[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: G4N14GEMProbability.cc,v 1.5 2006/06/29 20:22:47 gunter Exp $ |
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[1007] | 28 | // GEANT4 tag $Name: geant4-09-02 $ |
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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 "G4N14GEMProbability.hh" |
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| 36 | |
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| 37 | G4N14GEMProbability::G4N14GEMProbability() : |
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| 38 | G4GEMProbability(14,7,1.0) // A,Z,Spin |
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| 39 | { |
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| 40 | |
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| 41 | ExcitEnergies.push_back(2312.87*keV); |
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| 42 | ExcitSpins.push_back(0.0); |
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| 43 | ExcitLifetimes.push_back(60e-15*s); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(3947.8*keV); |
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| 46 | ExcitSpins.push_back(1.0); |
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| 47 | ExcitLifetimes.push_back(3.1e-15*s); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(4915.0*keV); |
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| 50 | ExcitSpins.push_back(0.0); |
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| 51 | ExcitLifetimes.push_back(5.3e-15*s); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(5105.87*keV); |
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| 54 | ExcitSpins.push_back(2.0); |
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| 55 | ExcitLifetimes.push_back(8.6e-12*s); |
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| 56 | |
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| 57 | ExcitEnergies.push_back(5689.6*keV); |
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| 58 | ExcitSpins.push_back(1.0); |
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| 59 | ExcitLifetimes.push_back(6.9e-15*s); |
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| 60 | |
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| 61 | ExcitEnergies.push_back(5832.4*keV); |
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| 62 | ExcitSpins.push_back(3.0); |
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| 63 | ExcitLifetimes.push_back(12.5e-12*s); |
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| 64 | |
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| 65 | ExcitEnergies.push_back(6203.5*keV); |
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| 66 | ExcitSpins.push_back(1.0); |
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| 67 | ExcitLifetimes.push_back(86e-15*s); |
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| 68 | |
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| 69 | ExcitEnergies.push_back(6444.4*keV); |
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| 70 | ExcitSpins.push_back(3.0); |
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| 71 | ExcitLifetimes.push_back(435e-15*s); |
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| 72 | |
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| 73 | ExcitEnergies.push_back(7027.9*keV); |
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| 74 | ExcitSpins.push_back(2.0); |
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| 75 | ExcitLifetimes.push_back(3.7e-15*s); |
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| 76 | |
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| 77 | ExcitEnergies.push_back(7966.6*keV); |
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| 78 | ExcitSpins.push_back(2.0); |
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| 79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.5E-3*keV)); |
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| 80 | |
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| 81 | ExcitEnergies.push_back(8487.7*keV); |
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| 82 | ExcitSpins.push_back(4.0); |
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| 83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(27E-6*keV)); |
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| 84 | |
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| 85 | ExcitEnergies.push_back(8618*keV); |
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| 86 | ExcitSpins.push_back(0.0); |
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| 87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7.0*keV)); |
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| 88 | |
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| 89 | ExcitEnergies.push_back(8790*keV); |
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| 90 | ExcitSpins.push_back(0.0); |
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| 91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(460*keV)); |
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| 92 | |
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| 93 | ExcitEnergies.push_back(8909.1*keV); |
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| 94 | ExcitSpins.push_back(3.0); |
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| 95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19.7*keV)); |
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| 96 | |
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| 97 | ExcitEnergies.push_back(8961.2 *keV); |
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| 98 | ExcitSpins.push_back(5.0); |
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| 99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7E-6*keV)); |
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| 100 | |
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| 101 | ExcitEnergies.push_back(8979*keV); |
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| 102 | ExcitSpins.push_back(2.0); |
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| 103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8*keV)); |
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| 104 | |
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| 105 | ExcitEnergies.push_back(9129*keV); |
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| 106 | ExcitSpins.push_back(2.0); |
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| 107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1*keV)); |
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| 108 | |
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| 109 | ExcitEnergies.push_back(9170.8*keV); |
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| 110 | ExcitSpins.push_back(2.0); |
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| 111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.074*keV)); |
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| 112 | |
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| 113 | ExcitEnergies.push_back(9386.0*keV); |
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| 114 | ExcitSpins.push_back(3.0); |
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| 115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15.6 *keV)); |
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| 116 | |
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| 117 | ExcitEnergies.push_back(9509*keV); |
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| 118 | ExcitSpins.push_back(2.0); |
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| 119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41*keV)); |
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| 120 | |
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| 121 | ExcitEnergies.push_back(9703 *keV); |
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| 122 | ExcitSpins.push_back(1.0); |
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| 123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV)); |
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| 124 | |
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| 125 | ExcitEnergies.push_back(10063*keV); |
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| 126 | ExcitSpins.push_back(3.0); |
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| 127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10*keV)); |
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| 128 | |
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| 129 | ExcitEnergies.push_back(10101*keV); |
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| 130 | ExcitSpins.push_back(1.0); |
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| 131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); |
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| 132 | |
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| 133 | ExcitEnergies.push_back(10228*keV); |
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| 134 | ExcitSpins.push_back(1.0); |
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| 135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80*keV)); |
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| 136 | |
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| 137 | ExcitEnergies.push_back(10434*keV); |
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| 138 | ExcitSpins.push_back(2.0); |
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| 139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(33*keV)); |
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| 140 | |
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| 141 | ExcitEnergies.push_back(10540*keV); |
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| 142 | ExcitSpins.push_back(1.0); |
