[819] | 1 | // |
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| 2 | // ******************************************************************** |
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| 3 | // * License and Disclaimer * |
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| 4 | // * * |
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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| 7 | // * conditions of the Geant4 Software License, included in the file * |
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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| 9 | // * include a list of copyright holders. * |
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| 10 | // * * |
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| 11 | // * Neither the authors of this software system, nor their employing * |
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| 12 | // * institutes,nor the agencies providing financial support for this * |
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| 13 | // * work make any representation or warranty, express or implied, * |
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| 14 | // * regarding this software system or assume any liability for its * |
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| 15 | // * use. Please see the license in the file LICENSE and URL above * |
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| 16 | // * for the full disclaimer and the limitation of liability. * |
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| 17 | // * * |
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| 18 | // * This code implementation is the result of the scientific and * |
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| 19 | // * technical work of the GEANT4 collaboration. * |
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| 20 | // * By using, copying, modifying or distributing the software (or * |
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| 21 | // * any work based on the software) you agree to acknowledge its * |
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| 22 | // * use in resulting scientific publications, and indicate your * |
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| 23 | // * acceptance of all terms of the Geant4 Software license. * |
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| 24 | // ******************************************************************** |
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| 25 | // |
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| 26 | // |
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[1196] | 27 | // $Id: G4N15GEMProbability.cc,v 1.6 2009/09/15 12:54:17 vnivanch Exp $ |
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[1228] | 28 | // GEANT4 tag $Name: geant4-09-03 $ |
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[819] | 29 | // |
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| 30 | // Hadronic Process: Nuclear De-excitations |
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| 31 | // by V. Lara (Nov 1999) |
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| 32 | // |
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| 33 | |
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| 34 | |
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| 35 | #include "G4N15GEMProbability.hh" |
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| 36 | |
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| 37 | G4N15GEMProbability::G4N15GEMProbability() : |
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| 38 | G4GEMProbability(15,7,1.0/2.0) // A,Z,Spin |
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| 39 | { |
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| 40 | ExcitEnergies.push_back(5270.40*keV); |
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| 41 | ExcitSpins.push_back(5.0/2.0); |
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| 42 | ExcitLifetimes.push_back(1.80e-12*s); |
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| 43 | |
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| 44 | ExcitEnergies.push_back(5298.87*keV); |
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| 45 | ExcitSpins.push_back(1.0/2.0); |
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| 46 | ExcitLifetimes.push_back(1.7E-14*s); |
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| 47 | |
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| 48 | ExcitEnergies.push_back(6323.85*keV); |
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| 49 | ExcitSpins.push_back(3.0/2.0); |
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| 50 | ExcitLifetimes.push_back(0.15E-15*s); |
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| 51 | |
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| 52 | ExcitEnergies.push_back(7155.36*keV); |
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| 53 | ExcitSpins.push_back(5.0/2.0); |
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| 54 | ExcitLifetimes.push_back(0.019e-12*s); |
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| 55 | |
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| 56 | ExcitEnergies.push_back(7301.09*keV); |
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| 57 | ExcitSpins.push_back(3.0/2.0); |
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| 58 | ExcitLifetimes.push_back(0.17E-15*s); |
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| 59 | |
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| 60 | ExcitEnergies.push_back(7567.1*keV); |
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| 61 | ExcitSpins.push_back(7.0/2.0); |
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| 62 | ExcitLifetimes.push_back(0.040e-12*s); |
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| 63 | |
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| 64 | ExcitEnergies.push_back(8312.79*keV); |
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| 65 | ExcitSpins.push_back(1.0/2.0); |
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| 66 | ExcitLifetimes.push_back(0.014e-12*s); |
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| 67 | |
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| 68 | ExcitEnergies.push_back(8571.4*keV); |
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| 69 | ExcitSpins.push_back(3.0/2.0); |
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| 70 | ExcitLifetimes.push_back(0.07e-12*s); |
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| 71 | |
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| 72 | ExcitEnergies.push_back(9050.0*keV); |
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| 73 | ExcitSpins.push_back(1.0/2.0); |
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| 74 | ExcitLifetimes.push_back(0.07e-12*s); |
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| 75 | |
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| 76 | ExcitEnergies.push_back(9152.24*keV); |
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| 77 | ExcitSpins.push_back(3.0/2.0); |
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| 78 | ExcitLifetimes.push_back(0.028e-12*s); |
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| 79 | |
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| 80 | ExcitEnergies.push_back(9155.27*keV); |
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| 81 | ExcitSpins.push_back(5.0/2.0); |
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| 82 | ExcitLifetimes.push_back(0.007e-12*s); |
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| 83 | |
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| 84 | ExcitEnergies.push_back(9225*keV); |
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| 85 | ExcitSpins.push_back(1.0/2.0); |
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| 86 | ExcitLifetimes.push_back(0.09e-12*s); |
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| 87 | |
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| 88 | ExcitEnergies.push_back(9829*keV); |
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| 89 | ExcitSpins.push_back(7.0/2.0); |
