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Transcript of 1 국제 Working Group 활동 보고 (Detector) Brief Report on LCWS05 at SLAC ILC Detector concept...
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국제 Working Group 활동 보고
(Detector)
• Brief Report on LCWS05 at SLAC
• ILC Detector concept
• Variety of Trackers, Calorimeters, Muons
• Beam tests and Organization
Reported by Il H. Park (Ewha)Based on summary talks of LCWS05
Korean ILC meeting, 건국대학교 , 2005 년 4 월 1 일
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Brief Report from LCWS05
• Please refer to our presentations at LCWS05 and summary talks on detector concepts, tracker, and calorimeter/muon (see the program who presented what)
• Three detector groups are organized: SiD, LDC, GLD• Korean Involved Area and technology: Silicon tracker,
Silicon Calorimeter, Scintillator Calorimeter• Korean activity(R&D on a tracker and calormeters, beam
tests of Silicon calorimeter prototype) is now exposed largely to the ILC community, particularly Korean silicon experience draws a serious attention at LCWS05
• At this workshop, we agree on joint activity of Korean Silicon Calorimeter with CALICE group and possibly with SiD in parallel as well. Foresee a substantial progress from such collaborative works this year
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Physics
Inclusive Higgs: Z Recoil mass
H Branching Ratios
Smuon pair-production
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• Performance goal (common to all det. concepts)
– Vertex Detector:
– Tracking:
– Jet energy res.:
Detector optimized for Particle Flow Algorithm (PFA)
Basic design concept
EEE
pp
pIP
tt
/3.0/
105/
sin/105)(52
2/3
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Tracker
• Momentum resolution set by recoil mass analysis of
• reconstruction and long-lived new particles (GMSB SUSY)
• Multiple scattering effects• Forward tracking• Measurement of Ecm,
differential luminosity and polarization using physics events
ZH l l X 0 0 , SK
52
2 10t
t
p
p
Recoil Mass (GeV)
52
8 10t
t
p
p
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Calorimeter
• Separate hadronically decaying W’s from Z’s in reactions where kinematic fits won’t work:
• Help solve combinatoric problem in reactions with 4 or more jets
E/E = 0.6/E
E/E = 0.3/E*e e ZH qqWW qqqql
e e ZHH qqbbbb
0 01 1 1 1
0 0 0 02 2 1 1
, e e W W ZZ
e e W W
e e ZZ
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SiD LDC GLD
Three Detector Concepts
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Comparison of parameters
SiD LDC GLD
Solenoid
B(T) 5 4 3
R(m) 2.48 3.0 3.75
L(m) 5.8 9.2 9.86
Est(GJ) 1.4 2.3 1.8
Main Tracker
Rmin (m) 0.2 0.36 0.4
Rmax(m) 1.25 1.62 2.0
m 7 150 150
Nsample 5 200 220
1/pt) 3.6e-5 1.5e-4 1.2 e-4
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GDE (Design) (Construction)
TechnologyChoice
Acc.
2004 2005 2006 2007 2008 2009 2010
CDR TDR Start Global Lab.
Det. Detector Outline Documents
CDRs LOIs
R&D PhaseCollaboration Forming Construction
Detector R&D Panel
TevatronSLAC B
LHCHERA
T2K
Done!
Detector
“Window for Detector R&D
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Review Tracking and Vertexing
Jan Timmermans - NIKHEF
32 presentations in total:
•12 vertex detector related
•10 on SI tracking
•10 on TPC R&D
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Vertex Detector•pixels ~ 20 x 20 μm2
•point resolution ~3 μm
•material <0.1% X0
•1st layer at ~1.5 cm
To keep occupancy below 1%:
•readout ~20 times during bunch train or store signals
•OR make pixels smaller ( FPCCD 5 x 5 μm2 )
Many variants: CPCCD, FPCCD, DEPFET, MAPS, FAPS, SoI, ISIS
New at LCWS05:
•(revolver)ISIS
•Add time stamping (Baltay, Bashindzhagyan)
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Vertex Detector Options
• FPCCD– Accumulate hit signals for one train and read out between
trains
– Keep low pixel occupancy by increasing number of pixels by x20 with respect to “standard” pixel detector
– As a result, pixel size should be as small as ~5x5m2
– Epitaxial layer has to be fully depleted to minimize charge spread by diffusion
– Operation at low temperature to keep dark current negligible (r.o. cycle=200ms)
Y.Sugimoto - KEK
Tracking efficiency under beam background is critical issue; simulation needed.
