micro pixel chamber operation with gas electron multiplier
play

Micro Pixel Chamber Operation with Gas Electron Multiplier Kyoto - PowerPoint PPT Presentation

Micro Pixel Chamber Operation with Gas Electron Multiplier Kyoto University dept. of physics Cosmic-ray group y g p K. Hattori Co te ts Contents 1. -PIC (Micro Pixel Chamber), micro-TPC (Time Projection Chamber based on -PIC) 2. For


  1. Micro Pixel Chamber Operation with Gas Electron Multiplier Kyoto University dept. of physics Cosmic-ray group y g p K. Hattori Co te ts Contents 1. μ -PIC (Micro Pixel Chamber), micro-TPC (Time Projection Chamber based on μ -PIC) 2. For detection of MIPs μ -PIC + GEM (gas electron multiplier) μ (g p ) 3. Performance of GEM + μ -PIC TPC 4 Summary 4.Summary 7 th International Conference on Position Sensitive Detectors

  2. Advanced Compton Camera p based on Micro Pixel Chamber(µ-PIC) sub MeV ~ MeV gamma-ray Compton scattering is dominant micro-TPC micro TPC energy and track of a recoil electron scintillator (surrounding micro-TPC) scintillator (surrounding micro-TPC) energy and position of a scattered gamma-ray g y 1photon : reconstruct completely energy & direction low background images Improvement of micro TPC Improvement of micro-TPC 7 th International Conference on Position Sensitive Detectors

  3. μ –PIC(Micro Pixel Chamber) & micro & micro - TPC TPC 2-dimensional imaging 400 μ m gaseous detector d t t (pitch 400 μ m, size 10cm × 10cm) larger one: Takada’s poster larger one: Takada s poster 10cm Max gas gain ~ 15000 Stable operation @gas gain @gas gain ~ 6000 6000 position resolution ~ 120 μ m ~ 120 μ m Electric micro -TPC field Time Projection Time Projection electron 8cm Chamber based on μ -PIC proton 7 th International Conference on Position Sensitive Detectors

  4. For MIP (Minimum Ionizing Particle) detection… Compton camera · · · · · detection of recoil electron by micro-TPC Recoil electron d E /d x ~ 2 ~ 3 × MIP µ-PIC stable operation µ p @ gas gain 6,000 Stable gas gain > 2 × 10 4 (We haven’t achieved because of discharge) sub amplification device GEM(Gas Electron Multiplier) F.Sauli(1997) Operated @ low gas gain(< 50) 7 th International Conference on Position Sensitive Detectors

  5. GEM + μ -PIC -HV system t 5M Ω Cu drift plane -HV HV (5 μ m) (5 μ m) electron cloud 7.5mm 0.5kV/cm polyimide 10M Ω (50 m) (50 μ m) GEM 5mm 2kV/cm 10M Ω μ -PIC GEM installed -HV just above μ -PIC Standard GEM design 70 μ m Mask developed by Hamagaki Lab. 140 μ m 140 μ m @ CNS Univ of Tokyo @ CNS Univ. of Tokyo Plasma etching method @Fuchigami Micro Co Ltd @Fuchigami Micro Co., Ltd. Holes with cylindrical shape 7 th International Conference on Position Sensitive Detectors CNS University of Tokyo

  6. gas gain spectrum Total Gain Total Gain 10 5 GEM Gain requirement requirement 10 4 10 4 s gain Ar 90% C 2 H 6 10% 55 Fe unt with gas flowing with gas flowing gas escape peak(Ar) cou 4 4 6 6 E Energy[keV] [k V] GEM Voltage[V] 20%(FWHM) @ 5.9keV gain 1.3 × 10 4 (1.6cm 2 ) 10 4 (1 6 i 1 3 2 ) μ -PIC gain fixed 2.6 × 10 3 Total Max Gain ~ 10 5 GEM Max Gain ~ 300 7 th International Conference on Position Sensitive Detectors enough to detect tracks of MIPs !

  7. Positive ion feedback Fractional ion current I D /I A I : the ion current I D : the ion current ck Feedbac on the drift plane I A : the electron current A ional Ion on anodes of µ-PIC the dependence of the fractional ion the dependence of the fractional ion Fracti current on the gain of the GEM Ion feedback less than 10% @ gas gain > 10 GEM gas gain without GEM 30% without GEM 30% total 10% µ-PIC 30% × GEM 30% GEM suppresses the positive ion feedback in a drift region Potential of µ-PIC + GEM system for high-rate condition operation 7 th International Conference on Position Sensitive Detectors

