LHC and R&D for High Luminosity Upgrade Frédérick Bordry TIARA - PP Final Meeting -. 27 th November 2013

LHC and R&D for High Luminosity UpgradeFrédérick Bordry TIARA - PP Final Meeting -. 27th November 2013

2LHC and R&D for High Luminosity UpgradeFrédérick Bordry TIARA - PP Final Meeting -. 27th November 2013

- Long Shutdown 1 (LS1 ) very short status

- Run 2 (from LS1 to LS2) 13-14 TeV- LS2 and Run 3 300 fb-1

- High Luminosity LHC project 3’000 fb-1

- Future Circular Colliders 100 TeV

- Conclusion

- Long Shutdown 1 (LS1 ) very short status

- Run 2 (from LS1 to LS2) 13-14 TeV- LS2 and Run 3 300 fb-1

- High Luminosity LHC project 3’000 fb-1

- Future Circular Colliders 100 TeV

- Conclusion

Outline

2


2010: 0.04 fb-1

7 TeV CoMCommissioning

2011: 6.1 fb-1

7 TeV CoM… exploring limits

2012: 23.3 fb-1

8 TeV CoM… production

BEH boson announce

2010-2012: LHC integrated luminosity

3.5 TeV and 4 TeV in 2012Up to 1380 bunches with1.5 1011 protons

Lpeak = 0.77. 1034


LS1 starts as the shutdown to repair the magnet interconnects to allow nominal current in the dipole and lattice quadrupole circuits of the LHC.

It has now become a major shutdown which, in addition, includes other repairs, maintenance, consolidation, upgrades and cabling across the whole accelerator complex and the associated experimental facilities.

All this in the shadow of the repair of the magnet interconnects.

Long Shutdown 1


LS1: LHC schedule

Courtesy of Katy Foraz

RE

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RE

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Pt 1LSS Arc 12 LSS Pt 2 LSS

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Electrical Maintenance - No accessElectrical Maintenance - No access

Electrical Maintenance - No access







Acc.

PAD_MADPAD_MAD

PAD_MAD

PAD_MAD PAD_MADPAD_MAD PAD_MAD

PAD_MAD

PAD_MAD PAD_MAD

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PAD_MADPAD_MAD

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Acc.

PAD_MAD

PAD_MAD

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Prepared by Checked by Approved by

M. BarberanM. BernardiniJ. CoupardK. Foraz

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13 TeV operation


3

Done Done Done

3000

60 % done


SMACC DashboardSuperconducting Magnets and Circuits Consolidation


PhysicsBeam commissioning

ShutdownPowering tests

F M A M J J A S O N D J F J FM A M J J A S O N D

2013 2014 2015

M A

LHC

SPS

PS

PS Booster

beam to beam

available for works

16th Feb. 27th November

LS 1 from 16th Feb. 2013 to Dec. 2014


http://cern.ch/ls1dashboard

So far, LS1 is on schedule for beams in January 2015 for LHC


Expectations after Long Shutdown 1 (2015)

• Collisions at 13 TeV c.m.

Run 2:Start with 6.5 TeVand later decision towards 7 TeV according to magnet training


Expectations after Long Shutdown 1 (2015)

• Collisions at 13 TeV c.m.• 25 ns bunch spacing

Using new injector beam production scheme (BCMS), resulting in brighter beams.

Number of

bunches

Intensity per bunch

Transverse emittance

Peak luminosity

Pile up

Int. yearlyluminosity

25 ns BCMS 2508 1.15 × 1011 1.9 µm 1.6×1034 cm-2s-1 ~43 ~42 fb-1

• β* ≤ 0.5m (was 0.6 m in 2012)• Other conditions:

– Similar turn around time– Similar machine availability

• Expected maximum luminosity: 1.6 x 1034 cm-2 s-1 ± 20%– Limited by inner triplet heat load limit, due to collisions debris

Courtesy of the LIU-PS project team

Batch Compression and Merging and splitting (BCMS)


~300 fb-1“Baseline” luminosity


LINAC4 – PS Booster:– H- injection and increase of PSB injection energy from 50 MeV to 160 MeV, to

increase PSB space charge threshold– New RF cavity system, new main power converters– Increase of extraction energy from 1.4 GeV to 2 GeV

These are only the main modifications and this list is far from exhaustive

Project leadership: R. Garoby and M. Meddahi

LS2 : (2018), LHC Injector Upgrades (LIU)

SPS− Electron Cloud mitigation – strong feedback system, or coating of the vacuum system− Impedance reduction, improved feedbacks− Large-scale modification to the main RF system

PS:− Increase of injection energy from 1.4 GeV to 2 GeV to increase PS

space charge threshold− Transverse resonance compensation− New RF Longitudinal feedback system − New RF beam manipulation scheme to increase beam brightness


Why High-Luminosity LHC ? (LS3)

By continuous performance improvement and consolidation

By implementing HL-LHC

Almost a factor 3

Goal of HL-LHC project:• 250 – 300 fb-1 per year• 3000 fb-1 in about 10 years

Around 300 fb-1 the present Inner Triplet

magnets reach the end of their useful life (due to

radiation damage)and must be replaced.


