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: G4C13GEMProbability.cc,v 1.5 2006/06/29 20:21:41 gunter Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-02 $ |
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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 "G4C13GEMProbability.hh" |
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36 | |
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37 | G4C13GEMProbability::G4C13GEMProbability() : |
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38 | G4GEMProbability(13,6,1.0/2.0) // A,Z,Spin |
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39 | { |
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40 | |
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41 | ExcitEnergies.push_back(3088.4*keV); |
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42 | ExcitSpins.push_back(1.0/2.0); |
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43 | ExcitLifetimes.push_back(1.04e-15*s); |
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44 | |
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45 | ExcitEnergies.push_back(3684.37*keV); |
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46 | ExcitSpins.push_back(3.0/2.0); |
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47 | ExcitLifetimes.push_back(1.04e-15*s); |
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48 | |
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49 | ExcitEnergies.push_back( 3853.62*keV); |
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50 | ExcitSpins.push_back(5.0/2.0); |
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51 | ExcitLifetimes.push_back(7.5e-12*s); |
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52 | |
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53 | ExcitEnergies.push_back(6864*keV); |
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54 | ExcitSpins.push_back(5.0/2.0); |
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55 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(6*keV)); |
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56 | |
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57 | ExcitEnergies.push_back(7492*keV); |
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58 | ExcitSpins.push_back(7.0/2.0); |
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59 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); |
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60 | |
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61 | ExcitEnergies.push_back(7547*keV); |
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62 | ExcitSpins.push_back(5.0/2.0); |
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63 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1.2*keV)); |
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64 | |
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65 | ExcitEnergies.push_back(7677*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)/(70*keV)); |
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68 | |
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69 | ExcitEnergies.push_back(8.2E3*keV); |
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70 | ExcitSpins.push_back(3.0/2.0); |
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71 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1000*keV)); |
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72 | |
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73 | ExcitEnergies.push_back(8860*keV); |
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74 | ExcitSpins.push_back(1.0/2.0); |
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75 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); |
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76 | |
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77 | ExcitEnergies.push_back(9498*keV); |
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78 | ExcitSpins.push_back(3.0/2.0); |
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79 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); |
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80 | |
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81 | ExcitEnergies.push_back(9897*keV); |
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82 | ExcitSpins.push_back(3.0/2.0); |
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83 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(26*keV)); |
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84 | |
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85 | ExcitEnergies.push_back(10753*keV); |
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86 | ExcitSpins.push_back(7.0/2.0); |
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87 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(55*keV)); |
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88 | |
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89 | ExcitEnergies.push_back(10818*keV); |
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90 | ExcitSpins.push_back(5.0/2.0); |
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91 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(24*keV)); |
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92 | |
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93 | ExcitEnergies.push_back(10996*keV); |
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94 | ExcitSpins.push_back(1.0/2.0); |
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95 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(37*keV)); |
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96 | |
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97 | ExcitEnergies.push_back(11080*keV); |
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98 | ExcitSpins.push_back(1.0/2.0); |
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99 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4*keV)); |
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100 | |
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101 | ExcitEnergies.push_back(11851*keV); |
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102 | ExcitSpins.push_back(3.0/2.0); |
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103 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(68*keV)); |
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104 | |
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105 | ExcitEnergies.push_back(11970*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)/(200*keV)); |
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108 | |
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109 | ExcitEnergies.push_back(12106*keV); |
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110 | ExcitSpins.push_back(9.0/2.0); |
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111 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(81*keV)); |
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112 | |
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113 | ExcitEnergies.push_back(12400*keV); |
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114 | ExcitSpins.push_back(7.0/2.0); |
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115 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(150*keV)); |
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116 | |
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117 | ExcitEnergies.push_back(13280*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)/(340*keV)); |
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120 | |
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121 | ExcitEnergies.push_back(13410*keV); |
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122 | ExcitSpins.push_back(9.0/2.0); |
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123 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(35*keV)); |
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124 | |
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125 | ExcitEnergies.push_back(13560*keV); |
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126 | ExcitSpins.push_back(5.0/2.0); |
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127 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(500*keV)); |
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128 | |
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129 | ExcitEnergies.push_back(13760*keV); |
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130 | ExcitSpins.push_back(3.0/2.0); |
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131 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300*keV)); |
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132 | |
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133 | ExcitEnergies.push_back(14120*keV); |
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134 | ExcitSpins.push_back(5.0/2.0); |
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135 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200*keV)); |
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136 | |
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137 | ExcitEnergies.push_back(14.39E3*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)/(260*keV)); |
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140 | |
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141 | ExcitEnergies.push_back(14940*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)/(380*keV)); |
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144 | |
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145 | ExcitEnergies.push_back(15106*keV); |
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146 | ExcitSpins.push_back(3.0/2.0); |
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147 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(5*keV)); |
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148 | |
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149 | ExcitEnergies.push_back(19500*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)/(450*keV)); |
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152 | |
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153 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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154 | SetExcitationSpinsPtr(&ExcitSpins); |
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155 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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156 | } |
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157 | |
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158 | |
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159 | G4C13GEMProbability::G4C13GEMProbability(const G4C13GEMProbability &) : G4GEMProbability() |
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160 | { |
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161 | throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::copy_constructor meant to not be accessable"); |
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162 | } |
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163 | |
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164 | |
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165 | |
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166 | |
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167 | const G4C13GEMProbability & G4C13GEMProbability:: |
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168 | operator=(const G4C13GEMProbability &) |
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169 | { |
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170 | throw G4HadronicException(__FILE__, __LINE__, "G4C13GEMProbability::operator= meant to not be accessable"); |
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171 | return *this; |
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172 | } |
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173 | |
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174 | |
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175 | G4bool G4C13GEMProbability::operator==(const G4C13GEMProbability &) const |
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176 | { |
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177 | return false; |
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178 | } |
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179 | |
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180 | G4bool G4C13GEMProbability::operator!=(const G4C13GEMProbability &) const |
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181 | { |
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182 | return true; |
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183 | } |
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184 | |
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185 | |
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186 | |
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