| 1 | //
|
|---|
| 2 | // ********************************************************************
|
|---|
| 3 | // * License and Disclaimer *
|
|---|
| 4 | // * *
|
|---|
| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
|
|---|
| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
|
|---|
| 7 | // * conditions of the Geant4 Software License, included in the file *
|
|---|
| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
|
|---|
| 9 | // * include a list of copyright holders. *
|
|---|
| 10 | // * *
|
|---|
| 11 | // * Neither the authors of this software system, nor their employing *
|
|---|
| 12 | // * institutes,nor the agencies providing financial support for this *
|
|---|
| 13 | // * work make any representation or warranty, express or implied, *
|
|---|
| 14 | // * regarding this software system or assume any liability for its *
|
|---|
| 15 | // * use. Please see the license in the file LICENSE and URL above *
|
|---|
| 16 | // * for the full disclaimer and the limitation of liability. *
|
|---|
| 17 | // * *
|
|---|
| 18 | // * This code implementation is the result of the scientific and *
|
|---|
| 19 | // * technical work of the GEANT4 collaboration. *
|
|---|
| 20 | // * By using, copying, modifying or distributing the software (or *
|
|---|
| 21 | // * any work based on the software) you agree to acknowledge its *
|
|---|
| 22 | // * use in resulting scientific publications, and indicate your *
|
|---|
| 23 | // * acceptance of all terms of the Geant4 Software license. *
|
|---|
| 24 | // ********************************************************************
|
|---|
| 25 | //
|
|---|
| 26 | //
|
|---|
| 27 | // $Id: G4StatMFMacroBiNucleon.cc,v 1.7 2008/10/24 22:56:42 dennis Exp $
|
|---|
| 28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
|
|---|
| 29 | //
|
|---|
| 30 | // Hadronic Process: Nuclear De-excitations
|
|---|
| 31 | // by V. Lara
|
|---|
| 32 |
|
|---|
| 33 | #include "G4StatMFMacroBiNucleon.hh"
|
|---|
| 34 |
|
|---|
| 35 | // Operators
|
|---|
| 36 |
|
|---|
| 37 | G4StatMFMacroBiNucleon & G4StatMFMacroBiNucleon::
|
|---|
| 38 | operator=(const G4StatMFMacroBiNucleon & )
|
|---|
| 39 | {
|
|---|
| 40 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroBiNucleon::operator= meant to not be accessable");
|
|---|
| 41 | return *this;
|
|---|
| 42 | }
|
|---|
| 43 |
|
|---|
| 44 |
|
|---|
| 45 | G4bool G4StatMFMacroBiNucleon::operator==(const G4StatMFMacroBiNucleon & ) const
|
|---|
| 46 | {
|
|---|
| 47 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroBiNucleon::operator== meant to not be accessable");
|
|---|
| 48 | return false;
|
|---|
| 49 | }
|
|---|
| 50 |
|
|---|
| 51 |
|
|---|
| 52 | G4bool G4StatMFMacroBiNucleon::operator!=(const G4StatMFMacroBiNucleon & ) const
|
|---|
| 53 | {
|
|---|
| 54 | throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMacroBiNucleon::operator!= meant to not be accessable");
|
|---|
| 55 | return true;
|
|---|
| 56 | }
|
|---|
| 57 |
|
|---|
| 58 |
|
|---|
| 59 | G4double G4StatMFMacroBiNucleon::CalcMeanMultiplicity(const G4double FreeVol, const G4double mu,
|
|---|
| 60 | const G4double nu, const G4double T)
|
|---|
| 61 | {
|
|---|
| 62 | const G4double ThermalWaveLenght = 16.15*fermi/std::sqrt(T);
|
|---|
| 63 |
|
|---|
| 64 | const G4double lambda3 = ThermalWaveLenght*ThermalWaveLenght*ThermalWaveLenght;
|
|---|
| 65 |
|
|---|
| 66 | const G4double degeneracy = 3.0;
|
|---|
| 67 |
|
|---|
| 68 | const G4double Coulomb = (3./5.)*(elm_coupling/G4StatMFParameters::Getr0())*
|
|---|
| 69 | (1.0 - 1.0/std::pow(1.0+G4StatMFParameters::GetKappaCoulomb(),1./3.));
|
|---|
| 70 |
|
|---|
| 71 | const G4double BindingE = G4NucleiProperties::GetBindingEnergy(theA,1); //old value was 2.796*MeV
|
|---|
| 72 | G4double exponent = (BindingE + theA*(mu+nu*theZARatio) -
|
|---|
| 73 | Coulomb*theZARatio*theZARatio*std::pow(G4double(theA),5./3.))/T;
|
|---|
| 74 |
|
|---|
| 75 | // To avoid numerical problems
|
|---|
| 76 | if (exponent < -700.0) exponent = -700.0;
|
|---|
| 77 | else if (exponent > 700.0) exponent = 700.0;
|
|---|
| 78 |
|
|---|
| 79 | _MeanMultiplicity = (degeneracy*FreeVol*static_cast<G4double>(theA)*std::sqrt(static_cast<G4double>(theA))/lambda3)*
|
|---|
| 80 | std::exp(exponent);
|
|---|
| 81 |
|
|---|
| 82 | return _MeanMultiplicity;
|
|---|
| 83 | }
|
|---|
| 84 |
|
|---|
| 85 |
|
|---|
| 86 | G4double G4StatMFMacroBiNucleon::CalcEnergy(const G4double T)
|
|---|
| 87 | {
|
|---|
| 88 | const G4double Coulomb = (3./5.)*(elm_coupling/G4StatMFParameters::Getr0())*
|
|---|
| 89 | (1.0 - 1.0/std::pow(1.0+G4StatMFParameters::GetKappaCoulomb(),1./3.));
|
|---|
| 90 |
|
|---|
| 91 | _Energy = -G4NucleiProperties::GetBindingEnergy(theA,1) +
|
|---|
| 92 | Coulomb * theZARatio * theZARatio * std::pow(G4double(theA),5./3.) +
|
|---|
| 93 | (3./2.) * T;
|
|---|
| 94 |
|
|---|
| 95 | return _Energy;
|
|---|
| 96 | }
|
|---|
| 97 |
|
|---|
| 98 |
|
|---|
| 99 |
|
|---|
| 100 | G4double G4StatMFMacroBiNucleon::CalcEntropy(const G4double T, const G4double FreeVol)
|
|---|
| 101 | {
|
|---|
| 102 | const G4double ThermalWaveLenght = 16.15*fermi/std::sqrt(T);
|
|---|
| 103 | const G4double lambda3 = ThermalWaveLenght*ThermalWaveLenght*ThermalWaveLenght;
|
|---|
| 104 |
|
|---|
| 105 | G4double Entropy = 0.0;
|
|---|
| 106 | if (_MeanMultiplicity > 0.0)
|
|---|
| 107 | // Is this formula correct?
|
|---|
| 108 | Entropy = _MeanMultiplicity*(5./2.+
|
|---|
| 109 | std::log(3.0*static_cast<G4double>(theA)*
|
|---|
| 110 | std::sqrt(static_cast<G4double>(theA))*FreeVol/
|
|---|
| 111 | (lambda3*_MeanMultiplicity)));
|
|---|
| 112 |
|
|---|
| 113 |
|
|---|
| 114 | return Entropy;
|
|---|
| 115 | }
|
|---|