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Published bySharon McCarthy Modified over 9 years ago
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A. Chukanov, S. Dmitrievsky, Yu. Gornushkin, D. Naumov JINR, Dubna Opera collaboration meeting 9 th March 2011, Nagoya
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Signal attenuation in strips Cross-talks simulation Geant 4 running Summary
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Signals from an isolated muon Signals from the left and right PMT’s are not well discribed by MC
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Model of light attenuation in a fiber PMT left PMT right E left E right 0 x E0E0 L 0 = 686 cm dL
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OpDigit: parametrization from muon tracks.16 different parameters for light attenuations for all detector Parametrization according to attenuation distributions for all detector (calibration)
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Signals from an isolated muon OpDigit New para- metrization
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Δ=9 Δ=-1 Δ=7 Δ=8 Δ=1 Δ=-7 Δ=-8 Δ=-9 1 8 56 64 PMT Measured CT fraction is equal 7.4%.
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CT Energy/Energy in plane, Threshold = 0.3 p.e. Measured from muon tracks CT fraction: 5.3%
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v 4.0 new
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VMC allow us to use different tracing programs: Geant 3 Geant 4 Fluka (for internal use only) Only Geant 3 is using now
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“OPERA” particle replaces and charm Charmed hadrons and -leptons are decayed in PYTHIA New names were introduced Valid for the -leptons Not valid for the charmed hadrons Geant 4 crashs because of introduction of “OPERA” particles Charmed hadrons
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OpSim scripts modification (manual is coming soon) Short live particles do not decay at event genertion level PYTHIA as external decay program at particle transportation level Longer computation time, need to choose proper physics list
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GEANT 3 GEANT 4
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TT fibers attenuation from testing beam gives a better Data by MC description Recalculated cross-talks fraction from 7.4% to 5.3% Migration to Geant 4 as transportation program
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