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• small pixels 20-30µm
• radiation tolerance (>200krad)
• low noise
• thin devices (50µm) S/N = 40
• low power (row-wise operation)
• fast readout (cold machine), 50MHz line rate
• zero suppressed datacharge collection in fully depleted substrate
drain bulksourcetop gate clear
p+
p+ n+
back contact
pn+
ninternal gate
n -
n+p+
--
++
++-
MIP
50 µ
m
--- ---
DEPFET (M. Trimpl) – Bonn, Mannheim, MPI
•FET transistor in every pixel (first amplification)
•Electrons collected at internal gate modulate the transistor current. Signal charge removed via CLEAR
•No charge transfer
•Low power consumption: ~5W for full VXD
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Flexible APS
• FAPS=Flexible APS– Every pixel has 10 deep
pipeline
• Designed for TESLA proposal. – Quick sampling during
bunch train and readout in long period between bunch trains
FAPS
Column Output
Write amplifier
RST_W
SELA
1
Memory Cell #0
Memory Cell #1
Memory Cell #9
Ibias
J. Velthuis –
UK MAPS
•S/N between 14.7 and 17.0
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Monolithic CMOS Pixel Detectors
Big Pixels50µ x 50µ
Small Pixels5µ x 5µ
Two active particle sensitive layers:
Big Pixels – High Speed Array – Hit trigger, time of hit Small Pixels – High Resolution Array – Precise x,y position, intensity
C. Baltay
After selecting hits in same bunch: occupancy ~10-6
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Designed for quick response.– Threshold detection only.
– Large pixels (~50 x 50 m).
Transmits X,Y location and time stamp of impact.
Array Designs
Contact Pads Pixel Array
Designed for resolution and querying.
– Smaller pixel size (~5 x 5 m).
– Random access addressability.
– Records intensity.
Provides intensity information only for pixel region queried.
High-speed arrays High-resolution arrays
Contact Pads Pixel Array
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Principle of SOI monolithic detector Integration of the pixel detector and readout electronics in a wafer-bonded SOI substrate
Detector handle wafer High resistive
(> 4 kcm,FZ) 400 m thick Conventional p+-n
Electronics active layer
Low resistive(9-13 cm, CZ)
1.5 m thick Standard CMOS
technology
Connection between pixel and readout channel
A. Bulgheroni - Como
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Si Tracking
T.Nelson
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Silicon Tracking System with a centralSilicon Tracking System with a centralgaseous detectorgaseous detector
The Silicon Envelope concept = The Silicon Envelope concept = ensemble of Si-trackers surrounding the TPC (ensemble of Si-trackers surrounding the TPC (LC-DET-2003-013)LC-DET-2003-013)
The Si-FCH: The Si-FCH: TPC to calorimetryTPC to calorimetry(SVX,FTD,(TPC),SiFCH)(SVX,FTD,(TPC),SiFCH) The FTD:The FTD: Microvertex to SiFCHMicrovertex to SiFCH The SIT: The SIT: Microvertex to TPCMicrovertex to TPC
The SET: The SET: TPC to calorimetryTPC to calorimetry(SVX, SIT, (TPC), SET)(SVX, SIT, (TPC), SET)
TPC
Microvertex
A. Savoy-Navarro
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Development of Double-sided Silicon Strip Detector
H. Park (BAERI, KNU)On behalf of Korean Silicon Group
• Introduction• Electrical Test• Source Test• Radiation Damage Test• Summary and Future Plan
•Fabrication “in house”
•5” wafers
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Digital Active Pixel Array
Position memory
Time memory
Position memory
Time memory
Position memory
Time memory
Position memory
Time memory
Position memory
Time memory
Position memory
Time memory
DAP Strip 1 DAP Strip 2
G.BashindzhagyanN.Sinev LCWS 2005
G.Bashindzhagyan25x25 μm2 pixels
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TPC R&D
•Gas amplification: GEM, Micromegas; compare with wires
•Different gases: Ar-CH4(5%)-CO2(2%) ‘TDR’
Ar-CH4(5%,10%) P5, P10
Ar-iC4H10(5%) Isobutane
Ar-CF4(2-10%) CF4
He-iC4H10(20%) Helium
•Laser studies
•Field cage optimisation
•Mapping a large parameter space
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Aachen
MPI/Asia
