| [807] | 1 | **********************************************
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| 2 | Geant4 version $Name: $
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| 3 | (31-Jul-2002)
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| 4 | Copyright : Geant4 Collaboration
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| 5 | **********************************************
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| 6 |
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| 7 | phot: Total cross sections from Sandia parametrisation.
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| 8 | B02PhysicsList::SetCuts:CutLength : 1 (mm)
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| 9 |
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| 10 | conv: Total cross sections from a parametrisation. Good description from 1.5 MeV to 100 GeV for all Z.
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| 11 | e+e- energies according Bethe-Heitler
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| 12 | PhysicsTables from 1.022 MeV to 100 GeV in 100 bins.
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| 13 |
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| 14 | compt: Total cross sections from a parametrisation. Good description from 10 KeV to (100/Z) GeV.
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| 15 | Scattered gamma energy according Klein-Nishina.
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| 16 | PhysicsTables from 1 keV to 100 GeV in 80 bins.
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| 17 |
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| 18 | msc: Tables of transport mean free paths.
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| 19 | New model of MSC , computes the lateral
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| 20 | displacement of the particle , too.
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| 21 | PhysicsTables from 100 eV to 100 TeV in 100 bins.
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| 22 |
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| 23 | eIoni: delta cross sections from Moller+Bhabha. Good description from 1 KeV to 100 GeV.
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| 24 | delta ray energy sampled from differential Xsection.
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| 25 | PhysicsTables from 1 keV to 100 TeV in 100 bins.
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| 26 |
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| 27 | eBrem: Total cross sections from a NEW parametrisation based on the EEDL data library.
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| 28 | Good description from 1 KeV to 100 GeV.
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| 29 | log scale extrapolation above 100 GeV
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| 30 | Gamma energy sampled from a parametrised formula.
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| 31 | PhysicsTables from 1 keV to 100 TeV in 100 bins.
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| 32 |
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| 33 | annihil: Total cross section from Heilter formula(annihilation into 2 photons).
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| 34 | gamma energies sampled according Heitler
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| 35 | PhysicsTables from 10 keV to 10 TeV in 100 bins.
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| 36 |
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| 37 | msc: Tables of transport mean free paths.
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| 38 | New model of MSC , computes the lateral
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| 39 | displacement of the particle , too.
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| 40 | PhysicsTables from 100 eV to 100 TeV in 100 bins.
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| 41 |
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| 42 | hIoni: Knock-on electron cross sections .
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| 43 | Good description above the mean excitation energy.
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| 44 | delta ray energy sampled from differential Xsection.
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| 45 | PhysicsTables from 1 keV to 100 TeV in 100 bins.
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| 46 |
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| 47 | msc: Tables of transport mean free paths.
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| 48 | New model of MSC , computes the lateral
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| 49 | displacement of the particle , too.
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| 50 | PhysicsTables from 100 eV to 100 TeV in 100 bins.
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| 51 |
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| 52 | MuIoni: Knock-on electron cross sections .
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| 53 | Good description above the mean excitation energy.
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| 54 | delta ray energy sampled from differential Xsection.
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| 55 | PhysicsTables from 1 keV to 1000 PeV in 150 bins.
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| 56 |
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| 57 | MuBrems: theoretical cross section
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| 58 | Good description up to 1000 PeV.
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| 59 | PhysicsTables from 1 keV to 1000 PeV in 150 bins.
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| 60 |
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| 61 | MuPairProd: theoretical cross sections
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| 62 | Good description up to 1000 PeV.
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| 63 | PhysicsTables from 1 keV to 1000 PeV in 150 bins.
