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 | G4ClassicalRK4 (default) is called |
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10 | Accuracy Parameters: MinStep=0.01 DeltaChord=3 DeltaOneStep=0.01 |
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11 | DeltaIntersection=0.1 EpsMin=2.5e-07 EpsMax=0.05 |
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12 | F04PhysicsList::AddPhysicsList: <emstandard_opt1> |
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13 | F04PhysicsList::AddPhysicsList: <QGSP_BERT> |
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14 | Visualization Manager instantiating... |
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15 | Visualization Manager initialising... |
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16 | Registering graphics systems... |
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17 | |
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18 | You have successfully registered the following graphics systems. |
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19 | Current available graphics systems are: |
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20 | ASCIITree (ATree) |
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21 | DAWNFILE (DAWNFILE) |
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22 | G4HepRep (HepRepXML) |
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23 | G4HepRepFile (HepRepFile) |
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24 | RayTracer (RayTracer) |
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25 | VRML1FILE (VRML1FILE) |
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26 | VRML2FILE (VRML2FILE) |
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27 | OpenGLImmediateX (OGLIX) |
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28 | OpenGLStoredX (OGLSX) |
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29 | |
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30 | Registering model factories... |
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31 | |
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32 | You have successfully registered the following model factories. |
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33 | Registered model factories: |
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34 | generic |
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35 | drawByCharge |
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36 | drawByParticleID |
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37 | drawByOriginVolume |
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38 | drawByAttribute |
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39 | |
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40 | Registered filter factories: |
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41 | chargeFilter |
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42 | particleFilter |
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43 | originVolumeFilter |
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44 | attributeFilter |
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45 | |
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46 | #/event/verbose 1 |
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47 | #/tracking/verbose 1 |
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48 | # |
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49 | /field04/SetWorldMat G4_AIR |
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50 | /field04/SetWorldR 5.0 m |
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51 | /field04/SetWorldZ 50.0 m |
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52 | # |
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53 | /field04/SetCaptureR 0.6 m |
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54 | /field04/SetCaptureZ 4.0 m |
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55 | /field04/SetCaptureB1 2.5 tesla |
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56 | /field04/SetCaptureB2 5.0 tesla |
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57 | # |
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58 | /field04/SetTransferR 0.3 m |
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59 | /field04/SetTransferZ 15.0 m |
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60 | /field04/SetTransferB 5.0 tesla |
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61 | /field04/SetTransferP 0.0 m |
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62 | # |
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63 | /field04/SetTgtMat G4_W |
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64 | /field04/SetTgtRad 0.4 cm |
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65 | /field04/SetTgtThick 16.0 cm |
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66 | /field04/SetTgtPos 0.0 cm |
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67 | /field04/SetTgtAng 170 |
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68 | # |
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69 | /field04/SetDgrMat G4_Pb |
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70 | /field04/SetDgrRad 30.0 cm |
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71 | /field04/SetDgrThick 0.1 cm |
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72 | #/field04/SetDgrPos -7.4 m |
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73 | # |
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74 | #/exp/phys/addPhysics emstandard_opt1 |
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75 | #/exp/phys/addPhysics QGSP_BERT |
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76 | #/exp/phys/removeHadronPhysics gamma_nuc |
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77 | /exp/phys/gammaCut 1.0 m |
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78 | /exp/phys/stepMax 2.0 mm |
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79 | /exp/phys/list |
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80 | ### PhysicsLists available: FTFC FTFP FTFP_EMV LHEP LHEP_BERT LHEP_EMV |
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81 | LHEP_PRECO_HP QBBC QBBCG QBEC QBBC_HP QBEC_HP |
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82 | QGSC QGSC_EFLOW QGSC_EMV QGSP QGSP_BERT QGSP_BER_EMV |
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83 | QGSP_BERT_HP QGSP_BERT_NQE QGSP_BERT_TRV |
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84 | QGSP_BIC QGSP_BIC_HP QGSP_EMV QGSP_EMV_NQE |
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85 | QGSC_EMX QGSP_NQE QGSP_QEL |
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86 | # |
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87 | #/decay/pienu |
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88 | #/decay/pimunu |
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89 | # |
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90 | /field/setStepperType 4 |
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91 | /field/setMinStep 10 mm |
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92 | /field/update |
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93 | G4ClassicalRK4 (default) is called |
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94 | Accuracy Parameters: MinStep=10 DeltaChord=3 DeltaOneStep=0.01 |
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95 | DeltaIntersection=0.1 EpsMin=2.5e-07 EpsMax=0.05 |
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96 | # |
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97 | /run/initialize |
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98 | G4NistMaterialBuilder::FindOrBuildMaterial G4_Galactic |
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99 | G4NistMaterialBuilder: BuildMaterial #286 |
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100 | New material nComponents= 1 |
