| 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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