| 1 | |
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| 2 | ************************************************************* |
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| 3 | Geant4 version Name: global-V09-00-03 (9-May-2008) |
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| 4 | Copyright : Geant4 Collaboration |
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| 5 | Reference : NIM A 506 (2003), 250-303 |
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| 6 | WWW : http://cern.ch/geant4 |
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| 7 | ************************************************************* |
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| 8 | |
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| 9 | B01PhysicsList::SetCuts:CutLength : 1 (mm) |
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| 10 | Going to assign importance: 1, to volume: cell_01 |
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| 11 | Going to assign importance: 2, to volume: cell_02 |
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| 12 | Going to assign importance: 4, to volume: cell_03 |
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| 13 | Going to assign importance: 8, to volume: cell_04 |
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| 14 | Going to assign importance: 16, to volume: cell_05 |
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| 15 | Going to assign importance: 32, to volume: cell_06 |
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| 16 | Going to assign importance: 64, to volume: cell_07 |
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| 17 | Going to assign importance: 128, to volume: cell_08 |
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| 18 | Going to assign importance: 256, to volume: cell_09 |
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| 19 | Going to assign importance: 512, to volume: cell_10 |
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| 20 | Going to assign importance: 1024, to volume: cell_11 |
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| 21 | Going to assign importance: 2048, to volume: cell_12 |
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| 22 | Going to assign importance: 4096, to volume: cell_13 |
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| 23 | Going to assign importance: 8192, to volume: cell_14 |
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| 24 | Going to assign importance: 16384, to volume: cell_15 |
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| 25 | Going to assign importance: 32768, to volume: cell_16 |
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| 26 | Going to assign importance: 65536, to volume: cell_17 |
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| 27 | Going to assign importance: 131072, to volume: cell_18 |
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| 28 | preparing importance sampling |
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| 29 | creating istore |
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| 30 | creating importance configurator |
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| 31 | entering configure |
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| 32 | importance configurator push_back |
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| 33 | pushed |
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| 34 | vsampler configurator loop |
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| 35 | looping 1 |
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| 36 | sampler configurator |
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| 37 | entering importance configure, paraflag 0 |
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| 38 | creating importance process, paraflag is: 0 |
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| 39 | importance process paraflag is: 0 |
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| 40 | === G4ProcessPlacer::AddProcessAsSecondDoIt: for: neutron |
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| 41 | Modifying Process Order for ProcessName: ImportanceProcess |
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| 42 | The initial AlongStep Vectors: |
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| 43 | GPIL Vector: |
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| 44 | Transportation |
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| 45 | DoIt Vector: |
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| 46 | Transportation |
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| 47 | The initial PostStep Vectors: |
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| 48 | GPIL Vector: |
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| 49 | Decay |
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| 50 | HadronCapture |
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| 51 | HadronFission |
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| 52 | inelastic |
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| 53 | HadronElastic |
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| 54 | Transportation |
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| 55 | DoIt Vector: |
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| 56 | Transportation |
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| 57 | HadronElastic |
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| 58 | inelastic |
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| 59 | HadronFission |
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| 60 | HadronCapture |
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| 61 | Decay |
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| 62 | The final AlongStep Vectors: |
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| 63 | GPIL Vector: |
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| 64 | ImportanceProcess |
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| 65 | Transportation |
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| 66 | DoIt Vector: |
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| 67 | Transportation |
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| 68 | ImportanceProcess |
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| 69 | The final PostStep Vectors: |
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| 70 | GPIL Vector: |
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| 71 | Decay |
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| 72 | HadronCapture |
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| 73 | HadronFission |
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| 74 | inelastic |
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| 75 | HadronElastic |
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| 76 | ImportanceProcess |
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| 77 | Transportation |
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| 78 | DoIt Vector: |
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| 79 | Transportation |
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| 80 | ImportanceProcess |
