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 | ### NIST DataBase for Materials is used |
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10 | G4Material: Mean excitation energy is changed for G4_AIR Iold= 85.627eV; Inew= 85.7 eV; |
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11 | G4Material: Mean excitation energy is changed for G4_Al Iold= 166.4eV; Inew= 166 eV; |
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12 | G4Material: Mean excitation energy is changed for G4_Si Iold= 173.6eV; Inew= 173 eV; |
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13 | G4Material: Mean excitation energy is changed for G4_Fe Iold= 286eV; Inew= 286 eV; |
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14 | G4Material: Mean excitation energy is changed for G4_CESIUM_IODIDE Iold= 491.166eV; Inew= 553.1 eV; |
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15 | /run/verbose 1 |
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16 | #/tracking/verbose 1 |
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17 | # |
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18 | # select EM PhysicsList |
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19 | # |
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20 | /testem/phys/addPhysics emstandard_opt1 |
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21 | PhysicsList::Set emstandard_opt1 EM physics |
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22 | # |
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23 | /testem/phys/setCuts 0.3 mm |
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24 | /testem/phys/VertexCuts 0.01 mm |
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25 | /testem/phys/MuonCuts 10.0 mm |
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26 | /testem/stepMax 100 mm |
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27 | # |
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28 | /testem/det/acceptance1 0.8271 0.02974 2.5 |
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29 | /testem/det/acceptance9 0.9570 0.01286 2.5 |
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30 | /testem/det/acceptance25 0.9793 0.00884 2.5 |
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31 | # |
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32 | #/process/eLoss/preciseRange true |
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33 | #/process/eLoss/integral true |
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34 | /run/initialize |
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35 | |
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36 | ***** Table : Nb of materials = 5 ***** |
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37 | |
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38 | 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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39 | ---> Element: C (C) Z = 6.0 N = 12.0 A = 12.01 g/mole |
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40 | ---> Isotope: C Z = 6 N = 12 A = 12.00 g/mole abundance: 98.93 % |
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41 | ---> Isotope: C Z = 6 N = 13 A = 13.00 g/mole abundance: 1.07 % ElmMassFraction: 0.01 % ElmAbundance 0.02 % |
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42 | ---> Element: N (N) Z = 7.0 N = 14.0 A = 14.01 g/mole |
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43 | ---> Isotope: N Z = 7 N = 14 A = 14.00 g/mole abundance: 99.63 % |
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44 | ---> Isotope: N Z = 7 N = 15 A = 15.00 g/mole abundance: 0.37 % ElmMassFraction: 75.53 % ElmAbundance 78.44 % |
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45 | ---> Element: O (O) Z = 8.0 N = 16.0 A = 16.00 g/mole |
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46 | ---> Isotope: O Z = 8 N = 16 A = 15.99 g/mole abundance: 99.76 % |
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47 | ---> Isotope: O Z = 8 N = 17 A = 17.00 g/mole abundance: 0.04 % |
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48 | ---> Isotope: O Z = 8 N = 18 A = 18.00 g/mole abundance: 0.20 % ElmMassFraction: 23.18 % ElmAbundance 21.07 % |
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49 | ---> Element: Ar (Ar) Z = 18.0 N = 40.0 A = 39.95 g/mole |
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50 | ---> Isotope: Ar Z = 18 N = 36 A = 35.97 g/mole abundance: 0.34 % |
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51 | ---> Isotope: Ar Z = 18 N = 38 A = 37.96 g/mole abundance: 0.06 % |
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52 | ---> Isotope: Ar Z = 18 N = 40 A = 39.96 g/mole abundance: 99.60 % ElmMassFraction: 1.28 % ElmAbundance 0.47 % |
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53 | |
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54 | Material: G4_Al density: 2.699 g/cm3 RadL: 8.896 cm Imean: 166.000 eV |
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55 | ---> Element: Al (Al) Z = 13.0 N = 27.0 A = 26.98 g/mole |
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56 | ---> Isotope: Al Z = 13 N = 27 A = 26.98 g/mole abundance: 100.00 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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57 | |
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58 | Material: G4_Si density: 2.330 g/cm3 RadL: 9.366 cm Imean: 173.000 eV |
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59 | ---> Element: Si (Si) Z = 14.0 N = 28.1 A = 28.09 g/mole |
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60 | ---> Isotope: Si Z = 14 N = 28 A = 27.98 g/mole abundance: 92.23 % |
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61 | ---> Isotope: Si Z = 14 N = 29 A = 28.98 g/mole abundance: 4.68 % |
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62 | ---> Isotope: Si Z = 14 N = 30 A = 29.97 g/mole abundance: 3.09 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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63 | |
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64 | Material: G4_Fe density: 7.874 g/cm3 RadL: 1.757 cm Imean: 286.000 eV |
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65 | ---> Element: Fe (Fe) Z = 26.0 N = 55.9 A = 55.85 g/mole |
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66 | ---> Isotope: Fe Z = 26 N = 54 A = 53.94 g/mole abundance: 5.84 % |
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67 | ---> Isotope: Fe Z = 26 N = 56 A = 55.93 g/mole abundance: 91.75 % |
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68 | ---> Isotope: Fe Z = 26 N = 57 A = 56.94 g/mole abundance: 2.12 % |
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69 | ---> Isotope: Fe Z = 26 N = 58 A = 57.93 g/mole abundance: 0.28 % ElmMassFraction: 100.00 % ElmAbundance 100.00 % |
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70 | |
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71 | Material: G4_CESIUM_IODIDE density: 4.510 g/cm3 RadL: 1.860 cm Imean: 553.100 eV |
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72 | ---> Element: I (I) Z = 53.0 N = 127.0 A = 126.90 g/mole |
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73 | ---> Isotope: I Z = 53 N = 127 A = 126.90 g/mole abundance: 100.00 % ElmMassFraction: 48.85 % ElmAbundance 50.00 % |
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74 | ---> Element: Cs (Cs) Z = 55.0 N = 133.0 A = 132.91 g/mole |
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75 | ---> Isotope: Cs Z = 55 N = 133 A = 132.91 g/mole abundance: 100.00 % ElmMassFraction: 51.15 % ElmAbundance 50.00 % |
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76 | |
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77 | |
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78 | Ecal is 36 cm of G4_CESIUM_IODIDE |
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79 | Absorber is 2 mm of G4_Al |
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80 | Vertex is 3 cm of 3 layers of Si of 100 um npads= 601 |
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81 | ### New geometry is constructed |
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82 | PhysicsList: world cuts are set cutG= 0.3 mm cutE= 0.3 mm |
