| 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: G4AlphaGEMProbability.cc,v 1.5 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 | // J.M. Quesada (July 2009) C's and k's values according to Furihata's paper |
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| 34 | // (based on notes added on proof in Dostrovskii's paper) |
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| 35 | |
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| 36 | #include "G4AlphaGEMProbability.hh" |
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| 37 | |
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| 38 | G4AlphaGEMProbability::G4AlphaGEMProbability() : |
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| 39 | G4GEMProbability(4,2,0.0) // A,Z,Gamma |
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| 40 | { |
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| 41 | ExcitEnergies.push_back(20.01E+3*keV); |
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| 42 | ExcitSpins.push_back(0.0); |
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| 43 | ExcitLifetimes.push_back(207.0*keV); |
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| 44 | |
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| 45 | ExcitEnergies.push_back(21.18E+3*keV); |
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| 46 | ExcitSpins.push_back(0.0); |
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| 47 | ExcitLifetimes.push_back(0.73*MeV); |
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| 48 | |
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| 49 | ExcitEnergies.push_back(22.02E+3*keV); |
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| 50 | ExcitSpins.push_back(2.0); |
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| 51 | ExcitLifetimes.push_back(1.83*MeV); |
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| 52 | |
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| 53 | ExcitEnergies.push_back(25.33E+3*keV); |
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| 54 | ExcitSpins.push_back(1.0); |
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| 55 | ExcitLifetimes.push_back(2.36*MeV); |
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| 56 | |
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| 57 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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| 58 | SetExcitationSpinsPtr(&ExcitSpins); |
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| 59 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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| 60 | } |
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| 61 | |
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| 62 | |
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| 63 | G4AlphaGEMProbability::G4AlphaGEMProbability(const G4AlphaGEMProbability &) : G4GEMProbability() |
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| 64 | { |
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| 65 | throw G4HadronicException(__FILE__, __LINE__, "G4AlphaGEMProbability::copy_constructor meant to not be accessable"); |
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| 66 | } |
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| 67 | |
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| 68 | |
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| 69 | |
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| 70 | |
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| 71 | const G4AlphaGEMProbability & G4AlphaGEMProbability:: |
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| 72 | operator=(const G4AlphaGEMProbability &) |
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| 73 | { |
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| 74 | throw G4HadronicException(__FILE__, __LINE__, "G4AlphaGEMProbability::operator= meant to not be accessable"); |
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| 75 | return *this; |
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| 76 | } |
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| 77 | |
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| 78 | |
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| 79 | G4bool G4AlphaGEMProbability::operator==(const G4AlphaGEMProbability &) const |
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| 80 | { |
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| 81 | return false; |
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| 82 | } |
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| 83 | |
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| 84 | G4bool G4AlphaGEMProbability::operator!=(const G4AlphaGEMProbability &) const |
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| 85 | { |
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| 86 | return true; |
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| 87 | } |
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| 88 | |
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| 89 | //JMQ 190709 C's values from Furihata's paper |
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| 90 | //(notes added on proof in Dostrovskii's paper) |
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| 91 | G4double G4AlphaGEMProbability::CCoeficient(const G4double/* aZ*/) const |
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| 92 | { |
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| 93 | return 0.; |
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| 94 | } |
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| 95 | |
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| 96 | |
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| 97 | //G4double G4AlphaGEMProbability::CCoeficient(const G4double aZ) const |
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| 98 | //{ |
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| 99 | // Data comes from |
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| 100 | // Dostrovsky, Fraenkel and Friedlander |
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| 101 | // Physical Review, vol 116, num. 3 1959 |
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| 102 | // |
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| 103 | // const G4int size = 5; |
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| 104 | // G4double Zlist[5] = { 10.0, 20.0, 30.0, 50.0, 70.0}; |
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| 105 | // G4double Calpha[5] = { 0.10, 0.10, 0.10, 0.08, 0.06}; |
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| 106 | // G4double C = 0.0; |
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| 107 | |
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| 108 | |
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| 109 | // if (aZ <= 30) { |
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| 110 | // C = 0.10; |
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| 111 | // } else if (aZ <= 50) { |
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| 112 | // C = 0.1 + -((aZ-50.)/20.)*0.02; |
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| 113 | // } else if (aZ < 70) { |
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| 114 | // C = 0.08 + -((aZ-70.)/20.)*0.02; |
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| 115 | // } else { |
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| 116 | // C = 0.06; |
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| 117 | // } |
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| 118 | // return C; |
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| 119 | //} |
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| 120 | |
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