Victoria
DESY
Cornell/ Purdue
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Calorimetry and Muons
Summary Talk
Andy White
University of Texas at Arlington
LCWS05, SLAC
March 22, 2005
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Physics examples driving calorimeter design
-All of these critical physics studies demand:
Efficient jet separation and reconstruction
Excellent jet energy resolution
Excellent jet-jet mass resolution
+ jet flavor tagging
Plus… We need very good forward calorimetry for e.g. SUSY selectron studies,
and… ability to find/reconstruct photons from secondary vertices e.g. from long-lived NLSP -> G
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Large Detector
GLD
Detectors with large inner calorimeter
radius
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SiDCompact detector
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• Area of EM CAL (Barrel + Endcap)– SD: ~40 m2 / layer
– TESLA: ~80 m2 / layer
– LD: ~ 100 m2 / layer
– (JLC: ~130 m2 / layer)
How big ??
Very large number of channels for ~0.5x0.5cm2 cell size!
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Can we use a “traditional” approach to calorimetry? (using only energy measurements
based on the calorimeter systems)
60%/E 30%/E
H. VideauTarget region for jet energy resolution
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Results from “traditional” calorimeter systems
- Equalized EM and HAD responses (“compensation”)
- Optimized sampling fractions
EXAMPLES:
ZEUS - Uranium/Scintillator
Single hadrons 35%/E 1%
Electrons 17%/E 1%
Jets 50%/E
D0 – Uranium/Liquid Argon
Single hadrons 50%/E 4%
Jets 80%/E
Clearly a significant improvement is needed for LC.
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Don’t underestimate the complexity!
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Integrated Detector Design
Tracking system
EM Cal HAD CalMuon
system/ tail
catcher
VXD tag b,c
jets
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Integrated Detector Design
So now we must consider the detector as a whole.
The tracker not only provides excellent momentum resolution (certainly good enough for replacing cluster energies in the calorimeter with track momenta), but also must:
- efficiently find all the charged tracks:
Any missed charged tracks will result in the corresponding energy clusters in the calorimeter being measured with lower energy resolution and a potentially larger confusion term.
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Integrated Detector Design
- provide excellent two track resolution for correct track/energy cluster association
-> tracker outer radius/magnetic field size – implications for e.m. shower separation/Moliere radius in ECal.
- Different technologies for the ECal and HCal ??
- do we lose by not having the same technology?
- compensation – is the need for this completely overcome by using the energy flow approach?
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Calorimeter System Design
Identify and measure each jet energy component as well as possible
Following charged particles through calorimeter demands high granularity…
Two options explored in detail:
(1) Analog ECal + Analog HCal
- for HCal: cost of system for required granularity?
(2) Analog ECal + Digital HCal
- high granularity suggests a digital HCal solution - resolution (for residual neutral energy) of a purely digital calorimeter??
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Calorimeter Technologies
Electromagnetic CalorimeterPhysics requirements emphasize
segmentation/granularity (transverse AND longitudinal) over intrinsic energy resolution.
Localization of e.m. showers and e.m./hadron separation -> dense (small X0) ECal with fine segmentation.
Moliere radius -> O(1 cm.)
Transverse segmentation Moliere radius
Charged/e.m. separation -> fine transverse segmentation (first layers of ECal).
Tracking charged particles through ECal -> fine longitudinal segmentation and high MIP efficiency.
Excellent photon direction determination (e.g. GMSB)
Keep the cost (Si) under control!