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101 | G4NistElementBuilder: Build Element <H> Z= 1 A= 1.00795 with natural isotope composition |
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102 | G4Material: Mean excitation energy is changed for G4_Galactic Iold= 21.8eV; Inew= 21.8 eV; |
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103 | G4NistMaterialBuilder::FindOrBuildMaterial G4_AIR |
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104 | G4NistMaterialBuilder::FindOrBuildMaterial G4_BERYLLIUM_OXIDE |
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105 | G4NistMaterialBuilder: BuildMaterial #115 |
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106 | New material nComponents= 2 |
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107 | G4NistElementBuilder: Build Element <Be> Z= 4 A= 9.01218 with natural isotope composition |
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108 | G4Material: Mean excitation energy is changed for G4_BERYLLIUM_OXIDE Iold= 83.2231eV; Inew= 93.2 eV; |
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109 | New material Scintillator is prepeared; nMaterials= 288 nComponents= 742 nCurrent= 2 |
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110 | ### NIST DataBase for Elements is used |
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111 | G4NistMaterialBuilder: BuildMaterial Scintillator |
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112 | G4NistMaterialBuilder: BuildMaterial #287 |
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113 | New material nComponents= 2 |
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114 | |
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115 | The materials defined are: |
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116 | |
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117 | |
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118 | ***** Table : Nb of materials = 6 ***** |
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119 | |
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120 | Material: G4_AIR density: 1.205 mg/cm3 RadL: 303.921 m Imean: 85.700 eV temperature: 273.15 K pressure: 1.00 atm |
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121 | ---> Element: C (C) Z = 6.0 N = 12.0 A = 12.01 g/mole |
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122 | ---> Isotope: C Z = 6 N = 12 A = 12.00 g/mole abundance: 98.93 % |
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123 | ---> Isotope: C Z = 6 N = 13 A = 13.00 g/mole abundance: 1.07 % ElmMassFraction: 0.01 % ElmAbundance 0.02 % |
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124 | ---> Element: N (N) Z = 7.0 N = 14.0 A = 14.01 g/mole |
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125 | ---> Isotope: N Z = 7 N = 14 A = 14.00 g/mole abundance: 99.63 % |
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126 | ---> Isotope: N Z = 7 N = 15 A = 15.00 g/mole abundance: 0.37 % ElmMassFraction: 75.53 % ElmAbundance 78.44 % |
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127 | ---> Element: O (O) Z = 8.0 N = 16.0 A = 16.00 g/mole |
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128 | ---> Isotope: O Z = 8 N = 16 A = 15.99 g/mole abundance: 99.76 % |
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129 | ---> Isotope: O Z = 8 N = 17 A = 17.00 g/mole abundance: 0.04 % |
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130 | ---> Isotope: O Z = 8 N = 18 A = 18.00 g/mole abundance: 0.20 % ElmMassFraction: 23.18 % ElmAbundance 21.07 % |
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131 | ---> Element: Ar (Ar) Z = 18.0 N = 40.0 A = 39.95 g/mole |
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132 | ---> Isotope: Ar Z = 18 N = 36 A = 35.97 g/mole abundance: 0.34 % |
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133 | ---> Isotope: Ar Z = 18 N = 38 A = 37.96 g/mole abundance: 0.06 % |
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134 | ---> Isotope: Ar Z = 18 N = 40 A = 39.96 g/mole abundance: 99.60 % ElmMassFraction: 1.28 % ElmAbundance 0.47 % |
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135 | |
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136 | Material: G4_W density: 19.300 g/cm3 RadL: 3.504 mm Imean: 727.000 eV |
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137 | ---> Element: W (W) Z = 74.0 N = 183.9 A = 183.84 g/mole |
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138 | ---> Isotope: W Z = 74 N = 180 A = 179.95 g/mole abundance: 0.12 % |
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139 | ---> Isotope: W Z = 74 N = 182 A = 181.95 g/mole abundance: 26.50 % |
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140 | ---> Isotope: W Z = 74 N = 183 A = 182.95 g/mole abundance: 14.31 % |
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141 | ---> Isotope: W Z = 74 N = 184 A = 183.95 g/mole abundance: 30.64 % |
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142 | ---> Isotope: W Z = 74 N = 186 A = 185.95 g/mole abundance: 28.43 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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143 | |
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144 | Material: G4_Pb density: 11.350 g/cm3 RadL: 5.613 mm Imean: 823.000 eV |
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145 | ---> Element: Pb (Pb) Z = 82.0 N = 207.2 A = 207.22 g/mole |
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146 | ---> Isotope: Pb Z = 82 N = 204 A = 203.97 g/mole abundance: 1.40 % |
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147 | ---> Isotope: Pb Z = 82 N = 206 A = 205.97 g/mole abundance: 24.10 % |
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148 | ---> Isotope: Pb Z = 82 N = 207 A = 206.98 g/mole abundance: 22.10 % |
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149 | ---> Isotope: Pb Z = 82 N = 208 A = 207.98 g/mole abundance: 52.40 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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150 | |
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151 | Material: G4_Galactic density: 0.000 mg/cm3 RadL: 204311173.221 pc Imean: 21.800 eV temperature: 2.73 K pressure: 0.00 atm |
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152 | ---> Element: H (H) Z = 1.0 N = 1.0 A = 1.01 g/mole |
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153 | ---> Isotope: H Z = 1 N = 1 A = 1.01 g/mole abundance: 99.99 % |
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154 | ---> Isotope: H Z = 1 N = 2 A = 2.01 g/mole abundance: 0.01 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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155 | |
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156 | Material: G4_BERYLLIUM_OXIDE density: 3.010 g/cm3 RadL: 13.722 cm Imean: 93.200 eV |
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157 | ---> Element: Be (Be) Z = 4.0 N = 9.0 A = 9.01 g/mole |
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158 | ---> Isotope: Be Z = 4 N = 9 A = 9.01 g/mole abundance: 100.00 % ElmMassFraction: 36.03 % ElmAbundance 50.00 % |
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159 | ---> Element: O (O) Z = 8.0 N = 16.0 A = 16.00 g/mole |
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160 | ---> Isotope: O Z = 8 N = 16 A = 15.99 g/mole abundance: 99.76 % |
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161 | ---> Isotope: O Z = 8 N = 17 A = 17.00 g/mole abundance: 0.04 % |
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162 | ---> Isotope: O Z = 8 N = 18 A = 18.00 g/mole abundance: 0.20 % ElmMassFraction: 63.97 % ElmAbundance 50.00 % |
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163 | |
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164 | Material: Scintillator density: 0.000 mg/cm3 RadL: 86.056 pc Imean: 63.913 eV |
