF-P.31 WEDSchnauber, Peter . . . . . . . . . . EA-8.5 WEDSchneeweiss, Philipp . . . . . . . . EA-2.5 SUNSchneider, Christian . . . . . . . CB-1.1 TUE,
EA-8.3 WED, EA-8.4 WED, EA-P.5 THUSchneider, Hans Christian .CB-P.29 MONSchneider, Katharina . . . . . . . EA-2.1 SUNSchneider, Philipp . . . . . . . . . . CH-2.1 SUNSchneider, Ulrich . . . . . . . . . .�EB-5.3 WEDSchoenhuber, Sebastian . . . . �CC-1.4 SUNSchöffler, Markus . . . . . . . . . . EE-4.3 SUN,
CG-6.5 WEDScholle, Karsten . . . . . . . . . . CB-P.7 MON,
CJ-7.2 WEDSchöning, Michael J. . . . . . . . CL-P.8 SUNSchötz, Gerhard . . . . . . . . . . .CA-P.21 SUNSchötz, Johannes . . . . . . . . . . CG-4.4 WEDSchrader, Sigurd . . . . . . . . . .CE-P.17 TUE,
CH-P.10 THUSchramm, Ulrich . . . . . . . . . CA-P.21 SUN,
CA-9.4 THUSchreiber, Thomas . . . . . . . . . CJ-4.5 SUN,
CJ-8.2 WED, CJ-P.17 WED,CJ-10.3 WED, CJ-10.6 WED,CJ-11.3 THU, CJ-11.4 THU
Schrempel, Frank . . . . . . . . . . CD-2.2 SUNSchrenk, Bernhard . . . . . . . . EB-4.4 WED,
EB-4.5 WED, EB-P.4 WEDSchrenk, Werner . . . . . . . . . . . CC-1.4 SUNSchriber, Cinia . . . . . . . . . . . . . CF-9.3 THUSchröder, Hartmut . . . . . . . . . CG-1.3 TUESchröder, Tim . . . . . . . . . . . �JSV-4.4 THUSchröder-Turk, Gerd . . . . . . . . CE-3.4 SUNSchroeder, Carl . . . . . . . . . �JSIII-1.3 MON,
JSIII-1.4 MONSchröter, Claus Dieter . . . . .CG-3.4 WED,
CG-5.5 WEDSchubert, Elise . . . . . . . . . . . CD-P.14 TUE,�CD-P.33 TUESchug, Michael . . . . . . . . . . . . EA-9.3 THUSchulte, Carsten . . . . . . . . . . . . CE-4.4 SUNSchultze, Marcel . . . . . . . . . . �CG-2.1 TUE,
CA-10.1 THUSchulz, Sabastian . . . . . . . . .CK-11.1 WEDSchulze, Christian . . . . . . . . . . CH-2.4 SUNSchulze, Jan-Hindrik . . . . . . . EA-8.5 WEDSchuneamann, Peter G. . . . . .CD-4.1 SUNSchunemann, P. G. . . . . . . . . . CD-4.3 SUNSchunemann, Peter . . . . . . . CD-10.5 TUESchunk, Gerhard . . . . . . . . . . �EB-3.1 WEDSchütte, Bernd . . . . . . . . . . . . . CG-1.4 TUESchwab, Christian . . . . . . . . . CH-7.4 WEDSchwartz, Sylvain . . . . . . . . . . EC-2.4 TUE,
CH-5.1 TUESchwartz, Tal . . . . . . . . . . . . �CK-6.4 MONSchwarz, Alexander . . . . . . . . CF-7.5 THU,�CG-P.3 THUSchwarzbäck, Thomas . . . CB-P.16 MON,
CB-P.18 MON, CB-3.4 TUESchwefel, Harald G. L. . . . . .EB-3.1 WED,�CH-P.23 THUSchweitzer, Susanne . . . . . . . EI-3a.1 THUSchwemmer, Christian . . . . . EB-1.3 MONSchweyer, Sebastian . . . . . . .CH-9.6 WED,�CJ-12.3 THUSchwob, Catherine . . . . . . . . .EH-P.2 WEDSciamanna, Marc . . . . . . . . . .EF-6.1 MON,
CB-8.5 THUSciarrino, Fabio . . . . . . . . . . . CM-4.4 SUN,
EA-7.1 TUE, EB-5.1 WED,EB-5.2 WED, JSV-2.2 THU,EA-P.27 THU, JSV-3.2 THU,JSV-3.4 THU
Scol, Florent . . . . . . . . . . . . . . . .CJ-3.3 SUNScopigno, Tullio . . . . . . . . . �CE-12.6 WEDScotognella, Francesco . . . . CM-P.9 SUN,
EE-P.7 SUN, JSIV-1.3 SUNScrinzi, Armin . . . . . . . . . . . . . CG-4.2 WEDSears, Chris . . . . . . . . . . . . . . . . CG-2.4 TUESeassal, Christian . . . . . . . . . . .JSI-1.5 SUNSeddon, A. . . . . . . . . . . . . . . . . CJ-7.2 WEDSederberg, Shawn . . . . . . . . . . CF-7.5 THUSedlmeir, Florian . . . . . . . . . . EB-3.1 WED,
CH-P.23 THUSeeds, Alwyn CC-5.6 MON, CB-9.2 THU
Segev, Mordechai . . . . . . . . JSIV-P.1 TUE,CK-13.1 WED
Segonds, Patricia . . . . . . . . . .CE-P.13 TUESei, Tomoaki . . . . . . . . . . . . . CM-6.1 MONSeidel, Marcus . . . . . . . . . . . CA-P.12 SUN,
CA-P.34 SUN, �CD-8.4 TUE,�CD-P.18 TUE, PD-A.1 WED,�CA-10.3 THU, CA-10.5 THUSeiffert, Lennart . . . . . . . . . . EG-5b.1 MONSeifried, Marc . . . . . . . . . . . . . EA-8.5 WEDSekikawa, Taro . . . . . . . . . . . �EE-P.18 SUNSekine, Norihiko . . . . . . . . . . CC-P.11 SUN,
CF-P.10 WEDSeletskiy, Denis V. . . . . . . . EE-5a.1 MON,
ED-P.7 MON, EG-P.14 MONSeleznev, Leonid V. . . . . . . . . CN-P.4 TUESelimis, Alexandros . . . . . . . �CM-1.3 SUN,
CE-3.3 SUNSellers, Andrew . . . . . . . . . . .CF-P.25 WEDSellés, Julien . . . . . . . . . . . . . . CB-4.3 WEDSelmi, Foued EF-4a.3 MON, �EF-8.1 TUESelva, Marco . . . . . . . . . . . . . . CM-3.1 SUNSelvaraja, Shankar Kumar . �CK-P.2 MONSemenov, Sergey . . . . . . . . . . . CJ-3.1 SUNSemenova, Elizaveta . . . . . . . CK-3.2 SUN,
CK-5.2 MONSemond, Fabrice . . . . . . . . . . .CB-4.3 WEDSen, Ranjan . . . . . . . . . . . . . . . CH-P.6 THUSenel, Cagri . . . . . . . . . . . . . . . . CJ-2.6 SUNSenellart, Pascale . . . . . . . . . . EA-9.6 THUSenftleben, Arne . . . . . . . . . . CG-3.4 WED,
CG-5.5 WEDSennaroglu, Alphan . . . . . . . CA-12.4 THUSentenac, Anne . . . . . . . . . . CK-11.3 WEDSenthil Murugan, Ganapathy
CK-10.6 WED, CJ-P.27 WEDSentis, Marc . . . . . . . . . . . . . CM-5b.2 MONSergeyev, Anton . . . . . . . . . . . �CD-2.2 SUNSergienko, Alexander . . . . . �EB-P.11 WEDSerna, Rosalia . . . . . . . . . . . . . CE-6.2 MONSerna, Samuel . . . . . . . . . . . CD-5a.1 MON,
CD-P.34 TUESerpengüzel, Ali . . . . . . . . . . . . CL-P.8 SUNSerra, Enrico . . . . . . . . . . . . . . . EA-4.5 SUNSerres, Josep Maria . . . . . . �CA-P.31 SUN,�CA-4.5 SUN, CA-5a.1 MON,
CA-5a.2 MON, CA-5b.3 MONSessions, Neil . . . . . . . . . . . . .CJ-P.27 WEDSetzpfandt, Frank . . . . . . . . CK-P.8 MON,�JSV-P.5 MON, CD-8.1 TUE,
CF-P.17 WED, EH-5.3 THU,�JSV-2.3 THU, �EF-P.21 THUSévigny, Benoit . . . . . . . . . . . . CJ-3.3 SUN,�CD-12.2 THUSévillano, Pierre . . . . . . . . . . . �CA-2.3 SUNSewell, Phillip . . . . . . . . . . . . EH-P.18 WEDSewell, Robert J. . . . . . . . . . . �EA-2.3 SUN,�EC-1.4 TUEShadbolt, Peter J. . . . . . . . . .PD-B.3 WEDShaddock, Daniel . . . . . . . . . . CH-P.3 THUShah, Yash . . . CC-2.3 SUN, CC-2.5 SUN,
CC-P.14 SUN, CB-6.4 WEDShaikh, Waseem . . . . . . . . . . . CA-3.6 SUN,
CF-P.25 WEDShaked, Yaakov . . . . . . . . . . . . EA-7.5 TUE
Shakfa, Mohammad Khaled CB-3.2 TUE,�CE-11.6 WEDShalabaeva, Victoria . . . . . . . . CL-P.6 SUNShalaby, Mostafa . . . . . . . . . . CC-P.2 SUN,�CC-P.16 SUN, �CC-3.4 SUNShalaev, Vladimir . . . . . . . . . . CE-3.2 SUN,
CE-P.30 TUEShalm, Lynden K. . . . . . . . . . EB-1.5 MONShamray, Alexander . . . . . . CK-P.13 MONSharapova, Polina . . . . . . . . . . EA-7.4 TUEShardlow, Peter . . . . . . . . . . CJ-P.10 WED,�CJ-P.29 WED, CJ-P.30 WED,�CJ-14.3 THU, �CJ-14.6 THUSharp, Adam . . . . . . . . . . . . . . CM-P.7 SUNSharshavina, Ksenia . . . . . .�CK-11.3 WEDShaw, Ed . . . . . . . . . . . . . . . . . . CB-3.6 TUEShelykh, Ivan . . . . . . . . . . . . . . CB-1.1 TUEShen, Baifen . . . . . . . . . . . . . . . CG-2.4 TUEShen, Li . . . . . . . . . . . . . . . . . . .CH-6.5 WEDShen, Pin-Chun . . . . . . . . . . . .CE-6.1 MONShen, Shyh-Chiang . . . . . . . . PD-A.2 WEDShen, Tien-Lin . . . . . . . . . . . �CE-P.10 TUEShen, Zexiang . . . . . . . . . . . . . . EG-3.5 SUNSheng, Yan . . . . . . . . . . . . . . CD-5b.1 MONShephard, Jonathan D. . . . . . CE-1.5 SUNShepherd, David . . . . . . . . . . CE-7.2 MON,
CD-P.17 TUE, CE-P.3 TUE,CJ-P.3 WED
Sher, Chin-Wei . . . . . . . . . . . .CE-P.10 TUEShi, Hongxing . . . . . . . . . . . . . CJ-13.6 THUShi, Lei . . . . . . . . . . . . . . . . . . . . JSI-1.2 SUNShi, Qiang . . . . . . . . . . . . . . . . . CK-2.2 SUNShi, Xiaohui . . . . . . . . . . . . . . .ED-P.3 MONShi, Yang . . . . . . . . . . . . . . . . . CA-P.18 SUNShigematsu, Kyohhei . . . . . �EE-P.15 SUNShih, Min-Hsiung . . . . . . . . . . CE-P.9 TUE,
CE-P.10 TUEShimizu, Naofumi . . . . . . . . . ED-2.5 MONShimko, Alexander . . . . . . . . . CF-P.3 WEDShimotsuma, Yasuhiko . . . .�CM-6.1 MONShinohara, Yasushi . . . . . . . . CG-P.14 THUShipilo, Daniil . . . . . . . . . . . . . . .EI-2.6 THUShirai, Hideto . . . . . . . . . . . . CF-P.30 WEDShirakawa, Akira . . . . . . . . . . .CA-2.4 SUN,
CA-2.5 SUN, CJ-P.14 WEDShiue, Ren-Jye . . . . . . . . . . . .JSIV-2.3 SUNShkurinov, Alexander . . . . . . . .EI-2.6 THUShlenov, Svyatoslav A. . . . . . CN-P.4 TUEShoji, Ichiro . . . . . . . . . . . . . . CA-11.5 THUShostak, Ivan . . . . . . . . . . . . . .CB-4.5 WEDShramenko, Mikhail . . . . . . . .CB-7.5 WEDShtyrina, Olga . . . . . . . . . . . �CJ-P.40 WEDShugurov, Alexander . . . . . . . .CC-6.1 TUEShum, Perry Ping . . . . . . . . . . . CI-2.3 SUNShum, Ping . . . . . . . . . . . . . . . . .CI-P.2 TUEShumakova, Valentina . . . . . .CF-2.1 TUE,�CF-3.5 TUEShunji, Takekawa . . . . . . . . . CD-P.37 TUEShurygin, Anton . . . . . . . . . . CA-P.41 SUNShvedov, Vladlen . . . . . . . . . . . CL-2.5 THUSi Fodil, Rachid . . . . . . . . . . . . CJ-2.1 SUN,
EF-8.3 TUE, �CJ-P.7 WEDSi, Kye Jye . . . . . . . . . . . . . . . . EH-2.5 WEDŠibalić, Nikola . . . . . . . . . . . . . EA-9.4 THUSibbett, Wilson . . . . . . . . . . CB-P.22 MON
223
Authors’ Index
Sibilia, Concita . . . . . . . . . . .CD-P.21 TUE,CN-P.1 TUE, CK-13.5 WED,EH-5.2 THU
Sibson, Philip . . . . . . . . . . . . �JSV-4.5 THUSiebold, Mathias . . . . . . . . . CA-P.21 SUN,
CA-9.4 THUSiegel, Jan . . . . . . . . . . . . . . CM-5b.3 MONSigaev, Vladimir . . . . . . . . . . CM-6.3 MONSigg, Hans . . . CB-1.4 TUE, CK-9.3 TUE,
CB-11.1 THUSigle, Wilfried . . . . . . . . . . . . . CK-6.2 MONSigletou, Maria . . . . . . . . . . . CM-7.3 MONSigmund, Ole . . . . . . . . . . . . . . CK-9.1 TUESiitonen, Samuli . . . . . . . . . . JSII-2.2 MONSikdar, Debabrata . . . . . . . . .�EH-2.5 WEDSilberberg, Yaron . . . . . . . . �CD-11.5 THUSilberhorn, Christine . . . . . JSV-P.1 MON,