Initial Milestones of High Luminosity LHC

July 2010: Start of the Design and target R&D, preparation of FP7-HiLumi Design Study application

Nov 2010: application FP7-Hilumi LHC Dec 2010: Official launch of the design study at CERNMar 2011: Approval FP7 HiLumi LHC by EC: 15/15

score, full request granted: 3.9 M€ (1.2 M€ CERN)

Nov 2011: Start FP7 HiLumi LHC design studyJuly 2012: Paper HiLumi for EU strategy (CERN ATS-2012-236)


c) Europe’s top priority should be the exploitation of the full potential of the LHC, including the high-luminosity upgrade of the machine and detectors with a

view to collecting ten times more data than in the initial design, by around 2030. This upgrade programme will also provide further exciting opportunities for the study of flavour physics and the quark-gluon plasma.

HL-LHC from a study to a PROJECT300 fb-1 → 3000 fb-1

including LHC injectors upgrade LIU (Linac 4, Booster 2GeV, PS and SPS upgrade)

The European Strategy for Particle Physics Update 2013


The HL-LHC Project

• New IR-quads Nb3Sn (inner triplets)

• New 11 T Nb3Sn (short) dipoles

• Collimation upgrade• Cryogenics upgrade• Crab Cavities• Cold powering• Machine protection• …

Major intervention on more than 1.2 km of the LHC Project leadership: L. Rossi and O. Brüning


Squeezing the beams: High Field SC Magnets

Courtesy Lucio Rossi

Quads for the inner triplet Decision 2012 for low-β quadsAperture 150 mm – 140 T/m (Bpeak ≈12.3 T)

(LHC: 8 T, 70 mm )

- Dipoles 11 T for LS2 (see later)

More focus strength, * as low as 15 cm (55 cm in LHC)thanks to ATS (Achromatic Telescopic Squeeze) opticsIn some scheme even * down to 7.5 cm are considered

- Dipoles for beam recombination/separation capable of 6-8 T with 150-180 mm aperture (LHC: 1.8 T, 70 mm)


LARP (US LHC program) MagnetsSQSM TQS

LR

LQS-4m

HQTQC


Target:200 T/m gradient at 1.9 K

LQS01a: 202 T/m at 1.9 KLQS01b: 222 T/m at 4.6 K 227 T/m at 1.9 K

LQS02: 198 T/m at 4.6 K 150 A/s 208 T/m at 1.9 K 150 A/s limited by one coil

LQS03: 208 T/m at 4.6 K 210 T/m at 1.9 K1st quench: 86% s.s. limit

3.3 m coils90 mm aperture

LQS of LARPCourtesy: G. Ambrosio FNALand G. Sabbi , LBNL


LS2 : collimators and 11T Dipole

X


Nb3Sn 11 T model program• Demonstrate the required performance (11.25 T at 11850 A)• Achieve accelerator field quality• Study in depth mechanics and manufacturing • Address specific issues such as quench protection

NOTE: virtual reality models

FNAL MBHSP02 ready for test

CERN 54/61 practice coil

Next 2 years !

By courtesy of D. Mitchell, F. Nobrega (FNAL) and M. Karppinen (CERN)

FNAL short model

CERN coil


Encouraging results !• Bmax= 11.7 T (78% of

expected SSL at 1.9 K)• Improving field quality

(reduced sub-element diameter, cored cable)

And there is more work to do:

• Ramp-rate quench dependence

• Holding current quenches

• Geometric harmonics

MBHSP01

MBHSP02

11850 A 4.2 K1.9 K

Performance from G. Chlachidze, J. Di Marco, images E. Barzi (FNAL)

Nb3Sn 11 T Performance


Type Material Field/Gradient(T)/(T/m)

Aperture(mm)

Length(m)

