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Spark probability measurement for GEM for CBM (Summary of the beam - PowerPoint PPT Presentation

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


  1. 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 1

  2. Outline of the talk — Motivation — Test set-up — Analysis and Results — Summary and future plan 2

  3. GEM for CBM — Triple GEM as a precise tracking detector in the Muon Chamber (MUCH) under the extreme conditions of the CBM experiment 3

  4. Objective — To measure the properties of GEM with shower and in particular Spark probabilities of Double mask and Single mask GEM 4

  5. Summary of beam test — Detectors — Measured parameters ◦ 2 Double mask GEM ◦ 1 Single mask GEM ◦ Current ◦ Voltage — Measurement with ◦ Trigger and GEM ◦ Pion beam Counts ◦ Pion beam with ◦ GEM signal absorber: Shower 5

  6. Voltage distribution in GEM *! 5*789! !"#! 5;<=0!>,1! (!::! ! *! !"$! ! " ) ! ! *! !"%! 9;,?@=+;!>,1!)! (!::! !! *! !"&! ! " ( ! ! *! !"'! 9;,?@=+;!>,1!(! (!::! !! *! !"(! ! " ' ! ! *! !")! ! 7?-/A0<.?!>,1! (!::! ! ! *+,-!./0! ! 1,-!23456! 6

  7. Details of the set up — Gas mixture: Ar/CO 2 : 70/30 — 7 channel HVG210 power supply — 2 sum-up boards are used for signal (2 × 128 6 × 6 mm 2 pads) for DM GEM — 4 sum-up boards are used for signal (4 × 128 4 × 4 mm 2 pads) for SM GEM — PXI LabView based DAQ is used 7

  8. Set-up for Pion beam 8

  9. Set-up for shower 9

  10. Particle production during shower from FLUKA simulation Ref. A. Senger 10

  11. Comparison of shower number from measurement and simulation 11

  12. Current 12

  13. Current and GEM counting rate: Pion beam 300 kHz 13

  14. Current and GEM counting rate during Shower: Beam rate300 kHz 14

  15. Current as a function of rate for DM GEM Pion beam Pion beam with absorber 15

  16. Charge Vs. current for DM GEM Slope: -2.04 × 10 -12 Slope: -1.38 × 10 -12 Pion beam Pion beam with absorber 16

  17. Current as a function of rate for SM GEM Pion beam Pion beam with absorber 17

  18. Charge Vs. current for SM GEM Slope: -1.52 × 10 -12 Slope: -1.35 × 10 -12 Pion beam Pion beam with absorber 18

  19. Efficiency 19

  20. Efficiency during shower 20

  21. Efficiency as a function of rate during shower 21

  22. Efficiency for pion beam 22

  23. Efficiency vs. rate for pion beam 23

  24. Spark probability measurement 24

  25. 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) 25

  26. No spark during a spill — Double Mask GEM with Fe Absorber 415_410_405 — Gas: Ar/CO 2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 26

  27. Drop in GEM counting rate — Double Mask GEM 415_410_405 with Fe Absorber — Gas: Ar/CO 2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 27

  28. Sudden increase in current — Double Mask GEM 415_410_405 with Fe Absorber — Gas: Ar/CO 2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 kHz, Pion beam 28

  29. Two sparks during a spill 412 - 407 - 402 — Double Mask GEM with Fe Absorber — Gas: Ar/CO 2 : 70/30, Gas flow rate: 5 lt/hr, Particle rate: ~300 415_410_405 kHz, Pion beam 29

  30. Spark probability vs. global voltage for shower Discharge probability: No. of Discharge/ No. of incident particle 30

  31. Spark probability vs. global voltage shower and pion beam 31

  32. Spark probability vs. gain shower and pion beam 32

  33. Spark probability vs. global voltage SM and DM 33

  34. Off spill spark rate as a function of global voltage 34

  35. 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 35

  36. Future plan: test beam — Optimized drift gap (3 mm) — Conditioned counters (SM and DM) — Pixel readout ? 36

  37. Acknowledgement Thanks to the RD51 collaboration for their support in the beam test…. Thank you for your kind attention ! 37

  38. Back up slides 38

  39. 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. 39

  40. Pulse height distribution 40

  41. Method — 100 sample is taken — Difference of the maximum and minimum value of the channel is taken as pulse height 41

  42. Fe 55 spectrum @ 400-395-390 V Resolution ~17.6% 42

  43. For DM GEM at 400-395-390 with pion beam: Rate 300 kHz 43

  44. For DM GEM at 415-410-405 during shower: Beam rate: 300 kHz 44

  45. For SM GEM at 400-395-390 with pion beam: Rate 300 kHz 45

  46. For SM GEM at 405-400-395 during shower: Beam rate: 300 kHz 46

  47. Geometry of the experimental set-up 47

  48. For SM GEM at 400-395-390 with pion beam: Rate 300 kHz 48

  49. Definitions R beam Spill: > 0.5 <R* beam > C GEM C beam < 0.2 Spark: ¡ <R GEM > <R beam > Spill 49

  50. Gain as a function of global voltage for SM GEM 50

  51. Corrected voltage for GEM3 51

  52. Discharge probability as a function of gain — Discharge probability: No. of Discharge/ No. of incident particle Ref: S. Bachmann et al., NIM A 470 (2001) 548–561 52

  53. Spark rate as a function of global voltage 53

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