JSV-P.4 MON, EB-2a.2 MON,JSV-1.5 THU, JSV-2.1 THU
Sildos, Ilmo . . . . . . . . . . . . . . . . CL-P.3 SUNSilva, Ana . . . . . . . . . . . . . . . .CF-P.31 WEDSilva, Fernando . . . . . . . . . . . . .EF-8.6 TUESilva, Francisco . . . . . . . . . . . . EE-1.5 SUN,
CG-3.2 WED, CF-P.31 WED,CF-5.3 WED, �CG-P.5 THU,CG-P.7 THU
Silveiro, Ivan . . . . . . . . . . . . . . CL-P.15 SUNSilverstone, Josh W. . . . . . . .JSV-1.1 THUSilverstone, Joshua W. . . . .PD-B.3 WED,
JSV-4.1 THUSilvestre, Enrique . . . . . . . . . . CD-P.9 TUESima, Chaotan . . . . . . . . . . . . . CE-2.3 SUNSima, Felix . . . . . . . . . . . . . CM/LIM.3 TUESimakov, Nikita . . . . . . . . . . CJ-11.6 THU,
CJ-13.2 THUSimbula, Angelica . . . . . . . . . .EA-7.6 TUE,
JSV-1.2 THUSimohamed, Lotfy Mokhtar
CK-P.27 MONSimon-Boisson, Christophe . CA-3.2 SUN,
CF-P.19 WED, CF-P.20 WEDSimon, David . . . . . . . . . . . . EB-P.11 WEDSimon, Peter . . . . . . . . . . . . . CD-P.27 TUESimonelli, Cristiano . . . . . . . .PD-B.5 WEDSimonetta, Marcello . . . . . . . . CC-6.6 TUESimozrag, Bouzid . . . . . . . . . CB-6.3 WED,
CB-11.6 THUSimpson, Robert Edward . . . EH-4.3 WEDSimsek, Ergun . . . . . . . . . . . . CM-7.1 MONSinclair, Gary . . . . . . . . . . . . . EA-P.28 THUSinclair, Josiah . . . . . . . . . . . . .CD-9.2 TUESingh, Anshuman . . . . . . . . . . �EG-4.5 SUNSingh, Gurpreet . . . . . . . . . . CK-12.2 WEDSingh, Harman . . . . . . . . . . . CJ-P.35 WEDSingh, Yeshpal . . . . . . . . . . . �ED-P.9 MONSinitsyn, Dmitry V. . . . . . . . . .CN-P.4 TUESipe, John . EB-1.2 MON, JSV-P.3 MONSiria, Alessandro . . . . . . . . . . . EC-3.4 TUESirigu, Gianluca . . . . . . . . . . �CE-5a.1 MONSirtori, Carlo . . CC-1.3 SUN, CC-2.2 SUNSivan, Vijay . . . . . . . . . . . . . . .CM-6.6 MONSiwicki, Bartłomiej . . . . . . . . �CJ-5.4 MONSkafidas, Efstratios . . . . . . . CH-P.19 THUSkala, Melissa . . . . . . . . . . . . . �CL-2.3 THUSkantzakis, E . . . . . . . . . . . . . . CF-8.5 THU
Skidin, Anton . . . . . . . . . . . . .CJ-P.40 WEDSkliutas, Edvinas . . . . . . . . . . .CM-1.5 SUNSkolnick, Maurice . . . . . . . . . �EB-3.5 WEDSkoptsov, Nikolai . . . . . . . . . . �CE-P.5 TUEŠkorić, Boris . . . . . . . . . . . . . . .EB-4.6 WEDSkryabin, Dmitry . . . . . . . . . . . EF-3.4 SUNSkupin, Stefan . . . . . . . . . . . . . EE-2.5 SUN,
CM-P.21 SUN, EE-P.1 SUN,CM-5a.1 MON
Slablab, Abdallah . . . . . . . . �CE-12.4 WEDSlavik, Radan . . . . . . . . . . . . . CH-6.4 WEDSlepneva, Svetlana . . . . . . . . .CB-7.1 WEDSlight, Thomas J. . . . . . . . . CE-11.3 WEDSliwinska, Dorota . . . . . . . . . . CF-P.5 WEDSlowik, Jay Gates . . . . . . . . . CD-P.14 TUESlussarenko, Sergei . . . . . . . . .EA-7.1 TUE,
EB-3.2 WEDSmektala, Frederic . . . . . . . . .CD-6.1 MONSmerieri, Anteo . . . . . . . . . . . . CI-5.1 MONSmerzi, Augusto . . . . . . . . . . EA-P.27 THUSmetanin, Sergei . . . . . . . . . CA-P.37 SUN,
CA-P.41 SUNSmetanina, Evgeniya Olegovna�CM-5a.2 MONSmilgevicius, Valerijus . . . . . EF-6.2 MON,
CA-11.2 THUSmirnov, Vadim . . . . . . . . . . . . CA-4.3 SUNSmirnova, Olga . . . . . . . . . . . CG-4.2 WED,
CG-5.4 WED, �CG-6.2 WED,CG-P.13 THU
Smirnova, Tatiana . . . . . . . . EF-P.15 THUSmit, Meint . . . CI-2.6 SUN, CK-3.1 SUNSmith, Brian . . . . . . . . . . . . .JSV-P.2 MON,
EA-P.15 THUSmith, Brian J . . . . . . . . . . . . JSV-1.3 THUSmith, David R. . . . . . . . . . . . CK-8.6 TUE,
EH-4.1 WEDSmith, Jason . . . . . . . . . . . . . . �EC-3.2 TUESmith, Jodie . . . . . . . . . . . . . . . CA-3.6 SUNSmith, Lyndsie . . . . . . . . . . . . ED-P.9 MONSmith, Peter . . . . . . . . . . . . . . JSV-3.1 THUSmith, Peter G. R. . . . . . . . . . CE-2.3 SUN,
CE-2.5 SUN, JSV-P.6 MON,JSV-P.7 MON, CE-10.4 WED,CE-10.5 WED, JSV-1.3 THU
Smotlacha, Vladimir . . . . . . . CH-6.4 WEDSmrz, Martin . . . . . . . . . . . . . CA-10.2 THUSnetkov, Ilya . . . . . . . . . . . . . .�CE-7.6 MONSo, Jinkyu EG-5a.3 MON, �CK-6.5 MONSoares, Francisco . . . . . . . . . . �CK-7.1 TUESoavi, Giancarlo . . . . . . . . . . .�EE-P.7 SUN,
EE-P.17 SUN, �JSIV-1.3 SUN,EE-5a.2 MON
Soboleva, Ksenia K. . . . . . . CB-P.22 MONSobon, Grzegorz . . . . . . . . . . . CF-P.5 WEDSoci, Cesare . . CE-2.6 SUN, CK-3.4 SUN,
EG-3.5 SUN, CD-P.11 TUE,CD-P.24 TUE, CI-P.1 TUE, CI-P.2 TUE,CE-12.3 WED, EI-1.3 THU
Soergel, Elisabeth . . . . . . . . . CM-6.6 MONSohler, Wolfgang . . . . . . . . . .EF-P.21 THUSokolovskii, Grigorii . . . . . . . . CA-P.7 SUNSokolovskii, Grigorii S. . . . CB-P.22 MON,
CE-11.2 WEDSola, Inigo . . . . . . . . . . . . . . . CD-5b.1 MON
Sola, Íñigo J. . . . . . . . . . . . . . . CG-P.7 THUSoler Penades, Jordi . . . . . . . �CK-7.2 TUESolinas, Xavier . . . . . . . . . . . . . CF-6.5 THUSolis, Javier . . . . . . . . . . . . . CM-5b.3 MONSolntsev, Alexander . . . . . . . . CD-3.2 SUN,
CD-P.12 TUESolntsev, Alexander S. . . . . . CD-2.2 SUN,
JSV-P.5 MON, JSV-2.3 THUSolomon, Glenn S. . . . . . . . . . EA-P.8 THUSomeya, Ryuta . . . . . . . . . . �CH-P.29 THUSommer, Christian . . . . . . . . . EI-3a.1 THUSommer, Ephraim . . . . . . . . . EG-7.6 MONSon, Jaehyeon . . . . . . . . . . . . . CK-3.5 SUNSon, Seong-Jin . . . . . . . . . . . . . CE-9.3 TUESondermann, Markus . . . . . . EA-P.1 THU,
EA-P.3 THU, EA-P.4 THUSones, Collin CL-P.16 SUN, CL-1.4 WEDSong, Qiyuan . . . . . . . . . . . . . .�CL-4.6 THUSong, Youjian CF-1.4 TUE, �CF-6.6 THU,
CF-9.4 THUSontheimer, Bernd . . . . . . . . .�CK-2.2 SUNSorba, Lucia . . . . . . . . . . . . . . . CF-7.1 THUSorel, Marc JSV-P.3 MON, CD-P.4 TUE,
CK-13.3 WED, CK-14.2 THU,JSV-4.1 THU
Sorensen, Stacey . . . . . . . . . . CG-5.1 WEDSoria, Silvia . . . . . . . . . . . . . . CH-P.24 THUSoriano, Miguel . . . . . . . . . . . .CB-7.2 WEDSoriano, Miguel C. . . . . . . .CB-P.27 MON,
EF-P.11 THUSorin, Fabien . . . . . . . . . . . . . CK-14.6 THUSorokin, Evgeni . . . . . . . . . . . . CJ-7.4 WEDSorokina, Irina . . . . . . . . . . . . CJ-7.4 WED,
CJ-P.32 WEDSorokina, Mariia CI-1.3 SUN, �CI-3.4 SUNSoskind, Michael . . . . . . . . . . CH-8.5 WEDSotelo, Felix . . . . . . . . . . . . . . . . CI-2.4 SUNSotgiu, Giovanna . . . . . . . . . . CL-P.13 SUNSoto-Crespo, Jose-Maria . . . . .EI-2.4 THUSotor, Jaroslaw . . . . . . . . . . . . CF-P.5 WEDSouhaité, Grégoire . . . . . . . . . CN-1.1 WEDSoujaeff, Alexandre . . . . . . . . . CA-3.2 SUNSoukoulis, Costas M. . . . . . . . CE-3.3 SUNSousa, Marilyne . . . . . . . . . . . . CD-P.1 TUESpagnolo, Nicolò . . . . . . . . . . �EA-7.1 TUE,�EB-5.2 WED, �EA-P.27 THU,
JSV-3.4 THUSpagnolo, Vincenzo . . . . . . . . �CH-3.1 SUNSpangenberg, Dirk-Mathys�CF-P.34 WEDSparrow, Chris . . . . . . . . . . . . PD-B.3 WEDSpasibko, Kirill . . . . . . . . . . . . �EA-7.4 TUESpäth, Florian . . . . . . . . . . . . CA-12.5 THUSpelaniak, Izabella . . . . . . . . .CH-7.4 WEDSpence, David . . . . . . . . . . . . . CA-1.5 SUN,
EH-P.12 WEDSpence, David J . . . . . . . . . . . CA-6.5 MONSperling, Jan . . . . . . . . . . . . . . EB-P.8 WEDSpielmann, Christian . . . . . . .CD-P.6 TUE,
CF-8.1 THUSpinicelli, Piernicola . . . . . . . EG-P.8 MONSpring, Justin . . . . . . . . . . . .JSV-P.6 MON,
JSV-3.1 THUSpring, Justin B. . . . . . . . . . JSV-P.7 MON,
JSV-1.3 THUSpringate, Emma . . . . . . . . . . CG-3.3 WEDSpuesens, Thijs . . . . . . . . . . . . . CJ-1.4 SUNSpurrell, Josh . . . . . . . . . . . . . . CJ-9.2 WEDSquier, Jeff . . . . . . . . . . . . . . . �CM-3.3 SUNSreseli, Olga M. . . . . . . . . . . �CK-P.1 MONSrivastava, Sachin Kumar . . �CH-4.5 SUNSrivathsan, Bharath . . . . . . . . EC-2.2 TUE,
EA-6.2 TUESt.J. Russell, Philip . . . . . . . .CJ-12.4 THUStaasmeyer, Jan-Helge . . . . CE-10.3 WEDStabinis, Algirdas . . . . . . . . . . EF-6.2 MONStaedter, David . . . . . . . . . . . .CG-6.1 WEDStaliunas, Kestutis . . . . . . . . . CK-1.4 SUN,
CK-1.5 SUN, CB-P.3 MON,CB-P.4 MON, CK-P.10 MON,EF-8.6 TUE, EH-P.16 WED,CH-P.21 THU
Stanciu, George . . . . . . . . . . . CA-P.32 SUNStańczyk, Tomasz . . . . . . . . �CE-P.28 TUEStandish, Robert . . . . . . . . . .CJ-P.29 WEDStanislauskas, Tomas . . . . . . . CF-2.5 TUEStanislovaitis, Paulius . . . . . . EF-6.2 MONStankovic, Stevan . . . . . . . . . . CK-7.2 TUEStarobor, Aleksey . . . . . . . . . . CE-7.6 MONStauber, Tobias . . . . . . . . . . . JSIV-2.2 SUNStaude, Isabelle . . . . . . . . . . . .EG-2.2 SUN,�CK-6.3 MON, �EH-3.1 WED,�EH-5.1 THU, EH-5.3 THUStec, Kamila . . . . . . . . . . . . . . CH-7.2 WEDSteel, Michael . . . . . . . . . . . . EF-P.24 THUSteel, Michael J. . . . . . . . . . . . EA-1.6 SUN,
JSV-1.4 THUSteel, Mike J. . . . . . . . . . . . . CK-P.21 MONSteer, Matthew . . . . . . . . . . . CK-14.2 THUStefani, Fabio . . . . . . . . . . . . ED-3.3 MON,
CH-P.33 THUStefani, Mário . . . . . . . . . . . . . . CL-P.1 SUNStefanov, André . . . . . . . . . . . . EA-7.2 TUEStefanov, Ivan . . . . . . . . . . . . CA-11.4 THUSteglich, Patrick . . . . . . . . . . CH-P.10 THUSteigerwald, Hendrik . . . . . . CM-6.6 MONSteinberg, Aephraim . . . . . . . EA-2.6 SUN,
EB-1.2 MON, CD-9.2 TUESteinbrecher, Gregory . . . . .CK-4b.1 MONSteiner, Rufolf . . . . . . . . . . . . . .CL-P.3 SUNSteinert, Michael . . . . . . . . . CF-P.17 WEDSteinke, Michael . . . . . . . . . �CJ-P.25 WEDSteinle, Tobias . . . . . . . . . . . . CD-4.6 SUN,�CD-11.1 THU, �CL-4.2 THUSteinmann, A. . . . . . . . . . . . . . CD-4.3 SUNSteinmann, Andy . . . . . . . . . . CD-4.6 SUN,
