[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: G4Na22GEMProbability.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 "G4Na22GEMProbability.hh" |
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| 36 | |
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| 37 | G4Na22GEMProbability::G4Na22GEMProbability() : |
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| 38 | G4GEMProbability(22,11,3.0) // A,Z,Spin |
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| 39 | { |
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| 40 | |
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| 41 | ExcitEnergies.push_back(583.03*keV); |
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| 42 | ExcitSpins.push_back(1.0); |
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| 43 | ExcitLifetimes.push_back(244.0e-3*picosecond); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(657.0*keV); |
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| 46 | ExcitSpins.push_back(0.0); |
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| 47 | ExcitLifetimes.push_back(14.0*picosecond); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(890.89*keV); |
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| 50 | ExcitSpins.push_back(4.0); |
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| 51 | ExcitLifetimes.push_back(10.4*picosecond); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(1528.06*keV); |
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| 54 | ExcitSpins.push_back(5.0); |
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| 55 | ExcitLifetimes.push_back(3.40*picosecond); |
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| 56 | |
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| 57 | ExcitEnergies.push_back(1936.9*keV); |
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| 58 | ExcitSpins.push_back(1.0); |
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| 59 | ExcitLifetimes.push_back(3.0e-3*picosecond); |
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| 60 | |
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| 61 | ExcitEnergies.push_back(1951.8*keV); |
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| 62 | ExcitSpins.push_back(2.0); |
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| 63 | ExcitLifetimes.push_back(6.0e-3*picosecond); |
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| 64 | |
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| 65 | ExcitEnergies.push_back(1983.8*keV); |
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| 66 | ExcitSpins.push_back(3.0); |
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| 67 | ExcitLifetimes.push_back(1.59*picosecond); |
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| 68 | |
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| 69 | ExcitEnergies.push_back(2211.5*keV); |
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| 70 | ExcitSpins.push_back(1.0); |
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| 71 | ExcitLifetimes.push_back(14.9*picosecond); |
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| 72 | |
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| 73 | ExcitEnergies.push_back(2571.5*keV); |
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| 74 | ExcitSpins.push_back(2.0); |
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| 75 | ExcitLifetimes.push_back(5.6*picosecond); |
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| 76 | |
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| 77 | ExcitEnergies.push_back(2968.7*keV); |
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| 78 | ExcitSpins.push_back(3.0); |
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| 79 | ExcitLifetimes.push_back(42.0e-3*picosecond); |
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| 80 | |
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| 81 | ExcitEnergies.push_back(3059.6*keV); |
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| 82 | ExcitSpins.push_back(2.0); |
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| 83 | ExcitLifetimes.push_back(28.0e-3*picosecond); |
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| 84 | |
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| 85 | ExcitEnergies.push_back(3519.2*keV); |
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| 86 | ExcitSpins.push_back(3.0); |
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| 87 | ExcitLifetimes.push_back(464.0e-3*picosecond); |
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| 88 | |
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| 89 | ExcitEnergies.push_back(3706.6*keV); |
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| 90 | ExcitSpins.push_back(6.0); |
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| 91 | ExcitLifetimes.push_back(76.0e-3*picosecond); |
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| 92 | |
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| 93 | ExcitEnergies.push_back(3943.5*keV); |
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| 94 | ExcitSpins.push_back(1.0); |
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| 95 | ExcitLifetimes.push_back(6.0e-3*picosecond); |
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| 96 | |
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| 97 | ExcitEnergies.push_back(4071.3*keV); |
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| 98 | ExcitSpins.push_back(4.0); |
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| 99 | ExcitLifetimes.push_back(3.0e-3*picosecond); |
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| 100 | |
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| 101 | ExcitEnergies.push_back(4296.1*keV); |
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| 102 | ExcitSpins.push_back(0.0); |
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| 103 | ExcitLifetimes.push_back(3.5*picosecond); |
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| 104 | |
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| 105 | ExcitEnergies.push_back(4319.0*keV); |
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| 106 | ExcitSpins.push_back(1.0); |
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| 107 | ExcitLifetimes.push_back(30.0e-3*picosecond); |
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| 108 | |
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| 109 | ExcitEnergies.push_back(4360.0*keV); |
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| 110 | ExcitSpins.push_back(2.0); |
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| 111 | ExcitLifetimes.push_back(11.0e-3*picosecond); |
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| 112 | |
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| 113 | ExcitEnergies.push_back(4468.3*keV); |
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| 114 | ExcitSpins.push_back(4.0); |
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| 115 | ExcitLifetimes.push_back(104.0e-3*picosecond); |
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| 116 | |
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| 117 | ExcitEnergies.push_back(4523.8*keV); |
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| 118 | ExcitSpins.push_back(7.0); |
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| 119 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
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| 120 | |
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| 121 | ExcitEnergies.push_back(4582.8*keV); |
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| 122 | ExcitSpins.push_back(2.0); |
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| 123 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
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| 124 | |
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| 125 | ExcitEnergies.push_back(4621.7*keV); |
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| 126 | ExcitSpins.push_back(1.0); |
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| 127 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
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| 128 | |
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| 129 | ExcitEnergies.push_back(4710.0*keV); |
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| 130 | ExcitSpins.push_back(5.0); |
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| 131 | ExcitLifetimes.push_back(42.0e-3*picosecond); |
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| 132 | |
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| 133 | ExcitEnergies.push_back(4771.0*keV); |
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| 134 | ExcitSpins.push_back(3.0); |
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| 135 | ExcitLifetimes.push_back(69.0*picosecond); |
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| 136 | |
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| 137 | ExcitEnergies.push_back(5062.4*keV); |