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CALICE – Si/W Electromagnetic Calorimeter Wafers:
Russia/MSU and Prague
PCB: LAL design, production – Korea/KNU
Evolution of FE chip: FLC_PHY3 -> FLC_PHY4 -> FLC_TECH1
New design for ECal active gap -> 40% reduction to 1.75m, Rm = 1.4cm
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ECal work in Asia
Rt= a layer / tungsten = 15.0/3.5 = 4.8 (CALICE ~ 2) Eff. Rm = 9mm * (1 + Rt) = 52mmTotal 20 layers = 20 X0, 30cm thick19 layers of shower sampling
Si/W ECal prototype from Korea
Results from CERN beam tests 2004:
29%/E (vs. 18%/E for GEANT4)
S/N = 5.2Fit curve of 29%/√E
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ECal work in Asia (Japan-Korea-Russia)Fine granularity Pb-Scintillator with strips/small tiles and SiPM
New GLD ECal design
Previous Pb/Scint module with MAPMT readout
Study covering
Laser hitting area(9 pixels)
ECal test at DESY in 2006? YAG - 2m precision
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Scintillator/W – U. Colorado
Half-cell tile offset geometry
Electronics development is being pursued with industry
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Hybrid Ecal – Scintillator/W with Si layers – LC-CAL (INFN)
• The LCcal prototype has been built and fully tested.• Energy and position resolution as expected:
E/E ~11.-11.5% /E, pos ~2 mm (@ 30 GeV)• Light uniformity acceptable.• e/ rejection very good ( <10-3)
•45 layers
•25 × 25 × 0.3 cm3 Pb
•25 × 25 × 0.3 cm3 Scint.: 25 cells 5 × 5 cm2
•3 planes: 252 .9 × .9 cm2 Si Pads at: 2, 6, 12 X0
11.1%E
Low energy data (BTF) confirmed at high energy !!!
e-
=2.16 mm
=2.45 mm
=3.27 mm
Si L1
Si L2
Si L3
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Hadron Calorimeter – CALICE/analog
Minical – results from electron test beam
Full 1m3 prototype stack – with SiPM readout. Goal is for Fermilab test beam exposure in Spring 2006
APD chips from Silicon Sensor used
AD 1100-8, Ø 1.1 mm, Ubias~ 160 V
SiPM
APD
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Hadron Calorimeter – CALICE/digital
(1) Gas Electron Multiplier (GEM) – based DHCAL
500 channel/5-layer test mid -’05 30x30cm2 foils
Recent results: efficiency measurements confirm simulation results, 95% for 40mV threshold. Multiplicity 1.27 for 95% efficiency.
Next: 1m x 30cm foil production in preparation for 1m3 stack assembly.
Joint development of ASIC with RPC
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Muon Detector Technologies
Scintillator-based muon system development
Extruded scintillator strips with wavelength shifting fibers.
Readout: Multi-anode PMTs
GOAL: 2.5m x 1.25m planes for Fermilab test beam
U.S. Collaboration
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Muon Detector Technologies
European – CaPiRe Collaboration
TB @ Frascati
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Tail Catcher / Muon Tracker – CALICE/NIU
Goal: Test Beam Fermilab/2005
SiPM location
Extrusion Cassette
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Timescales for LC Calorimeter and Muon development
We have maybe 3-5 years to build, test*, and understand, calorimeter and muon technologies for the Linear Collider.
By “understand” I mean that the cycle of testing, data analysis, re-testing etc. should have converged to the point at which we can reliably design calorimeter and muon systems from a secure knowledge base.
For the calorimeter, this means having trusted Monte Carlo simulations of technologies at unprecedented small distance scales (~1cm), well-understood energy cut-offs, and demonstrated, efficient, complete energy flow algorithms.
Since the first modules are only now being built, 3-5 years is not an over-estimate to accomplish these tasks!
