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Status of the ANTARES Neutrino-Telescope Alexander Kappes Physics Institute University Erlangen-Nuremberg for the ANTARES Collaboration WIN´05, 6.–11. June 2005 Delphi, Greece Introduction The ANTARES Detector First Results from Test- Lines Outlook

Status of the ANTARES Neutrino-Telescope

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Status of the ANTARES Neutrino-Telescope. Alexander Kappes Physics Institute University Erlangen-Nuremberg for the ANTARES Collaboration. WIN´05, 6.–11. June 2005 Delphi, Greece. Introduction The ANTARES Detector First Results from Test-Lines Outlook. - PowerPoint PPT Presentation

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Page 1: Status of the ANTARES Neutrino-Telescope

Status of the ANTARES Neutrino-Telescope

Alexander KappesPhysics InstituteUniversity Erlangen-Nurembergfor the ANTARES Collaboration

WIN´05, 6.–11. June 2005Delphi, Greece

Introduction The ANTARES Detector First Results from Test-Lines Outlook

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2Alexander Kappes University Erlangen-Nuremberg

Active Galactic Nuclei

Supernova Remnant (RX J1713.7-3946)

Gamma Ray Burst

Cosmic accelerators

(Bepposax)

Hubble

H.E.S.S.

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3Alexander Kappes University Erlangen-Nuremberg

Detection of Cosmic Neutrinos

A ! X

Earth used as shield against all other particles

Čerenkov light:

Čerenkov angle: 42o

wave lengths used: 350 – 500 nm

low cross section requires large detector volumes

key reaction: + A ! + X

Detector deployed in deep water / ice to reduce downgoing atmospheric muons

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4Alexander Kappes University Erlangen-Nuremberg

Physics with Neutrino Telescopes

Searching for point-like neutrino sources

Measurement of diffuse neutrino flux

Search for Dark Matter (WIMPs)

Search for exotic particles:e.g. magnetic monopoles

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5Alexander Kappes University Erlangen-Nuremberg

Why a Neutrino Telescope in the Mediterranean Sea? Sky coverage complementary to telescopes at South Pole Allows to observe the region of the Galactic Centre

Not seenNot seenMkn 501Mkn 501

Mkn 421Mkn 421

CrabCrab

SS433SS433

Mkn 501Mkn 501

GX339-4GX339-4SS433SS433

CrabCrab

VELAVELA

GalacticGalacticCenterCenter

Not seenNot seen

South Pole Mediterranean Sea

Sources of VHE emission (HESS 2005)

Page 6: Status of the ANTARES Neutrino-Telescope

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6Alexander Kappes University Erlangen-Nuremberg

The ANTARES Collaboration

20 institutions from 20 institutions from 6 European countries6 European countries

Page 7: Status of the ANTARES Neutrino-Telescope

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7Alexander Kappes University Erlangen-Nuremberg

The ANTARES Detector46

0 m

70 m

14.5

m

Str

ing

OpticalModule

JunctionBox

Buoy

Submersible

Cab

le to

Sho

re s

tatio

n

artist´s view(not to scale)

Hostile environment: pressure up to 240 bar sea water (corrosion)

Page 8: Status of the ANTARES Neutrino-Telescope

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8Alexander Kappes University Erlangen-Nuremberg

One of 12 ANTARES Strings

Buoy keeps string vertical

(horizontal displacement < 20 m)

Storey 3 optical modules (45o downwards) electronics in titanium cylinder

EMC cable copper wires + glass fibres mechanical connection between storeys

Anchor connector for cable to junction box control electronics for string dead weight acoustic release mechanism

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9Alexander Kappes University Erlangen-Nuremberg

Optical ModuleGlass spheres: material: borosilicate glass (free of 40K) diameter: 43 cm; 1.5 cm thick qualified for pressures up to 650 bar

BB-screening-screening

optical moduleoptical module

Photomultipliers (PMT): Ø 10 inch (Hamamatsu) transfer time spread (TTS) = 1.3 ns quantum efficiency:

> 20% @ 1760 V (360 < < 460 nm)

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10Alexander Kappes University Erlangen-Nuremberg