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165 | ---> Element: C (C) Z = 6.0 N = 12.0 A = 12.01 g/mole |
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166 | ---> Isotope: C Z = 6 N = 12 A = 12.00 g/mole abundance: 98.93 % |
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167 | ---> Isotope: C Z = 6 N = 13 A = 13.00 g/mole abundance: 1.07 % ElmMassFraction: 91.47 % ElmAbundance 47.37 % |
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168 | ---> Element: H (H) Z = 1.0 N = 1.0 A = 1.01 g/mole |
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169 | ---> Isotope: H Z = 1 N = 1 A = 1.01 g/mole abundance: 99.99 % |
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170 | ---> Isotope: H Z = 1 N = 2 A = 2.01 g/mole abundance: 0.01 % ElmMassFraction: 8.53 % ElmAbundance 52.63 % |
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171 | |
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172 | |
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173 | G4NistMaterialBuilder::FindOrBuildMaterial G4_Galactic |
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174 | G4NistMaterialBuilder::FindOrBuildMaterial G4_AIR |
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175 | G4NistMaterialBuilder::FindOrBuildMaterial G4_Pb |
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176 | G4NistMaterialBuilder::FindOrBuildMaterial G4_W |
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177 | F04ExtraPhysics:: Add Extra Physics Processes |
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178 | Thank you for using G4BinaryCascade. |
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179 | ### Adding Neutron tracking cut for neutron |
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180 | ### cut value is 10 microseconds |
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181 | =========================================================================================== |
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182 | |
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183 | Hadronic Processes for anti_neutron |
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184 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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185 | |
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186 | Hadronic Processes for anti_proton |
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187 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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188 | |
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189 | Hadronic Processes for kaon+ |
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190 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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191 | |
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192 | Hadronic Processes for kaon- |
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193 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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194 | |
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195 | Hadronic Processes for lambda |
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196 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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197 | |
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198 | Hadronic Processes for neutron |
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199 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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200 | |
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201 | Hadronic Processes for pi+ |
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202 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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203 | |
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204 | Hadronic Processes for pi- |
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205 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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206 | |
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207 | Hadronic Processes for proton |
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208 | hElastic Models: elastic Emin(GeV)= 0 Emax(GeV)= 100000 |
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209 | =========================================================================================== |
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210 | F04PhysicsList::SetCuts:CutLength : 1 mm |
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211 | # |
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212 | #/process/inactivate msc |
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213 | #/process/activate msc |
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214 | # |
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215 | #/field04/SetTgtMat G4_Pb |
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216 | #/field04/SetCaptureR 0.6 m |
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217 | #/field04/Update |
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218 | # |
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219 | /gun/particle proton |
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220 | /gun/energy 500.0 MeV |
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221 | #/gun/momentumAmp 1.09008 GeV |
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222 | /gun/random on |
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223 | # |
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224 | #/control/execute vis.mac |
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225 | # |
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226 | #/rndm/save 2 |
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227 | #/rndm/read random/run0evt8268.rndm |
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228 | #/random/resetEngineFrom random/run0evt40.rndm |
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229 | # |
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230 | /run/beamOn 1000 |
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231 | G4VRangeToEnergyConverter::ConvertCutToKineticEnergy for gamma |
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232 | The cut in range [1000 (mm)] is too big for material idx=1 |
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233 | The cut in energy is set1.79769e+305GeV |
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234 | G4VRangeToEnergyConverter::ConvertCutToKineticEnergy for gamma |
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235 | The cut in range [1000 (mm)] is too big for material idx=2 |
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236 | The cut in energy is set1.79769e+305GeV |
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237 | |
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238 | phot: Total cross sections from Sandia parametrisation. |
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239 | Sampling according PhotoElectric model |
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240 | |
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241 | compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV |
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242 | Sampling according Klein-Nishina model |
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243 | tables are built for gamma |
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244 | Lambda tables from 100 eV to 100 GeV in 90 bins. |
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245 | |
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246 | conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z; |
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247 | sampling secondary e+e- according Bethe-Heitler model |
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248 | tables are built for gamma |
