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, 13-15 June 2012, CERN
Outline of the talk Motivation Test set-up Analysis and Results Summary and future plan
GEM for CBM Triple GEM as a precise tracking detector in the Muon Chamber (MUCH) under the extreme conditions of the CBM experiment
Objective To measure the properties of GEM with shower and in particular Spark probabilities of Double mask and Single mask GEM
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
Voltage distribution in GEM
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
Set-up for Pion beam
Set-up for shower
Particle production during shower from FLUKA simulation Ref. A. Senger
Comparison of shower number from measurement and simulation
Current
Current and GEM counting rate: Pion beam 300 kHz
Current and GEM counting rate during Shower: Beam rate300 kHz
Current as a function of rate for DM GEM Pion beam with absorber Pion beam
Charge Vs. current for DM GEM Slope: -1.38×10-12 Slope: -2.04×10-12 Pion beam with absorber Pion beam
Current as a function of rate for SM GEM Pion beam with absorber Pion beam
Charge Vs. current for SM GEM Slope: -1.35×10-12 Slope: -1.52×10-12 Pion beam with absorber Pion beam
Efficiency
Efficiency during shower
Efficiency as a function of rate during shower
Efficiency for pion beam
Efficiency vs. rate for pion beam
Spark probability measurement
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)
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
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
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
Two sparks during a spill 412 - 407 - 402 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
Spark probability vs. global voltage for shower Discharge probability: No. of Discharge/ No. of incident particle
Spark probability vs. global voltage shower and pion beam
Spark probability vs. gain shower and pion beam
Spark probability vs. global voltage SM and DM
Off spill spark rate as a function of global voltage
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
Future plan: test beam Optimized drift gap (3 mm) Conditioned counters (SM and DM) Pixel readout ?
Acknowledgement Thanks to the RD51 collaboration for their support in the beam test…. Thank you for your kind attention !
Back up slides
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.
Pulse height distribution
Method 100 sample is taken Difference of the maximum and minimum value of the channel is taken as pulse height
Fe55 spectrum @ 400-395-390 V Resolution ~17.6%
For DM GEM at 400-395-390 with pion beam: Rate 300 kHz
For DM GEM at 415-410-405 during shower: Beam rate: 300 kHz
For SM GEM at 400-395-390 with pion beam: Rate 300 kHz
For SM GEM at 405-400-395 during shower: Beam rate: 300 kHz
Geometry of the experimental set-up
For SM GEM at 400-395-390 with pion beam: Rate 300 kHz
Definitions Spill: > 0.5 < 0.2 Spark: Spill Rbeam <R*beam> CGEM Cbeam <RGEM> <Rbeam> < 0.2 Spill
Gain as a function of global voltage for SM GEM
Corrected voltage for GEM3
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
Spark rate as a function of global voltage