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| 143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); |
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| 144 | |
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| 145 | ExcitEnergies.push_back(10811*keV); |
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| 146 | ExcitSpins.push_back(5.0); |
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| 147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.39*eV)); |
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| 148 | |
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| 149 | ExcitEnergies.push_back(11050*keV); |
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| 150 | ExcitSpins.push_back(3.0); |
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| 151 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2*keV)); |
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| 152 | |
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| 153 | ExcitEnergies.push_back(11070*keV); |
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| 154 | ExcitSpins.push_back(1.0); |
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| 155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 156 | |
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| 157 | ExcitEnergies.push_back(11240*keV); |
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| 158 | ExcitSpins.push_back(3.0); |
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| 159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(20*keV)); |
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| 160 | |
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| 161 | ExcitEnergies.push_back(11290*keV); |
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| 162 | ExcitSpins.push_back(2.0); |
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| 163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); |
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| 164 | |
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| 165 | ExcitEnergies.push_back(11357*keV); |
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| 166 | ExcitSpins.push_back(1.0); |
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| 167 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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| 168 | |
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| 169 | ExcitEnergies.push_back(11513.6*keV); |
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| 170 | ExcitSpins.push_back(3.0); |
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| 171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(7.0*keV)); |
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| 172 | |
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| 173 | ExcitEnergies.push_back(11680*keV); |
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| 174 | ExcitSpins.push_back(2.0); |
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| 175 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); |
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| 176 | |
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| 177 | ExcitEnergies.push_back(11741*keV); |
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| 178 | ExcitSpins.push_back(2.0); |
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| 179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40*keV)); |
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| 180 | |
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| 181 | ExcitEnergies.push_back(11761*keV); |
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| 182 | ExcitSpins.push_back(4.0); |
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| 183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(78*keV)); |
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| 184 | |
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| 185 | ExcitEnergies.push_back(11807*keV); |
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| 186 | ExcitSpins.push_back(2.0); |
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| 187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(119*keV)); |
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| 188 | |
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| 189 | ExcitEnergies.push_back(11874*keV); |
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| 190 | ExcitSpins.push_back(2.0); |
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| 191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(101*keV)); |
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| 192 | |
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| 193 | ExcitEnergies.push_back(12200*keV); |
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| 194 | ExcitSpins.push_back(2.0); |
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| 195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 196 | |
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| 197 | ExcitEnergies.push_back(12408*keV); |
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| 198 | ExcitSpins.push_back(3.0); |
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| 199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(37*keV)); |
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| 200 | |
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| 201 | ExcitEnergies.push_back(12418*keV); |
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| 202 | ExcitSpins.push_back(4.0); |
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| 203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(41*keV)); |
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| 204 | |
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| 205 | ExcitEnergies.push_back(12594*keV); |
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| 206 | ExcitSpins.push_back(3.0); |
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| 207 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(48*keV)); |
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| 208 | |
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| 209 | ExcitEnergies.push_back(12688*keV); |
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| 210 | ExcitSpins.push_back(3.0); |
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| 211 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(22*keV)); |
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| 212 | |
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| 213 | ExcitEnergies.push_back(12792*keV); |
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| 214 | ExcitSpins.push_back(4.0); |
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| 215 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18*keV)); |
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| 216 | |
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| 217 | ExcitEnergies.push_back(12819*keV); |
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| 218 | ExcitSpins.push_back(4.0); |
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| 219 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8*keV)); |
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| 220 | |
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| 221 | ExcitEnergies.push_back(12923*keV); |
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| 222 | ExcitSpins.push_back(4.0); |
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| 223 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25*keV)); |
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| 224 | |
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| 225 | ExcitEnergies.push_back(13166*keV); |
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| 226 | ExcitSpins.push_back(1.0); |
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| 227 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15*keV)); |
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| 228 | |
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| 229 | ExcitEnergies.push_back(13192*keV); |
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| 230 | ExcitSpins.push_back(3.0); |
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| 231 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65*keV)); |
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| 232 | |
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| 233 | ExcitEnergies.push_back(13243*keV); |
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| 234 | ExcitSpins.push_back(2.0); |
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| 235 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(92*keV)); |
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| 236 | |
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| 237 | ExcitEnergies.push_back(13300*keV); |
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| 238 | ExcitSpins.push_back(2.0); |
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| 239 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); |
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| 240 | |
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| 241 | ExcitEnergies.push_back(13656*keV); |
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| 242 | ExcitSpins.push_back(3.0); |
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| 243 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90*keV)); |
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| 244 | |
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| 245 | ExcitEnergies.push_back(13714*keV); |
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| 246 | ExcitSpins.push_back(3.0); |
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| 247 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(105*keV)); |
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| 248 | |