* See talk by Jae Yu for Test Beam details
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Calorimeter Technology Groups
Electromagnetic
Silicon-Tungsten BNL, Oregon, SLAC
Silicon-Tungsten UK, Czech, France, Korea, Russia
Silicon-Tungsten Korea
Scintillator/Silicon-Lead Italy
Scintillator/Silicon-Tungsten Kansas, Kansas State
Scintillator-Lead Japan, Russia
Scintillator-Tungsten Japan, Korea, Russia
Scintillator-Tungsten Colorado
Calorimeter Technology Groups
Hadronic (analog)Scintillator-Steel Czech, Germany, Russia, NIU
Scintillator-Lead Japan
Hadronic (digital)
GEM-Steel FNAL, UTA
RPC-Steel Russia
RPC-Steel ANL, Boston, Chicago, FNAL
Scintillator – Steel Northern Illinois/ NICADD
Scintillator – Lead/Steel Japan, Korea, Russia
Tail catcherScintillator-Steel FNAL, Northern Illinois
RPC-Steel Italy
From K.Kawagoe @ ACFA 07
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ILC Test Beam
*On behalf of the HEP group at UTA.
• Introduction• What has been happening?• Beam Test Timeline• World-wide TB Organization• Conclusions
LCWS2005 at StanfordMarch 18 – 22, 2005
Jae Yu University of Texas at
Arlington
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What has been happening?• Tremendous activities
– Calorimeter related• CALICE ECAL electronics run at DESY together with
Asian drift chambers
• Korean SiW ECAL at CERN
– Tracker TB’s– MDI and beam instrumentation related activities– Etc..
• A lot of groups are preparing for TB in the next couple of years
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Structure 1.4(1.4mm of W plates)
Structure 2.8 (2×1.4mm of W plates)
Structure 4.6(3×1.4mm of W plates)
ACTIVE ZONE(18×18 cm2)
Multi-layer (30) W-Si Prototype :
• 3 independent C-W alveolar structures according to the thickness of tungsten plates (1.4, 2.8 and 4.2 mm)
• 30 detector slabs which are slid into central and bottom cells of each structure
• Active zone : 33 wafers 30 layers
270 Wafers Si with 6×6 pads (10×10 mm2)
Design and Prod : LLR Integration : LLR
Prod : 150 MSU (Russia) 150 IOP (Czech republic)
3 structures W-CFi (1,2,3 x1.4mm)
30 « detteur slabs » Dimension 200x360x360 mm 9720 channels in the proto.
CALICE ECAL Test Beam at DESY
G. Geycken
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50 GeV Electron
50 GeV pion
150 GeV Muon
Total ADC of an event / 640
Beam Direction
Layers of Si sensorsand Tungstens
Frontend readout boards
Digitaland ControlBoards
Korean SiW ECAL TB at CERNPEDs
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Rt= a layer / tungsten = 15.0/3.5 = 4.8 (CALICE ~ 2) Eff. Rm = 9mm * (1 + Rt) = 52mmTotal 20 layers = 20 X0, 30cm thick19 layers of shower sampling
CERN Beam Test of Si/W ECal prototype from Korea
Results from CERN beam tests 2004:
29%/E (vs. 18%/E for GEANT4)
S/N = 5.2Fit curve of 29%/√E
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Hybrid Ecal – Scintillator/W with Si layers – LC-CAL (INFN)
• The LCcal prototype has been built and fully tested.• Energy and position resolution as expected:
E/E ~11.-11.5% /E, pos ~2 mm (@ 30 GeV)• Light uniformity acceptable.• e/ rejection very good ( <10-3)
•45 layers
•25 × 25 × 0.3 cm3 Pb
•25 × 25 × 0.3 cm3 Scint.: 25 cells 5 × 5 cm2
•3 planes: 252 .9 × .9 cm2 Si Pads at: 2, 6, 12 X0
11.1%E
Low energy data (BTF) confirmed at high energy !!!
e-
=2.16 mm
=2.45 mm
=3.27 mm
Si L1
Si L2
Si L3
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Hadron Calorimeter – CALICE/analog
Minical – results from electron test beam
Full 1m3 prototype stack – with SiPM readout. Goal is for Fermilab test beam exposure in Spring 2006
APD chips from Silicon Sensor used
AD 1100-8, Ø 1.1 mm, Ubias~ 160 V
SiPM
APD
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