CD-11.1 THU, CL-4.2 THUSteinmeyer, Guenter . . . . . .EF-4a.1 MON,
CF-5.1 WEDSteinmeyer, Günter . . . . . . . . CD-1.2 SUN,
EE-P.14 SUN, EF-3.3 SUN,EE-5b.2 MON, CF-4.3 WED,CF-6.6 THU, CF-9.4 THU
Stellinga, Daan . . . . . . . . . . . . �CK-1.1 SUNStenning, Gavin . . . . . . . . . . EH-P.14 WEDStepanenko, Oleksandr . . . . CD-P.20 TUEStepanenko, Yuriy . . . . . . . . . CF-P.8 WEDStepanov, Dmitrii . . . . . . . . . CJ-13.2 THUStepanov, Eugene A. . . . . . . . CF-3.4 TUE
Stepanov, Serguei . . . . . . . . CK-P.13 MONStephens, Marc . . . . . . . . . . . . �CI-P.5 TUEStepień, Ryszard . . . . . . . . . . CJ-5.4 MON,
CE-P.33 TUESteponkevičius, Kestutis . . �CD-P.29 TUESterr, Uwe . . . . . . . . . . . . . . . . ED-P.9 MONSteveler, Emilie . . . . . . . . . . . . CD-8.6 TUEStevens, Benjamin J. . . . . . CE-11.1 WEDStevens, Martin . . . . . . . . . . CK-4a.2 MONStewart, William . . . . . . . . . CK-10.2 WEDStierle, Johannes . . . . . . . . . EG-5b.1 MONStiller, Birgit . . . . . . . . . . . . . . . EA-1.2 SUNStobbe, Søren . . . . . . . . . . . . .PD-B.7 WEDStock, Johannes . . . . . . . . . . . EH-5.5 THUStockman, Mark . . . . . . . . . . .CG-4.4 WEDStöferle, Thilo . . . . . . . . . . . . . CD-P.1 TUEStoian, Razvan . . . . . . . . . . . .CM-2.4 SUN,
CD-P.2 TUEStolz, Wolfgang . . . . . . . . . . CE-11.6 WEDStomeo, Tiziana . . . . . . . . . . . .CK-1.6 SUNStopiński, Stanisław . . . . . . �CH-6.3 WEDStorz, Patrick . . . . . . . . . . . . . �CF-1.1 TUEStrafford, Simon . . . . . . . . . . CM-7.5 MONStraigis, Šarunas . . . . . . . . . . . CF-2.5 TUEStrain, Michael . . . . . . . . . . JSV-P.3 MON,
CD-P.4 TUEStrain, Michael J. . . . . . . . . . JSV-4.1 THUStrasser, Gottfried . . . . . . . . . . CC-1.4 SUNStratakis, Emmanuel . . . . . . CM-1.3 SUN,�CM-7.3 MONStratakis, Emmmanuel . . . . . CM-P.3 SUNStrauss, Hencharl . . . . . . . . . CA-12.6 THUStrecker, Maximilian . . . . . .CJ-10.3 WED,
CJ-11.4 THUStrekalov, Dmitry . . . . . . . . . .EB-3.1 WEDStrelkov, Vasily V. . . . . . . . . . CG-P.8 THUStrittmatter, Andre . . . . . . . . EA-8.5 WEDStritzel, Jenny . . . . . . . . . . . . . CL-3.1 THUStrutynski, Clement . . . . . . . CD-6.1 MONStuhler, Jürgen . . . . . . . . . . . .ED-P.9 MONStützer, Simon CI-1.2 SUN, CE-3.1 SUN,�JSIV-P.1 TUEStutzki, Fabian . . . . . . . . . . . . .CJ-1.2 SUN,
CJ-5.5 MON, �CJ-13.1 THU,CJ-13.4 THU, CJ-13.5 THU
Stylianakis, Minas M. . . . . . CM-7.3 MONSu, Jingqin . . . . . . . . . . . . . . .CF-P.22 WEDSu Lee, Jun . . . . . . . . . . . . . . . . CJ-1.4 SUNSu, Zhan . . . . . . . . . . . . . . . . .CK-12.2 WEDSuarez, Jaime . . . . . . . . . . . . . CG-6.2 WEDSuárez, Noslen . . . . . . . . . . . . CG-3.2 WEDSubramaniam, Vinod . . . . . . .CL-2.1 THU,
CK-14.1 THUSuche, Hubertus . . . . . . . . . .JSV-P.1 MONSuchkov, Sergey . . . . . . . . . .�CD-10.2 TUESudhir, Vivishek . . . . . . . . . . . �EA-4.2 SUNSudirman, Aziza . . . . . . . . . . .CD-6.3 MONSüdmeyer, Thomas . . . . . . . CA-6.1 MON,
CJ-8.4 WED, CH-8.2 WED,CB-7.3 WED, CF-9.3 THU
Sugavanam, Srikanth . . . . . . �CJ-4.2 SUN,�CJ-P.8 WED, EF-P.6 THU,EF-P.29 THU
Sugioka, Koji . . . . . . . . . . �CM/LIM.3 TUESugita, Atsushi . . . . . . . . . . . �CE-8.4 TUE,
224
Authors’ Index
�EH-P.10 WEDSujecki, Slawomir . . . . . . . . . . CJ-7.2 WEDSukhorukov, Andrey . . . . . . . CD-3.2 SUN,
CD-P.8 TUE, �CD-P.12 TUE,CD-10.2 TUE
Sukhorukov, Andrey A. . . . . CD-2.2 SUN,JSV-P.5 MON, JSV-2.3 THU
Sulaev, Azat . . . . . . . . . . . . . . EH-2.1 WEDSulc, Jan . . �CA-P.24 SUN, CA-P.25 SUNSulmoni, Luca . . . . . . . . . . . . . CB-8.1 THUSulzer, Philipp . . . . . . . . . . . . ED-P.7 MONSumetsky, Mikhail . . . . . . . . .CD-10.2 TUESumpf, Bernd . . . . . . . . . . . . CB-P.6 MON,
CB-P.10 MON, �CB-11.2 THUSun, Hong-Bo . . . . . . . . . . . . �CM-1.1 SUNSun, Li . . . . . . . . . . . . . . . . . . .CF-P.22 WEDSun, Shulin . . . . . . . . . . . . . . . . CE-3.5 SUNSun, Tong . . . . . . . . . . . . . . . . . CH-P.6 THUSun, Yi-Jian . . . . . . . . . . . . . . CA-P.19 SUNSunchugasheva, Elena S. . . �CN-P.4 TUESundaram, Suresh . . . . . . . . CE-11.4 WEDSung, Jae Hee . . . . . . . . . . . JSIII-1.1 MONSuret, Pierre . . . . . . . . . . . . . . .EF-5.2 MONSuriano, Raffaella . . . . . . . . . . CM-1.4 SUNSurrente, Alessandro . . . . . .CK-10.1 WEDSüßmann, Frederik . . . . . . . EG-5b.1 MON,
CG-4.4 WEDSussman, Benjamin . . . . . . . EA-10.1 THUSutter, Dirk .CA-P.1 SUN, CA-P.12 SUN,
CA-P.22 SUN, CA-10.1 THU,CA-10.5 THU, CA-12.3 THU
Sutton, Andrew . . . . . . . . . . . .CH-P.3 THUSuzuki, Masato . . . . . . . . . . . �EE-P.9 SUN,
EE-P.15 SUN, CF-P.28 WEDSuzuki, Takakazu . . . . . . . . . CF-P.16 WEDSuzuki, Takayuki . . . . . . . . . .CD-11.3 THUSuzuki, Takenobu . . . . . . . . .CE-P.12 TUE,
CJ-P.43 WED, CJ-P.45 WEDSuzuki, Tetsuhito . . . . . . . . . . .CE-P.4 TUESvinkina, Elena . . . . . . . . . . . . .CC-6.2 TUESvirko, Yuri CD-P.16 TUE, CK-14.4 THUSvozilík, Jiří . . . . . . . . . . . . . CK-P.32 MONSvyakhovskiy, Sergey . . . . . . CD-P.31 TUEŚweirad, Dariusz . . . . . . . . . . ED-P.9 MONSwillo, Marcin . . . . . . . . . . . . .CK-5.3 MONSych, Denis . . . . . . . . . . . . . �EB-2a.3 MONSygletos, Stelianos . . . . . . . . . . CI-1.3 SUNSygletos, Stylianos . . . . . . . . . . CI-3.4 SUNSygletou, Maria . . . . . . . . . . . �CM-P.3 SUNSylla, François . . . . . . . . . . . JSIII-1.1 MONSylvestre, Thibaut . . . . . . . . . CD-1.3 SUN,
CD-6.3 MON, CD-P.23 TUE,CD-P.25 TUE, CD-10.1 TUE
Sylvia, Jeney . . . . . . . . . . . . . CK-14.5 THUSylvie, Roke . . . . . . . . . . . . . . .CL-P.10 SUNSymes, Dan . . . . . . . . . . . . . . CF-P.25 WEDSysoliatin, Alexej . . . . . . . . . . . CI-4.2 SUN,
EF-P.27 THUSyvridis, Dimitris . . . . . . . . . . CI-5.3 MON,
CB-P.23 MON, CB-P.31 MONSzameit, Alexander . . . . . . . . EA-1.3 SUN,
CI-1.2 SUN, CH-2.4 SUN, CE-3.1 SUN,CK-4a.3 MON, CK-4b.2 MON,CD-P.12 TUE, JSIV-P.1 TUE,EB-3.3 WED, EB-P.1 WED,
CK-13.1 WED, EA-P.9 THU,�JSV-3.3 THU, JSV-3.5 THU,�JSV-4.6 THUSzczepanek, Jan . . . . . . . . . . �CF-P.8 WEDSzczepański, Paweł . . . . . . . . CH-6.3 WEDSzidarovszky, Tamas . . . . . . . . EE-4.3 SUNSzostkiewicz, Lukasz . . . . . . . �CE-1.6 SUNSzriftgiser, Pascal . . . . . . . . . . CD-8.3 TUESzymanski, Michal . . . . . . . . . CE-1.6 SUN,
CI-1.4 SUNT. Alkeskjold, Thomas . . . . CJ-P.14 WEDTabani, Andrea . . . . . . . . . . . JSIV-2.5 SUNTaddei, Caterina . . . . . . . . . . . . CI-4.5 SUNTaghizadeh, Alireza . . . . . . �CB-P.35 MONTaghizadeh, Mohammad Reza
CH-9.5 WEDTagoudi, Eirini . . . . . . . . . . . �CH-P.26 THUTahara, Hirokazu . . . . . . . . . . �CF-7.4 THUTaichenachev, Alexey . . . . . .EF-P.26 THUTaimre, Thomas . . . . . . . . . . .CH-8.1 WEDTainta, Santiago . . . . . . . . . . �CF-P.9 WEDTaira, Takunori . . . . . . . . . . . . CA-P.8 SUNTajahuerce, Enrique . . . . . . . CL-P.17 SUNTajalli, Ayhan �EE-P.14 SUN, EF-3.3 SUNTakahashi, Eiji . . . . . . . . . . . .CG-P.18 THUTakahashi, Eiji J . . . . . . . . . . .CG-6.4 WEDTakahashi, Fuyuto . . . . . . . . �CM-3.4 SUNTakai, Mayuko . . . . . . . . . . . . �CC-5.3 MONTakamoto, Masao . . . . . . . . . ED-3.2 MONTakan, Taylan . . . . . . . . . . . . CC-P.18 SUN,�CE-P.11 TUETakashima, Hideaki . . . . . . CK-P.12 MONTakeda, Koji . . . . . . . . . . . . . . . CK-3.3 SUNTakeda, Shuntaro . . . . . . . . . .EB-P.3 WEDTakemura, Naotomo . . . . . . �EG-P.5 MONTaketsugu, Tetsuya . . . . . . . .EE-P.18 SUNTakeuchi, Shigeki . . . . . . . . CK-P.12 MONTakeuchi, Yu-ichi . . . . . . . . . . CJ-14.4 THUTaki, Majid . . .EF-3.4 SUN, EF-P.2 THU,
EF-P.7 THUTakida, Yuma . . . . . . . . . . . . . . CC-P.7 SUNTakizawa, Syun . . . . . . . . . . . . CM-3.4 SUNTalebi, Nahid . . . . . . . . . . . . . CK-6.2 MON,�EH-2.2 WEDTamošauskas, Gintaras . . . CM-5a.3 MONTanabe, Takasumi . . . . . . . . . CK-9.2 TUE,
CK-9.4 TUE, CK-9.6 TUETanaka, Hiroki . . . . . . . . . . . CA-P.23 SUN,�CA-6.2 MON, CA-8.1 TUETanaka, Nobuhiko . . . . . . . . . . CA-2.4 SUNTang, Mincheng . . . . . . . . . . . .CJ-2.4 SUN,
EF-4b.1 MON, CJ-8.5 WEDTang, Ming . . . . . . . . . . . . . . . . . CI-2.3 SUNTang, Mingchu . . . . . . . . . . . . �CB-9.2 THUTang, Yunxin . . . . . . . . . . . . . . CG-P.1 THUTani, Francesco . . . . . . . . . . PD-A.7 WED,
CG-P.11 THUTani, Masahiko . . . . . . . . . . . . .CC-6.1 TUETanner, Michael . . . . . . . . . . .JSV-4.5 THUTanner, Michael G. . . . . . . . EA-P.28 THU,
JSV-4.1 THUTantussi, Francesco . . . . . �EG-P.10 MON,
EH-5.6 THUTao, YuLiang . . . . . . . . . . . . . CA-P.17 SUNTarasov, Nikita . . . . . . . . . . . . EF-P.6 THU,
�EF-P.29 THUTarazona, Antulio . . . . . . . . . . CE-4.3 SUNtardif, Samuel . . . . . . . . . . . . CB-11.1 THUTardy, Camille . . . . . . . . . . . . . CB-7.3 WEDTarka, Jan . . . . . . . . . . . . . . . . CF-P.5 WEDTasco, Vittorianna . . . . . . . .CK-13.5 WEDTassin, Philippe . . . . . . . . . . . EH-3.3 WEDTavast, Miki . . . . . . . . . . . . . . . CB-3.1 TUETavernarakis, Alexandros . . . �CH-1.1 SUNTaximaiti, Yusufu . . . . . . . . . �CA-7.6 MONTaylor, James . . . . . . . . . . . . . . CD-1.4 SUNTaylor, James Roy . . . . . . . . . CJ-9.6 WEDTchahame, Joel cabrel . . . . . CD-1.3 SUN,