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83 | Vertex cuts are set |
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84 | Muon cuts are set |
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85 | # |
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86 | #/testem/histo/fileName e_pr.root |
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87 | #/testem/histo/fileType root |
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88 | /gun/particle e- |
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89 | /gun/energy 1 GeV |
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90 | /run/beamOn 100 |
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91 | |
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92 | phot: Total cross sections from Sandia parametrisation. |
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93 | Sampling according PhotoElectric model |
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94 | |
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95 | compt: Total cross sections has a good parametrisation from 10 KeV to (100/Z) GeV |
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96 | Sampling according Klein-Nishina model |
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97 | tables are built for gamma |
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98 | Lambda tables from 100 eV to 100 GeV in 90 bins. |
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99 | |
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100 | conv: Total cross sections has a good parametrisation from 1.5 MeV to 100 GeV for all Z; |
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101 | sampling secondary e+e- according Bethe-Heitler model |
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102 | tables are built for gamma |
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103 | Lambda tables from 1.022 MeV to 100 GeV in 100 bins. |
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104 | |
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105 | msc: Model variant of multiple scattering for e- |
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106 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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107 | LateralDisplacementFlag= 1 Skin= 0 |
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108 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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109 | |
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110 | eIoni: tables are built for e- |
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111 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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112 | Lambda tables from threshold to 100 TeV in 120 bins. |
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113 | Delta cross sections and sampling from MollerBhabha model |
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114 | Good description from 1 KeV to 100 GeV. |
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115 | Step function: finalRange(mm)= 1, dRoverRange= 0.8, integral: 1, fluct: 1 |
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116 | |
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117 | eBrem: tables are built for e- |
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118 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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119 | Lambda tables from threshold to 100 TeV in 120 bins. |
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120 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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121 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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122 | |
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123 | eIoni: tables are built for e+ |
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124 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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125 | Lambda tables from threshold to 100 TeV in 120 bins. |
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126 | Delta cross sections and sampling from MollerBhabha model |
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127 | Good description from 1 KeV to 100 GeV. |
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128 | Step function: finalRange(mm)= 1, dRoverRange= 0.8, integral: 1, fluct: 1 |
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129 | |
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130 | eBrem: tables are built for e+ |
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131 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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132 | Lambda tables from threshold to 100 TeV in 120 bins. |
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133 | Total cross sections and sampling from StandBrem model (based on the EEDL data library) |
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134 | Good description from 1 KeV to 100 GeV, log scale extrapolation above 100 GeV. LPM flag 1 |
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135 | |
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136 | annihil: Sampling according eplus2gg model |
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137 | tables are built for e+ |
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138 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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139 | |
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140 | msc: Model variant of multiple scattering for proton |
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141 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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142 | LateralDisplacementFlag= 1 Skin= 0 |
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143 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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144 | |
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145 | hIoni: tables are built for proton |
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146 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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147 | Lambda tables from threshold to 100 TeV in 120 bins. |
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148 | Scaling relation is used from proton dE/dx and range. |
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149 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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150 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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151 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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152 | |
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153 | msc: Model variant of multiple scattering for GenericIon |
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154 | LateralDisplacementFlag= 0 Skin= 0 |
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155 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 1 |
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156 | |
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157 | ionIoni: tables are built for GenericIon |
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158 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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159 | Lambda tables from threshold to 100 TeV in 120 bins. |
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160 | Scaling relation is used from proton dE/dx and range. |
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161 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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162 | Parametrisation from BraggIon for protons below. NuclearStopping= 1 |
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163 | |
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164 | Stopping Power data for 8 ion/material pairs are used. |