Q1,Q3Q2 Single aperture Nb3Sn (12.1) 140 150

86.7

D1 Single aperture Nb-Ti 5.2 150 6.7

D2 Twin aperture Nb-Ti 3.5…5.0 95…105 7…10

Q4 Twin aperture Nb-Ti (5.9) 120 90 4.2

DS 11T Twin aperture Nb3Sn 10.8 60 11

Courtesy Ezio Todesco

HL-LHC (main) magnet demands


A GLOBAL PROJECT

20 40 60 80 100 120 140 160 180distance to IP (m)

Q1 Q3Q2a Q2b D1

Q1-3: 140 T/mMCBX: 2.2 T 2.5/4.5 T mD1: 5.6 T 35 T mD2: 3.5 T 35 T mQ4: 120 T/m D2 Q4

Baseline layout of HL-LHC IR region

Setting up International collaboration

but also involving industrial firms with national laboratories

http://www.iconarchive.com/show/flag-icons-by-gosquared/United-States-icon.html

http://www.iconarchive.com/show/flag-icons-by-gosquared/United-Kingdom-icon.html


Approximately 30-40 tons of HEP-grade material (Note: ITER = 600 tons)

required

procured

Focussed and sustained effort from industry and scientists Our thanks to the team in CEA-Saclay for the special (and significant) contribution to FReSCa-II wire procurement

FReSCa-II

11 T DS-MB

IR quadrupoles

Statistics by A. Ballarino and CERN TE-MSC/SCD

Production quantities (and orders)


IR Collimation Upgrade

Update of present collimation system during LS1:– Replace existing collimators – Reduce setup time (gain of factor ~100)– Improved monitoring

For HL-LHC add dispersion suppressor collimation– Eliminate off-momentum particles in a region with high dispersion– Technology of choice for the DS collimators is warm with by-pass

cryostat

– low impedance collimators: coating with Molybdenum– Design completed with 4.5 m integration length.– Prototyping on-going


Crab Cavities, Increase “Head on”

Aim: reduce the effect of the crossing angle

DQWR prototype17-Jan-2013

RF-Dipole Nb prototype

Without crabbing Without crabbing

• 3 proto types available• Cavity tests are on-going• Test with beam in SPS foreseen in

2015-2016• Beam test in LHC foreseen in 2017

New crossing strategy under study to soften the pile-up density: some new schemas have interesting potential as “crab-kissing”, to be discussed with all experiments(“Pile-up at HL-LHC and possible mitigation” Stephane Fartoukh on Wed. 2nd Oct.)


First test of RF dipole (April 2013)(ODU-SLAC at J-LAB)

Courtesy A. Ratti, LBL


Thinking to cryomodule…

D2Q4

Q4

D2IP

11 meters

Courtesy Lucio Rossi


Cryo layout…and to test with beam in the CERN SPS (2016-2017)


R2E: Removal of Power Converter (200kA-5 kV SC cable, 100 m height)

Φ = 62 mm

7 × 14 kA, 7 × 3 kA and 8 × 0.6 kA cables – Itot120 kA @ 30 K

MgB2

(or other HTS)

Also DFBs (current lead boxes) removed to surface Final solution to R2E problem – in some pointsMake room for shielding un-movable electronicsMake the maintenance and application of ALARA principle much easier and effective


tod

ay

“…exploitation of the full potential of the LHC, including the high-luminosity upgrade of the machine and detectors…”

=> High Luminosity LHC project

ProjectKick-off meeting: 11th Nov. 2013

(Daresbury)

http://cern.ch/hilumilhc

http://cern.ch/hilumilhc


Total integrated luminosity of 3000 fb-1 for p-p by 2035, with LSs taken into account and 1 month for ion physics per year.

The plan of HL-LHC (baseline)

Levelling at 5 1034 cm-2 s-1: 140 events/crossing in average, at 25 ns; several scenarios under study to limit to 1.0 → 1.3 event/mm

~3000 fb-1


Next Milestones: High Luminosity LHC

Jun. 2014: PDR (Preliminary Design Report) and re-baseline (costing, time) of the project

Sep. 2015: First short model QXF (inner triplet)Nov. 2015: TDR and end of FP7 Design StudySep. 2016: First full size MQXF (long triplet Quad)2016-17: Test Crab Cavities in SPS

Start Construction LS2 : Installation in LS2 of Cryogenics P4, SC

horizontal link P7, 11 T dipole and DS collimators in P2, first Molybdenum collimators

LS3 : installation of all HL-LHC hardware synchronized with long detector shutdown


with emphasis on proton-proton and electron-positron high-energy frontier machines. These design studies should be coupled to a vigorous accelerator R&D

programme, including high-field magnets and high-gradient accelerating structures, in collaboration with national institutes, laboratories and universities worldwide.