CD-P.23 TUETchahame Nougnihi, Joël Cabrel�CD-P.25 TUETchofo-Dinda, Patrice . . . . . . EI-P.3 TUE,�EI-P.5 TUETchomgo-Felenou, Emmanuel EI-P.3 TUEteam, SOC2 . . . . . . . . . . . . . . ED-P.9 MONTeamir, Tesfay . . . . . . . . . . . �CJ-P.26 WEDTegin, Ugur . . . . . . . . . . . . . . . .�CJ-2.6 SUNTei, Kazuyoku . . . . . . . . . . . . CH-P.29 THUTeichmann, Stephan . . . . . . . EE-1.5 SUN,
EG-5b.2 MONTeichmann, Stephan M. . . . CG-3.2 WED,
CG-P.5 THUTeimourpour, Mohammad . . . EI-P.6 TUETeisseire, Jeremie . . . . . . . . �CK-14.6 THUTeisset, Catherine . . . . . . . . . . CG-2.1 TUETeisset, Catherine Y. . . . . . . CA-10.1 THUTejerina, Matias . . . . . . . . . .CK-P.28 MONTekce, Kemal . . . . . . . . . . . . . . CD-2.4 SUNTekeli, Isil . . . . . . . CLEO/ECBO-1.2 WEDTenderenda, Tadeusz . . . . . . .CE-1.6 SUN,
CE-P.28 TUETeng, Fei . . . . . . . . . . . . . . . . �CH-P.14 THUTengattini, Andrea . . . . . . . . EA-P.32 THUTeodonio, Lorenzo . . . . . . . . . .CC-P.6 SUNTeppitaksak, Achaya . . . . . . . �CA-3.4 SUNTerada, Sumio . . . . . . . . . . . . CD-11.3 THUTerai, Hirotaka . . . . . . . . . . . EA-P.25 THU,
EA-P.28 THU, JSV-4.1 THU,JSV-4.5 THU
Terazzi, Romain . . . . . . . . . . . CB-7.3 WEDTerekhov, Ivan . . . . . . . . . . . . . . EI-2.2 THUTervo, Jani CK-P.20 MON, CD-P.16 TUETesio, Enrico . .EC-P.6 TUE, EC-3.3 TUETessier, Mickael . . . . . . . . . �CK-4a.1 MONTetsumoto, Tomohiro . . . . . . CK-9.2 TUE,�CK-9.4 TUETeulon, Claire . . . . . . . . . . . . . CL-P.12 SUNTezuka, Hiroshige . . . . . . . . .CJ-P.45 WEDThai, Alexandre . . . . . . . . . EG-5b.2 MON,
CF-P.27 WEDThayne, Iain . . . . . . . . . . . . . . CK-14.2 THUTheeg, Thomas . . . . . . . . . . . �CE-2.4 SUN,
CJ-P.42 WEDTheisen-Kunde, Dirk . . . . . . CA-P.28 SUNThew, Robert . . . . . . . . . . . . . EB-1.4 MONThiel, Valerian . . . . . . . . . . . �ED-P.4 MONThienpont, Hugo . . . . . . . . . .EF-P.14 THUThilmann, Nicky . . . . . . . . . . CD-P.41 TUEThipparapu, Naresh Kumar�CJ-P.33 WED
Thire, Nicolas . . . . . . . . . . . . . CG-6.2 WEDTholl, Hans . . . . . . . . . . . . . . �CN-1.2 WEDThoma, Alexander . . . . . . . . �EA-8.5 WEDThomas, Fabrice . . . . . . . . . . . CK-7.5 TUEThomas, Gabrielle . . . . . . . . �CA-P.2 SUN,
CA-3.4 SUN, CA-6.4 MONThomas, Jens . . . . . . . . . . . . . .CM-3.3 SUNThomas, Jens U. . . . . . . . . . CM-P.10 SUNThomin, Stéphane . . . . . . . . . CH-9.2 WEDThompson, Mark . . . . . . . . . . JSV-4.5 THUThompson, Mark G. . . . . . . . EA-6.1 TUE,
PD-B.3 WED, �JSV-1.1 THU,EA-P.28 THU, JSV-4.1 THU
Thomson, Caroline . . . . . . . . CM-7.5 MONThomson, Robert . . . . . . . . . .CN-2.4 WEDThourhout, Dries V. . . . . . . CB-11.3 THUThurston, Iain . . . . . . . . . . . . . CH-9.5 WEDThyrrestrup, Henri . . . . . . . �EE-P.16 SUN,�EG-6.4 MON, CD-P.32 TUETian, Bin . . . . . . . . . . . . . . . . �CB-11.3 THUTian, Haochen . . . . . . . . . . . . �CF-1.4 TUETiana-Alsina, Jordi . . . . . . . . EF-P.22 THUTiarks, Daniel . . . . . . . . . . . . . �EA-2.1 SUNTichy, Malte . . . . . . . . . . . . . . JSV-3.5 THUTichy, Malte Christopher . . JSV-4.6 THUTielrooij, Klaas-Jan . . . . . . . JSIV-2.2 SUNTien Dat, Pham . . . . . . . . . . . . .CI-2.2 SUNTiess, Tobias . . . . . . . . . . . . . . CJ-9.5 WEDTighineanu, Petru . . . . . . . . �PD-B.7 WEDTignon, Jérome . . . . . . . . . . . . CC-1.3 SUNTijero, Jose Manuel Garcia CB-5.2 WED,
CB-7.6 WEDTikan, Alexey . . . . . . . . . . . . . . CD-P.8 TUETikhonchuk, Vladimir . . . .CM-5a.1 MON,
EI-P.1 TUETikhonova, Olga . . . . . . . . . . . EA-7.4 TUETilma, Bauke W. . . . . . . . . . .CF-4.1 WED,
CH-8.3 WEDTimmerman, Dolf . . . . . . . . . CE-P.19 TUETimoney, Nuala . . . . . . . . . . . .EA-2.4 SUN,
EA-P.31 THUTinnefeld, Philip . . . . . . . . . . CL-P.18 SUN,�EH-6.2 THUTiofack, Gaston Camus . . . . �EF-P.7 THUTisch, John . . CG-1.2 TUE, CF-5.3 WEDTisch, John W.G. . . . . . . . . . .CG-3.3 WEDTischler, Nora . . . . . . . . . . . . . . EA-1.6 SUNTissoni, Giovanna . . . . . . . . . . EF-1.4 SUN,
EF-1.6 SUN, EE-3.6 SUN, CB-7.4 WEDTitchener, James . . . . . . . . . . JSV-2.3 THUTitkov, Ilya . . . . . . . . . . . . . . .CM-P.15 SUNTitkov, Ilya E . . . . . . . . . . . . CE-11.2 WED,
CE-11.3 WEDTittel, Frank K. . . . . . . . . . . . . CH-3.1 SUNTjörnhammar, Staffan . . . . . �CE-9.2 TUETlidi, Mustapha . . . . . . . . . . . . EF-P.9 THUToda, Yasunori . . . . . . . . . . . . EE-P.9 SUN,
EE-P.15 SUN, CF-P.28 WEDToenger, Shanti . . . . . . . . . . �EF-P.25 THUTohyama, Takeshi . . . . . . . . . EB-P.3 WEDToivonen, Harri . . . . . . . . . . . .CN-2.3 WEDToivonen, Juha . . . . . . . . . . . CM-P.5 SUN,�CH-7.5 WED, CN-2.3 WED,
CH-P.11 THU, CH-P.16 THUTojo, Koji . . . . . . . . . . . . . . . . CA-P.43 SUN
Tokel, Onur CM-P.18 SUN, CM-4.5 SUN,CK-P.3 MON, �CK-P.34 MON
Tokizane, Yu . . . . . . . . . . . . . . �CC-P.7 SUNTokunaga, Yuuki . . . . . . . . . .�EB-P.7 WEDTokurakawa, Masaki . . . . . .�CA-12.1 THUTolstik, Nikolai . . . . . . . . . . . . .CJ-7.4 WEDToma, Andrea . . . . . . . . . . . . . EH-5.6 THUToma, Kazunori . . . . . . . . . . . CK-6.1 MONTomasi, Alessandro . . . . . . . EA-P.32 THUTombelli, Sara . . . . . . . . . . . . CL-P.13 SUNTombez, Lionel . . . . . . . . . . . . CB-7.3 WEDTomita, Yasuo . . . . . . . . . . . . . �CE-8.5 TUETomlinson, Steph . . . . . . . . . . .CA-3.6 SUNTomohiro, Tsukihana . . . . . .CD-P.37 TUETonelli, Mauro CA-2.1 SUN, CA-4.4 SUNTonello, Alessandro . . . . . . . . . CJ-1.5 SUNTong, Xiao-Min . . . . . . . . . . . CG-5.5 WEDToninelli, Costanza . . . . . . . .JSIV-2.5 SUNTöppel, Falk . EA-1.2 SUN, �EI-3a.3 THUTorchia, Gustavo . . . . . . . . �CK-P.28 MONTorlina, Lisa . . . . . . . . . . . . . . �CG-4.2 WEDTorregrosa, Adrián J. . . . . . . CD-6.4 MONTorrent, Maria del Carme . .EF-P.22 THUTorres-Castro, Alejandro . . . . CL-P.4 SUNTorres-Company, Victor . . . .CD-P.9 TUE,
CF-P.9 WEDTorres, Juan . . . . . . . . . . . . . �EA-P.14 THUTorres, Juan P. . . . . . . . . . . . . CH-6.6 WEDTorres-Mendieta, Rafael . . . �CM-P.4 SUNTosa, Valer . . .CG-1.4 TUE, CG-P.2 THUToschek, Peter E. . . . . . . . . . .�EC-2.1 TUETosi, Daniele . . . . . . . . . . . . . . CL-P.14 SUNTotero Gongora, Juan Sebastian�EH-7.1 THUToth, Csaba . . . . . . . . . . . . . JSIII-1.4 MONToth, Geza . . . .EA-2.3 SUN, EC-1.4 TUETown, Graham . . . . . . . . . .�CK-P.39 MON,�CE-P.20 TUEToyoshima, Naoko . . . . . . . . CH-P.29 THUTrabattoni, Andrea . . . . . . . �CG-6.3 WED,
CF-8.4 THUTrabold, Barbara . . . . . . . . . . . CD-1.1 SUNTrabold, Barbara M. . . . . . . . EF-6.5 MONTradonsky, Chene . . . . . . . . . . CA-P.4 SUNTrägårdh, Johanna . . . . . . . . �CL-3.4 THUTran, Truong . . . . . . . . . . . . . CD-12.3 THUTränkle, Günther . . . . . . . . . CB-P.6 MON,
CB-P.12 MON, CD-P.35 TUE,CD-P.40 TUE, CB-5.4 WED,CB-10.4 THU, CB-11.2 THU
Trapateau, Julien . . . . . . . . . �EB-P.5 WEDTraum, Christian . . . . . . . . . EE-5a.1 MONTravers, John EE-1.2 SUN, CG-P.11 THUTravers, John C. . . . . . . . . . . . EE-1.1 SUN,
CD-P.39 TUE, PD-A.7 WEDTravis, Christopher . . . . . . . . . CL-3.4 THUTrawiński, Ryszard S. . . . . . . CH-7.2 WEDTraynor, Nicholas . . . . . . . . . .CJ-11.1 THUTrebaol, Stéphane . . . . . . . . EG-P.5 MON,
CD-9.4 TUETredicucci, Alessandro . . . . . CB-6.4 WEDTrefflich, Lukas . . . . . . . . . . . . CD-P.6 TUETrepat, Xavier . . . CLEO/ECBO-1.2 WEDTrepes, Nicolas . . . . . . . . . . . . EB-P.8 WEDTreps, Nicolas . . . . . . . . . . . . ED-P.4 MON,
225
Authors’ Index
ED-1b.3 MON, EB-P.6 WEDTriana, Cristian . . . . . . . . . . . �CH-P.5 THUTriches, Marco . . . . . . . . . . . . �CH-5.4 TUETrichet, Aurelien . . . . . . . . . . . EC-3.2 TUETrifonov, Anton . . . . . . . . . . .CA-11.4 THUTrillo, S. . . . . . . . . . . . . . . . . . .EF-P.17 THUTrillo, Stefano . . . . . . . . . . . . EE-P.12 SUN,
EF-5.5 MON, CD-8.3 TUE, EI-2.1 THUTrinité, Virginie . . . . . . . . . . . CB-11.6 THUTroccoli, Mariano . . . . . . . . . . CC-1.1 SUNTroles, Johann . . . . . . . . . . . . CN-1.5 WEDTronciu, Vasile . . . . . . . . . . �CB-P.25 MONTronciu, Vasile Z. . . . . . . . . CB-P.28 MONTrono, Cosimo . . . . . . . . . . . . CL-P.13 SUNTrubetskov, Michael . . . . . . . CF-7.5 THU,
CA-10.5 THU, CG-P.12 THUTrull, Jose . . . CK-1.4 SUN, CK-1.5 SUN,
CD-5b.1 MON, CH-P.21 THUTrusheim, Matthew E. . . . . . JSV-4.4 THUTrushin, Maxim . . . . . . . . . . .EE-5a.2 MONTrushin, Sergei . . . . . . . . . . . EG-5b.1 MONTsai, Din Ping . . . . . . . . . . . . . . EI-1.4 THUTsang, Kim . . . . . . . . . . . . . . . . EF-8.2 TUETsarev, Andrei . . . . . . . . . . . . �CK-1.3 SUN,�CK-P.30 MONTsatsulnikov, Andrey . . . . . .CE-11.3 WEDTsatsulnikov, Andrey F . . . .CE-11.2 WEDTserepi, Angeliki . . . . . . . . . .CM-P.16 SUNTsiminis, Georgios . . . . . . . . . �CH-5.6 TUETsioutsios, Ioannis . . . . . . . . . CH-1.1 SUN,
CK-10.3 WEDTsou, Yu-Jung . . . . . . . . . . . . . .CF-3.1 TUETsubouchi, Masaaki . . . . . . . �CC-6.4 TUETsvetkov, Vladimir . . . . . . . . �CH-P.1 THUTsvetkov, Vladimir B. . . . . . CE-P.25 TUETsvirkun, Viktor . . . . . . . . . �CK-10.1 WEDTu, Chao-Yang . . . . . . . . . . . CA-P.16 SUN,
CA-P.19 SUNTu, Zong-Yi . . . . . . . . . . . . . . . .CE-P.9 TUETuchak, Anton . . . . . . . . . . . . CC-P.19 SUNTumaikin, Anatoly . . . . . . . . EF-P.26 THUTuniz, Alessandro . . . . . . . . �PD-A.8 WEDTünnermann, Andreas . . . . . . CJ-1.2 SUN,