DAQ and Online Trigger Data acquisition:

signals digitized in situ(either wave-form or single photo-electron (SPE))

all data above low threshold (0.3 SPE)sent to shore

no hardware trigger

Online trigger: computer farm at shore station (~100 PCs) data rate from detector ~1GB/s

(dominated by background) trigger criteria: hit amplitudes,

local coincidences, causality of hits trigger output ~1MB/s = 30 TB/year

Computer CentreComputer Centre

Control room

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11Alexander Kappes University Erlangen-Nuremberg

Online Trigger Level 1: coincidences at one storey (t < 20 ns)

or large individual signal (> 2.4 SPE) Level 2: causality condition

t < n / c · x

Level 3: accept if sufficiently many causally related hits exist

EfficiencyEfficiency

cos C = 1 / n

Advanced algorithms under development

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12Alexander Kappes University Erlangen-Nuremberg

Calibration devices (Overview)

Time calibration system 1 LED in each optical module Optical beacons

- LED beacons at 4 different storeys- Laser beacon at anchor

Acoustic positioning receivers (hydrophones) at 5 storeys 1 transceiver at anchor autonomous transceivers on sea floor

Tiltmeter and compass at each storey

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13Alexander Kappes University Erlangen-Nuremberg

Time-Calibration Systems timing resolution of PMT signals determines pointing accuracy

limited by intrinsic TTS of PMTs (1.3 ns)) resolution of time calibration has to be better than 0.5 ns

expected variations of individual time offsets of PMT signals ~10 ns

complete calibration performed prior to deployment

two independent in situ calibration systems for PMTs available:

Flashed LEDs in optical modules: blue LED attached to back of each PMT illuminates only local PMT

Flashed optical beacons: illuminate mainly PMTs on neighbouring strings each beacon contains PMT for recording of emission time

OMPMT

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14Alexander Kappes University Erlangen-Nuremberg

Positioning System motion of lines due to sea current (up to 30 cm/s) 0.5 ns timing resolution requires 10 cm position accuracy for each PMT

Tiltmeters and compasses: resolutions: tiltmeters = 0.2o , compasses = 1o

Acoustic system: transmitter frequencies: 8–16 kHz (long distance)

40–60 kHz (short distance) distance measurements via run time of acoustic signals reconstruction of storey positions via triangulation

System designed to provide PMT position accuracy better than 10 cm.

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15Alexander Kappes University Erlangen-Nuremberg

Environmental Parameters

Continuously measured with various instruments on a dedicated string (Instrumentation Line) or at string anchors

quantities directly influencing reconstruction attenuation length (25–60 m, depending on wave length and time)

resolution ¼ 4 m sound velocity ) acoustic positioning system

resolution = 0.1 m/s

other quantities measured direction/speed of water current (via Doppler effect)

precision: v = 0.5 cm/s, = 0.5o

temperature, salinity (via conductivity) water pressure (device attached to anchor)

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16Alexander Kappes University Erlangen-Nuremberg

Angular resolution (simulation) E < 10 TeV: dominated by

kinematics (Æ[, E > 10 TeV: dominated by reconstruction accuracy

Muon Reconstruction

Energy resolution (simulation)

low E: muon track length E > 1 TeV: Čerenkov light from

radiative losses (small elm. showers)

< 0.3o (E > 10 TeV) (log E) ¼ 0.3 (E > 1 TeV)

Muon momentum

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17Alexander Kappes University Erlangen-Nuremberg

Detector Infrastructure and Prototype Lines

Deep-sea cable to shore station deployed

Junction box deployed and connected to deep-sea cable

Prototype lines deployed, connected to junction box and successfully recovered after 5 months

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Results from Prototype Lines (2003)

Long term measurements of optical background in the deep sea:

0.4 seconds0.4 seconds 3.53.5 monthsmonths

Baseline rateBaseline rate

Technical problems: damaged optical fibre inside cable + water leak in electronics container

) no data with ns time resolution + loss of a storey

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19Alexander Kappes University Erlangen-Nuremberg

New Test-Lines: MILOM and Line0

Deployed March 2005, connected April 2005

MILOM: Mini Instrumentation Line with Optical Modules

Line0: full line without electronics(test of mechanical structure)

