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Published byNigel Wilson Modified over 9 years ago
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Development of timing RPCs Presented by P.Fonte for the TOF-RPC group
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CBM meeting 8.3.2005 - TOF-RPC Outline Current activities of the TOF-RPC group Test facility at ELBE/Rosendorf Physics simulation studies RPC properties Analytic model of the RPC rate properties (NEW - post TSR) Aging tests Improvement of the rate capability by using semiconducting glasses by using commercially available ceramic materials (NEW) through temperature increase RPC layout options Single cell chambers Shielded timing RPCs Multistrip counters Readout electronics Preamplifier/discriminator FOPI-RPC electronics Time measurement and digital backend
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CBM meeting 8.3.2005 - TOF-RPC Test facility at ELBE/Rosendorf The Rossendorf electron accelerator ELBE provides electrons up to 40 MeV in beam packets with a time spread better than 10 ps. Ready for users!
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CBM meeting 8.3.2005 - TOF-RPC Physics simulation ,K,p momentum distributions Occupancy on TOF plane
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CBM meeting 8.3.2005 - TOF-RPC RPC properties Analytic model of the RPC rate properties (NEW) Aging
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CBM meeting 8.3.2005 - TOF-RPC Primary statistics Gas response [A. Mangiarotti, P.Fonte, A.Gobbi NIM A 533(2004)16] σ τ (n 0 ’) [1/s units] n0’n0’ Ineff (%) Analytical model of the rate effect (NEW)
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CBM meeting 8.3.2005 - TOF-RPC Intrinsic time resolutionFluctuations in the fieldDrop in the field [Mangiarotti et al. NIM A 535 (2004) 272 ] (var E ) 1/2 /E σ τ (n 0 ’) [1/s units] Analytical model of the rate effect (NEW) For any source of E variation
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CBM meeting 8.3.2005 - TOF-RPC HV = 3.1 kV/gap HV = 3.2 kV/gap HV = 3.3 kV/gap HV = 3.4 kV/gap NOT FITTED! FITTED Data [re-scaled ‘prompt charge’] Analytical model of the rate effect (NEW)
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CBM meeting 8.3.2005 - TOF-RPC Aging (2002-2003) - humid, cold After accumulating 800mC/cm 2 (equiv. 8.5 years of normal operation) we don't observe any systematic long-term increase of dark current with time. made some changes on the experimental setup. 6 counters Room temperature “Standard” timing RPCs gas 85%C 2 H 2 F 4 +10%SF 6 + 5% iso-C 4 H 10, with 10% relative humidity Primary charges were created by an UV lamp No problem up to ~8 years equiv. charge (800 mC/cm 2 )
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CBM meeting 8.3.2005 - TOF-RPC Aging (2004-05) – humid, hot After more than 80 days we don’t observe any increase of the dark current. Which seems to stabilize. In chambers that operate at more than 2 kHz cm -2. And accumulated 200 mC cm -2 No problem so far (90 days = 200 mC/cm 2 ) Tenfold higher current
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CBM meeting 8.3.2005 - TOF-RPC Improvement of the rate capability (0.4 to 20 kHz/cm 2 foreseen, current designs: 1 kHz/cm2) by using semiconducting glasses by using commercially available ceramic materials (NEW!) through temperature increase
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CBM meeting 8.3.2005 - TOF-RPC Rate / semiconducting glass Silicate glassPhosphate glass
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CBM meeting 8.3.2005 - TOF-RPC Rate / semiconducting glass
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CBM meeting 8.3.2005 - TOF-RPC Rate / ceramics (NEW) Commercial “controlled resistivity” alumina, Al940CD, from Wesgo® Ceramics Volume resistivity between 1×10 9 and 2 × 10 9 cm at room temperature. Seems to be electronic conductor (no charge-up effects). Good (hard, dense) surface. Not straightforward (~1 year R&D) Benchtop test setup 22 Na Reference Chamber (identical) Test Chamber 10 cm 2 (CBM granularity) X-ray Generator Photon conversion on RPC yields an exponential pulse-charge distribution Less favourable than the reasonable peak found in a charged beam.
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CBM meeting 8.3.2005 - TOF-RPC Rate / ceramics (NEW) Efficiency is kept up to 100 kHz/cm 2. Very encouraging…
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CBM meeting 8.3.2005 - TOF-RPC Rate / ceramics (NEW) Sigma ~ 100ps seems to be kept up to 50 kHz/cm 2 Random Coincid. Signal But background of random coincidences fit with gaussian + symmetric exponential How does it affect the measurement of the real sigma? visit Rosendorf… CBM goal well in reach
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CBM meeting 8.3.2005 - TOF-RPC Rate / Temperature Presented last meeting by D.Gonzalez
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CBM meeting 8.3.2005 - TOF-RPC Rate / Temperature Beam test in November When run warm (~50ºC) may comfortably reach a few 1000 Hz/cm2 Geometric acceptance ≈ 87 % Extrapolated from beam- tests on the previous HADES prototype, assuming a 25ºC temperature increase 0 75ºC=CBM goal…
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CBM meeting 8.3.2005 - TOF-RPC Rate / Temperature Test bench with 25 elements Heating and sensing element 20 W heater Hardware temperature limiter 1-WIRE® interface + power Thermometer Distributed temperature control system (in development) Reasonable cabling. Present accuracy ~1 ºC.
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CBM meeting 8.3.2005 - TOF-RPC RPC layout options Single cell chambers Shielded timing RPCs Multistrip counter
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CBM meeting 8.3.2005 - TOF-RPC Single cell chambers Coincides with the semiconducting glass effort
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CBM meeting 8.3.2005 - TOF-RPC Shielded timing RPCs Actual parts, industrially produced. Uniformity tests with 22 Na (positron ) source Crosstalk for avalanches is below the noise level Beam test in November Final prototype of the HADES RPC-TOF wall Designed to run warm (up to 60ºC)
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CBM meeting 8.3.2005 - TOF-RPC Multistrip counters (FOPI) Present design: 8 gaps Very pure gaussian distribution
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CBM meeting 8.3.2005 - TOF-RPC Multistrip counters Single hitDouble hit 1kHz/cm 2 100Hz/cm 2
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CBM meeting 8.3.2005 - TOF-RPC RPC electronics Preamplifier/discriminator FOPI-RPC electronics Time measurement and digital backend
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CBM meeting 8.3.2005 - TOF-RPC Preamplifier / discriminator Performance of the existing front-end based on a multichip design Likely, for CBM an integrated design will be needed
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CBM meeting 8.3.2005 - TOF-RPC FOPI-RPC electronics TAQUILA system resolution of 33 ps demonstrated Possible concept for CBM
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CBM meeting 8.3.2005 - TOF-RPC Conclusion Many developments and studies are under way in key aspects like Aging Physics simulation Rate capability System layout Test facilities Theoretical understanding Some significant progress has been made. Further results from beam tests expected later this year.
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