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| 90 | ExcitLifetimes.push_back(0.13e-12*s); |
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| 91 | |
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| 92 | ExcitEnergies.push_back(9928*keV); |
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| 93 | ExcitSpins.push_back(3.0/2.0); |
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| 94 | ExcitLifetimes.push_back(0.07e-12*s); |
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| 95 | |
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| 96 | ExcitEnergies.push_back(10449.7*keV); |
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| 97 | ExcitSpins.push_back(5.0/2.0); |
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| 98 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 99 | |
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| 100 | ExcitEnergies.push_back(10701.9*keV); |
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| 101 | ExcitSpins.push_back(3.0/2.0); |
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| 102 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.2*keV)); |
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| 103 | |
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| 104 | ExcitEnergies.push_back(10804*keV); |
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| 105 | ExcitSpins.push_back(3.0/2.0); |
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| 106 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1E-3*keV)); |
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| 107 | |
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| 108 | ExcitEnergies.push_back(11235*keV); |
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| 109 | ExcitSpins.push_back(3.0/2.0); |
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| 110 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.3*keV)); |
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| 111 | |
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| 112 | ExcitEnergies.push_back(11292.9*keV); |
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| 113 | ExcitSpins.push_back(1.0/2.0); |
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| 114 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8*keV)); |
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| 115 | |
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| 116 | ExcitEnergies.push_back(11437.5*keV); |
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| 117 | ExcitSpins.push_back(1.0/2.0); |
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| 118 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41.4*keV)); |
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| 119 | |
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| 120 | ExcitEnergies.push_back(11615*keV); |
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| 121 | ExcitSpins.push_back(1.0/2.0); |
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| 122 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(405*keV)); |
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| 123 | |
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| 124 | ExcitEnergies.push_back(11778*keV); |
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| 125 | ExcitSpins.push_back(3.0/2.0); |
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| 126 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV)); |
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| 127 | |
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| 128 | ExcitEnergies.push_back(11876*keV); |
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| 129 | ExcitSpins.push_back(3.0/2.0); |
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| 130 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25*keV)); |
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| 131 | |
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| 132 | ExcitEnergies.push_back(11942*keV); |
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| 133 | ExcitSpins.push_back(11.0/2.0); |
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| 134 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0*keV)); |
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| 135 | |
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| 136 | ExcitEnergies.push_back(11965*keV); |
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| 137 | ExcitSpins.push_back(1.0/2.0); |
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| 138 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(17*keV)); |
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| 139 | |
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| 140 | ExcitEnergies.push_back(12095*keV); |
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| 141 | ExcitSpins.push_back(5.0/2.0); |
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| 142 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(14*keV)); |
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| 143 | |
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| 144 | ExcitEnergies.push_back(12145*keV); |
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| 145 | ExcitSpins.push_back(3.0/2.0); |
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| 146 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(47*keV)); |
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| 147 | |
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| 148 | ExcitEnergies.push_back(12327*keV); |
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| 149 | ExcitSpins.push_back(5.0/2.0); |
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| 150 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(22*keV)); |
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| 151 | |
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| 152 | ExcitEnergies.push_back(12493*keV); |
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| 153 | ExcitSpins.push_back(5.0/2.0); |
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| 154 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV)); |
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| 155 | |
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| 156 | ExcitEnergies.push_back(12522*keV); |
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| 157 | ExcitSpins.push_back(5.0/2.0); |
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| 158 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(58*keV)); |
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| 159 | |
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| 160 | ExcitEnergies.push_back(12920*keV); |
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| 161 | ExcitSpins.push_back(3.0/2.0); |
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| 162 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(56*keV)); |
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| 163 | |
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| 164 | ExcitEnergies.push_back(12940*keV); |
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| 165 | ExcitSpins.push_back(5.0/2.0); |
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| 166 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(81*keV)); |
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| 167 | |
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| 168 | ExcitEnergies.push_back(13173*keV); |
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| 169 | ExcitSpins.push_back(9.0/2.0); |
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| 170 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7*keV)); |
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| 171 | |
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| 172 | ExcitEnergies.push_back(13362*keV); |
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| 173 | ExcitSpins.push_back(3.0/2.0); |
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| 174 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(16*keV)); |
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| 175 | |
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| 176 | ExcitEnergies.push_back(13390*keV); |