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249 | Lambda tables from 1.022 MeV to 100 GeV in 100 bins. |
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250 | |
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251 | msc: Model variant of multiple scattering for e- |
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252 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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253 | LateralDisplacementFlag= 1 Skin= 0 |
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254 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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255 | |
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256 | eIoni: tables are built for e- |
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257 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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258 | Lambda tables from threshold to 100 TeV in 120 bins. |
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259 | Delta cross sections and sampling from MollerBhabha model |
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260 | Good description from 1 KeV to 100 GeV. |
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261 | Step function: finalRange(mm)= 1, dRoverRange= 0.8, integral: 1, fluct: 1 |
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262 | |
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263 | eBrem: tables are built for e- |
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264 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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265 | Lambda tables from threshold to 100 TeV in 120 bins. |
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266 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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267 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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268 | |
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269 | eIoni: tables are built for e+ |
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270 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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271 | Lambda tables from threshold to 100 TeV in 120 bins. |
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272 | Delta cross sections and sampling from MollerBhabha model |
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273 | Good description from 1 KeV to 100 GeV. |
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274 | Step function: finalRange(mm)= 1, dRoverRange= 0.8, integral: 1, fluct: 1 |
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275 | |
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276 | eBrem: tables are built for e+ |
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277 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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278 | Lambda tables from threshold to 100 TeV in 120 bins. |
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279 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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280 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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281 | |
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282 | annihil: Sampling according eplus2gg model |
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283 | tables are built for e+ |
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284 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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285 | |
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286 | msc: Model variant of multiple scattering for proton |
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287 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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288 | LateralDisplacementFlag= 1 Skin= 0 |
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289 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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290 | |
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291 | hIoni: tables are built for proton |
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292 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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293 | Lambda tables from threshold to 100 TeV in 120 bins. |
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294 | Scaling relation is used from proton dE/dx and range. |
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295 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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296 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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297 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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298 | |
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299 | msc: Model variant of multiple scattering for GenericIon |
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300 | LateralDisplacementFlag= 0 Skin= 0 |
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301 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 1 |
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302 | |
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303 | ionIoni: tables are built for GenericIon |
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304 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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305 | Lambda tables from threshold to 100 TeV in 120 bins. |
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306 | Scaling relation is used from proton dE/dx and range. |
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307 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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308 | Parametrisation from BraggIon for protons below. NuclearStopping= 1 |
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309 | |
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310 | Stopping Power data for 8 ion/material pairs are used. |
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311 | Step function: finalRange(mm)= 0.1, dRoverRange= 0.1, integral: 1, fluct: 1 |
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312 | |
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313 | hIoni: tables are built for anti_proton |
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314 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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315 | Lambda tables from threshold to 100 TeV in 120 bins. |
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316 | Scaling relation is used from proton dE/dx and range. |
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317 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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318 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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319 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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320 | |
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321 | msc: Model variant of multiple scattering for mu+ |
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322 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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323 | LateralDisplacementFlag= 1 Skin= 0 |
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324 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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325 | |
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326 | muIoni: tables are built for mu+ |
