| 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: G4B10GEMProbability.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 "G4B10GEMProbability.hh" |
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| 36 | |
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| 37 | G4B10GEMProbability::G4B10GEMProbability() : |
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| 38 | G4GEMProbability(10,5,3.0) // A,Z,Spin |
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| 39 | { |
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| 40 | ExcitEnergies.push_back(718.35*keV); |
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| 41 | ExcitSpins.push_back(1.0); |
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| 42 | ExcitLifetimes.push_back(0.707e-9*s); |
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| 43 | |
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| 44 | ExcitEnergies.push_back(1740.15*keV); |
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| 45 | ExcitSpins.push_back(0.0); |
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| 46 | ExcitLifetimes.push_back(5.0e-15*s); |
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| 47 | |
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| 48 | ExcitEnergies.push_back(2154.3*keV); |
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| 49 | ExcitSpins.push_back(1.0); |
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| 50 | ExcitLifetimes.push_back(1.48e-12*s); |
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| 51 | |
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| 52 | ExcitEnergies.push_back(3587.1*keV); |
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| 53 | ExcitSpins.push_back(2.0); |
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| 54 | ExcitLifetimes.push_back(106.0e-15*s); |
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| 55 | |
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| 56 | ExcitEnergies.push_back(4774.0*keV); |
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| 57 | ExcitSpins.push_back(3.0); |
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| 58 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(8.7*keV)); |
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| 59 | |
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| 60 | ExcitEnergies.push_back(5110.3*keV); |
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| 61 | ExcitSpins.push_back(2.0); |
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| 62 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.98*keV)); |
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| 63 | |
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| 64 | ExcitEnergies.push_back(5163.9*keV); |
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| 65 | ExcitSpins.push_back(2.0); |
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| 66 | ExcitLifetimes.push_back(4.2e-15*s); |
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| 67 | |
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| 68 | ExcitEnergies.push_back(5180.0*keV); |
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| 69 | ExcitSpins.push_back(1.0); |
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| 70 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(110.0*keV)); |
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| 71 | |
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| 72 | ExcitEnergies.push_back(5919.5*keV); |
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| 73 | ExcitSpins.push_back(2.0); |
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| 74 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6.0*keV)); |
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| 75 | |
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| 76 | ExcitEnergies.push_back(6025.0*keV); |
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| 77 | ExcitSpins.push_back(4.0); |
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| 78 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.05*keV)); |
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| 79 | |
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| 80 | ExcitEnergies.push_back(6127.2*keV); |
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| 81 | ExcitSpins.push_back(3.0); |
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| 82 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.36*keV)); |
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| 83 | |
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| 84 | ExcitEnergies.push_back(6561.0*keV); |
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| 85 | ExcitSpins.push_back(4.0); |
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| 86 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(25.1*keV)); |
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| 87 | |
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| 88 | ExcitEnergies.push_back(6873.0*keV); |
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| 89 | ExcitSpins.push_back(1.0); |
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| 90 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(120.0*keV)); |
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| 91 | |
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| 92 | ExcitEnergies.push_back(7002.0*keV); |
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| 93 | ExcitSpins.push_back(2.0); |
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| 94 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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| 95 | |
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| 96 | ExcitEnergies.push_back(7430.0*keV); |
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| 97 | ExcitSpins.push_back(2.0); |
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| 98 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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| 99 | |
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| 100 | ExcitEnergies.push_back(7467.0*keV); |
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| 101 | ExcitSpins.push_back(1.0); |
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| 102 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(65.0*keV)); |
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| 103 | |
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| 104 | ExcitEnergies.push_back(7479.0*keV); |
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| 105 | ExcitSpins.push_back(2.0); |
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| 106 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(74.0*keV)); |
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| 107 | |
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| 108 | ExcitEnergies.push_back(7560.7*keV); |
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| 109 | ExcitSpins.push_back(0.0); |
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| 110 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.65*keV)); |
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| 111 | |
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| 112 | ExcitEnergies.push_back(7670.0*keV); |
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| 113 | ExcitSpins.push_back(1.0); |
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| 114 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(250.0*keV)); |
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| 115 | |
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| 116 | ExcitEnergies.push_back(7819.0*keV); |
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| 117 | ExcitSpins.push_back(1.0); |
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| 118 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260.0*keV)); |
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| 119 | |
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| 120 | ExcitEnergies.push_back(8070.0*keV); |