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| 138 | ExcitSpins.push_back(2.0); |
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| 139 | ExcitLifetimes.push_back(14.0e-3*picosecond); |
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| 140 | |
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| 141 | ExcitEnergies.push_back(5100.6*keV); |
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| 142 | ExcitSpins.push_back(4.0); |
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| 143 | ExcitLifetimes.push_back(38.0e-3*picosecond); |
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| 144 | |
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| 145 | ExcitEnergies.push_back(5167.0*keV); |
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| 146 | ExcitSpins.push_back(1.0); |
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| 147 | ExcitLifetimes.push_back(69.0*picosecond); |
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| 148 | |
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| 149 | |
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| 150 | ExcitEnergies.push_back(7153.0*keV); |
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| 151 | ExcitSpins.push_back(3.0); |
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| 152 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 153 | |
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| 154 | ExcitEnergies.push_back(7221.0*keV); |
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| 155 | ExcitSpins.push_back(2.0); |
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| 156 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.4*keV)); |
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| 157 | |
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| 158 | ExcitEnergies.push_back(7241.0*keV); |
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| 159 | ExcitSpins.push_back(2.0); |
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| 160 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.3*keV)); |
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| 161 | |
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| 162 | ExcitEnergies.push_back(7279.0*keV); |
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| 163 | ExcitSpins.push_back(1.0); |
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| 164 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 165 | |
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| 166 | ExcitEnergies.push_back(7280.0*keV); |
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| 167 | ExcitSpins.push_back(4.0); |
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| 168 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.5*keV)); |
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| 169 | |
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| 170 | ExcitEnergies.push_back(7361.0*keV); |
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| 171 | ExcitSpins.push_back(3.0); |
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| 172 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.0*keV)); |
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| 173 | |
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| 174 | ExcitEnergies.push_back(7373.0*keV); |
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| 175 | ExcitSpins.push_back(2.0); |
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| 176 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 177 | |
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| 178 | ExcitEnergies.push_back(7379.2*keV); |
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| 179 | ExcitSpins.push_back(2.0); |
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| 180 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 181 | |
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| 182 | ExcitEnergies.push_back(7402.0*keV); |
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| 183 | ExcitSpins.push_back(1.0); |
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| 184 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.5*keV)); |
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| 185 | |
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| 186 | ExcitEnergies.push_back(7409.6*keV); |
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| 187 | ExcitSpins.push_back(1.0); |
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| 188 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.5*keV)); |
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| 189 | |
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| 190 | ExcitEnergies.push_back(7472.6*keV); |
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| 191 | ExcitSpins.push_back(2.0); |
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| 192 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.5*keV)); |
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| 193 | |
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| 194 | ExcitEnergies.push_back(7516.2*keV); |
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| 195 | ExcitSpins.push_back(3.0); |
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| 196 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 197 | |
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| 198 | ExcitEnergies.push_back(7547.9*keV); |
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| 199 | ExcitSpins.push_back(2.0); |
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| 200 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV)); |
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| 201 | |
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| 202 | ExcitEnergies.push_back(7574.4*keV); |
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| 203 | ExcitSpins.push_back(5.0); |
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| 204 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 205 | |
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| 206 | ExcitEnergies.push_back(7600.0*keV); |
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| 207 | ExcitSpins.push_back(2.0); |
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| 208 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.9*keV)); |
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| 209 | |
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| 210 | ExcitEnergies.push_back(7606.0*keV); |
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| 211 | ExcitSpins.push_back(1.0); |
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| 212 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV)); |
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| 213 | |
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| 214 | ExcitEnergies.push_back(7637.0*keV); |
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| 215 | ExcitSpins.push_back(2.0); |
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| 216 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 217 | |
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| 218 | ExcitEnergies.push_back(7684.0*keV); |
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| 219 | ExcitSpins.push_back(2.0); |
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| 220 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 221 | |
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| 222 | ExcitEnergies.push_back(7779.0*keV); |
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| 223 | ExcitSpins.push_back(1.0); |
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| 224 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.8*keV)); |
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| 225 | |
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| 226 | ExcitEnergies.push_back(7801.5*keV); |
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| 227 | ExcitSpins.push_back(1.0); |
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| 228 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.4*keV)); |
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| 229 | |
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| 230 | ExcitEnergies.push_back(7821.9*keV); |
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| 231 | ExcitSpins.push_back(1.0); |
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| 232 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 233 | |
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| 234 | ExcitEnergies.push_back(7890.0*keV); |
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| 235 | ExcitSpins.push_back(3.0); |
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| 236 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 237 | |
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| 238 | ExcitEnergies.push_back(7920.0*keV); |
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| 239 | ExcitSpins.push_back(2.0); |
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| 240 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(17.0*keV)); |
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| 241 | |