CM-P.10 SUN, CM-4.1 SUN,CJ-4.5 SUN, CJ-5.5 MON,CM-6.2 MON, CG-2.5 TUE,CG-3.1 WED, CJ-8.1 WED,CJ-8.2 WED, CJ-P.17 WED,CJ-10.1 WED, CJ-10.2 WED,CJ-10.3 WED, CJ-10.6 WED,CJ-11.3 THU, CJ-11.4 THU,CG-P.12 THU, CJ-13.1 THU,CJ-13.4 THU, CJ-13.5 THU,CF-8.1 THU, CF-9.2 THU
Turan, Rasid . . . . . . . . . . . . . . . JSI-P.1 TUETurduev, Mirbek . . . . . . . . . EH-P.16 WEDTureci, Hakan . . . . . . . . . . . . EH-P.15 WEDTurella, Fabio . . . . . . . . . . . . . �CE-3.4 SUNTuritsyn, Sergei CI-1.3 SUN, CI-3.2 SUN,
CI-3.4 SUN, CJ-4.2 SUN, �EF-5.1 MON,CF-P.6 WED, CJ-P.40 WED,EF-P.19 THU, EI-2.1 THU
Turitsyn, Sergei K. . . . . . . . . . . CI-3.1 SUNTuritsyn, Sergey . . . . . . . . . . . . EI-2.2 THUTuritsyna, Elena . . . . . . . . . . . . CE-1.4 SUN
Turkdogan, Sunay . . . . . . . . . CB-4.1 WEDTurnali, Ahmet . . . . . . . . . . . �CM-4.5 SUN,
CK-P.34 MONTurpin, Alex .CA-P.7 SUN, �EC-P.8 TUE,�CL-2.5 THUTurquet, Léo . . . . . . . . . . . . �EG-P.11 MONTurri, Stefano . . . . . . . . . . . . . CM-1.4 SUNTürschmann, Pierre . . . . . . . . �EG-3.2 SUNTurtaev, Sergey N. . . . . . . . . CD-P.28 TUETurunen, Jari . . . . . . . . . . . . . . EE-3.1 SUN,
CK-P.20 MON, CD-P.16 TUETurutsyn, Sergei . . . . . . . . . . . . EF-3.5 SUNTuthill, Peter . . . . . . . . . . . . . . CM-P.8 SUNTuzakli, Refik . . . . . . . . . . . �CK-P.35 MONTwitchen, Daniel . . . . . . . . . CE-10.1 WEDTwitchen, Daniel L. . . . . . . . JSV-4.4 THUTykalewicz, Boguslaw . . . . CB-P.24 MON,
CB-7.4 WEDTyrk, Mateusz . . . . . . . . . . . . . CM-3.5 SUNTyrtyshnyy, Valentin . . . . . . �CJ-10.4 WEDTzallas, Paraskevas . . . . . . . . �EE-1.4 SUNTzallas, Paris . . . . . . . . . . . . . . .CG-1.3 TUETzortzakis, Stelios . . . . . . . . . . CC-P.8 SUNTzou, An-Jye . . . . . . . . . . . . . CK-14.3 THUU. Wetter, Niklaus . . . . . . . . . CA-P.9 SUNUdem, Thomas . . . . . . . . . . . �SH-7.1 SUN,
CA-10.3 THUUebel, Patrick . . . . . . . . . . . . PD-A.7 WEDUeda, Ken-ichi . . . . . . . . . . . . . CA-2.4 SUNUeffing, Moritz . . . . . . . . . . . . CA-P.1 SUN,�CA-12.3 THUUemoto, Mitsuharu . . . . . . . . �EH-7.6 THUUlliac, G. . . . . . . . . . . . . . . . . CK-11.2 WEDUlliac, Gwenn . . . . . . . . . . . . . . CK-7.5 TUEUllrich, Joachim . . . . . . . . . . CG-3.4 WED,
CG-5.5 WEDUlysse, Christian . . . . . . . . . CK-12.3 WEDUmezawa, Toshimasa . . . . . . . �CI-3.6 SUNUminska, Ada . . . . . . . . . . . .�CH-P.18 THUUmnikov, Andrey . . . . . . . . . CJ-P.33 WEDUmnikov, Andrey A. . . . . . . . .CJ-9.2 WEDUng, Thi Phuong Lien . . . .CK-P.15 MONUnger, Peter . . . . . . . . . . . . . . CB-P.2 MONUno, Shingo . . . . . . . . . . . . . . CA-P.43 SUNUnterholzer, Thomas . . . . . . CJ-12.3 THUUnterrainer, Karl . . . . . . . . . . .CC-1.4 SUN,
CC-2.4 SUN, CC-P.4 SUN, EH-P.1 WEDUphoff, Manuel . . . . . . . . . . . �EA-P.6 THUUren, Robin . . . . . . . . . . . . . . . CA-7.5 MONUrsescu, Daniel . . . . . . . . . . .CF-P.20 WEDUshijima, Ichiro . . . . . . . . . . . ED-3.2 MONUsmani, Imam . . . . . . . . . . . . EA-P.31 THUUstimchik, Vasily . . . . . . . . . CJ-10.5 WEDUstinov, Victor M. . . . . . . . CB-P.22 MONUteza, Olivier . . . . . . . . . . . �CM-5b.2 MONUtikal, Tobias EG-3.1 SUN, EG-3.2 SUN,
EA-5.3 MONUusimaa, Petteri . . . . . . . . . . .CB-5.3 WEDUusitalo, Sanna . . . . . . . . . . . JSII-2.2 MONUusitalo, Topi . . . . . . . . . . . �CB-P.26 MONUždavinys, Tomas Kristijonas CE-9.2 TUEVahala, Kerry . . . . . . . . . . . . ED-1a.1 MONVaičaitis, Virgilijus . . . . . . . . CD-P.29 TUEVainio, Markku . . . . . . . . . . . . .CH-3.3 SUNValado, Maria . . . . . . . . . . . . .PD-B.5 WED
Valente, João CI-1.1 SUN, CK-6.6 MON,CH-7.3 WED, CF-9.6 THU
Valentin, Constance . . . . . . . . .CJ-3.3 SUNVallan, Alberto . . . . . . . . . . . . CL-P.14 SUNValle, Ángel . . . . . . . . . . . . . �EF-P.12 THU,�EF-P.14 THUValle, Stefano . . . . . . . . . . . . . CJ-14.6 THUVallee, Real . . . . . . . . . . . . . . . �CJ-5.3 MONVallet, Marc . . EF-2.2 SUN, CI-5.5 MON,
CN-1.4 WED, EF-P.1 THUVallon, Raphael . . . . . . . . . . . .CH-P.2 THUVallone, Steven . . . . . . . . . . . . EH-6.5 THUValmorra, Federico . . . . . . . . PD-B.8 WEDVámos, Lénárd . . . . . . . . . . . .CA-P.35 SUNVamvakaki, Maria . . . . . . . . . . CE-3.3 SUNvan Aken, Peter . . . . . . . . . . CK-6.2 MON,
EH-2.2 WEDvan de Kruijs, Robbert . . . . CH-P.35 THUvan de Walle, Aymeric . . . �CF-P.27 WEDvan der Slot, Peter . . . . . . . .CK-5.4 MON,
CJ-12.2 THUvan der Wal, Caspar . . . . . EG-P.12 MON,
EA-10.2 THUvan der Wel, Ruben . . . . . . . �EG-4.2 SUN,
CD-P.5 TUEVan Dijk, Frédéric . . . . . . . . . CI-5.5 MON,
CB-5.2 WEDVan Exter, Martin P. . . . . . . �EA-6.4 TUE,�EB-P.13 WEDVan Howe, James . . . . . . . . . . . CI-4.1 SUNvan Hulst, Niek . . . . . . . . . . . . EH-6.3 THUvan Hulst, Niek F. . . . . . . . . . �CK-2.1 SUNvan Loock, Peter . . . . . . . . . . EA-1.5 SUN,
EB-P.3 WEDvan Putten, Elbert G. . . . . . . .CL-4.5 THUvan Rees, Albert . . . . . . . . . . .CK-5.4 MONVan Thourhout, Dries . . . . . �SH-8.1 SUN,
EG-P.13 MON, CK-11.6 WEDvan Tilborg, Jeroen . . . . . . JSIII-1.4 MONvan Zanten, Thomas . . . . . . . EH-6.1 THUVanetsev, Alexander . . . . . . . . CL-P.3 SUNVanvincq, Olivier . . . . . . . . . . .CJ-3.5 SUN,
CJ-3.6 SUN, CD-12.2 THUVanwolleghem, Mathias . . . �EH-2.6 WEDVaranavičius, Arunas . . . . . . . .CF-2.5 TUEVarchi, Greta . . . . . . . . . . . . . .CL-P.13 SUNVargas-Velez, Kevin . . . . . . . . CC-4.1 SUNVarin, Charles . . . . . . . . . . . . CG-P.19 THUVarjú, Katalin CG-1.4 TUE, CG-P.2 THUVarkentin, Arthur . . . . . . . . . . CL-3.1 THUVarón-Durán, Margarita . . . . CH-P.5 THUVasilantonakis, Nikolaos . . . �EH-4.4 WEDVatnik, Ilya . . . �CD-P.8 TUE, EI-2.2 THUVatnik, Sergei . . . . . . . . . . . . . .CA-8.5 TUEVaurette, François . . . . . . . . . EH-2.6 WEDVay, Jean-Luc . . . . . . . . . . . JSIII-1.3 MON,
JSIII-1.4 MONVázquez-Córdova, Sergio . . .CE-7.3 MONVazquez-Zuniga, Luis . . . . .CK-P.26 MONVeber, Alexander A. . . . . . . . CE-P.25 TUEVedagarbha, Praveen . . . . . .CD-11.4 THUVeglione, Manuela . . . . . . . . CL-P.11 SUN,
JSII-1a.1 MON, CL-1.3 WEDVehmas, Tapani . . . . . . . . . . . . CI-P.7 TUE,
CH-6.1 WED
Veisz, László . . . . . . . . . . . . EG-5b.2 MON,CG-1.3 TUE, CG-2.4 TUE
Velazquez, Martin Nunez . . . CJ-9.2 WEDVella, Angela . . . . . . . . . . . . CM-5b.1 MONVenck, Sébastien . . . . . . . . . . CN-1.5 WEDVenkitesh, Deepa . . . . . . . . . . . .CI-4.4 SUNVennekel, Maike . . . . . . . . . . . EH-7.3 THUVenon, Bertrand . . . . . . . . . . ED-P.9 MONVenturini, Francesca . . . . . �CH-P.31 THUVeretennicoff, Irina . . . . . . . . EH-3.3 WEDVergeles, Sergey . . . . . . . . . . . . EI-2.2 THUVerhagen, Ewold . . . . . . . . . . EG-6.3 MON,
CK-10.5 WEDVerheyen, Peter . . . . . . . . . . . . .CJ-1.4 SUNVerhoef, Aart . . . . . . . . . . . . . . .CJ-2.5 SUNVerlot, Pierre CH-1.1 SUN, CK-2.4 SUN,�EC-3.4 TUEVerma, Varun B. . . . . . . . . CK-4a.2 MON,
EB-1.5 MONVermillac, Manuel . . . . . . . . . CE-P.31 TUEVernac, Laurent . . . . . . . . . . . . EC-1.3 TUEVernaz-Gris, Pierre . . . . . . . . �EB-P.2 WEDVeronesi, Stefano . . . . . . . . . . CA-2.1 SUN,
CA-4.4 SUNVershinin, Oleg . . . . . . . . . . . CE-P.21 TUE,
CJ-10.4 WEDVest, Benjamin . . . . . . . . . . . . CD-8.6 TUEVetter, Christian . . . . . . . . . . .�CH-2.4 SUNVezzoli, Stefano . . . . . . . . . . . EG-3.5 SUN,
CF-9.6 THUViana, Bruno . . . . . . . . . . . . . �CE-6.5 MONVicario, Carlo . . . . . . . . . . . . . �CC-P.2 SUN,�CC-3.2 SUN, �CC-3.6 SUNVidal, Cynthia . . . . . . . . . . . . .EH-P.5 WEDVidal, François . . . . . . . . . . . . CD-7.4 MONVidmar, Lev . . . . . . . . . . . . . . .EE-P.17 SUNVieille, Thibault . . . . . . . . . . . . EE-1.3 SUNVietz, Carolin CL-P.18 SUN, EH-6.2 THUViggianiello, Niko . . . . . . . . . JSV-3.4 THUViheriälä, Jukka . . . . . . . . . CB-P.26 MON,�CB-5.1 WED, CB-11.4 THUVijayraghavan, Karun . . . . . . . CC-1.1 SUNViktorov, Evgeniy A. . . . . .�CB-P.22 MONViktorov, Evgeny A. . . . . . . CB-P.24 MONVilaseca, Ramon . . . . . . . . . . .CK-1.5 SUN,
EF-4a.2 MON, CD-5b.1 MONVilera, Mariafernanda . . . . . CB-5.2 WED,
CB-7.6 WEDVillares, Gustavo . . . . . . . . . . .CB-6.2 WEDVillatoro, Joel . . . . . . . . . . . . �CH-5.2 TUE,
CH-6.2 WEDVillegas, Irma Lorena . . . . . CH-P.27 THUVilokkinen, Ville . . . . . . . . . . . CB-5.3 WEDVincenti, Maria Antonietta �CK-1.6 SUN,
EH-7.4 THUVinckier, Quentin . . . . . . . . . . �CI-5.1 MONVinet, Eric . . . . . . . . . . . . . . . . CB-5.2 WEDViolante, Claudia . . . . . . . . . . . CC-P.6 SUNVirtanen, Heikki . . . . . . . . . CB-P.26 MON,
CB-5.1 WEDVirte, Martin . . . . . . . . . . . . . . �CB-8.5 THUVishnubhatla, Krishna Chaitanya
CM-P.9 SUNViskontas, Karolis . . . . . . . . �CE-P.35 TUEVistas, Cláudia . . . . . . . . . . . .CA-11.6 THU
Vitelli, Chiara . . . . . . . . . . . . . EB-5.2 WED,EA-P.27 THU, JSV-3.4 THU
Viti, Leonardo . . . . . . . . . . . . . .CF-7.1 THUVitiello, Miriam S. . . . . . . . . . CC-4.5 SUN,
CF-7.1 THUVitkin, Vladimir . . . . . . . . . . . . CE-P.5 TUEVivas, Marcelo . . . . . . . . . . . . CE-P.16 TUEVivas’, Marcelo G. . . . . . . . . . .CE-9.6 TUEVivien, Laurent . . . . . . . . . . . JSV-4.2 THUVladimirov, Andrei . . . . . . . . CB-7.1 WED,�EF-P.4 THUVocke, David . . . . . . . . . . . . . . �EF-2.1 SUNVogel, Nicolas . . . . . . . . . . . .CK-P.35 MONVogel, Werner . . . . . . . . . . . . . EB-P.8 WEDVogelgesang, Ralf . . . . . . . . .EG-P.6 MON,
