| 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: G4StatMFMacroNucleon.cc,v 1.6 2008/07/25 11:20:47 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
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| 32 |
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| 33 | #include "G4StatMFMacroNucleon.hh"
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| 34 |
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| 35 | // Operators
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| 36 |
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| 37 | G4StatMFMacroNucleon & G4StatMFMacroNucleon::
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| 38 | operator=(const G4StatMFMacroNucleon & )
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| 39 | {
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| 40 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroNucleon::operator= meant to not be accessable");
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| 41 | return *this;
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| 42 | }
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| 43 |
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| 44 |
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| 45 | G4bool G4StatMFMacroNucleon::operator==(const G4StatMFMacroNucleon & ) const
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| 46 | {
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| 47 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroNucleon::operator== meant to not be accessable");
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| 48 | return false;
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| 49 | }
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| 50 |
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| 51 |
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| 52 | G4bool G4StatMFMacroNucleon::operator!=(const G4StatMFMacroNucleon & ) const
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| 53 | {
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| 54 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroNucleon::operator!= meant to not be accessable");
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| 55 | return true;
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| 56 | }
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| 57 |
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| 58 | G4double G4StatMFMacroNucleon::CalcMeanMultiplicity(const G4double FreeVol, const G4double mu,
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| 59 | const G4double nu, const G4double T)
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| 60 | {
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| 61 | if (T <= 0.0) throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroNucleon::CalcMeanMultiplicity: Temperature less or equal 0");
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| 62 | const G4double ThermalWaveLenght = 16.15*fermi/std::sqrt(T);
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| 63 |
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| 64 | const G4double lambda3 = ThermalWaveLenght*ThermalWaveLenght*ThermalWaveLenght;
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| 65 |
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| 66 | const G4double degeneracy = 2.0;
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| 67 |
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| 68 | const G4double Coulomb = (3./5.)*(elm_coupling/G4StatMFParameters::Getr0())*
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| 69 | (1.0 - 1.0/std::pow(1.0+G4StatMFParameters::GetKappaCoulomb(),1./3.));
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| 70 |
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| 71 | G4double exponent_proton = (mu+nu-Coulomb)/T;
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| 72 | G4double exponent_neutron = mu/T;
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| 73 |
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| 74 | if (exponent_neutron > 700.0) exponent_neutron = 700.0;
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| 75 | if (exponent_proton > 700.0) exponent_proton = 700.0;
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| 76 |
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| 77 | _NeutronMeanMultiplicity = (degeneracy*FreeVol/lambda3)*std::exp(exponent_neutron);
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| 78 |
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| 79 | _ProtonMeanMultiplicity = (degeneracy*FreeVol/lambda3)*std::exp(exponent_proton);
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| 80 |
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| 81 |
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| 82 |
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| 83 | return _MeanMultiplicity = _NeutronMeanMultiplicity + _ProtonMeanMultiplicity;
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| 84 |
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| 85 | }
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| 86 |
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| 87 |
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| 88 | G4double G4StatMFMacroNucleon::CalcEnergy(const G4double T)
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| 89 | {
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| 90 | const G4double Coulomb = (3./5.)*(elm_coupling/G4StatMFParameters::Getr0())*
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| 91 | (1.0 - 1.0/std::pow(1.0+G4StatMFParameters::GetKappaCoulomb(),1./3.));
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| 92 |
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| 93 | return _Energy = Coulomb * theZARatio * theZARatio + (3./2.) * T;
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| 94 |
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| 95 | }
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| 96 |
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| 97 | G4double G4StatMFMacroNucleon::CalcEntropy(const G4double T, const G4double FreeVol)
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| 98 | {
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| 99 | const G4double ThermalWaveLenght = 16.15*fermi/std::sqrt(T);
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| 100 | const G4double lambda3 = ThermalWaveLenght*ThermalWaveLenght*ThermalWaveLenght;
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| 101 |
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| 102 | G4double NeutronEntropy = 0.0;
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| 103 | if (_NeutronMeanMultiplicity > 0.0)
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| 104 | NeutronEntropy = _NeutronMeanMultiplicity*(5./2.+
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| 105 | std::log(2.0*static_cast<G4double>(theA)*FreeVol/
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| 106 | (lambda3*_NeutronMeanMultiplicity)));
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| 107 |
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| 108 |
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| 109 | G4double ProtonEntropy = 0.0;
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| 110 | if (_ProtonMeanMultiplicity > 0.0)
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| 111 | ProtonEntropy = _ProtonMeanMultiplicity*(5./2.+
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| 112 | std::log(2.0*static_cast<G4double>(theA)*FreeVol/
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| 113 | (lambda3*_ProtonMeanMultiplicity)));
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| 114 |
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| 115 |
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| 116 | return NeutronEntropy+ProtonEntropy;
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| 117 | }
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| 118 |
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