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| 121 | ExcitSpins.push_back(2.0); |
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| 122 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV)); |
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| 123 | |
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| 124 | ExcitEnergies.push_back(8700.0*keV); |
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| 125 | ExcitSpins.push_back(1.0); |
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| 126 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
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| 127 | |
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| 128 | ExcitEnergies.push_back(8889.0*keV); |
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| 129 | ExcitSpins.push_back(3.0); |
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| 130 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(84.0*keV)); |
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| 131 | |
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| 132 | ExcitEnergies.push_back(8895.0*keV); |
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| 133 | ExcitSpins.push_back(2.0); |
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| 134 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV)); |
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| 135 | |
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| 136 | ExcitEnergies.push_back(9700.0*keV); |
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| 137 | ExcitSpins.push_back(0.0); |
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| 138 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(700.0*keV)); |
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| 139 | |
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| 140 | ExcitEnergies.push_back(10840.0*keV); |
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| 141 | ExcitSpins.push_back(4.0); |
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| 142 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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| 143 | |
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| 144 | ExcitEnergies.push_back(11520.0*keV); |
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| 145 | ExcitSpins.push_back(0.0); |
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| 146 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500.0*keV)); |
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| 147 | |
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| 148 | ExcitEnergies.push_back(12560.0*keV); |
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| 149 | ExcitSpins.push_back(2.0); |
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| 150 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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| 151 | |
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| 152 | ExcitEnergies.push_back(13490.0*keV); |
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| 153 | ExcitSpins.push_back(2.0); |
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| 154 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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| 155 | |
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| 156 | ExcitEnergies.push_back(14.4e3*keV); |
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| 157 | ExcitSpins.push_back(0.0); |
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| 158 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(800.0*keV)); |
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| 159 | |
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| 160 | ExcitEnergies.push_back(18.2e3*keV); |
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| 161 | ExcitSpins.push_back(0.0); |
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| 162 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1500.0*keV)); |
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| 163 | |
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| 164 | ExcitEnergies.push_back(18430.0*keV); |
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| 165 | ExcitSpins.push_back(2.0); |
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| 166 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(340.0*keV)); |
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| 167 | |
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| 168 | ExcitEnergies.push_back(18800.0*keV); |
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| 169 | ExcitSpins.push_back(1.0); |
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| 170 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV)); |
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| 171 | |
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| 172 | ExcitEnergies.push_back(19290.0*keV); |
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| 173 | ExcitSpins.push_back(2.0); |
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| 174 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(190.0*keV)); |
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| 175 | |
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| 176 | |
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| 177 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 178 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 179 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 180 | } |
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| 181 | |
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| 182 | |
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| 183 | G4B10GEMProbability::G4B10GEMProbability(const G4B10GEMProbability &) : G4GEMProbability() |
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| 184 | { |
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| 185 | throw G4HadronicException(__FILE__, __LINE__, "G4B10GEMProbability::copy_constructor meant to not be accessable");} |
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| 186 | |
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| 187 | |
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| 188 | |
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| 189 | |
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| 190 | const G4B10GEMProbability & G4B10GEMProbability:: |
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| 191 | operator=(const G4B10GEMProbability &) |
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| 192 | { |
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| 193 | throw G4HadronicException(__FILE__, __LINE__, "G4B10GEMProbability::operator= meant to not be accessable"); |
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| 194 | return *this; |
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| 195 | } |
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| 196 | |
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| 197 | |
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| 198 | G4bool G4B10GEMProbability::operator==(const G4B10GEMProbability &) const |
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| 199 | { |
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| 200 | return false; |
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| 201 | } |
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| 202 | |
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| 203 | G4bool G4B10GEMProbability::operator!=(const G4B10GEMProbability &) const |
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| 204 | { |
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| 205 | return true; |
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| 206 | } |
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| 207 | |
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| 208 | |
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| 209 | |
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