HGA

And also R&D on Proton-Driven Plasma Wakefield Acceleration (AWAKE Expt at CERN)

“to propose an ambitious post-LHC accelerator project at CERN by the time of the next Strategy update”d) CERN should undertake design studies for accelerator projects in a global context, d) CERN should undertake design studies for accelerator projects in a global context,


Tunnel implementations (laser straight)

Central MDI & Interaction Region

CLIC developments towards 2018

A re-baselined staged project plan, cost and power optimisation,

increased industrialisation effort for cost-drivers

High Gradient structure development and significantly increased test-

capacity for X-band RF-structures

System-test programmes in CTF3, at ATF and FACET, as well as system-tests in collaborative

programmes with light-source laboratories

Technical systems developments, related among others to complete

modules, alignment/stability, instrumentation and power sources

Physics studies related to energy frontier capabilities and potential

new physics as it emerges from LHC


with emphasis on proton-proton and electron-positron high-energy frontier machines. These design studies should be coupled to a vigorous accelerator R&D

programme, including high-field magnets and high-gradient accelerating structures, in collaboration with national institutes, laboratories and universities worldwide.

HFMHGA

And also R&D on Proton-Driven Plasma Wakefield Acceleration (AWAKE Expt at CERN)

“to propose an ambitious post-LHC accelerator project at CERN by the time of the next Strategy update”d) CERN should undertake design studies for accelerator projects in a global context, d) CERN should undertake design studies for accelerator projects in a global context,


Malta Workshop: HE-LHC @ 33 TeV c.o.m.14-16 October 2010

0

20

40

60

80

0 20 40 60 80 100 120

y (m

m)

x (mm)

HTS

HTS

Nb3Snlow j

Nb-Ti

Nb-TiNb3Snlow j

Nb3Snlow j

Nb3Snhigh j

Nb3Snhigh j

Nb3Snhigh j

Nb3Snhigh j

Material N. turns Coil fraction Peak field Joverall (A/mm2) Nb-Ti 41 27% 8 380 Nb3Sn (high Jc) 55 37% 13 380 Nb3Sn (Low Jc) 30 20% 15 190 HTS 24 16% 20.5 380

Magnet design (20 T): very challenging but not impossible. 300 mm inter-beamMultiple powering in the same magnet (and more sectioning for energy)Work for 4 years to assess HTS for 2X20T to open the way to 16.5 T/beam .Otherwise limit field to 15.5 T for 2x13 TeVHigher INJ energy is desirable (2xSPS)

The synchrotron light is not a stopper by operating the beam screen at 60 K. The beam stability looks « easier » than LHC thanks to dumping time.Collimation is possibly not more difficult than HL-LHC. Reaching 2x1034 appears reasonable.The big challenge, after main magnet technology, is beam handling for INJ & beam dump: new kicker technology is needed since we cannot make twice more room for LHC kickers.


parameter LHC HL-LHC HE-LHCc.m. energy [TeV] 14 33circumference C [km] 26.7 26.7dipole field [T] 8.33 20dipole coil aperture [mm] 56 40beam half aperture [cm] ~2 1.3injection energy [TeV] 0.45 >1.0no. of bunches 2808 2808bunch population Nb [1011] 1.15 2.2 0.94init. tr. norm. emittance [mm] 3.75 2.5 1.38init. longit. emittance [eVs] 2.5 3.8no. IPs contributing to DQ 3 2 2max. total b-b tune shift DQ 0.01 0.015 0.01beam current [A] 0.584 1.12 0.478rms bunch length [cm] 7.55 7.55IP beta function [m] 0.55 0.15 0.35rms IP spot size [mm] 16.7 7.1 (min.) 5.2

O. Dominguez, L. Rossi, F. Zimmermann

HE-LHC main parameters


The grand challenge of today is to develop the technology of high-field superconductors

(field quality,…)

From Luca Bottura

Superconductors: from materials to applications

10T

16T20+ T


EuCARD2: Develop 10 kA class HTS accelerator cable using Bi-2212 and YBCO. Test stability, magnetization, and strain tolerance

WP10: a 5 T, 40 mm bore HTS dipole

YBCO

Program Eucard2 on HTS


"Very High Energy LHC"

First studies on a new 80 km tunnel in the Geneva area

42 TeV with 8.3 T using present LHC dipoles

80 TeV with 16 T based on Nb3Sn dipoles

100 TeV with 20 T based on HTS dipoles

HE-LHC :33 TeVwith 20T magnets


16 T 100 TeV in 100 km20 T 100 TeV in 80 km

FCC (Future Circular Colliders)

