Gabriele Cosmo
330 lines
13 KiB
Plaintext
330 lines
13 KiB
Plaintext
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*************************************************************
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Geant4 version Name: geant4-08-03-cand-00 (5-May-2007)
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Copyright : Geant4 Collaboration
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Reference : NIM A 506 (2003), 250-303
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WWW : http://cern.ch/geant4
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*************************************************************
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B01PhysicsList::SetCuts:CutLength : 1 (mm)
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Going to assign importance: 1, to volume: cell_01
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Going to assign importance: 2, to volume: cell_02
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Going to assign importance: 4, to volume: cell_03
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Going to assign importance: 8, to volume: cell_04
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Going to assign importance: 16, to volume: cell_05
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Going to assign importance: 32, to volume: cell_06
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Going to assign importance: 64, to volume: cell_07
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Going to assign importance: 128, to volume: cell_08
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Going to assign importance: 256, to volume: cell_09
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Going to assign importance: 512, to volume: cell_10
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Going to assign importance: 1024, to volume: cell_11
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Going to assign importance: 2048, to volume: cell_12
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Going to assign importance: 4096, to volume: cell_13
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Going to assign importance: 8192, to volume: cell_14
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Going to assign importance: 16384, to volume: cell_15
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Going to assign importance: 32768, to volume: cell_16
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Going to assign importance: 65536, to volume: cell_17
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Going to assign importance: 131072, to volume: cell_18
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=== G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
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ProcessName: MScoreProcess
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The initial Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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Transportation
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DoIt Vector:
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Transportation
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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The final Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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Transportation
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DoIt Vector:
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Transportation
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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================================================
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=== G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron
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ProcessName: MassImportanceProcess
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The initial Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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Transportation
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DoIt Vector:
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Transportation
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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The final Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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MassImportanceProcess
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Transportation
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DoIt Vector:
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Transportation
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MassImportanceProcess
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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================================================
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conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z;
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sampling secondary e+e- according Bethe-Heitler model
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tables are built for gamma
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Lambda tables from 1.022 MeV to 100 GeV in 100 bins.
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compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV
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Sampling according Klein-Nishina model
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tables are built for gamma
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Lambda tables from 100 eV to 100 GeV in 90 bins.
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phot: Total cross sections from Sandia parametrisation.
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Sampling according PhotoElectric model
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msc: Model variant of multiple scattering for e-
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Lambda tables from 100 eV to 100 TeV in 120 bins.
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LateralDisplacementFlag= 1 Skin= 0
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Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
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eIoni: tables are built for e-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Delta cross sections and sampling from MollerBhabha model
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Good description from 1 KeV to 100 GeV.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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eBrem: tables are built for e-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Total cross sections and sampling from StandBrem model (based on the EEDL data library)
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Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
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eIoni: tables are built for e+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Delta cross sections and sampling from MollerBhabha model
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Good description from 1 KeV to 100 GeV.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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eBrem: tables are built for e+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Total cross sections and sampling from StandBrem model (based on the EEDL data library)
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Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV.
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annihil: Sampling according eplus2gg model
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tables are built for e+
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Lambda tables from 100 eV to 100 TeV in 120 bins.
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msc: Model variant of multiple scattering for proton
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Lambda tables from 100 eV to 100 TeV in 120 bins.
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LateralDisplacementFlag= 1 Skin= 0
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Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
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hIoni: tables are built for proton
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Scaling relation is used from proton dE/dx and range.
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Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
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Parametrisation from Bragg for protons below.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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msc: Model variant of multiple scattering for GenericIon
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LateralDisplacementFlag= 0 Skin= 0
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Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
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hIoni: tables are built for anti_proton
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Scaling relation is used from proton dE/dx and range.
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Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV
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Parametrisation from Bragg for protons below.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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msc: Model variant of multiple scattering for mu+
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Lambda tables from 100 eV to 100 TeV in 120 bins.
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LateralDisplacementFlag= 1 Skin= 0
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Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
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muIoni: tables are built for mu+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
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radiative corrections for E > 1 GeV
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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muBrems: tables are built for mu+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Parametrised model
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muPairProd: tables are built for mu+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Parametrised model
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muIoni: tables are built for mu-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below,
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radiative corrections for E > 1 GeV
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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muBrems: tables are built for mu-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Parametrised model
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muPairProd: tables are built for mu-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Parametrised model
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hIoni: tables are built for pi+
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Scaling relation is used from proton dE/dx and range.