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165 | Step function: finalRange(mm)= 0.1, dRoverRange= 0.1, integral: 1, fluct: 1 |
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166 | |
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167 | hIoni: tables are built for anti_proton |
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168 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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169 | Lambda tables from threshold to 100 TeV in 120 bins. |
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170 | Scaling relation is used from proton dE/dx and range. |
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171 | Delta cross sections and sampling from BetheBloch model for scaled energy > 2 MeV |
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172 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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173 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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174 | |
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175 | msc: Model variant of multiple scattering for mu+ |
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176 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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177 | LateralDisplacementFlag= 1 Skin= 0 |
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178 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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179 | |
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180 | muIoni: tables are built for mu+ |
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181 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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182 | Lambda tables from threshold to 100 TeV in 120 bins. |
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183 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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184 | radiative corrections for E > 1 GeV |
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185 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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186 | |
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187 | muBrems: tables are built for mu+ |
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188 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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189 | Lambda tables from threshold to 100 TeV in 120 bins. |
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190 | Parametrised model |
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191 | |
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192 | muPairProd: tables are built for mu+ |
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193 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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194 | Lambda tables from threshold to 100 TeV in 120 bins. |
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195 | Parametrised model |
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196 | |
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197 | muIoni: tables are built for mu- |
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198 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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199 | Lambda tables from threshold to 100 TeV in 120 bins. |
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200 | Bether-Bloch model for E > 0.2 MeV, parametrisation of Bragg peak below, |
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201 | radiative corrections for E > 1 GeV |
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202 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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203 | |
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204 | muBrems: tables are built for mu- |
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205 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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206 | Lambda tables from threshold to 100 TeV in 120 bins. |
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207 | Parametrised model |
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208 | |
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209 | muPairProd: tables are built for mu- |
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210 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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211 | Lambda tables from threshold to 100 TeV in 120 bins. |
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212 | Parametrised model |
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213 | |
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214 | hIoni: tables are built for pi+ |
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215 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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216 | Lambda tables from threshold to 100 TeV in 120 bins. |
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217 | Scaling relation is used from proton dE/dx and range. |
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218 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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219 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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220 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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221 | |
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222 | msc: Model variant of multiple scattering for pi- |
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223 | Lambda tables from 100 eV to 100 TeV in 120 bins. |
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224 | LateralDisplacementFlag= 1 Skin= 0 |
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225 | Boundary/stepping algorithm is active with RangeFactor= 0.2 Step limit type 0 |
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226 | |
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227 | hIoni: tables are built for pi- |
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228 | dE/dx and range tables from 100 eV to 100 TeV in 120 bins. |
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229 | Lambda tables from threshold to 100 TeV in 120 bins. |
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230 | Scaling relation is used from proton dE/dx and range. |
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231 | Delta cross sections and sampling from BetheBloch model for scaled energy > 0.297504 MeV |
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232 | Parametrisation from Bragg for protons below. NuclearStopping= 1 |
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233 | Step function: finalRange(mm)= 1, dRoverRange= 0.2, integral: 1, fluct: 1 |
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234 | |
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235 | ========= Table of registered couples ============================== |
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236 | |
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237 | Index : 0 used in the geometry : Yes recalculation needed : No |
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238 | Material : G4_AIR |
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239 | Range cuts : gamma 300 um e- 300 um e+ 300 um |
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240 | Energy thresholds : gamma 990 eV e- 990 eV e+ 990 eV |
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241 | Region(s) which use this couple : |
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242 | DefaultRegionForTheWorld |
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243 | |
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244 | Index : 1 used in the geometry : Yes recalculation needed : No |
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245 | Material : G4_CESIUM_IODIDE |