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| 81 | HadronElastic |
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| 82 | inelastic |
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| 83 | HadronFission |
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| 84 | HadronCapture |
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| 85 | Decay |
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| 86 | ================================================ |
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| 87 | configure preconf |
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| 88 | |
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| 89 | conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z; |
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| 90 | sampling secondary e+e- according Bethe-Heitler model |
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| 91 | tables are built for gamma |
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| 92 | Lambda tables from 1.022 MeV to 100 GeV in 100 bins. |
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| 93 | |
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| 94 | compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV |
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| 95 | Sampling according Klein-Nishina model |
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| 96 | tables are built for gamma |
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| 97 | Lambda tables from 100 eV to 100 GeV in 90 bins. |
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| 98 | |
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| 99 | phot: Total cross sections from Sandia parametrisation. |
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| 100 | Sampling according PhotoElectric model |
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| 101 | |
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| 102 | msc: Model variant of multiple scattering for e- |
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| 103 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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| 104 | LateralDisplacementFlag= 1 Skin= 0 |
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| 105 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1 |
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| 106 | |
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| 107 | eIoni: tables are built for e- |
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| 108 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 109 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 110 | Delta cross sections and sampling from MollerBhabha model |
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| 111 | Good description from 1 KeV to 100 GeV. |
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| 112 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 113 | |
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| 114 | eBrem: tables are built for e- |
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| 115 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 116 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 117 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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| 118 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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| 119 | |
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| 120 | eIoni: tables are built for e+ |
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| 121 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 122 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 123 | Delta cross sections and sampling from MollerBhabha model |
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| 124 | Good description from 1 KeV to 100 GeV. |
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| 125 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 126 | |
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| 127 | eBrem: tables are built for e+ |
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| 128 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 129 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 130 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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| 131 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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| 132 | |
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| 133 | annihil: Sampling according eplus2gg model |
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| 134 | tables are built for e+ |
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| 135 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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| 136 | |
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| 137 | msc: Model variant of multiple scattering for proton |
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| 138 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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| 139 | LateralDisplacementFlag= 1 Skin= 0 |
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| 140 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1 |
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| 141 | |
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| 142 | hIoni: tables are built for proton |
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| 143 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 144 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 145 | Scaling relation is used from proton dE/dx and range. |
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| 146 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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| 147 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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| 148 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 149 | |
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| 150 | msc: Model variant of multiple scattering for GenericIon |
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| 151 | LateralDisplacementFlag= 0 Skin= 0 |
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| 152 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 1 |
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| 153 | |
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| 154 | hIoni: tables are built for anti_proton |
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| 155 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 156 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 157 | Scaling relation is used from proton dE/dx and range. |
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| 158 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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| 159 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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| 160 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 161 | |