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Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
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Parametrisation from Bragg for protons below.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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msc: Model variant of multiple scattering for pi-
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Lambda tables from 100 eV to 100 TeV in 120 bins.
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LateralDisplacementFlag= 1 Skin= 0
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Boundary/stepping algorithm is active with facrange= 0.02 Step limitation 1
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hIoni: tables are built for pi-
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dE/dx and range tables from 100 eV to 100 TeV in 120 bins.
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Lambda tables from threshold to 100 TeV in 120 bins.
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Scaling relation is used from proton dE/dx and range.
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Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV
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Parametrisation from Bragg for protons below.
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Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1
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Volume name | Importance| Tr.Entering| Population| Collisions| Coll*WGT| NumWGTedE| FluxWGTedE| Av.Tr.WGT|
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cell_01_rep:0............ | 1 | 118 | 150 | 149 | 149 | 7.2096509 | 8.5785508 | 1 |
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cell_02_rep:0............ | 2 | 87 | 192 | 189 | 94.5 | 8.2328232 | 8.660209 | 1 |
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cell_03_rep:0............ | 4 | 99 | 212 | 240 | 60 | 6.6805827 | 7.9415373 | 1 |
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cell_04_rep:0............ | 8 | 119 | 258 | 287 | 35.875 | 6.957465 | 7.8605556 | 1 |
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cell_05_rep:0............ | 16 | 150 | 321 | 396 | 24.75 | 5.1009587 | 7.099783 | 1 |
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cell_06_rep:0............ | 32 | 162 | 353 | 426 | 13.3125 | 4.6037023 | 7.0570615 | 1 |
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cell_07_rep:0............ | 64 | 205 | 416 | 568 | 8.875 | 4.8261852 | 6.6681408 | 1 |
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cell_08_rep:0............ | 128 | 223 | 486 | 656 | 5.125 | 0.53648464 | 6.6539856 | 1 |
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cell_09_rep:0............ | 256 | 251 | 519 | 751 | 2.9335938 | 4.943392 | 6.39047 | 1 |
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cell_10_rep:0............ | 512 | 288 | 597 | 875 | 1.7089844 | 4.3487469 | 6.110481 | 1 |
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cell_11_rep:0............ | 1024 | 337 | 698 | 1058 | 1.0332031 | 4.4329506 | 6.0885935 | 1 |
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cell_12_rep:0............ | 2048 | 393 | 782 | 1238 | 0.60449219 | 4.4763037 | 6.0639968 | 1 |
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cell_13_rep:0............ | 4096 | 451 | 930 | 1440 | 0.3515625 | 4.2499709 | 5.7580044 | 1 |
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cell_14_rep:0............ | 8192 | 472 | 985 | 1522 | 0.18579102 | 0.072154763 | 5.4255988 | 1 |
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cell_15_rep:0............ | 16384 | 503 | 1014 | 1715 | 0.10467529 | 0.87569507 | 5.1929267 | 1 |
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cell_16_rep:0............ | 32768 | 576 | 1204 | 2080 | 0.063476562 | 0.13469363 | 4.97975 | 1 |
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cell_17_rep:0............ | 65536 | 635 | 1281 | 2314 | 0.035308838 | 3.3098112 | 4.7409862 | 1 |
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cell_18_rep:0............ | 131072 | 565 | 1356 | 2505 | 0.019111633 | 3.1110957 | 4.603961 | 1 |
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rest_rep:0............... | 131072 | 601 | 601 | 0 | 0 | 0 | 0 | 0 |
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shieldWorld_rep:0........ | 1 | 14 | 114 | 0 | 0 | 10 | 10 | 1 |
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=== G4ProcessPlacer::RemoveProcess: for: neutron
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ProcessName: MassImportanceProcess, will be removed!
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The initial Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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MassImportanceProcess
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Transportation
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DoIt Vector:
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Transportation
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MassImportanceProcess
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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The final Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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Transportation
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DoIt Vector:
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Transportation
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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================================================
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=== G4ProcessPlacer::RemoveProcess: for: neutron
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ProcessName: MScoreProcess, will be removed!
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The initial Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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MScoreProcess
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Transportation
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DoIt Vector:
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Transportation
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MScoreProcess
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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The final Vectors:
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GPIL Vector:
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Decay
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HadronCapture
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HadronFission
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inelastic
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HadronElastic
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Transportation
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DoIt Vector:
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Transportation
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HadronElastic
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inelastic
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HadronFission
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HadronCapture
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Decay
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================================================
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