1 | ********************************************** |
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2 | Geant4 version $Name: geant4-09-04-beta-01 $ |
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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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