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| 242 | ExcitEnergies.push_back(7978.0*keV); |
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| 243 | ExcitSpins.push_back(1.0); |
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| 244 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.0*keV)); |
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| 245 | |
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| 246 | ExcitEnergies.push_back(8019.0*keV); |
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| 247 | ExcitSpins.push_back(4.0); |
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| 248 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.0*keV)); |
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| 249 | |
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| 250 | ExcitEnergies.push_back(8041.0*keV); |
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| 251 | ExcitSpins.push_back(2.0); |
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| 252 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.5*keV)); |
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| 253 | |
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| 254 | ExcitEnergies.push_back(8102.0*keV); |
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| 255 | ExcitSpins.push_back(1.0); |
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| 256 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.8*keV)); |
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| 257 | |
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| 258 | ExcitEnergies.push_back(8108.0*keV); |
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| 259 | ExcitSpins.push_back(3.0); |
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| 260 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.5*keV)); |
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| 261 | |
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| 262 | ExcitEnergies.push_back(8115.0*keV); |
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| 263 | ExcitSpins.push_back(3.0); |
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| 264 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.1*keV)); |
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| 265 | |
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| 266 | ExcitEnergies.push_back(8166.0*keV); |
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| 267 | ExcitSpins.push_back(3.0); |
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| 268 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(22.5*keV)); |
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| 269 | |
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| 270 | ExcitEnergies.push_back(8198.0*keV); |
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| 271 | ExcitSpins.push_back(2.0); |
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| 272 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV)); |
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| 273 | |
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| 274 | ExcitEnergies.push_back(8212.0*keV); |
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| 275 | ExcitSpins.push_back(1.0); |
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| 276 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.1*keV)); |
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| 277 | |
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| 278 | ExcitEnergies.push_back(8234.0*keV); |
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| 279 | ExcitSpins.push_back(1.0); |
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| 280 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV)); |
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| 281 | |
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| 282 | ExcitEnergies.push_back(8288.0*keV); |
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| 283 | ExcitSpins.push_back(0.0); |
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| 284 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.5*keV)); |
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| 285 | |
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| 286 | ExcitEnergies.push_back(8329.0*keV); |
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| 287 | ExcitSpins.push_back(0.0); |
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| 288 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.7*keV)); |
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| 289 | |
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| 290 | ExcitEnergies.push_back(8436.0*keV); |
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| 291 | ExcitSpins.push_back(0.0); |
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| 292 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.4*keV)); |
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| 293 | |
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| 294 | ExcitEnergies.push_back(8497.0*keV); |
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| 295 | ExcitSpins.push_back(1.0); |
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| 296 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(44.0*keV)); |
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| 297 | |
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| 298 | ExcitEnergies.push_back(8538.0*keV); |
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| 299 | ExcitSpins.push_back(0.0); |
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| 300 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(13.2*keV)); |
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| 301 | |
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| 302 | ExcitEnergies.push_back(8602.0*keV); |
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| 303 | ExcitSpins.push_back(0.0); |
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| 304 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.2*keV)); |
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| 305 | |
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| 306 | ExcitEnergies.push_back(8637.0*keV); |
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| 307 | ExcitSpins.push_back(0.0); |
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| 308 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV)); |
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| 309 | |
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| 310 | } |
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| 311 | |
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| 312 | |
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| 313 | G4Na22GEMProbability::G4Na22GEMProbability(const G4Na22GEMProbability &) : G4GEMProbability() |
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| 314 | { |
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| 315 | throw G4HadronicException(__FILE__, __LINE__, "G4Na22GEMProbability::copy_constructor meant to not be accessable"); |
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| 316 | } |
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| 317 | |
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| 318 | |
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| 319 | |
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| 320 | |
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| 321 | const G4Na22GEMProbability & G4Na22GEMProbability:: |
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| 322 | operator=(const G4Na22GEMProbability &) |
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| 323 | { |
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| 324 | throw G4HadronicException(__FILE__, __LINE__, "G4Na22GEMProbability::operator= meant to not be accessable"); |
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| 325 | return *this; |
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| 326 | } |
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| 327 | |
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| 328 | |
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| 329 | G4bool G4Na22GEMProbability::operator==(const G4Na22GEMProbability &) const |
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| 330 | { |
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| 331 | return false; |
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| 332 | } |
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| 333 | |
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| 334 | G4bool G4Na22GEMProbability::operator!=(const G4Na22GEMProbability &) const |
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| 335 | { |
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| 336 | return true; |
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| 337 | } |
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| 338 | |
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| 339 | |
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| 340 | |
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