CK-6.2 MONVogl, Tobias . . . . . . . . . . . . . . .EB-4.1 WEDVogl, Ulrich EB-3.1 WED, �PD-B.2 WEDVogt, Stefan . . . . . . . . . . . . . . ED-P.9 MONVoicu, Flavius . . . . . . . . . . . . CA-10.4 THUVoigtländer, Christian . . . . CM-P.10 SUN,
CM-4.1 SUN, �CJ-11.3 THUVoisin, Christophe . . . . . . . . . . EG-3.4 SUNVojtech, Josef . . . . . . . . . . . . �CH-6.4 WEDVolker, Sebastien . . . . . . . . . EG-P.12 MONVollmer, Frank . . . . . . . . . . . . �CH-4.2 SUNVolz, Jürgen . . . . . . . . . . . . . . .�EA-2.2 SUNVolz, Kerstin . . . . . . . . . . . .�CE-5b.1 MON,
CE-11.6 WEDVolz, Thomas CL-2.2 THU, EA-10.6 THUVomiero, Alberto . . . . . . . . . CE-5a.1 MONvon Brunn, Patrick . . . . . . . �CE-P.22 TUEvon den Driesch, Nils . . . . . . . CB-1.4 TUEvon Edlinger, Michael . . . . . . CB-6.1 WEDvon Freymann, Georg . . . . . . CC-5.2 MONvon Grafenstein, Lorenz . . . . �CF-1.2 TUEVorholt, Christian . . . . . . . . �CA-P.10 SUNVoronin, Aleksandr . . . . . . . . CG-2.3 TUE,
CF-5.2 WEDVoronin, Aleksandr A. . . . . . . CF-3.4 TUEVoronin, Alexander . . . . . . . . CD-4.5 SUN,
CF-3.5 TUEVörös, Zoltán . . . . . . . . . . . . . EG-6.6 MONVorotynskii, Andrei . . . . . . . .CJ-10.5 WEDVos, Willem CE-2.2 SUN, �EG-7.2 MON,
CK-13.2 WEDVos, Willem L. . . . . . . . . . . . EE-P.16 SUN,
EG-6.4 MON, CL-4.5 THUVoss, Paul L . . . . . . . . . . . . . .CE-11.4 WEDVrakking, Marc . . . . . . . . . . . . CG-1.4 TUEVtyurina, Daria N. . . . . . . . . �CE-P.25 TUEVu, Khu . . . . CH-3.2 SUN, �CE-7.1 MON,
CJ-P.2 WEDVuckovic, Jelena . . . . . . . . . . �EA-8.1 WEDVujicic, Vidak . . . . . . . . . . . . . . . CI-2.5 SUNVukovic, Ana . . . . . . . . . . . . .EH-P.18 WEDVuković, Nikola . . . . . . . . . . �EF-P.10 THUVuong, Luat.T. . . . . . . . . . . . . EH-6.5 THUVynck, Kévin . . . . . . . . . . . . .CK-11.1 WEDWabnitz, Stefan . . . . . . . . . . . �CI-4.2 SUN,
EF-4b.2 MON, EF-4b.3 MON,CD-8.3 TUE, CD-P.20 TUE,EF-P.6 THU, EF-P.27 THU, EI-2.5 THU
Wabnitz, Stefano . . . . . . . . . EF-P.20 THU,CD-13.5 THU
226
Authors’ Index
Wada, Satoshi . . . . . . . . . . . .CA-P.36 SUN,CL-4.4 THU
Waddie, Andrew John . . . . . CH-9.5 WEDWade, Christopher . . . . . . . . �EA-9.4 THUWade, Scott . . . . . . . . . . . . . . CM-6.6 MONWadsworth, William . . . . . . . �CJ-5.1 MONWagner, Joachim . . . . . . . . . CB-P.7 MON,
CN-1.2 WED, CN-2.2 WEDWagner, Markus R. . . . . . . . CE-5a.2 MONWagner, Patrick . . . . . . . . . . . . CL-P.8 SUNWahle, Markus . . . . . . . . . . . . �CE-P.7 TUEWahls, Sander . . . . . . . . . . . . . . CI-3.2 SUNWahlstrand, Jared . . . . . . . . . . EE-2.1 SUNWahyutama, Imam Setiawan
CG-4.6 WEDWajnchold, Barbara . . . . . . .CH-P.18 THUWalasik, Wiktor . . . . . . . . . . . . EF-P.8 THUWalborn, Stephen P. . . . . . . . .EA-7.1 TUEWalczak, Pierre . . . . . . . . . . . �EF-5.2 MONWalczakowski, Michal . . . . . CC-P.17 SUNWaldburger, Dominik . . . . . . CF-4.1 WEDWale, Michael . . . . . . . . . . . . . . .CI-2.6 SUNWalke, Daniel . . . . . . . . . . . . . . CG-1.2 TUEWallis, Robert . . . . . . . . . . . . �CC-2.3 SUN,
CC-2.5 SUN, �CC-P.14 SUNWalmsley, Ian . . . . . . . . . . . . �JSV-3.1 THUWalmsley, Ian A. . . . . . . . . . JSV-P.6 MON,
JSV-P.7 MON, EA-6.3 TUE,JSV-1.3 THU
Walser, Reinhold . . . . . . . . . EA-P.16 THU,EA-P.17 THU
Walsh, Michael . . . . . . . . . . . JSV-4.4 THUWalther, Philip . . . . . . . . . . . . EB-5.4 WEDWan, Chenchen . . . . . . . . . . . .�CF-1.6 TUEWandt, Dieter . . . . . . . . . . . . . .CA-4.1 SUNWang, Bingxia . . . . . . . . . . �CD-5b.1 MONWang, Chao EB-1.2 MON, CJ-P.46 WEDWang, Chingyue . . . . . . . . . . . .CF-1.4 TUEWang, Chuncan . . . . . . . . . . . �CF-3.3 TUEWang, Daqing . . . . . . . . . . . . . EG-6.1 MONWang, Donfang . . . . . . . . . . . CL-P.18 SUNWang, Dongfang . . . . . . . . . . . EH-6.2 THUWang, Hong . . . . . . . . . . . . . . �CI-P.14 TUEWang, Hongjie . . . . . . . . . . . . . CJ-2.4 SUN,
CM-5b.1 MONWang, Huolei . . . . . . . . . . . . . CB-10.3 THUWang, Jinxiong . . . . . . . . . . . . CA-3.5 SUNWang, Jun . . . . . . . . . . . . . . . .CE-P.18 TUEWang, Kai . . . . . . . . . . . . . . �CK-4b.2 MONWang, Kuan-Yu . . . . . . . . . . . CE-P.10 TUEWang, Lan . . . . . . . . . . . . . . . . EH-2.1 WEDWang, Lihua . . EF-2.2 SUN, CI-5.5 MONWang, Pu . . . . . . . . . . . . . . . . .CJ-13.6 THUWang, Qi . . . . . . . . . . . . . . . . . CE-P.18 TUEWang, Qi Jie . . . . . . . . . . . . . . EH-2.1 WEDWang, Qian . . . . . . . . . . . . . . . EH-3.2 WEDWang, Qiang . . . . . . . . . . . . . . .EA-6.4 TUEWang, Rongping . . . . . . . . . . . CD-1.5 SUNWang, Shaofei . . . . . . . . . . . .�EE-P.10 SUNWang, Sheng-Min . . . . . . . . CF-P.11 WEDWang, Shuo . . . . . . . . . . . . . . CA-P.18 SUNWang, Xiaodong . . . . . . . . . .CF-P.22 WEDWang, Xiaojun . . . . . . . . . . . . . CC-1.1 SUNWang, Yue . . . . . . . . . . . . . . . . .CK-1.1 SUNWang, Yulei . . . . . . . . . . . . . . CA-P.13 SUN
Wang, Zengbo . . . . . . . . . . . . .CM-P.6 SUNWang, Zhechao . . . . . . . . . . . CB-11.3 THUWang, Zhen . . . . . . . . . . . . . . EA-P.25 THUWang, Zilong . . .CI-P.1 TUE, EI-1.3 THUWard, Jon . . . CJ-7.2 WED, CJ-14.6 THUWard, Robert . . . . . . . . . . . . . .CH-P.3 THUWarren-Smith, Stephen . . . . . CH-4.1 SUNWarrier, Aravindan . . . . . . . EH-P.12 WEDWatanabe, Shinichi . . . . . . . CC-P.12 SUN,
CC-5.3 MONWatanabe, Shuntaro . . . . . . . .CF-2.2 TUEWaters, Robin F. . . . . . . . . . . �CD-8.5 TUEWatts, Michael R. . . . . . . . . CK-12.2 WEDWatts, Regan . . . . . . . . . . . . . . �CI-2.5 SUNWeatherill, Kevin . . . . . . . . . . .EA-9.4 THUWebb, Colin . . . . . . . . . . . . . . . CJ-5.1 MONWeber, Christoph . . . . . . . . �CB-P.20 MONWeber, Markus . . . . . . . . . . . . EG-P.2 MONWeber, Paul . . . . . . . . . . . . . . . CG-1.4 TUEWeber, Peter . . . . . . . . . . . . �CK-10.3 WEDWeber, Sébastien . . . . . . . . . . CG-6.1 WEDWeeber, Jean-Claude . . . . CK-P.15 MON,
EG-P.8 MONWegener, Martin . . . . . . . . . . . CK-2.2 SUNWegner, Ulrike . . . . . . . . . . . . . CA-3.5 SUNWei, Haoyun . . . . . . . . . . . . . CH-P.28 THUWei, Wei . . CE-5a.3 MON, �CE-6.4 MONWei, Zhiyi . .CA-P.12 SUN, PD-A.1 WEDWeidlich, Stefan . . . . . . . . . . PD-A.8 WEDWeidman, Matthew . . . . . . . . CG-1.3 TUEWeih, Robert . . . . . . . . . . . . . .CB-6.1 WEDWeihs, Gregor . . . . . . . . . . . . EG-6.6 MON,
EA-8.2 WED, EA-P.5 THU,EA-P.7 THU, EA-P.8 THU,EA-P.26 THU, JSV-3.5 THU
Weimann, Steffen . . . . . . . .CK-4b.2 MON,JSV-3.5 THU, JSV-4.6 THU
Weinfurter, Harald . . . . . . . . EB-1.3 MON,EG-P.2 MON, EB-4.1 WED,EB-4.3 WED, EB-P.12 WED
Weingarten, Kurt . . . . . . . . . . CA-6.1 MONWeiss, Thomas . . . . . . . . . . . . EH-1.2 WEDWeitenberg, Johannes . . . . .CE-10.3 WEDWellmann, Barbara . . . . . . . �CA-6.5 MONWenclawiak, Moritz . . . . . . . �EH-P.1 WEDWender, Christiene . . . . . . . CF-P.24 WEDWenger, Jérôme . . . . . . . . . . . EG-7.3 MONWenzel, Hans . . . . . . . . . . . CB-P.19 MON,
CB-P.28 MON, CD-P.40 TUE,CB-11.5 THU
Wenzl, Franz P. . . . . . . . . . . . .EI-3a.1 THUWerner, Christoph Sebastian�CD-10.4 TUEWerschler, Florian . . . . . . . �EG-P.14 MONWesemann, Lukas . . . . . . . . . �CD-2.4 SUNWest, Paul . . . . . . . . . . . . . . . . . CE-3.2 SUNWestberg, Jonas . . . . . . . . . . .CH-8.5 WEDWestbergh, Petter . . . . . . . . . .CB-2.4 TUEWestbrook, Chris . . . . . . . . . . . EC-2.4 TUEWestbrook, Paul . . . . . . . . . . . . CJ-4.6 SUNWesterberg, Niclas . . . . . . . . . .EE-3.3 SUNWeston, Morgan . . . . . . . . . . . EB-3.2 WEDWetter, Niklaus . . . . . . . . . . . �CA-1.2 SUN,
CH-1.3 SUNWetzel, Benjamin . . . . . . . . . . EA-7.3 TUE,
PD-B.9 WED, �CD-13.5 THUWeyers, Markus . . . . . . . . . . .CD-P.40 TUEWhalen, Patrick . . . . . . . . . . . . EE-2.2 SUNWheaton, Skyler . . . . . . . . . . EG-7.1 MON,
CL-2.4 THUWhite, Andrew . . . . . . . . . . . . EB-1.1 MONWhite, Andrew G. . . . . . . . . EB-2a.1 MONWhite, William . . . . . . . . . . . CF-P.23 WEDWichmann, Matthias . . . . . . . CB-3.2 TUEWicht, Andreas . . . . . . . . . .CB-P.12 MON,
CB-P.28 MON, CD-P.40 TUEWick, Sebastian . . . . . . . . . . . CJ-12.3 THUWickham, Simon J. . . . . . . . . . EI-P.7 TUEWidiez, Julie . . . . . . . . . . . . . .CB-11.1 THUWieck, Andreas . . . . . . . . . . EG-P.12 MONWiegele, Sarah . . . . . . . . . . . . . CK-9.5 TUEWiemer, Martin . . . . . . . . . . CE-11.6 WEDWienke, Andreas . . . . . . . . . . �CA-4.1 SUNWiens, Eugen . . . . . . . . . . . . . ED-3.4 MONWiersig, Jan . . . . . . . . . . . . . . .CB-4.2 WEDWiersma, Diederik . . . . . . . . . CK-1.4 SUN,
CK-9.5 TUE, CH-P.21 THUWiersma, Noémi . . . . . . . . . . �EF-6.1 MONWieser, Wolfgang . . . . . . . . . CD-P.19 TUEWieśniak, Marcin . . . . . . . . . . EB-1.3 MONWijayanto, Yusuf Nur . . . . . . �CI-5.6 MONWilcox, Keith CB-3.3 TUE, �CB-3.6 TUEWilhelm, Christophe . . . . . . . �CK-3.4 SUNWilkinson, James . . . . . . . . . CJ-P.27 WEDWilkowski, David . . . . . . . . . . . EG-2.1 SUNWill, Elisa . . . . . . . . . . . . . . . . . .EA-2.2 SUNWilliams, John . . . . . . . . . . . . . CE-1.4 SUNWilliams, Robert . . . . . . . . . . .CM-4.3 SUNWilson, Dalziel . . . . . . . . . . . . . EA-4.2 SUNWilson, Rab . . . . . . . . . . . . . . JSII-2.4 MONWilson-Rae, Ignacio . . . . . . �EA-P.30 THUWimmer, Lara . . . . . . . . . . . �EG-5a.2 MONWimmer, Martin . . . . . . . . . . . �EF-2.3 SUNWindeler, Robert . . . . . . . . . . . CJ-4.6 SUNWinkler, Dominik . . . . . . . . . . EB-4.5 WEDWinterfeldt, Martin . . . . . . . �CB-P.5 MONWinters, David . . . . . . . . . . . . CM-3.3 SUNWintersperger, Karen . . . . . . CG-4.4 WEDWirths, Stephan . . . . . . . . . . . �CB-1.4 TUEWismer, Michael . . . . . . . . . �CF-P.32 WEDWissmann, Laurens . . . . . . . . .CA-3.5 SUNWithford, Michael . . . . . . . . . CM-P.8 SUN,
