| 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: G4Be11GEMProbability.cc,v 1.5 2006/06/29 20:21:25 gunter Exp $ |
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| 28 | // GEANT4 tag $Name: geant4-09-02-ref-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 "G4Be11GEMProbability.hh" |
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| 36 | |
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| 37 | G4Be11GEMProbability::G4Be11GEMProbability() : |
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| 38 | G4GEMProbability(11,4,1.0/2.0) // A,Z,Spin |
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| 39 | { |
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| 40 | ExcitEnergies.push_back(320.04*keV); |
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| 41 | ExcitSpins.push_back(1.0/2); |
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| 42 | ExcitLifetimes.push_back(115.0e-15*s); |
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| 43 | |
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| 44 | ExcitEnergies.push_back(1778.0*keV); |
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| 45 | ExcitSpins.push_back(5.0/2.0); |
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| 46 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV)); |
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| 47 | |
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| 48 | ExcitEnergies.push_back(2.69e3*keV); |
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| 49 | ExcitSpins.push_back(3.0/2.0); |
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| 50 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV)); |
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| 51 | |
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| 52 | ExcitEnergies.push_back(3.41e3*keV); |
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| 53 | ExcitSpins.push_back(3.0/2.0); |
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| 54 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(125.0*keV)); |
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| 55 | |
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| 56 | ExcitEnergies.push_back(3887.0*keV); |
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| 57 | ExcitSpins.push_back(7.0/2.0); |
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| 58 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.0*keV)); |
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| 59 | |
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| 60 | ExcitEnergies.push_back(3956.0*keV); |
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| 61 | ExcitSpins.push_back(3.0/2.0); |
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| 62 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(15.0*keV)); |
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| 63 | |
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| 64 | ExcitEnergies.push_back(5240.0*keV); |
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| 65 | ExcitSpins.push_back(0.0); |
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| 66 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(45.0*keV)); |
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| 67 | |
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| 68 | ExcitEnergies.push_back(5.86e3*keV); |
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| 69 | ExcitSpins.push_back(0.0); |
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| 70 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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| 71 | |
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| 72 | ExcitEnergies.push_back(6.51e3*keV); |
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| 73 | ExcitSpins.push_back(0.0); |
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| 74 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(120.0*keV)); |
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| 75 | |
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| 76 | ExcitEnergies.push_back(6705.0*keV); |
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| 77 | ExcitSpins.push_back(0.0); |
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| 78 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV)); |
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| 79 | |
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| 80 | ExcitEnergies.push_back(7.03e3*keV); |
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| 81 | ExcitSpins.push_back(0.0); |
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| 82 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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| 83 | |
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| 84 | ExcitEnergies.push_back(8816.0*keV); |
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| 85 | ExcitSpins.push_back(0.0); |
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| 86 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV)); |
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| 87 | |
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| 88 | ExcitEnergies.push_back(10.59e3*keV); |
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| 89 | ExcitSpins.push_back(0.0); |
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| 90 | ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(210.0*keV)); |
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| 91 | |
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| 92 | |
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| 93 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 94 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 95 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 96 | } |
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| 97 | |
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| 98 | |
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| 99 | G4Be11GEMProbability::G4Be11GEMProbability(const G4Be11GEMProbability &) : G4GEMProbability() |
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| 100 | { |
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| 101 | throw G4HadronicException(__FILE__, __LINE__, "G4Be11GEMProbability::copy_constructor meant to not be accessable"); |
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| 102 | } |
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| 103 | |
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| 104 | |
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| 105 | |
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| 106 | |
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| 107 | const G4Be11GEMProbability & G4Be11GEMProbability:: |
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| 108 | operator=(const G4Be11GEMProbability &) |
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| 109 | { |
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| 110 | throw G4HadronicException(__FILE__, __LINE__, "G4Be11GEMProbability::operator= meant to not be accessable"); |
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| 111 | return *this; |
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| 112 | } |
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| 113 | |
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| 114 | |
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| 115 | G4bool G4Be11GEMProbability::operator==(const G4Be11GEMProbability &) const |
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| 116 | { |
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| 117 | return false; |
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| 118 | } |
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| 119 | |
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| 120 | G4bool G4Be11GEMProbability::operator!=(const G4Be11GEMProbability &) const |
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| 121 | { |
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| 122 | return true; |
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| 123 | } |
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| 124 | |
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| 125 | |
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| 126 | |
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