scintillation hodoscope with sipm readout for the clas detector s. stepanyan (jlab) ieee conference,...
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Scintillation hodoscope with SiPM readout
for the CLAS detector
S. Stepanyan (JLAB)
IEEE conference, Dresden, October 21, 2008
S. Stepanyan, Jefferson Lab (USA)
TOF counters
Drift chambers
Beam line and the target
Electromagnetic calorimeters
6 Superconducting toroidal coils
Cherenkov counters
CEBAF Large Acceptance Spectrometer at JLAB
Multipurpose spectrometer based on a superconducting toroidal magnet. Managed by the CLAS collaboration (170 scientists from 40 institutions)
Conducts experiments in the field of high energy nuclear and particle physics using high energy electron and tagged photon beams at luminosities of up to 2x1034 cm2 sec-1, with variety of liquid and solid targets
Best suited for multi-particle final states
S. Stepanyan, Jefferson Lab (USA)
Small angle electromagnetic calorimeter
For detection of high energy photons in forward region (> 4o), 424 channel PbWO4 crystal calorimeter (IC) installed inside the CLAS boar is used
In the IC APDs are used as a photodetector due to tight space constraints and the presence of 5T solenoid field
Calorimeter performed well during the high luminosity electron run. However, lack of ability of separating electromagnetic showers induced by electrons and photons limited access to an interesting physics at low Q2 (small electron scattering angle)
For electron identification, highly segmented, lightweight charged particle detector with compact readout, immune to magnetic field is necessary in front of IC
Solenoid
Calorimeter
S. Stepanyan, Jefferson Lab (USA)
Charged particle detector in front of IC
Thin scintillation pixel hodoscope with light readout via green wave shifting fibers embedded in the surface of scintillator plates
Location of photo-detectors
Rohacell back plate
Location of readout electronicsPixels of 1 cm thick 3.8x3.8 cm2
scintillator plates arranged in octagonal shape to match the calorimeter acceptance (projected from the target)
Each pixel has one spiral and one straight grove in each side
Group of 3(4) pixels have one common fiber running through the straight groove
Total number of pixels 56, total number of fiber readout 72
Arrangement of pixels and readout in ¼ of the detector. Photo-detectors and electronics are in the “shadow” of the coils of toroidal magnet
S. Stepanyan, Jefferson Lab (USA)
Photodetectors for the hodoscope
Traditional PMTs are big and difficult to operate in high magnetic field
APDs have very low gain and hard to use in low light yield detectors
Newly developed, high gain SiPMs are ideal for a single [1mm] fiber readout
Our choice: Multi Pixel Photon Counter (MPPC) – S10362-11-100U by Hamamatsu
Gai
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S. Stepanyan, Jefferson Lab (USA)
Light yield measurements
MIP
Cosmic ray muons were selected by a coincidence between a scintillator counter positioned above the test pixel and the PMT connected directly to the test pixel
Light yield of16 photo-electrons for 2 MeV energy deposition from both, spiral and straight fibers are measured
S. Stepanyan, Jefferson Lab (USA)
MPPC grouping
Manufactures suggested voltage Range of linear operation
Each readout corner contains 18 MPPCs, divided into two groups of 9 MPPCs
Group of 9 MPPCs have common bias voltage
Gain vs. V for 100 samples of S10362-11-100U were measured
Manufacture provided and measured gains were in good agreement
MPPCs with closest median bias voltages of linear region were grouped in groups of 12
S. Stepanyan, Jefferson Lab (USA)
S. Stepanyan, Jefferson Lab (USA)
Pixel and fiber assembly
Place for readout electronicsScintillator pixels
S. Stepanyan, Jefferson Lab (USA)
Final assembly
S. Stepanyan, Jefferson Lab (USA)
Photon beam run
No selection cuts
After timing cut
.75..1 channep
~15p.e.
First beam run during April-May ’08. Photon beam with up to 5.7 GeV energy, 40 cm long LH2 target
Hodoscope covered forward scattering angles between 2 to 6.5 degrees
ADC distributions of hits in the coincidence window with CLAS selects hits from high energy charged particles.
LV
Amp Disc
ADC
TDC
Scal
Delay MPPC
S. Stepanyan, Jefferson Lab (USA)
Summery
Scintillation pixel detector for the forward region of the CLAS detector was built using 1cm thick, 3.8x3.8 cm2 scintillator plates (pixels) with embedded 1 mm diameter green WS fibers for light transport
As photo detectors, HAMAMATSU MPPC S10362-11-100U with average gain of 2x106 were used
During the beam run detector showed stable performance. Preliminary analysis showed good agreement between expected (16 p.e.) and measured (15 p.e.) light yields corresponding to high energy charged particles
Gain vs. V dependences of all 72 MPPCs were measured after two months of high luminosity beam run. No visible change in the dark currents or in the gains were observed
Scintillation detector will be used in upcoming CLAS electroproduction experiment together with PbWO4 calorimeter for electron detection at small angles