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| 162 | msc: Model variant of multiple scattering for mu+ |
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| 163 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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| 164 | LateralDisplacementFlag= 1 Skin= 0 |
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| 165 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1 |
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| 166 | |
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| 167 | muIoni: tables are built for mu+ |
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| 168 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 169 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 170 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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| 171 | radiative corrections for E > 1 GeV |
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| 172 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 173 | |
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| 174 | muBrems: tables are built for mu+ |
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| 175 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 176 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 177 | Parametrised model |
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| 178 | |
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| 179 | muPairProd: tables are built for mu+ |
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| 180 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 181 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 182 | Parametrised model |
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| 183 | |
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| 184 | muIoni: tables are built for mu- |
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| 185 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 186 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 187 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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| 188 | radiative corrections for E > 1 GeV |
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| 189 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 190 | |
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| 191 | muBrems: tables are built for mu- |
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| 192 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 193 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 194 | Parametrised model |
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| 195 | |
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| 196 | muPairProd: tables are built for mu- |
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| 197 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 198 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 199 | Parametrised model |
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| 200 | |
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| 201 | hIoni: tables are built for pi+ |
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| 202 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 203 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 204 | Scaling relation is used from proton dE/dx and range. |
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| 205 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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| 206 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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| 207 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 208 | |
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| 209 | msc: Model variant of multiple scattering for pi- |
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| 210 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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| 211 | LateralDisplacementFlag= 1 Skin= 0 |
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| 212 | Boundary/stepping algorithm is active with RangeFactor= 0.02 Step limit type 1 |
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| 213 | |
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| 214 | hIoni: tables are built for pi- |
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| 215 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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| 216 | Lambda tables from threshold to 100 TeV in 120 bins. |
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| 217 | Scaling relation is used from proton dE/dx and range. |
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| 218 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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| 219 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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| 220 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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| 221 | ++ ConcreteSD/Collisions id 0 |
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| 222 | ++ ConcreteSD/CollWeight id 1 |
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| 223 | ++ ConcreteSD/Population id 2 |
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| 224 | ++ ConcreteSD/TrackEnter id 3 |
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| 225 | ++ ConcreteSD/SL id 4 |
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| 226 | ++ ConcreteSD/SLW id 5 |
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| 227 | ++ ConcreteSD/SLWE id 6 |
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| 228 | ++ ConcreteSD/SLW_V id 7 |
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| 229 | ++ ConcreteSD/SLWE_V id 8 |
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| 230 | ### Run 0 start. |
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| 231 | ###### EndOfRunAction |
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| 232 | ============================================================= |
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| 233 | Number of event processed : 100 |
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| 234 | ============================================================= |
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| 235 | Volume | Tr.Entering | Population | Collisions | Coll*WGT | NumWGTedE | FluxWGTedE | Av.Tr.WGT | SL | SLW | SLW_v | SLWE | SLWE_v | |
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| 236 | cell_00 | 15 | 115 | 0 | 0 | 6.3966059 | 7.4018992 | 1 | 2718.4878 | 2718.4878 | 82.42747 | 20121.972 | 527.25604 | |
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| 237 | cell_01 | 110 | 134 | 145 | 145 | 7.2822789 | 8.8443266 | 1 | 11666.037 | 11666.037 | 340.22197 | 103178.24 | 2477.5913 | |
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| 238 | cell_02 | 70 | 164 | 176 | 88 | 7.0660843 | 8.6092149 | 0.5 | 15544.352 | 7772.1759 | 230.58237 | 66912.332 | 1629.3145 | |
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| 239 | cell_03 | 97 | 220 | 279 | 69.75 | 6.5176502 | 7.9386173 | 0.25 | 23499.237 | 5874.8093 | 179.88741 | 46637.863 | 1172.4432 | |