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| 64 | +++ G4ProcessPlacer::G4ProcessPlacer: for: neutron
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| 65 | === G4ProcessPlacer::AddProcessAsSecondDoIt ===
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| 66 | ProcessName: PScoreProcess
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| 67 | The initial Vectors:
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| 68 | GPIL Vector:
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| 69 | Decay
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| 70 | LCapture
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| 71 | LFission
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| 72 | inelastic
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| 73 | LElastic
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| 74 | Transportation
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| 75 | DoIt Vector:
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| 76 | Transportation
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| 77 | LElastic
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| 78 | inelastic
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| 79 | LFission
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| 80 | LCapture
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| 81 | Decay
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| 82 | The final Vectors:
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| 83 | GPIL Vector:
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| 84 | Decay
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| 85 | LCapture
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| 86 | LFission
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| 87 | inelastic
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| 88 | LElastic
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| 89 | PScoreProcess
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| 90 | Transportation
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| 91 | DoIt Vector:
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| 92 | Transportation
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| 93 | PScoreProcess
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| 94 | LElastic
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| 95 | inelastic
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| 96 | LFission
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| 97 | LCapture
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| 98 | Decay
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| 99 | ================================================
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| 100 | === G4ProcessPlacer::AddProcessAsSecondDoIt ===
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| 101 | ProcessName: ParallelTransport
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| 102 | The initial Vectors:
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| 103 | GPIL Vector:
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| 104 | Decay
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| 105 | LCapture
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| 106 | LFission
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| 107 | inelastic
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| 108 | LElastic
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| 109 | PScoreProcess
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| 110 | Transportation
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| 111 | DoIt Vector:
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| 112 | Transportation
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| 113 | PScoreProcess
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| 114 | LElastic
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| 115 | inelastic
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| 116 | LFission
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| 117 | LCapture
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| 118 | Decay
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| 119 | The final Vectors:
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| 120 | GPIL Vector:
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| 121 | Decay
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| 122 | LCapture
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| 123 | LFission
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| 124 | inelastic
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| 125 | LElastic
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| 126 | PScoreProcess
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| 127 | ParallelTransport
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| 128 | Transportation
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| 129 | DoIt Vector:
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| 130 | Transportation
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| 131 | ParallelTransport
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| 132 | PScoreProcess
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| 133 | LElastic
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| 134 | inelastic
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| 135 | LFission
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| 136 | LCapture
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| 137 | Decay
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| 138 | ================================================
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| 139 | output pScorer, scoring detector, neutron
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| 140 | Volume name = score_worldCylinder_phys, Replica number = -1
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| 141 | HistorysEntering
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| 142 | entries : 331
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| 143 | Sum(w) : 331
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| 144 | Sum(w*x) : 331
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| 145 | Sum(w*x*x) : 331
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| 146 | mean=Sum(w*x) / Sum(w) : 1
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| 147 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 148 | Sum(x) : 331
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| 149 | Sum(x^2) : 331
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| 150 | EnergyEnteringHistory
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| 151 | entries : 331
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| 152 | Sum(w) : 331
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| 153 | Sum(w*x) : 2868.82
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| 154 | Sum(w*x*x) : 26144.9
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| 155 | mean=Sum(w*x) / Sum(w) : 8.66714
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| 156 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 1.96678
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| 157 | Sum(x) : 2868.82
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| 158 | Sum(x^2) : 26144.9
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| 159 | Volume name = scorecell: M1, Replica number = 0
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| 160 | HistorysEntering
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| 161 | entries : 1794
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| 162 | Sum(w) : 1794
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| 163 | Sum(w*x) : 1794
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| 164 | Sum(w*x*x) : 1794
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| 165 | mean=Sum(w*x) / Sum(w) : 1
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| 166 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 167 | Sum(x) : 1794
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| 168 | Sum(x^2) : 1794
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| 169 | EnergyEnteringHistory
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| 170 | entries : 1794
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| 171 | Sum(w) : 1794
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| 172 | Sum(w*x) : 17426.6
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| 173 | Sum(w*x*x) : 171284
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| 174 | mean=Sum(w*x) / Sum(w) : 9.71383
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| 175 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 1.05729
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| 176 | Sum(x) : 17426.6
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| 177 | Sum(x^2) : 171284
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| 178 | Collisions
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| 179 | entries : 1263
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| 180 | Sum(w) : 1263
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| 181 | Sum(w*x) : 1263
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| 182 | Sum(w*x*x) : 1263
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| 183 | mean=Sum(w*x) / Sum(w) : 1
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| 184 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 185 | Sum(x) : 1263
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| 186 | Sum(x^2) : 1263
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| 187 | Volume name = scorecell: D1, Replica number = 0
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| 188 | HistorysEntering
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| 189 | entries : 858
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| 190 | Sum(w) : 858
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| 191 | Sum(w*x) : 858
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| 192 | Sum(w*x*x) : 858
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| 193 | mean=Sum(w*x) / Sum(w) : 1
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| 194 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 195 | Sum(x) : 858
