| 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: G4C12GEMProbability.cc,v 1.6 2009/09/15 12:54:16 vnivanch Exp $ |
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| 28 | // GEANT4 tag $Name: geant4-09-03-ref-09 $ |
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| 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 "G4C12GEMProbability.hh" |
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| 36 | |
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| 37 | G4C12GEMProbability::G4C12GEMProbability() : |
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| 38 | G4GEMProbability(12,6,0.0) // A,Z,Spin |
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| 39 | { |
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| 40 | |
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| 41 | ExcitEnergies.push_back(4438.91*keV); |
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| 42 | ExcitSpins.push_back(2.0); |
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| 43 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.8e-3*eV)); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(7654.2*keV); |
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| 46 | ExcitSpins.push_back(0.0); |
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| 47 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.5*keV)); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(9641*keV); |
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| 50 | ExcitSpins.push_back(3.0); |
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| 51 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(34*keV)); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(1.03E+4*keV); |
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| 54 | ExcitSpins.push_back(0.0); |
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| 55 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0e3*keV)); |
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| 56 | |
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| 57 | ExcitEnergies.push_back(10844*keV); |
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| 58 | ExcitSpins.push_back(1.0); |
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| 59 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(315*keV)); |
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| 60 | |
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| 61 | ExcitEnergies.push_back(1.116E+4*keV); |
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| 62 | ExcitSpins.push_back(2.0); |
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| 63 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(430*keV)); |
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| 64 | |
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| 65 | ExcitEnergies.push_back(1.1828E+4*keV); |
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| 66 | ExcitSpins.push_back(2.0); |
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| 67 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260*keV)); |
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| 68 | |
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| 69 | ExcitEnergies.push_back(12710*keV); |
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| 70 | ExcitSpins.push_back(1.0); |
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| 71 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(18.1*eV)); |
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| 72 | |
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| 73 | ExcitEnergies.push_back(13352*keV); |
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| 74 | ExcitSpins.push_back(2.0); |
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| 75 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(375*keV)); |
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| 76 | |
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| 77 | ExcitEnergies.push_back(14083*keV); |
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| 78 | ExcitSpins.push_back(4.0); |
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| 79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(258*keV)); |
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| 80 | |
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| 81 | ExcitEnergies.push_back(15110*keV); |
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| 82 | ExcitSpins.push_back(1.0); |
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| 83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(42*eV)); |
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| 84 | |
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| 85 | ExcitEnergies.push_back(16106.7*keV); |
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| 86 | ExcitSpins.push_back(2.0); |
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| 87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5.2*keV)); |
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| 88 | |
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| 89 | ExcitEnergies.push_back(16.57E+3*keV); |
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| 90 | ExcitSpins.push_back(2.0); |
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| 91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 92 | |
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| 93 | ExcitEnergies.push_back(17.23E+3*keV); |
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| 94 | ExcitSpins.push_back(1.0); |
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| 95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1150*keV)); |
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| 96 | |
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| 97 | ExcitEnergies.push_back(17.76E+3*keV); |
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| 98 | ExcitSpins.push_back(0.0); |
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| 99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(80*keV)); |
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| 100 | |
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| 101 | ExcitEnergies.push_back(18.13E+3*keV); |
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| 102 | ExcitSpins.push_back(1.0); |
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| 103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600*keV)); |
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| 104 | |
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| 105 | ExcitEnergies.push_back(18.27E+3*keV); |
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| 106 | ExcitSpins.push_back(4.0); |
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| 107 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 108 | |
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| 109 | ExcitEnergies.push_back(18.38E+3*keV); |
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| 110 | ExcitSpins.push_back(3.0); |
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| 111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(220*keV)); |
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| 112 | |
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| 113 | ExcitEnergies.push_back(18.39E+3*keV); |
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| 114 | ExcitSpins.push_back(2.0); |
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| 115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(43*keV)); |
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| 116 | |
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| 117 | ExcitEnergies.push_back(18.6E+3*keV); |
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| 118 | ExcitSpins.push_back(3.0); |
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| 119 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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| 120 | |
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| 121 | ExcitEnergies.push_back(18.80E+3*keV); |
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| 122 | ExcitSpins.push_back(2.0); |
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| 123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 124 | |
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| 125 | ExcitEnergies.push_back(19.2E+3*keV); |
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| 126 | ExcitSpins.push_back(1.0); |
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| 127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1100*keV)); |
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| 128 | |
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| 129 | ExcitEnergies.push_back(19.39E+3*keV); |
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| 130 | ExcitSpins.push_back(2.0); |
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| 131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); |
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| 132 | |
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| 133 | ExcitEnergies.push_back(19.55E+3*keV); |