CM-4.3 SUN, CH-7.4 WED,CJ-P.41 WED, CH-P.6 THU
Withford, Michael J. . . . . . . . . CI-1.5 SUN,CM-P.7 SUN, CB-5.5 WED,JSV-1.4 THU
Withford, Michael W . . . . . .CJ-P.18 WEDWitte, Christian . . . . . . . . . . JSII-2.4 MONWitte, Stefan . . . . . . . . . . . . . . CH-1.4 SUNWitting, Tobias . . . . . . . . . . . .CG-1.2 TUE,
CG-2.3 TUE, CF-5.2 WED, CF-5.3 WEDWittmann, Emanuel . . . . . . . �CF-3.2 TUEWittrock, Ulrich . . . . . . . . . . CA-P.10 SUN,
CE-7.5 MONWittwer, Valentin Johannes CA-6.1 MON,
CJ-9.6 WEDWoerner, Michael . . . . . . . . .EE-5b.2 MONWoessner, Achim . . . . . . . . . JSIV-2.2 SUNWohlfeil, Benjamin . . . . . . . . EA-8.5 WED
Wojdyr, Michael . . . . . . . . . . . . CJ-1.2 SUNWójtewicz, Szymon . . . . . . . .CH-7.2 WEDWojtkowski, Maciej . . . . . . . . CB-7.1 WEDWoldering, Lèon . . . . . . . . . . . . CE-2.2 SUNWolf, Adriana . . . . . . . . . . . . . . CB-1.1 TUEWolf, Alexey A. . . . . . . . . . . . �CM-4.2 SUNWolf, Jean-Pierre . . . . . . . . .CD-P.14 TUE,
CD-P.33 TUE, CD-P.38 TUE,CF-P.24 WED, CG-P.16 THU
Wolfersberger, Delphine . . . . EF-6.1 MONWolfesberger, Clemens . . . . CM-6.4 MONWolff, Christian . . . . . . . . . �CK-P.21 MON,
EF-P.24 THUWollhofen, Richard . . . . . . . �CM-6.4 MONWollmann, Sabine . . . . . . . . .�EB-3.2 WEDWollweber, Merve . . . . . . . . . . CE-8.3 TUEWolter, Benjamin . . . . . . . . . CG-3.4 WED,�CG-5.5 WEDWolterink, Tom A.W. . . . . . . �EA-3.2 SUNWolters, Janik . . . . . . . . . . . . EG-7.4 MON,
EA-8.3 WEDWong, Gordon Kwan Leung . .CI-3.3 SUNWong, Michael C. H. . . . . . . CG-6.2 WEDWood, Christopher . . . . . . . . EB-1.1 MONWoodroofe, Emily P. . . . . . . . . EI-P.4 TUEWoodward, Nathaniel . . . . .CE-5b.2 MONWoodward, Robert Ian . . . . EF-5.4 MON,�CJ-9.6 WEDWorhoff, Kerstin . . . . . . . . . . CK-14.1 THUWörister, Christian . . . . . . . . EH-P.5 WEDWorschech, Lukas . . . . . . . . . . CB-1.1 TUEWorthmann, Lukas . . . . . . . . EG-P.2 MONWoste, Ludger . . . . . . . . . . . .CG-P.16 THUWouters, Michiel . . . . . . . . . . . CD-9.4 TUEWrachtrup, Jörg . . . . . . . . . . . .EG-3.3 SUNWright, Ewan . . . . . . . . . . . . . . EF-2.1 SUNWright, Laura . . . . . . . . . . . . JSV-P.2 MONWu, Che Wen . . . . . . . . . . . . . JSV-2.3 THUWu, Dong . . . . . . . . . . . . . . CM/LIM.3 TUEWu, Jiang . . CK-10.2 WED, CB-9.2 THUWu, Kan . . . . . . . . . . . . . . . . . . . CI-P.2 TUEWu, Qiong . . . . . . . . . . . . . . . . . .CI-2.3 SUNWu, Tao . . . . . . . . . . . . . . . . . CH-P.28 THUWu, Tsung-Han . . . . . . . . . . .ED-2.2 MON,
CF-9.5 THUWu, Wei . . . . . . . . . . . . . . . . . . ED-P.3 MONWu, Weiping . .EH-3.5 WED, EI-1.3 THUWu, Xiaojun . . . . . . . . . . . . . . . CC-3.3 SUNWu, Yao . . . . . . . . . . . . . . . . . CE-5a.3 MONWubs, Martijn . . . . . . . . . . . . . EG-7.2 MONWuensch, Bettina . . . . . . . . . CL-P.18 SUNWuilpart, Marc . . . . . . . . . . . . . CJ-2.2 SUNWulfmeyer, Volker . . . . . . . . CA-12.5 THUWulterkens, Gerben . . . . . . . . CB-6.5 WEDWunram, Marcel . . . . . . . . . . . CF-1.1 TUEWünsch, Bettina . . . . . . . . . . . EH-6.2 THUWünsche, Hans-Jürgen . . . CB-P.19 MONWurtz, Gregory . . . . . . . . . . . CD-7.3 MON,
EH-4.2 WEDWurtz, Gregory A. . . . . . . . . . EH-4.4 WEDWyatt, Adam . . . . . . . . . . . . . �CG-P.1 THUWyatt, Adam S. . . . . . . . . . . �CG-3.3 WEDWysocki, Gerard . . . . . . . . . . . CH-8.5 WEDWysokiński, Karol . . . . . . . . . CE-P.28 TUEXi, Xiaoming . . . . . . . . . . . . . . . .CI-3.3 SUN
Xia, Tian . . . . . . . . . . . . . . . . . JSV-2.5 THUXiao, Hu . . . . . . . . . . . . . . . . . .CJ-11.5 THUXiao, Limin . �CH-4.4 SUN, �CE-P.8 TUEXiao, Shiyi . . . . . . . . . . . . . . . . . CE-3.5 SUNXiao, Xiao . . . . . . . . . . . . . . . .CD-P.18 TUEXie, Chen . . . . EE-2.4 SUN, EE-P.3 SUN,
CM-7.2 MONXie, Hongen . . . . . . . . . . . . . . PD-A.2 WEDXie, Na . . . . . . . . . . . . . . . . . �CF-P.22 WEDXie, Shangran . . . . . . . . . . . . �PD-A.9 WEDXie, Xinhua . . .EE-P.8 SUN, EE-4.3 SUN,
CG-6.5 WED, CG-6.6 WEDXie, Z. . . . . . . . . . . . . . . . . . . .CK-11.2 WEDXiong, Chunle . . . . . . . . . . . �PD-B.4 WED,
JSV-2.3 THUXiong, Qihua . . . . . . . . . . . . . . .CK-3.4 SUNXomalis, Aggelos . . . . . . . . . . �CE-3.3 SUNXu, Gang . . . . . . . . . . . . . . . . . . �EI-2.1 THUXu, J . . . . . . . . . . . . . . . . . . . . .CA-P.40 SUNXu, Jian . . . . . . . . . . . . . . . .CM/LIM.3 TUEXu, Jiancai . . . . . . . . . . . . . . . . CG-2.4 TUEXu, Jiangming . . . . . . . . . . . . �CJ-11.5 THUXu, Jin-Long . . . . . . . . . . . . . CA-P.16 SUN,
CA-P.19 SUNXu, Lin . . . . . . . . . . . . . . . . . . �CD-P.17 TUEXu, Wen-Cheng . . . . . . . . . . .JSIV-1.4 SUNXu, X. . . . . . . . . . . . . . . . . . . . CK-11.2 WEDXu, Xiaodong . . . . . . . . . . . . . CA-P.40 SUNXu, Yan . . . . . . . . . . . . . . . . . . . CB-2.3 TUEXu, Yiqing . . . . . . . . . . . . . . . . . EE-3.4 SUNXu, Zetian . . . . . . . . . . . . . . . . ED-P.3 MONXu, Zhilin . . . . . . . . . . . . . . . . . . .CI-2.3 SUNXue, Weiqi . . . . . . . . . . . . . . . . �CK-3.2 SUNXue, Xiaojie . . . . . . . . . . . . . �CE-P.12 TUE,
CJ-P.43 WED, CJ-P.45 WEDYabana, Kazuhiro . . . . . . . . . CG-P.14 THUYacomotti, Alejandro . . . . . . .�EF-2.4 SUNYadav, Amit . . . . . . . . . . . . . CM-P.15 SUN,�CE-11.2 WEDYagi, Hideki . . . . . . . . . . . . . . . .CA-2.5 SUNYakovlev, Vladislav . . . . . . . CF-P.32 WEDYakubovich, Sergei . . . . . . . . CB-7.5 WEDYakunin, Pavel . . . . . . . . . . . . CC-P.19 SUNYalunin, Sergey V. . . . . . . . EG-5a.1 MON,
EG-5a.2 MONYam, Vy . . . . . . . . . . . . . . . . . . . CK-8.3 TUEYamada, Itsunari . . . . . . . . �CK-P.17 MONYamagami, Ryu-ichi . . . . . . . . CE-8.5 TUEYamaguchi, Shigeru . . . . . . .CH-P.29 THUYamamoto, Naokatsu . . . . . . . .CI-3.6 SUNYamamoto, Takashi . . . . . . . EA-P.25 THUYamamoto, Yoshihisa . . . . . . CB-1.1 TUE,
CD-9.5 TUEYamanaka, Kazuhiro . . . . . . .ED-3.2 MONYamanaka, Masahito . . . . . . . CL-5.2 THUYamane, Keisaku . . . . . . . . . . EE-P.9 SUN,
EE-P.15 SUN, CA-7.6 MON,�CF-P.28 WEDYamanouchi, Kaoru . . . . . . . . EE-4.3 SUN,
CG-6.4 WED, CG-6.5 WED,CG-P.18 THU
Yamashita, Naoto . . . . . . . . CK-P.17 MONYamashita, Taro . . . . . . . . . .EA-P.25 THU,
EA-P.28 THU, JSV-4.1 THU,JSV-4.5 THU
227
Authors’ Index
Yamauchi, Taiki . . . . . . . . . . CA-11.5 THUYamazaki, Masaaki . . . . . . . . CJ-P.9 WED,
CJ-P.38 WEDYan, Kunlun . . . . . . . . . . . . . . . CJ-P.2 WEDYan, Xin . . �CE-5a.3 MON, CE-6.4 MONYan, Zhizhong . . . . . . . . . . . �JSV-1.4 THUYanagitani, Takagimi . . . . . . . CA-2.5 SUNYanchuk, Serhiy . . . . . . . . . . . . EF-P.4 THUYang, Biao . . . . . . . . . . . . . . . . EH-1.5 WEDYang, Chao . . . . . . . . . . . . . . . CJ-14.2 THUYang, Guoqing . . . . . . . . . . . . . EA-9.5 THUYang, Hua . . . . . . . . . . . . . . �CB-P.30 MONYang, Mingqi . . . . . . . . . . . . CB-P.30 MONYang, Quankui . . . . . . . . . . . .CN-1.2 WED,
CN-2.2 WEDYang, Shang-Da . . . . . . . . . . . . CF-3.1 TUEYang, Tie CL-P.11 SUN, �JSII-1a.1 MON,
CLEO/ECBO-2.2 WED, �CL-1.3 WEDYang, Xu . . . . . . . . . . . . . . . . . EA-10.2 THUYang, Xuezong . . . . . . . . . . . CJ-P.11 WEDYang, Yudong . . . . . . . . . . . . . CG-P.4 THUYang, Yujia . . . . . . . . . . . . . . .EE-5a.3 MONYang, Zhiyong CD-1.5 SUN, CH-3.2 SUNYao, Alison . . EF-5.3 MON, EC-P.3 TUE,
EF-9.1 THUYao, BaoQuan . . . . . . . . . . . . .CA-P.5 SUN,
CA-P.17 SUN, CJ-14.2 THUYao, Weiming . . . . . . . . . . . . . . �CI-2.6 SUNYarutkina, Irina . . . . . . . . . . . CJ-P.40 WEDYasuhara, Ryo . . . . . . . . . . . . . CE-7.6 MONYasui, Kei . . . . . . . . . . . . . . . . . .CE-2.1 SUNYasui, Shuto . . . . . . . . . . . . . .EA-P.25 THUYasukevich, Anatol . . . . . . . CA-P.38 SUN,
CA-9.3 THUYasukevich, Anatoly . . . . . . . . CA-8.5 TUEYasumatsu, Naoya . . . . . . . . CC-P.12 SUNYavsin, Denis A. . . . . . . . . . . .CK-P.1 MONYavuz, Özgün . . . . . . . . . . . �CM-P.18 SUN,
CK-P.3 MONYe, Fangwei . . . . . . . . . . . . . . . .EF-P.8 THUYe, Feihong . . . . . . . . . . . . . . . .CI-P.10 TUEYe, Guangchao . . . . . . . . . . . . �CN-P.2 TUEYe, Jun . . . . . . . . . . . . . . . . . . �ED-3.1 MONYe, Qing . . . . . . . . . . . . . . . . . .CA-P.18 SUNYeap, WengSiang . . . . . . . . . . .CL-P.8 SUNYee, Ki-Ju . . . . . . . . . . . . . . . . . EH-5.4 THUYeh, Dung-Han . . . . . . . . . . �CF-P.11 WEDYehouessi, Jean-Paul . . . . . . . CJ-3.5 SUN,�CJ-3.6 SUNYeminy, Tomer . . . . . . . . . . . . �CI-P.15 TUEYeo, Inah . . . . . . . . . . . . . . . . . . EF-2.5 SUNYeom, Dong-Il . . . . . . . . . . . . . CE-P.6 TUE,�CJ-P.23 WED, CF-4.5 WED,
CA-9.5 THU