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| 177 | ExcitSpins.push_back(3.0/2.0); |
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| 178 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(56*keV)); |
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| 179 | |
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| 180 | ExcitEnergies.push_back(13537*keV); |
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| 181 | ExcitSpins.push_back(3.0/2.0); |
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| 182 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(85*keV)); |
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| 183 | |
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| 184 | ExcitEnergies.push_back(13608*keV); |
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| 185 | ExcitSpins.push_back(5.0/2.0); |
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| 186 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18*keV)); |
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| 187 | |
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| 188 | ExcitEnergies.push_back(13612*keV); |
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| 189 | ExcitSpins.push_back(1.0/2.0); |
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| 190 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90*keV)); |
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| 191 | |
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| 192 | ExcitEnergies.push_back(13840*keV); |
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| 193 | ExcitSpins.push_back(3.0/2.0); |
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| 194 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(75*keV)); |
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| 195 | |
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| 196 | ExcitEnergies.push_back(13900*keV); |
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| 197 | ExcitSpins.push_back(1.0/2.0); |
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| 198 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(930*keV)); |
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| 199 | |
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| 200 | ExcitEnergies.push_back(14100*keV); |
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| 201 | ExcitSpins.push_back(3.0/2.0); |
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| 202 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 203 | |
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| 204 | ExcitEnergies.push_back(14162*keV); |
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| 205 | ExcitSpins.push_back(3.0/2.0); |
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| 206 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(27*keV)); |
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| 207 | |
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| 208 | ExcitEnergies.push_back(14240*keV); |
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| 209 | ExcitSpins.push_back(5.0/2.0); |
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| 210 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); |
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| 211 | |
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| 212 | ExcitEnergies.push_back(14380*keV); |
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| 213 | ExcitSpins.push_back(7.0/2.0); |
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| 214 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 215 | |
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| 216 | ExcitEnergies.push_back(16667*keV); |
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| 217 | ExcitSpins.push_back(3.0/2.0); |
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| 218 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90*keV)); |
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| 219 | |
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| 220 | ExcitEnergies.push_back(16850*keV); |
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| 221 | ExcitSpins.push_back(5.0/2.0); |
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| 222 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110*keV)); |
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| 223 | |
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| 224 | ExcitEnergies.push_back(19160*keV); |
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| 225 | ExcitSpins.push_back(1.0/2.0); |
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| 226 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(130*keV)); |
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| 227 | |
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| 228 | ExcitEnergies.push_back(19500*keV); |
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| 229 | ExcitSpins.push_back(3.0/2.0); |
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| 230 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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| 231 | |
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| 232 | ExcitEnergies.push_back(20500*keV); |
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| 233 | ExcitSpins.push_back(3.0/2.0); |
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| 234 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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| 235 | |
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| 236 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 237 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 238 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 239 | } |
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| 240 | |
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| 241 | |
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| 242 | G4N15GEMProbability::G4N15GEMProbability(const G4N15GEMProbability &) : G4GEMProbability() |
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| 243 | { |
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| 244 | throw G4HadronicException(__FILE__, __LINE__, "G4N15GEMProbability::copy_constructor meant to not be accessable"); |
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| 245 | } |
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| 246 | |
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| 247 | |
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| 248 | |
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| 249 | |
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| 250 | const G4N15GEMProbability & G4N15GEMProbability:: |
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| 251 | operator=(const G4N15GEMProbability &) |
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| 252 | { |
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| 253 | throw G4HadronicException(__FILE__, __LINE__, "G4N15GEMProbability::operator= meant to not be accessable"); |
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| 254 | return *this; |
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| 255 | } |
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| 256 | |
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| 257 | |
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| 258 | G4bool G4N15GEMProbability::operator==(const G4N15GEMProbability &) const |
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| 259 | { |
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| 260 | return false; |
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| 261 | } |
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| 262 | |
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| 263 | G4bool G4N15GEMProbability::operator!=(const G4N15GEMProbability &) const |
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| 264 | { |
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| 265 | return true; |
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| 266 | } |
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| 267 | |
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| 268 | |
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| 269 | |
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