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246 | Range cuts : gamma 300 um e- 300 um e+ 300 um |
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247 | Energy thresholds : gamma 18.1187 keV e- 288.607 keV e+ 278.143 keV |
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248 | Region(s) which use this couple : |
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249 | DefaultRegionForTheWorld |
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250 | |
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251 | Index : 2 used in the geometry : Yes recalculation needed : No |
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252 | Material : G4_Al |
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253 | Range cuts : gamma 300 um e- 300 um e+ 300 um |
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254 | Energy thresholds : gamma 3.89739 keV e- 258.339 keV e+ 252.056 keV |
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255 | Region(s) which use this couple : |
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256 | DefaultRegionForTheWorld |
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257 | |
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258 | Index : 3 used in the geometry : Yes recalculation needed : No |
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259 | Material : G4_AIR |
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260 | Range cuts : gamma 10 um e- 10 um e+ 10 um |
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261 | Energy thresholds : gamma 990 eV e- 990 eV e+ 990 eV |
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262 | Region(s) which use this couple : |
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263 | VertexDetector |
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264 | |
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265 | Index : 4 used in the geometry : Yes recalculation needed : No |
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266 | Material : G4_Al |
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267 | Range cuts : gamma 10 um e- 10 um e+ 10 um |
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268 | Energy thresholds : gamma 990 eV e- 33.8876 keV e+ 33.4729 keV |
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269 | Region(s) which use this couple : |
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270 | VertexDetector |
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271 | |
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272 | Index : 5 used in the geometry : Yes recalculation needed : No |
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273 | Material : G4_Si |
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274 | Range cuts : gamma 10 um e- 10 um e+ 10 um |
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275 | Energy thresholds : gamma 990 eV e- 31.4747 keV e+ 31.0896 keV |
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276 | Region(s) which use this couple : |
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277 | VertexDetector |
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278 | |
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279 | Index : 6 used in the geometry : Yes recalculation needed : No |
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280 | Material : G4_Fe |
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281 | Range cuts : gamma 1 cm e- 1 cm e+ 1 cm |
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282 | Energy thresholds : gamma 60.4019 keV e- 12.9518 MeV e+ 12.0297 MeV |
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283 | Region(s) which use this couple : |
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284 | MuonDetector |
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285 | |
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286 | Index : 7 used in the geometry : Yes recalculation needed : No |
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287 | Material : G4_Al |
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288 | Range cuts : gamma 1 cm e- 1 cm e+ 1 cm |
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289 | Energy thresholds : gamma 20.4949 keV e- 4.54874 MeV e+ 4.2772 MeV |
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290 | Region(s) which use this couple : |
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291 | MuonDetector |
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292 | |
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293 | ==================================================================== |
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294 | |
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295 | ### Run 0 start |
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296 | HistoManager: Histograms are booked and run has been started |
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297 | Start Run processing. |
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298 | Run terminated. |
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299 | Run Summary |
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300 | Number of events processed : 100 |
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301 | User=4.19s Real=4.21s Sys=0s |
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302 | RunAction: End of run actions are started |
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303 | HistoManager: End of run actions are started |
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304 | ================================================================= |
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305 | Number of events 100 |
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306 | Average number of e- 1320 |
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307 | Average number of gamma 701.3 |
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308 | Average number of e+ 48.12 |
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309 | Average number of steps 3980 |
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310 | Edep 1x1 = 0.8336 +- 0.002518 res= 3.021 % |
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311 | Edep 3x3 = 0.9601 +- 0.001163 res= 1.212 % |
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312 | Edep 5x5 = 0.9807 +- 0.0007853 res= 0.8007 % |
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313 | =========== Mean values without trancating ===================== |
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314 | Edep 1x1 = 0.8327 +- 0.002681 res= 3.219 % |
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315 | Edep 3x3 = 0.9596 +- 0.001241 res= 1.293 % |
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316 | Edep 5x5 = 0.9807 +- 0.0007853 res= 0.8007 % |
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317 | ================================================================== |
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318 | |
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319 | |
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320 | <<<<<ACCEPTANCE>>>>> 100 events for Crystal Calorimeter |
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321 | Edep1x1: 0.8336 delEdep1x1= 0.006515 nrms= 2.191 |
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322 | Erms1x1: 0.02518 delErms1x1= -0.00456 nrms= -1.533 |
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323 | Edep3x3: 0.9601 delEdep3x3= 0.003087 nrms= 2.401 |
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324 | Erms3x3: 0.01163 delErms3x3= -0.001226 nrms= -0.9531 |
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325 | Edep5x5: 0.9807 delEdep5x5= 0.001428 nrms= 1.615 |
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326 | Erms5x5: 0.007853 delErms5x5= -0.0009872 nrms= -1.117 |
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327 | <<<<<END>>>>> IS ACCEPTED |
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328 | |
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329 | # |
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330 | G4 kernel has come to Quit state. |
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