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| 249 | ExcitEnergies.push_back(13710*keV); |
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| 250 | ExcitSpins.push_back(1.0); |
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| 251 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180*keV)); |
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| 252 | |
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| 253 | ExcitEnergies.push_back(14250*keV); |
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| 254 | ExcitSpins.push_back(3.0); |
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| 255 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(420*keV)); |
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| 256 | |
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| 257 | ExcitEnergies.push_back(14660*keV); |
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| 258 | ExcitSpins.push_back(2.0); |
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| 259 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 260 | |
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| 261 | ExcitEnergies.push_back(16800*keV); |
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| 262 | ExcitSpins.push_back(4.0); |
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| 263 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 264 | |
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| 265 | ExcitEnergies.push_back(16910*keV); |
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| 266 | ExcitSpins.push_back(5.0); |
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| 267 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 268 | |
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| 269 | ExcitEnergies.push_back(17170*keV); |
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| 270 | ExcitSpins.push_back(4.0); |
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| 271 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 272 | |
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| 273 | ExcitEnergies.push_back(18100*keV); |
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| 274 | ExcitSpins.push_back(2.0); |
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| 275 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 276 | |
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| 277 | ExcitEnergies.push_back(18100*keV); |
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| 278 | ExcitSpins.push_back(4.0); |
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| 279 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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| 280 | |
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| 281 | ExcitEnergies.push_back(18200*keV); |
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| 282 | ExcitSpins.push_back(3.0); |
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| 283 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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| 284 | |
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| 285 | ExcitEnergies.push_back(18400*keV); |
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| 286 | ExcitSpins.push_back(3.0); |
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| 287 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 288 | |
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| 289 | ExcitEnergies.push_back(18500*keV); |
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| 290 | ExcitSpins.push_back(5.0); |
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| 291 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(60 *keV)); |
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| 292 | |
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| 293 | ExcitEnergies.push_back(18800*keV); |
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| 294 | ExcitSpins.push_back(4.0); |
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| 295 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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| 296 | |
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| 297 | ExcitEnergies.push_back(20100*keV); |
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| 298 | ExcitSpins.push_back(1.0); |
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| 299 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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| 300 | |
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| 301 | ExcitEnergies.push_back(20800*keV); |
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| 302 | ExcitSpins.push_back(5.0); |
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| 303 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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| 304 | |
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| 305 | ExcitEnergies.push_back(20800*keV); |
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| 306 | ExcitSpins.push_back(4.0); |
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| 307 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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| 308 | |
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| 309 | ExcitEnergies.push_back(21300*keV); |
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| 310 | ExcitSpins.push_back(4.0); |
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| 311 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); |
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| 312 | |
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| 313 | ExcitEnergies.push_back(21500*keV); |
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| 314 | ExcitSpins.push_back(3.0); |
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| 315 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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| 316 | |
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| 317 | ExcitEnergies.push_back(21700*keV); |
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| 318 | ExcitSpins.push_back(5.0); |
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| 319 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); |
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| 320 | |
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| 321 | ExcitEnergies.push_back(23000*keV); |
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| 322 | ExcitSpins.push_back(1.0); |
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| 323 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3000*keV)); |
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| 324 | |
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| 325 | ExcitEnergies.push_back(23.3E3*keV); |
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| 326 | ExcitSpins.push_back(5.0); |
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| 327 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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| 328 | |
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| 329 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 330 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 331 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 332 | } |
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| 333 | |
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| 334 | |
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| 335 | G4N14GEMProbability::G4N14GEMProbability(const G4N14GEMProbability &) : G4GEMProbability() |
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| 336 | { |
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| 337 | throw G4HadronicException(__FILE__, __LINE__, "G4N14GEMProbability::copy_constructor meant to not be accessable"); |
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| 338 | } |
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| 339 | |
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| 340 | |
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| 341 | |
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| 342 | |
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| 343 | const G4N14GEMProbability & G4N14GEMProbability:: |
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| 344 | operator=(const G4N14GEMProbability &) |
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| 345 | { |
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| 346 | throw G4HadronicException(__FILE__, __LINE__, "G4N14GEMProbability::operator= meant to not be accessable"); |
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| 347 | return *this; |
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| 348 | } |
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| 349 | |
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| 350 | |
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| 351 | G4bool G4N14GEMProbability::operator==(const G4N14GEMProbability &) const |
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| 352 | { |
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| 353 | return false; |
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| 354 | } |
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| 355 | |
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| 356 | G4bool G4N14GEMProbability::operator!=(const G4N14GEMProbability &) const |
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| 357 | { |
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| 358 | return true; |
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| 359 | } |
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| 360 | |
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| 361 | |
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| 362 | |
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