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MILOM setupOptical components: equipped with final electronics 3+1 optical modules at two storeys timing calibration system:

two LED beacons at two storeys Laser Beacon attached to anchor

acoustic positioning system: receiver at 1 storey transceiver (transmitter + receiver)

at anchor

allows to test all aspects of optical line

Instrumentation components: current profiler (ADCP) sound velocimeter water properties (CSTAR, CT)

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First results from MILOMTiming calibration with LED beacons: Measured relative offset of 3 optical modules on same storey Large light pulses used ) TTS of PMT small

Optical beacon signal

Time (ns)

Am

plit

ud

e

Time difference between optical modules

electronics contribution to resolution around 0.5 ns investigations in progress to separate various contributions

t OM1 – OM0 t OM2 – OM0

=0.75ns =0.68ns

beacon signal

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First results from MILOMAcoustic positioning: Several acoustic transponders installed Currently only results from 1D measurements available

Systematic effects under control on the level of 2 mm.

Time (day)2 4 6 8 10 12 14 16 18 20

96.58

96.59

96.60

96.61

Dis

tan

ce (

m)

distance from transponder (anchor) to receiver (first storey) vs. time

distribution around daily average

8 6 4 2 0 2 4 6 8Distance (mm)

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23Alexander Kappes University Erlangen-Nuremberg

First Results from MILOM

Compass headings from all three MILOM storeys:

mostly synchronous movement of all storeys

Page 24: Status of the ANTARES Neutrino-Telescope

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24Alexander Kappes University Erlangen-Nuremberg

First results from MILOM

Environmental data:

Water temperature

+ sound velocity

Temperature almost constant at 13.2oC

Water temperature determines sound velocity (at given depth)

Water temperature

Sound velocity

Vel

oci

ty (

m/s

)

Page 25: Status of the ANTARES Neutrino-Telescope

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25Alexander Kappes University Erlangen-Nuremberg

First results from MILOM

Environmental data: Sea current (current profiler)

Most times sea current < 15 cm/s Significant changes of direction over periods from hours to days

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26Alexander Kappes University Erlangen-Nuremberg

First results from MILOM

MILOM is a big success:

Data readout (waveforms + SPE) is working as expectedand yields ns timing information

In situ timing calibration and acoustic positioning reach expected resolution

All environmental sensors are working well

Continuous data from Slow Control (monitoring of various detector components)

Lots of environmental and PMT data available; intensive studies ongoing

Page 27: Status of the ANTARES Neutrino-Telescope

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27Alexander Kappes University Erlangen-Nuremberg

Line0 deployed to test mechanical structure equipped with autonomous recording devices

water leak sensors sensors connected to electrical and fibre loops

for attenuation measurements recovered in May 2005

Results: no water leaks occurred optical transmission losses at various points on fibres

evidently all losses occur inside electronics container at entry and exit from cylinder

presently under intense investigations

On first prototype strings fibres inside cables were

damaged

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28Alexander Kappes University Erlangen-Nuremberg

ANTARES: further schedule

First full string (Line1) to be deployed and connected end of 2005

Full detector installed in 2007

From 2006 on: physics analysis !

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The future: KM3NeT

common effort of European telescope groups(ANTARES, NEMO, NESTOR) + associated sciences

aim: build and operate a km3 neutrino telescope in the Mediterranean Sea

complementary to IceCube at the South Pole

expect to get EU funding (10 MEuro) for a design study (total budget 24 MEuro) by beginning of 2006

Technical Design Report early 2009

km3 detectors required to exploit full physics potential of neutrino telescopes

Page 30: Status of the ANTARES Neutrino-Telescope

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30Alexander Kappes University Erlangen-Nuremberg

Conclusions MILOM proved to be a big success

data readout is working as expected in situ timing and position resolution sufficient to reach

angular resolution < 0.3o for neutrinos with E > 10 TeV many more data to analyse

Line0 results mechanical structure water tight and pressure resistant optical losses in fibres currently under

intense investigation

First full string expected to be deployed this year;Full detector in 2007

Well prepared for physics data to come in 2006