CDR and cost reviewfor the next ESU (2018)(including injectors)

80-100 km tunnel infrastructure in Geneva area – design driven by pp-collider requirements

with possibility of e+-e- (TLEP) and p-e (VLHeC)


Infrastructuretunnels, surface buildings, transport (access roads), civil engineering, cooling

ventilation, electricity, cryogenics, communication & IT, fabrication and installation processes, maintenance, environmental impact and monitoring, safety

Hadron colliderOptics and beam dynamics

Functional specificationsPerformance specs

Critical technical systemsRelated R+D programsHE-LHC comparisonOperation conceptDetector concept

Physics requirements

Hadron injectorsBeam optics and

dynamicsFunctional specs

Performance specsCritical technical

systemsOperation concept

e+ e- colliderOptics and beam dynamics

Functional specificationsPerformance specs

Critical technical systemsRelated R+D programs

Injector (Booster)Operation conceptDetector concept

Physics requirements

e- p option: Physics, Integration, additional requirements

Future Circular Colliders - Conceptual Design Study

for next European Strategy Update (2018)

FCC Study Scope and Structure


tod

ay

“CERN should undertake design studies for accelerator projects in a global context, with emphasis on proton-proton and electron- positron high-energy frontier machines.”

Project

FCC Study : p-p towards 100 TeV

Kick-off meeting: 12th-14th Feb. 2014

FCC: Future Circular Colliders

CDR and Cost Review 2018

The scope of FCC kick-off meeting will be to discuss the main study topics and to prepare the groundwork for the establishment of international collaborations.

The formal part of the meeting will start at noon on 12th Feb. and last until noon on 14th Feb. and will be followed by informal discussions focused on international collaboration until the afternoon of 15th Feb.


- LS1 [2013-2014] : 1st beams in 2015- Run 2 : 13 TeV – 25 ns – up to 1.7 1034 cm-2.s-1, 40-45 fb-1 per year- LS2 (higher intensity - LIU) [2018 or 2019] - Run 3 (up to ~2.0 1034 cm-2.s-1)

- HL-LHC : R&D => approved project with a kick-off meeting on 11th Nov. 2013

A lot of technical and operation challenges : - Nb3Sn magnets (accelerator field quality) (HFM roadmap) - Collimators- Superconducting links - Crab cavities- Increased availability (machine protection,…)- …Accelerator-experiment interface are central:- Bunch spacing, pile-up density, crossing schemas, background,

forward detectors, collimation,…

Conclusion: “Exploitation of the full potential of the LHC"

300 fb-1 before LS3

3000 fb-1 before 2035


CERN is undertaking international studies for the design of two alternatives for post-LHC machine

• highest possible energy e+-e- with CLIC• future circular colliders (FCC) in the 100 km range

CDR and cost review for the next ESU (target 2018)

For FCC, the main emphasis is on a hadron collider with a c.m. energy of ~100 TeV at the energy frontier, determining the infrastructure.

The common study will also contain an e+e- collider, as potential intermediate step, and look at an e-p option.

• Preparation of FCC Design Study kick-off meeting:12-14th February 2014 in Geneva area

- Establishing international collaborations - Set-up study groups and study committees

Thanks for your attention

Conclusion cont’d : CLIC-LC and FCC


Luminosity Levelling, a key to success

• High peak luminosity• Minimize pile-up in

experiments and provide “constant” luminosity

• Obtain about 3 - 4 fb-1/day (40% stable beams)

• About 250 to 300 fb-1/year


25 ns 50 ns

# Bunches 2808 1404

p/bunch [1011] 2.0 (1.01 A) 3.3 (0.83 A)

eL [eV.s] 2.5 2.5

sz [cm] 7.5 7.5

sdp/p [10-3] 0.1 0.1

gex,y [mm] 2.5 3.0

b* [cm] (baseline) 15 15

X-angle [mrad] 590 (12.5 s) 590 (11.4 s)

Loss factor 0.30 0.33

Peak lumi [1034] 6.0 7.4

Virtual lumi [1034] 20.0 22.7

Tleveling [h] @ 5E34 7.8 6.8

#Pile up @5E34 123 247

25 ns is the option However:50 ns should be kept as alive and possible because we DO NOT have enough experience on the actual limit (e-clouds, Ibeam)

Baseline parameters of HL for reaching 250 -300 fb-1/year

Courtesy Oliver Brüning

Continuous global optimisation with LIU

Documents

LHC and R&D for High Luminosity Upgrade Frédérick Bordry TIARA - PP Final Meeting -. 27 th November 2013