  8. A GEM + µ-PIC TPC -muon track- µ µ-PIC plastic scintillator Ar 90% Ar 90% e - coincidence for C 2 H 6 10% muon trigger e - 0cm drift plane drift plane @ @ total gas gain of 2 × 10 4 l i f 4 10 e - Landau Typical event GEM Distribution 0.2cm Cosmic µ Cosmic µ 8cm 2.5kV/cm 0.4kV/cm track efficiency (hit point > 3) / (trigger) 97% ( p ) ( gg ) dE/dx 7 th International Conference on Position Sensitive Detectors

  9. Position resolution Difference between hit points and tracks obtained from fitting and tracks obtained from fitting 2-dimensional Gauss distribution (the position resolution in the direction of a track is unknown) 0.05 0.05 residual[cm] residual[cm] σ ~ 370µm transverse diffusion 460µm Z-pitch (DAQ clock) ~ 400µm reasonable reasonable 7 th International Conference on Position Sensitive Detectors

  10. Summary & Future Works µ-PIC + GEM PIC GEM stable gas gain of 2 × 10 4 , ion feedback < 10% µ-PIC + GEM TPC 30cm μ -PIC Fine tracks of MIPs were obtained. Fine tracks of MIPs were obtained. track efficiency 97% 30cm position resolution 370µm position resolution 370µm Future Works µ-PIC & GEM with a larger detection area 30cmGEM about 30cm × 30cm(takada’s poster) φ 70 μ m pitch 140 μ m 28cm standard standard design 7 th International Conference on Position Sensitive Detectors 23cm

  11. Performance of μ –PIC (Mi (Micro Pixel Chamber) Pi l Ch b ) 2-dimensional imaging gaseous detector anode 256 × cathode 256 ~ 65000pixels 400 μ m Max gas gain ~ 15000 g g 10cm St bl Stable operation for 1000h ti f 1000h (gas gain ~ 6000) Energy Resolution Energy Resolution 30%(FWHM)@5.9keV(100cm 2 ) ) position resolution p ~ 120 μ m 7 th International Conference on Position Sensitive Detectors

  12. Performance of μ –PIC μ - uniformity - σ ~ 7% 7 th International Conference on Position Sensitive Detectors

  13. μ -TPC ( Time Projection Chamber based on μ -PIC) ( Time Projection Chamber based on μ PIC) 10cm × 10cm μ -PIC Electric field Electron cloud 2-D hit position pos o (Analog & digital) 100MHz encoder time drift distance 3-D tracking electron Electric field field proton t 8cm Applications Compton camera (recoil electron) (recoil electron) Dark Matter search 7 th International Conference on Position Sensitive Detectors

  14. • DAQ system DAQ system Encoder μ -TPC TPC ASD 512ch digital 512ch 32bit summed analog VME (8ch) Memory Board Memory Board VME FADC 100MH 8 h 100MHz 8ch 7 th International Conference on Position Sensitive Detectors

  15. GEM GEM Mask by Hamagaki Lab. @ CNS Univ. of Tokyo Plasma etching method @Fuchigami Micro Co., Ltd. Holes with cylindrical shape CERN : holes with a double-conical shape p CNS-GEM 7 th International Conference on Position Sensitive Detectors

  16. Setup How to glue a GEM -HV drift plane drift plane -HV 5M Ω weight 10M Ω 10M Ω 7.5mm 0.5kV/cm 7 5 0 5kV/ GEM GEM G10 frame 5mm 2kV/cm GEM GEM 10M Ω 10M Ω μ -PIC Glued with -HV epoxy(Araldite) p y( ) aging I d In dry nitrogen gas it Δ V GEM ~ 500V 7 th International Conference on Position Sensitive Detectors

  17. Dependence of total gain on p g induction field Δ V GEM = 250V(gain 10) E D = 0.5kV/cm as gain plateau wasn’t observed p ateau was t obse ved ctive ga the system unstable @ gas gain of ~ 10 5 @ gas gain of ~ 10 Effec Induction Field[kV/cm] 7 th International Conference on Position Sensitive Detectors

  18. Long-term gas gain stability g g g y µ-PIC 6% for 70h 120h gas gain g 70 70 0 0 Time[h] Ti [h] Th The gain increased 50% i i d 50% for 120h 7 th International Conference on Position Sensitive Detectors Hamagaki, CNS Univ. of Tokyo

  19. Performance of micro-TPC - uniformity - 0 1 0.1 0 7 th International Conference on Position Sensitive Detectors

  20. Performance of Hybrid micro-TPC - gamma – ray - gamma ray micro -TPC energy micro TPC energy μ TPC μ TPC mumber of sampling TPC TPC mumber of sampling b b f f li li 13%`20keV(FWHM) Points for one electron track Points for one electron track X-ray from Cu ray from Cu electrode in μ PIC electrode in PIC 7 th International Conference on Position Sensitive Detectors

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend