[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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| 27 | // $Id: G4O15GEMProbability.cc,v 1.5 2006/06/29 20:23:25 gunter Exp $ |
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[962] | 28 | // GEANT4 tag $Name: geant4-09-02-ref-02 $ |
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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 "G4O15GEMProbability.hh" |
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| 36 | |
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| 37 | G4O15GEMProbability::G4O15GEMProbability() : |
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| 38 | G4GEMProbability(15,8,1.0/2.0) // A,Z,Spin |
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| 39 | { |
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| 40 | |
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| 41 | ExcitEnergies.push_back(5183.0*keV); |
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| 42 | ExcitSpins.push_back(1.0/2.0); |
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| 43 | ExcitLifetimes.push_back(0.07*picosecond); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(5240.9*keV); |
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| 46 | ExcitSpins.push_back(5.0/2.0); |
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| 47 | ExcitLifetimes.push_back(2.2*picosecond); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(6176.3*keV); |
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| 50 | ExcitSpins.push_back(3.0/2.0); |
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| 51 | ExcitLifetimes.push_back(33.0E-3*picosecond); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(6793.1*keV); |
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| 54 | ExcitSpins.push_back(3.0/2.0); |
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| 55 | ExcitLifetimes.push_back(19.0E-3*picosecond); |
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| 56 | |
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| 57 | ExcitEnergies.push_back(6859.4*keV); |
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| 58 | ExcitSpins.push_back(5.0/2.0); |
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| 59 | ExcitLifetimes.push_back(0.07*picosecond); |
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| 60 | |
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| 61 | ExcitEnergies.push_back(7556.8*keV); |
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| 62 | ExcitSpins.push_back(1.0/2.0); |
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| 63 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.6*keV)); |
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| 64 | |
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| 65 | ExcitEnergies.push_back(8284.3*keV); |
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| 66 | ExcitSpins.push_back(3.0/2.0); |
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| 67 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.6*keV)); |
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| 68 | |
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| 69 | ExcitEnergies.push_back(8743.0*keV); |
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| 70 | ExcitSpins.push_back(1.0/2.0); |
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| 71 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(32.0*keV)); |
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| 72 | |
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| 73 | ExcitEnergies.push_back(8922.0*keV); |
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| 74 | ExcitSpins.push_back(5.0/2.0); |
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| 75 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); |
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| 76 | |
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| 77 | ExcitEnergies.push_back(8927.0*keV); |
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| 78 | ExcitSpins.push_back(1.0/2.0); |
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| 79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.0*keV)); |
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| 80 | |
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| 81 | ExcitEnergies.push_back(8982.4*keV); |
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| 82 | ExcitSpins.push_back(1.0/2.0); |
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| 83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.9*keV)); |
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| 84 | |
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| 85 | ExcitEnergies.push_back(9487.0*keV); |
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| 86 | ExcitSpins.push_back(5.0/2.0); |
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| 87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.1*keV)); |
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| 88 | |
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| 89 | ExcitEnergies.push_back(9527.0*keV); |
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| 90 | ExcitSpins.push_back(1.0/2.0); |
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| 91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(280.0*keV)); |
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| 92 | |
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| 93 | ExcitEnergies.push_back(9610.0*keV); |
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| 94 | ExcitSpins.push_back(3.0/2.0); |
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| 95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.8*keV)); |
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| 96 | |
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| 97 | ExcitEnergies.push_back(9662.0*keV); |
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| 98 | ExcitSpins.push_back(7.0/2.0); |
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| 99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.0*keV)); |
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| 100 | |
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| 101 | ExcitEnergies.push_back(9720.0*keV); |
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| 102 | ExcitSpins.push_back(1.0/2.0); |
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| 103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1185.0*keV)); |
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| 104 | |
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| 105 | ExcitEnergies.push_back(10291.0*keV); |
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| 106 | ExcitSpins.push_back(5.0/2.0); |
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| 107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0*keV)); |
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| 108 | |
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| 109 | ExcitEnergies.push_back(10296.0*keV); |
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| 110 | ExcitSpins.push_back(5.0/2.0); |
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| 111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV)); |
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| 112 | |
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| 113 | ExcitEnergies.push_back(10478.0*keV); |
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| 114 | ExcitSpins.push_back(3.0/2.0); |
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| 115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.0*keV)); |
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| 116 | |
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| 117 | ExcitEnergies.push_back(10506.0*keV); |
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| 118 | ExcitSpins.push_back(3.0/2.0); |
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| 119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140.0*keV)); |
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| 120 | |
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| 121 | ExcitEnergies.push_back(10917.0*keV); |
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| 122 | ExcitSpins.push_back(7.0/2.0); |
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| 123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90.0*keV)); |
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| 124 | |
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| 125 | ExcitEnergies.push_back(10938.0*keV); |
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| 126 | ExcitSpins.push_back(1.0/2.0); |
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| 127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(99.0*keV)); |
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| 128 | |
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| 129 | ExcitEnergies.push_back(11025.0*keV); |
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| 130 | ExcitSpins.push_back(1.0/2.0); |
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| 131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.0*keV)); |
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| 132 | |
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| 133 | ExcitEnergies.push_back(11218.0*keV); |
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| 134 | ExcitSpins.push_back(3.0/2.0); |
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| 135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV)); |
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| 136 | |
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| 137 | ExcitEnergies.push_back(11569.0*keV); |
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| 138 | ExcitSpins.push_back(5.0/2.0); |
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| 139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20.0*keV)); |
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| 140 | |
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| 141 | ExcitEnergies.push_back(11616.0*keV); |
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| 142 | ExcitSpins.push_back(3.0/2.0); |
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| 143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80.0*keV)); |
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| 144 | |
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| 145 | ExcitEnergies.push_back(11748.0*keV); |
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| 146 | ExcitSpins.push_back(5.0/2.0); |
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| 147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(99.0*keV)); |
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| 148 | |
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| 149 | ExcitEnergies.push_back(11846.0*keV); |
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| 150 | ExcitSpins.push_back(5.0/2.0); |
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| 151 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
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| 152 | |
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| 153 | ExcitEnergies.push_back(11980.0*keV); |
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| 154 | ExcitSpins.push_back(5.0/2.0); |
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| 155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20.0*keV)); |
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| 156 | |
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| 157 | ExcitEnergies.push_back(12129.0*keV); |
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| 158 | ExcitSpins.push_back(5.0/2.0); |
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| 159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
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| 160 | |
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| 161 | ExcitEnergies.push_back(12471.0*keV); |
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| 162 | ExcitSpins.push_back(5.0/2.0); |
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| 163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(77.0*keV)); |
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| 164 | |
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| 165 | ExcitEnergies.push_back(12835.0*keV); |
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| 166 | ExcitSpins.push_back(1.0/2.0); |
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| 167 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(16.0*keV)); |
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| 168 | |
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| 169 | ExcitEnergies.push_back(13450.0*keV); |
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| 170 | ExcitSpins.push_back(1.0/2.0); |
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| 171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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| 172 | |
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| 173 | ExcitEnergies.push_back(14030.0*keV); |
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| 174 | ExcitSpins.push_back(1.0/2.0); |
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| 175 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(160.0*keV)); |
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| 176 | |
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| 177 | ExcitEnergies.push_back(14270.0*keV); |
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| 178 | ExcitSpins.push_back(1.0/2.0); |
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| 179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340.0*keV)); |
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| 180 | |
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| 181 | ExcitEnergies.push_back(14465.0*keV); |
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| 182 | ExcitSpins.push_back(3.0/2.0); |
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| 183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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| 184 | |
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| 185 | ExcitEnergies.push_back(15100.0*keV); |
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| 186 | ExcitSpins.push_back(1.0/2.0); |
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| 187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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| 188 | |
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| 189 | ExcitEnergies.push_back(15900.0*keV); |
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| 190 | ExcitSpins.push_back(1.0/2.0); |
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| 191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(350.0*keV)); |
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| 192 | |
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| 193 | ExcitEnergies.push_back(16430.0*keV); |
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| 194 | ExcitSpins.push_back(1.0/2.0); |
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| 195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(560.0*keV)); |
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| 196 | |
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| 197 | ExcitEnergies.push_back(16900.0*keV); |
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| 198 | ExcitSpins.push_back(1.0/2.0); |
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| 199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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| 200 | |
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| 201 | ExcitEnergies.push_back(17510.0*keV); |
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| 202 | ExcitSpins.push_back(1.0/2.0); |
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| 203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV)); |
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| 204 | |
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| 205 | ExcitEnergies.push_back(17990.0*keV); |
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| 206 | ExcitSpins.push_back(1.0/2.0); |
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| 207 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
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| 208 | |
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| 209 | ExcitEnergies.push_back(18400.0*keV); |
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| 210 | ExcitSpins.push_back(1.0/2.0); |
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| 211 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000.0*keV)); |
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| 212 | |
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| 213 | ExcitEnergies.push_back(20500.0*keV); |
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| 214 | ExcitSpins.push_back(1.0/2.0); |
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| 215 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV)); |
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| 216 | |
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| 217 | ExcitEnergies.push_back(22000.0*keV); |
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| 218 | ExcitSpins.push_back(1.0/2.0); |
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| 219 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV)); |
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| 220 | |
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| 221 | ExcitEnergies.push_back(26000.0*keV); |
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| 222 | ExcitSpins.push_back(13.0/2.0); |
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| 223 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV)); |
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| 224 | |
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| 225 | ExcitEnergies.push_back(28000.0*keV); |
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| 226 | ExcitSpins.push_back(9.0/2.0); |
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| 227 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2500.0*keV)); |
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| 228 | |
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| 229 | |
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| 230 | } |
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| 231 | |
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| 232 | |
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| 233 | G4O15GEMProbability::G4O15GEMProbability(const G4O15GEMProbability &) : G4GEMProbability() |
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| 234 | { |
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| 235 | throw G4HadronicException(__FILE__, __LINE__, "G4O15GEMProbability::copy_constructor meant to not be accessable"); |
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| 236 | } |
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| 237 | |
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| 238 | |
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| 239 | |
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| 240 | |
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| 241 | const G4O15GEMProbability & G4O15GEMProbability:: |
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| 242 | operator=(const G4O15GEMProbability &) |
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| 243 | { |
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| 244 | throw G4HadronicException(__FILE__, __LINE__, "G4O15GEMProbability::operator= meant to not be accessable"); |
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| 245 | return *this; |
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| 246 | } |
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| 247 | |
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| 248 | |
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| 249 | G4bool G4O15GEMProbability::operator==(const G4O15GEMProbability &) const |
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| 250 | { |
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| 251 | return false; |
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| 252 | } |
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| 253 | |
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| 254 | G4bool G4O15GEMProbability::operator!=(const G4O15GEMProbability &) const |
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| 255 | { |
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| 256 | return true; |
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| 257 | } |
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| 258 | |
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| 259 | |
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| 260 | |
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