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-cand-01 $ |
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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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