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Spark probability measurement for GEM for CBM (Summary of the beam test at CERN SPS, October 2011)
Saikat Biswas, A. Abuhoza, U. Frankenfeld, C. Garabatos, J. Hehner, T. Morhardt, C.J. Schmidt, H.R. Schmidt, J. Wiechula GSI Detector Laboratory RD51 Mini week, June 2012, CERN
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Outline of the talk Motivation Test set-up Analysis and Results
Summary and future plan
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GEM for CBM Triple GEM as a precise tracking detector in the Muon Chamber (MUCH) under the extreme conditions of the CBM experiment
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Objective To measure the properties of GEM with shower and in particular Spark probabilities of Double mask and Single mask GEM
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Summary of beam test Detectors Measurement with Measured parameters
2 Double mask GEM 1 Single mask GEM Measurement with Pion beam Pion beam with absorber: Shower Measured parameters Current Voltage Trigger and GEM Counts GEM signal
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Voltage distribution in GEM
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Details of the set up Gas mixture: Ar/CO2: 70/30
7 channel HVG210 power supply 2 sum-up boards are used for signal (2×128 6×6 mm2 pads) for DM GEM 4 sum-up boards are used for signal (4×128 4×4 mm2 pads) for SM GEM PXI LabView based DAQ is used
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Set-up for Pion beam
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Set-up for shower
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Particle production during shower from FLUKA simulation
Ref. A. Senger
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Comparison of shower number from measurement and simulation
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Current
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Current and GEM counting rate: Pion beam 300 kHz
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Current and GEM counting rate during Shower: Beam rate300 kHz
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Current as a function of rate for DM GEM
Pion beam with absorber Pion beam
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Charge Vs. current for DM GEM
Slope: -1.38×10-12 Slope: -2.04×10-12 Pion beam with absorber Pion beam
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Current as a function of rate for SM GEM
Pion beam with absorber Pion beam
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Charge Vs. current for SM GEM
Slope: -1.35×10-12 Slope: -1.52×10-12 Pion beam with absorber Pion beam
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Efficiency
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Efficiency during shower
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Efficiency as a function of rate during shower
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Efficiency for pion beam
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Efficiency vs. rate for pion beam
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Spark probability measurement
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Methods of Spark detection
Absence of signal Drop in the counting rate of GEM signals Data from sampling ADC Detection of high current Sudden increase in the Current (Slow) Built in Trip checker in HVG210 Power supply (Fast)
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No spark during a spill Double Mask GEM with Fe Absorber
Gas: Ar/CO2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 415_410_405
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Drop in GEM counting rate
Double Mask GEM with Fe Absorber Gas: Ar/CO2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 415_410_405
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Sudden increase in current
Double Mask GEM with Fe Absorber Gas: Ar/CO2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 415_410_405
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Two sparks during a spill
Double Mask GEM with Fe Absorber Gas: Ar/CO2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 415_410_405
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Spark probability vs. global voltage for shower
Discharge probability: No. of Discharge/ No. of incident particle
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Spark probability vs. global voltage shower and pion beam
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Spark probability vs. gain shower and pion beam
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Spark probability vs. global voltage SM and DM
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Off spill spark rate as a function of global voltage
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Summary SPS test line has good conditions for our purpose
2 mm drift gap sub-optimal (3 mm standard!) Efficiency Rate dependency of efficiency observed Pion (signal close to threshold!) Shower (signal below threshold! Pick-up noise) Spark probability Spark measurement reliable also with noise (high thresholds) Comparable spark probability for pion beam and shower (high rate) ! Higher spark probabilities for lower intensities (shower) SM GEM Was in conditioning phase. No indication for different performance
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Future plan: test beam Optimized drift gap (3 mm)
Conditioned counters (SM and DM) Pixel readout ?
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Acknowledgement Thanks to the RD51 collaboration for their support in the beam test…. Thank you for your kind attention !
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Back up slides
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Conclusion The spark probability for pion beam is high.
May be the gain is not measured correctly!! Effect of space charge !! Investigated in different conditions. to be understood the different spark probabilities.
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Pulse height distribution
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Method 100 sample is taken Difference of the maximum and minimum value of the channel is taken as pulse height
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Fe V Resolution ~17.6%
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For DM GEM at 400-395-390 with pion beam: Rate 300 kHz
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For DM GEM at 415-410-405 during shower: Beam rate: 300 kHz
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For SM GEM at 400-395-390 with pion beam: Rate 300 kHz
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For SM GEM at 405-400-395 during shower: Beam rate: 300 kHz
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Geometry of the experimental set-up
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For SM GEM at 400-395-390 with pion beam: Rate 300 kHz
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Definitions Spill: > 0.5 < 0.2 Spark: Spill Rbeam <R*beam>
CGEM Cbeam <RGEM> <Rbeam> < 0.2 Spill
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Gain as a function of global voltage for SM GEM
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Corrected voltage for GEM3
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Discharge probability as a function of gain
No. of Discharge/ No. of incident particle Ref: S. Bachmann et al., NIM A 470 (2001) 548–561
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Spark rate as a function of global voltage
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