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| 240 | cell_04 | 107 | 253 | 363 | 45.375 | 5.4125517 | 7.0721743 | 0.125 | 28079.769 | 3509.9711 | 120.28028 | 24823.127 | 651.02321 | |
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| 241 | cell_05 | 124 | 275 | 393 | 24.5625 | 5.0245006 | 6.8916189 | 0.0625 | 30553.015 | 1909.5634 | 69.40684 | 13159.983 | 348.7347 | |
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| 242 | cell_06 | 139 | 310 | 440 | 13.75 | 5.2835284 | 7.0172979 | 0.03125 | 34126.865 | 1066.4645 | 37.356314 | 7483.6993 | 197.37314 | |
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| 243 | cell_07 | 157 | 370 | 493 | 7.703125 | 5.5558117 | 6.9976454 | 0.015625 | 40462.287 | 632.22324 | 21.14872 | 4424.0741 | 117.4983 | |
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| 244 | cell_08 | 191 | 423 | 583 | 4.5546875 | 0.32471447 | 6.83361 | 0.0078125 | 44570.287 | 348.20536 | 196.83204 | 2379.4996 | 63.914211 | |
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| 245 | cell_09 | 209 | 508 | 780 | 3.046875 | 5.0725839 | 6.5643746 | 0.00390625 | 56497.818 | 220.6946 | 7.8116315 | 1448.722 | 39.625157 | |
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| 246 | cell_10 | 209 | 490 | 750 | 1.4648438 | 4.2152478 | 6.4791598 | 0.001953125 | 54129.392 | 105.72147 | 4.4552242 | 684.98629 | 18.779874 | |
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| 247 | cell_11 | 237 | 520 | 750 | 0.73242188 | 0.11190762 | 6.2612863 | 0.0009765625 | 55200.57 | 53.906807 | 83.848515 | 337.52595 | 9.3832878 | |
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| 248 | cell_12 | 279 | 627 | 978 | 0.47753906 | 0.36186788 | 5.9200159 | 0.00048828125 | 65901.469 | 32.178451 | 14.991671 | 190.49694 | 5.4250043 | |
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| 249 | cell_13 | 323 | 701 | 1173 | 0.28637695 | 0.36848322 | 5.7881594 | 0.00024414062 | 79304.733 | 19.361507 | 8.7598914 | 112.06749 | 3.227873 | |
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| 250 | cell_14 | 376 | 846 | 1398 | 0.1706543 | 0.17152547 | 5.5058521 | 0.00012207031 | 96136.852 | 11.735456 | 11.136915 | 64.613683 | 1.9102646 | |
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| 251 | cell_15 | 411 | 923 | 1583 | 0.096618652 | 3.7639995 | 5.2299054 | 6.1035156e-05 | 107618.6 | 6.5685181 | 0.27495831 | 34.352728 | 1.0349429 | |
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| 252 | cell_16 | 456 | 1005 | 1797 | 0.054840088 | 3.7486376 | 5.2165757 | 3.0517578e-05 | 117973.81 | 3.6002748 | 0.15117532 | 18.781106 | 0.56670149 | |
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| 253 | cell_17 | 509 | 1163 | 2231 | 0.034042358 | 0.20193182 | 4.8897997 | 1.5258789e-05 | 133150.38 | 2.0317135 | 1.5335292 | 9.9346721 | 0.30966836 | |
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| 254 | cell_18 | 495 | 1197 | 2241 | 0.017097473 | 0.20257811 | 4.6206295 | 7.6293945e-06 | 139424.93 | 1.0637278 | 0.7729574 | 4.9150921 | 0.15658425 | |
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| 255 | cell_19 | 544 | 544 | 0 | 0 | 2.9819583 | 4.7405471 | 7.6293945e-06 | 81292.743 | 0.62021441 | 0.03100179 | 2.9401557 | 0.092446045 | |
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| 256 | ============================================= |
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| 257 | === G4ProcessPlacer::RemoveProcess: for: neutron |
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| 258 | ProcessName: ImportanceProcess, will be removed! |
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| 259 | The initial AlongStep Vectors: |
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| 260 | GPIL Vector: |
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| 261 | ImportanceProcess |
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| 262 | Transportation |
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| 263 | DoIt Vector: |
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| 264 | Transportation |
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| 265 | ImportanceProcess |
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| 266 | The initial PostStep Vectors: |
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| 267 | GPIL Vector: |
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| 268 | Decay |
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| 269 | HadronCapture |
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| 270 | HadronFission |
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| 271 | inelastic |
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| 272 | HadronElastic |
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| 273 | ImportanceProcess |
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| 274 | Transportation |
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| 275 | DoIt Vector: |
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| 276 | Transportation |
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| 277 | ImportanceProcess |
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| 278 | HadronElastic |
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| 279 | inelastic |
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| 280 | HadronFission |
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| 281 | HadronCapture |
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| 282 | Decay |
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| 283 | The final AlongStep Vectors: |
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| 284 | GPIL Vector: |
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| 285 | Transportation |
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| 286 | DoIt Vector: |
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| 287 | Transportation |
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| 288 | The final PostStep Vectors: |
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| 289 | GPIL Vector: |
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| 290 | Decay |
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| 291 | HadronCapture |
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| 292 | HadronFission |
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| 293 | inelastic |
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| 294 | HadronElastic |
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| 295 | Transportation |
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| 296 | DoIt Vector: |
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| 297 | Transportation |
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| 298 | HadronElastic |
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| 299 | inelastic |
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| 300 | HadronFission |
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| 301 | HadronCapture |
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| 302 | Decay |
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| 303 | ================================================ |
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