Yilmaz, Hasan . . . . . . . . . . . CK-13.2 WED,�CL-4.5 THUYin, Chunming . . . . . . . . . . . . EA-5.2 MONYin, Jun . . . . CE-12.3 WED, �EI-1.3 THUYin, Ke . . . . . . . . . . . . . . . . . . . �CJ-7.5 WEDYin, Xinghui . . . . . . . . . . . . . . .EH-1.2 WEDYlinen, Sami . .CI-P.7 TUE, CH-6.1 WEDYoder, Paul . . . . . . . . . . . . . . . PD-A.2 WEDYohann, Franz . . . . . . . . . . . . . .CE-4.2 SUNYokota, Yuya . . . . . . . . . . . . . . .CE-P.4 TUEYong, Yean-Seng . . . . . . . . . .CJ-6a.3 MONYong, Yean-Sheng . . . . . . . . �CE-7.3 MONYoo, Kichoen . . . . . . . . . . . . . . JSI-1.4 SUNYoo, KyungWan . . . . . . . . . . . EG-P.6 MONYoon, Sung Jin . . . . . . . . . . . �CE-P.34 TUEYoshida, Fumiko . . . . . . . . . . . CC-6.4 TUEYoshida, Minoru . . . . . . . . . .CJ-P.37 WED,
CJ-P.38 WEDYoshida, Shuhei . . . . . . . . . . . . EE-P.8 SUNYoshikawa, Jun-ichi . . . . . . . . EA-1.5 SUN,
EB-P.3 WEDYoshikawa, Masashi . . . . . . . CJ-P.37 WEDYoshiki, Wataru . . . . . . . . . . . . CK-9.2 TUEYoshioka, Hiroaki . . . . . . . . . . . CE-2.1 SUNYoshioka, Kosuke . . . . . . . . . . .CC-6.3 TUEYoung, Andrew . . . . . . . . . . EG-P.16 MON,
EA-8.4 WEDYoung, Michael . . . . . . . . . . . . CM-3.3 SUNYoungs, Ian J. . . . . . . . . . . . . . . EI-1.4 THUYroala, Eduardo . . . . . . . . . . . EH-P.2 WEDYu, Fei . . . . . . . . . . . . . . . . . . . . .CE-1.5 SUNYu, Hao . . . . . . . . . . . . . . . . . . CL-P.14 SUNYu, Lule . . . . . . . . . . . . . . . . . JSIII-1.3 MONYu, Nan Ei . . . . . . . . . . . . . . . . . CE-9.3 TUEYu, Peichen . . . . . . . . . . . . . . . . CE-P.9 TUEYu, Yi . . . . . . �CD-1.5 SUN, CK-3.2 SUN,
CH-3.2 SUN, CK-P.9 MON,CB-10.1 THU
Yu, Zhangwei . . . . . . . . . . . . . CJ-14.5 THUYuan, Guanghui . . . . . . . . . . . �EG-3.5 SUNYuan, Hang . . . . . . . . . . . . . . .CA-P.13 SUNYuan, Jun . . . . . . . . . . . . . . . . �CF-P.1 WEDYuan, Wei . . . . . . . . . . . . . . . . . CN-P.2 TUEYuan, Wenhao . . . . . . . . . . . . ED-P.3 MONYüce, Emre EE-P.16 SUN, �CD-P.32 TUEYudin, Valeriy . . . . . . . . . . . . .EF-P.26 THUYudistira, Didit . . . . . . . . . . . CM-6.6 MONYulin, Alexey . . . . . . . . . . . . . .EF-P.16 THUYumashev, Konstantin . . . . CA-P.31 SUN,
CA-4.5 SUN, CA-5a.1 MON,CA-5a.2 MON, CA-5b.3 MON,CA-8.5 TUE, CE-P.5 TUE, CE-P.13 TUE
Yumashev, Konstantin V. . . CE-P.25 TUEYumoto, Masaki . . . . . . . . . .�CA-P.36 SUN
Yvind, Kresten . . . . . . . . . . . . .CK-3.2 SUN,CK-5.2 MON, CK-9.1 TUE,CB-10.1 THU
Z. Zhang, Jin . . . . . . . . . . . . . . CL-P.4 SUNZabel, Thomas . . . . . . . . . . . . CK-9.3 TUE,
CB-11.1 THUZahedpour, Sina . . . . . . . . . . . . EE-2.1 SUNZahzam, Nassim . . . . . . . . . . CD-P.36 TUEZaldo, Carlos . . . . . . . . . . . . . . .CA-2.2 SUNZalevsky, Zeev . . . . . . . . . . . . . CI-P.15 TUEZaltron, Annamaria . . . . . . . .CD-6.6 MONZalvidea, Dobryna�CLEO/ECBO-1.2 WEDZamfirescu, Marian . . . . . . . .CA-P.29 SUNZamora-Munt, Jordi . . . . . . EF-4a.2 MONZandrini, Tommaso . . . . . . . �CM-1.4 SUNZang, Leyun EG-1.1 SUN, CK-10.4 WEDZang, Xiaorun . . . . . . . . . . . .CK-11.1 WEDZanotto, Simone . . . . . . . . �CK-P.11 MON,�EH-7.5 THUZaouter, Yoann CJ-1.1 SUN, CJ-1.3 SUN,
CF-P.27 WEDZapalova, Svetlana . . . . . . . . . CE-P.5 TUEZapata, Kelly . . . . . . . . . . . . . CA-10.2 THUZapata, Luis E. . . . . . . . . . . . CA-10.2 THUZaquine, Isabelle . . . . . . . . . . EB-P.5 WEDZaramenskikh, Ksenia S. . . .CE-P.25 TUEZaukevičius, Audrius . . . . . CF-P.15 WED,
CA-11.2 THUZavelani-Rossi, Margherita CE-5a.1 MONZawilski, K. T. . . . . . . . . . . . . . CD-4.3 SUNZawilski, Kevin T. . . . . . . . . . .CD-4.1 SUNZayats, Anatoly . . . . . . . . . . .CD-7.3 MON,
EH-4.2 WEDZayats, Anatoly V. . . . . . . . . .EH-4.4 WEDZbinden, Hugo . . . . . . . . . . . . EB-1.4 MONZeijlemaker, Hans . . . . . . . . . EH-1.3 WEDZeil, Peter �CD-P.41 TUE, CJ-P.15 WEDZeitlmair, Martin . . . . . . . . . �EG-P.2 MONZeltner, Richard . . . . . . . . . . CH-P.23 THUŽeludevičius, Julijanas . . . . . CF-P.4 WED,�CJ-P.39 WEDZendzian, Waldemar . . . . . . CA-P.25 SUNZeng, Hao . . . CK-1.4 SUN, CK-9.5 TUE,
CH-P.21 THUZeng, Heping . . . . . . . . . . . . .�CJ-P.6 WED,�CJ-P.46 WEDZeng, Xi . . . . . . . . . . . . . . . . . . .CB-8.1 THUZeng, Xianglong . . . . . . . . . . EE-P.10 SUN,
EE-P.11 SUN, CF-P.1 WEDZeng, Xiaoming . . . . . . . . . . CF-P.22 WEDZeng, Xiaoyi . . . . . . . . . . . . . . ED-P.3 MONZeng, Yijia . . . . . . . . . . . . . . . . CB-4.3 WEDZengerle, Thomas . . . . . . . . . . CF-9.3 THU
Zéninari, Virginie . . . . . . . . . . CH-P.2 THUZentgraf, Thomas . . . . . . . . CK-P.16 MONZeppenfeld, Martin . . . . . . . . . EC-2.5 TUEZergioti, Ioanna . . . . . . . . . . CM-P.16 SUNZerkani, Salim . . . . . . . . . . . . . EA-4.4 SUN,
EA-P.18 THUZervas, Michalis . . . . . . . . . . CK-10.6 WEDZervas, Michalis N. . . . . . . . . . CJ-4.3 SUNZeuner, Julia . . . . . . . . . . . . . JSIV-P.1 TUEZeuner, Julia M. . . . . . . . . . �CK-13.1 WEDZhai, Chengcheng . . . . . . . . . . CD-1.5 SUNZhai, Yueyang . . . . . . . . . . . . . .EC-P.2 TUEZhang, Bin . . . CD-1.5 SUN, CJ-7.5 WEDZhang, Chunxi . . . . . . . . . . . .CH-P.14 THUZhang, Eric . . . . . . . . . . . . . . . CH-8.5 WEDZhang, Fan . . . . . . . . . . . . . . . . CB-3.2 TUEZhang, Haiyang . . . . . . . . . . . CN-1.4 WEDZhang, Haojie . . . . . . . . . . . . �CH-6.5 WEDZhang, Jian . . . . . . . . . . . . . . .CA-P.18 SUNZhang, Jianguo . . . . . . . . . . . . CE-7.1 MONZhang, Jie . . . . . . . . . . . . . . . . ED-P.3 MONZhang, Jinwei . . . . . . . . . . . �CA-P.12 SUN,�PD-A.1 WED, CA-10.5 THUZhang, Lei . . . CI-2.3 SUN, CE-P.12 TUE,�CJ-P.11 WEDZhang, Rui . . . . . . . . . . . . . . . . . CI-2.3 SUNZhang, Shuang . . . . . . . . . . . . EH-1.5 WEDZhang, Xia . CE-5a.3 MON, CE-6.4 MONZhang, Xiang . . . . . . . . . . . . . PD-B.4 WEDZhang, Xing-Yu . . . . . . . . . . . . CA-1.4 SUNZhang, Zhaowei . . . . . . . . . . ED-P.6 MON,
CN-2.1 WED, �PD-A.6 WEDZhang, Zuchen . . . . . . . . . . . CH-P.14 THUZhang, Zuxing . . . . . . . . . . . �CD-P.22 TUEZhao, Haiguang . . . . . . . . . . CE-5a.1 MONZhao, Haitao . . . . . . . . . . . . . . CF-P.2 WEDZhao, Jian . . CJ-P.6 WED, CJ-P.46 WEDZhao, Zhuang CA-P.27 SUN, CE-8.2 TUEZheltikov, Aleksei . . . . . . . . . .CD-4.5 SUN,
CF-3.5 TUE, CG-2.3 TUE, CF-5.2 WEDZheltikov, Aleksei M. . . . . . . . CF-3.4 TUEZheludev, Nikolay . . . . . . . . . . EG-2.1 SUN,
CI-P.2 TUE, EH-2.1 WED, EH-3.2 WED,CF-9.6 THU
Zheludev, Nikolay I. . . . . . . . . .CI-1.1 SUN,EG-2.3 SUN, EG-3.5 SUN,EG-5a.3 MON, CK-6.5 MON,CK-6.6 MON, CD-8.5 TUE,EH-1.4 WED, CH-7.3 WED,EH-3.5 WED, EH-4.5 WED, EI-1.3 THU,EI-1.4 THU, EA-P.23 THU
Zheng, Jiabao . . . . . . . . . . . . .JSV-4.4 THUZheng, Lihe . . . . . . . . . . . . . . . CE-7.4 MONZheng, Zhenxing . . . . . . . . . . CA-P.13 SUN
Zherebtsov, Sergey . . . . . . �EG-5b.1 MONZhigadlo, Nikolai . . . . . . . . . . EE-P.17 SUNZhilin, Alexander . . . . . . . . . . . CE-P.5 TUEZhou, Binbin EE-P.11 SUN, EF-3.6 SUN,
CF-3.6 TUE, �CF-P.14 WED,CF-P.17 WED
Zhou, Kaiming . . . . . . . . . . . CM-P.15 SUNZhou, Kainan . . . . . . . . . . . . CF-P.22 WEDZhou, Lei . . . . . . . . . . . . . . . . . . CE-3.5 SUNZhou, Pu . . . . . CI-P.9 TUE, CJ-11.5 THUZhou, Shuyu . . . . . . . . . . . . . . ED-P.3 MONZhou, Xiao-Qi . . . . . . . . . . . . . EB-5.5 WEDZhou, Zili . . . . . . . . . . . . . . . . . . EA-6.4 TUEZhu, Chengyu . . . . . . . . . . . . .CA-P.13 SUNZhu, Lingxiao . . . . . . . . . . . . . . .CJ-2.5 SUNZhu, Qihua . . . . . . . . . . . . . . .CF-P.22 WEDZhu, Wanxin . . . . . . . . . . . . . .CE-P.19 TUEZhu, Weiren . . . . . . . . . . . . . . .EH-2.5 WEDZhu, Yifu . . . . . . . . . . . . . . . . . �EA-9.5 THUZhuang, Leimeng . . . . . . . . . . . .CI-4.5 SUNZhukov, Alexey . . . . . . . . . . . . CB-4.5 WEDZhukov, Alexey E. . . . . . . . .CB-P.22 MONZhukovsky, Sergei V. . . . . . CK-P.40 MONZiebell, Melissa . . . . . . . . . . . JSV-4.2 THUZiegler, Johannes . . . . . . . . . �EH-P.5 WEDZielinski, Alejandro . . . . . . . . CG-4.2 WEDZilio, Pierfrancesco . . . . . . . . �CL-P.6 SUN,
EG-P.10 MONZilio, Pierfrancessco . . . . . . . �EH-5.6 THUZilio, Sergio . . . . . . . . . . . . . CD-5b.2 MON,
CD-P.15 TUEZilk, Matthias . . . . . . . . . . . . . .CD-8.1 TUEZimer, Hagen . . . . . . . . . . . . CM-P.10 SUNZimmermann, Felix . . . . . . . �CM-6.2 MONZimmermann, Thomas . . . . CG-5.3 WED,
CG-P.10 THUZiolowicz, Anna . . . . . . . . . . . .CE-1.6 SUN,�CI-1.4 SUN, CE-P.28 TUEZisis, Grigorios . . . . . . . . . . . . . CE-4.2 SUNZobenica, Žarko . . . . . . . . . . .JSV-2.5 THUZolotovskaya, Svetlana . . . . CM-P.6 SUN,
CM-3.5 SUN, CD-P.30 TUE,�CE-P.1 TUEZou, Bichen . . . . . . . . . . . . . . . EA-9.5 THUZubia, Joseba . . . . . . . . . . . . . . CH-5.2 TUEZukauskas, Andrius . . . . . . . CE-P.32 TUE,
CE-9.2 TUEZulonas, Modestas . . . . . . . �CE-11.3 WEDZürch, Michael . . . . . . . . . . . . CD-P.6 TUE,�CF-8.1 THUZwerger, Wilhelm . . . . . . . . . EA-P.30 THUZwier, Olger . . . . . . . . . . . . . . EA-10.2 THUZybala, Rafal . . . . . . . . . . . . . . CF-P.5 WEDZyss, Joseph CK-8.1 TUE, CK-12.3 WED
228
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229
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230
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231
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232
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233
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