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327 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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328 | Lambda tables from threshold to 100 TeV in 120 bins. |
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329 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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330 | radiative corrections for E > 1 GeV |
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331 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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332 | |
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333 | muBrems: tables are built for mu+ |
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334 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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335 | Lambda tables from threshold to 100 TeV in 120 bins. |
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336 | Parametrised model |
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337 | |
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338 | muPairProd: tables are built for mu+ |
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339 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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340 | Lambda tables from threshold to 100 TeV in 120 bins. |
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341 | Parametrised model |
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342 | |
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343 | muIoni: tables are built for mu- |
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344 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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345 | Lambda tables from threshold to 100 TeV in 120 bins. |
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346 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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347 | radiative corrections for E > 1 GeV |
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348 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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349 | |
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350 | muBrems: tables are built for mu- |
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351 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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352 | Lambda tables from threshold to 100 TeV in 120 bins. |
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353 | Parametrised model |
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354 | |
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355 | muPairProd: tables are built for mu- |
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356 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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357 | Lambda tables from threshold to 100 TeV in 120 bins. |
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358 | Parametrised model |
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359 | |
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360 | G4UHadronElasticProcess for neutron PDGcode= 2112 Elow(MeV)= 19 Elowest(eV)= 0 |
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361 | |
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362 | hIoni: tables are built for pi+ |
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363 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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364 | Lambda tables from threshold to 100 TeV in 120 bins. |
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365 | Scaling relation is used from proton dE/dx and range. |
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366 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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367 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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368 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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369 | |
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370 | msc: Model variant of multiple scattering for pi- |
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371 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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372 | LateralDisplacementFlag= 1 Skin= 0 |
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373 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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374 | |
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375 | hIoni: tables are built for pi- |
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376 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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377 | Lambda tables from threshold to 100 TeV in 120 bins. |
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378 | Scaling relation is used from proton dE/dx and range. |
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379 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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380 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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381 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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382 | |
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383 | ========= Table of registered couples ============================== |
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384 | |
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385 | Index : 0 used in the geometry : Yes recalculation needed : No |
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386 | Material : G4_AIR |
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387 | Range cuts : gamma 1 m e- 1 mm e+ 1 mm |
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388 | Energy thresholds : gamma 3.07332 keV e- 990 eV e+ 990 eV |
---|
389 | Region(s) which use this couple : |
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390 | DefaultRegionForTheWorld |
---|
391 | |
---|
392 | Index : 1 used in the geometry : Yes recalculation needed : No |
---|
393 | Material : G4_Galactic |
---|
394 | Range cuts : gamma 1 m e- 1 mm e+ 1 mm |
---|
395 | Energy thresholds : gamma 990 eV e- 990 eV e+ 990 eV |
---|
396 | Region(s) which use this couple : |
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397 | DefaultRegionForTheWorld |
---|
398 | |
---|
399 | Index : 2 used in the geometry : Yes recalculation needed : No |
---|
400 | Material : G4_W |
---|
401 | Range cuts : gamma 1 m e- 1 mm e+ 1 mm |
---|
402 | Energy thresholds : gamma 2.88022e+295 J e- 2.31122 MeV e+ 2.14666 MeV |
---|
403 | Region(s) which use this couple : |
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404 | DefaultRegionForTheWorld |
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405 | |
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406 | Index : 3 used in the geometry : Yes recalculation needed : No |
---|
407 | Material : G4_Pb |
---|
408 | Range cuts : gamma 1 m e- 1 mm e+ 1 mm |
---|
409 | Energy thresholds : gamma 2.88022e+295 J e- 1.37814 MeV e+ 1.28002 MeV |
---|
410 | Region(s) which use this couple : |
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411 | DefaultRegionForTheWorld |
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412 | |
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413 | ==================================================================== |
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616 | # |
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617 | Graphics systems deleted. |
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618 | Visualization Manager deleting... |
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