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| 134 | ExcitSpins.push_back(4.0); |
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| 135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(490*keV)); |
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| 136 | |
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| 137 | ExcitEnergies.push_back(19.69E+3*keV); |
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| 138 | ExcitSpins.push_back(1.0); |
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| 139 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); |
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| 140 | |
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| 141 | ExcitEnergies.push_back(20.0E+3*keV); |
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| 142 | ExcitSpins.push_back(2.0); |
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| 143 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100*keV)); |
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| 144 | |
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| 145 | ExcitEnergies.push_back(20.27E+3*keV); |
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| 146 | ExcitSpins.push_back(1.0); |
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| 147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140*keV)); |
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| 148 | |
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| 149 | ExcitEnergies.push_back(20.5E+3*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)/(180*keV)); |
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| 152 | |
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| 153 | ExcitEnergies.push_back(20.62E+3*keV); |
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| 154 | ExcitSpins.push_back(3.0); |
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| 155 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); |
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| 156 | |
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| 157 | ExcitEnergies.push_back(21.60E+3*keV); |
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| 158 | ExcitSpins.push_back(2.0); |
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| 159 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1200*keV)); |
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| 160 | |
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| 161 | ExcitEnergies.push_back(22.0E+3*keV); |
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| 162 | ExcitSpins.push_back(1.0); |
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| 163 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800*keV)); |
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| 164 | |
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| 165 | ExcitEnergies.push_back(22.40E+3*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)/(275*keV)); |
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| 168 | |
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| 169 | ExcitEnergies.push_back(22.65E+3*keV); |
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| 170 | ExcitSpins.push_back(1.0); |
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| 171 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3200*keV)); |
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| 172 | |
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| 173 | ExcitEnergies.push_back(23.04E+3 *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)/(60*keV)); |
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| 176 | |
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| 177 | ExcitEnergies.push_back(23.52E+3*keV); |
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| 178 | ExcitSpins.push_back(1.0); |
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| 179 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(230*keV)); |
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| 180 | |
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| 181 | ExcitEnergies.push_back(23.92E+3*keV); |
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| 182 | ExcitSpins.push_back(1.0); |
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| 183 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400*keV)); |
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| 184 | |
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| 185 | ExcitEnergies.push_back(25.30E+3*keV); |
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| 186 | ExcitSpins.push_back(1.0); |
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| 187 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(510*keV)); |
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| 188 | |
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| 189 | ExcitEnergies.push_back(25.4E+3*keV); |
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| 190 | ExcitSpins.push_back(1.0); |
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| 191 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000*keV)); |
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| 192 | |
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| 193 | ExcitEnergies.push_back(27.0E+3*keV); |
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| 194 | ExcitSpins.push_back(1.0); |
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| 195 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1400*keV)); |
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| 196 | |
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| 197 | ExcitEnergies.push_back(27595.0*keV); |
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| 198 | ExcitSpins.push_back(0.0); |
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| 199 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30*keV)); |
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| 200 | |
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| 201 | ExcitEnergies.push_back(28.2E+3*keV); |
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| 202 | ExcitSpins.push_back(1.0); |
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| 203 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1600*keV)); |
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| 204 | |
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| 205 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 206 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 207 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 208 | } |
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| 209 | |
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| 210 | |
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| 211 | G4C12GEMProbability::G4C12GEMProbability(const G4C12GEMProbability &) : G4GEMProbability() |
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| 212 | { |
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| 213 | throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::copy_constructor meant to not be accessable"); |
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| 214 | } |
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| 215 | |
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| 216 | |
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| 217 | |
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| 218 | |
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| 219 | const G4C12GEMProbability & G4C12GEMProbability:: |
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| 220 | operator=(const G4C12GEMProbability &) |
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| 221 | { |
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| 222 | throw G4HadronicException(__FILE__, __LINE__, "G4C12GEMProbability::operator= meant to not be accessable"); |
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| 223 | return *this; |
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| 224 | } |
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| 225 | |
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| 226 | |
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| 227 | G4bool G4C12GEMProbability::operator==(const G4C12GEMProbability &) const |
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| 228 | { |
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| 229 | return false; |
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| 230 | } |
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| 231 | |
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| 232 | G4bool G4C12GEMProbability::operator!=(const G4C12GEMProbability &) const |
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| 233 | { |
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| 234 | return true; |
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| 235 | } |
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| 236 | |
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| 237 | |
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| 238 | |
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