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| 196 | Sum(x^2) : 858
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| 197 | EnergyEnteringHistory
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| 198 | entries : 858
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| 199 | Sum(w) : 858
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| 200 | Sum(w*x) : 8292.88
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| 201 | Sum(w*x*x) : 81250.1
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| 202 | mean=Sum(w*x) / Sum(w) : 9.66536
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| 203 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 1.13047
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| 204 | Sum(x) : 8292.88
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| 205 | Sum(x^2) : 81250.1
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| 206 | Collisions
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| 207 | entries : 512
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| 208 | Sum(w) : 512
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| 209 | Sum(w*x) : 512
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| 210 | Sum(w*x*x) : 512
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| 211 | mean=Sum(w*x) / Sum(w) : 1
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| 212 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 213 | Sum(x) : 512
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| 214 | Sum(x^2) : 512
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| 215 | Volume name = scorecell: M2, Replica number = 0
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| 216 | HistorysEntering
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| 217 | entries : 845
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| 218 | Sum(w) : 845
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| 219 | Sum(w*x) : 845
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| 220 | Sum(w*x*x) : 845
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| 221 | mean=Sum(w*x) / Sum(w) : 1
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| 222 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 223 | Sum(x) : 845
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| 224 | Sum(x^2) : 845
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| 225 | EnergyEnteringHistory
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| 226 | entries : 845
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| 227 | Sum(w) : 845
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| 228 | Sum(w*x) : 7918.1
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| 229 | Sum(w*x*x) : 76692.5
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| 230 | mean=Sum(w*x) / Sum(w) : 9.37053
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| 231 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 1.71858
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| 232 | Sum(x) : 7918.1
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| 233 | Sum(x^2) : 76692.5
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| 234 | Collisions
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| 235 | entries : 696
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| 236 | Sum(w) : 696
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| 237 | Sum(w*x) : 696
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| 238 | Sum(w*x*x) : 696
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| 239 | mean=Sum(w*x) / Sum(w) : 1
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| 240 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 241 | Sum(x) : 696
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| 242 | Sum(x^2) : 696
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| 243 | Volume name = scorecell: D2, Replica number = 0
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| 244 | HistorysEntering
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| 245 | entries : 392
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| 246 | Sum(w) : 392
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| 247 | Sum(w*x) : 392
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| 248 | Sum(w*x*x) : 392
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| 249 | mean=Sum(w*x) / Sum(w) : 1
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| 250 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 251 | Sum(x) : 392
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| 252 | Sum(x^2) : 392
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| 253 | EnergyEnteringHistory
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| 254 | entries : 392
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| 255 | Sum(w) : 392
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| 256 | Sum(w*x) : 3630.15
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| 257 | Sum(w*x*x) : 34992.4
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| 258 | mean=Sum(w*x) / Sum(w) : 9.26058
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| 259 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 1.87297
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| 260 | Sum(x) : 3630.15
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| 261 | Sum(x^2) : 34992.4
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| 262 | Collisions
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| 263 | entries : 233
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| 264 | Sum(w) : 233
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| 265 | Sum(w*x) : 233
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| 266 | Sum(w*x*x) : 233
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| 267 | mean=Sum(w*x) / Sum(w) : 1
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| 268 | sigma=sqrt(Sum(w*x*x)/Sum(w)-mean^2): 0
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| 269 | Sum(x) : 233
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| 270 | Sum(x^2) : 233
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| 271 |
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| 272 | ----------------------------------------------
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| 273 | Volume name | AV E/Track | sigma | Coll_Ent.Tr|
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| 274 | score_worldCylinder_phys. | 8.66714 | 1.96678 | 0 |
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| 275 | scorecell: M1............ | 9.71383 | 1.05729 | 0.704013 |
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| 276 | scorecell: D1............ | 9.66536 | 1.13047 | 0.596737 |
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| 277 | scorecell: M2............ | 9.37053 | 1.71858 | 0.823669 |
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| 278 | scorecell: D2............ | 9.26058 | 1.87297 | 0.594388 |
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| 279 | +++ G4ProcessPlacer::G4ProcessPlacer: for: neutron
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| 280 | ProcessName: PScoreProcess, will be removed!
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| 281 | The initial Vectors:
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| 282 | GPIL Vector:
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| 283 | Decay
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| 284 | LCapture
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| 285 | LFission
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| 286 | inelastic
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| 287 | LElastic
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| 288 | PScoreProcess
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| 289 | ParallelTransport
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| 290 | Transportation
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| 291 | DoIt Vector:
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| 292 | Transportation
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| 293 | ParallelTransport
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| 294 | PScoreProcess
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| 295 | LElastic
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| 296 | inelastic
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| 297 | LFission
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| 298 | LCapture
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| 299 | Decay
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| 300 | The final Vectors:
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| 301 | GPIL Vector:
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| 302 | Decay
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| 303 | LCapture
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| 304 | LFission
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| 305 | inelastic
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| 306 | LElastic
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| 307 | ParallelTransport
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| 308 | Transportation
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| 309 | DoIt Vector:
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| 310 | Transportation
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| 311 | ParallelTransport
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| 312 | LElastic
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| 313 | inelastic
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| 314 | LFission
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| 315 | LCapture
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| 316 | Decay
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| 317 | WARNING - Attempt to delete the physical volume store while geometry closed !
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| 318 | WARNING - Attempt to delete the logical volume store while geometry closed !
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| 319 | WARNING - Attempt to delete the solid store while geometry closed !
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