| 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 | // 18-Sep-2003 First version is written by T. Koi
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| 27 | // 10-Nov-2003 Bug fix at Cal. ke_per_n and D T. Koi
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| 28 | // 12-Nov-2003 Add energy check at lower side T. Koi
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| 29 | // 26-Dec-2006 Add isotope dependence D. Wright
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| 30 |
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| 31 | #include "G4IonsKoxCrossSection.hh"
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| 32 | #include "G4ParticleTable.hh"
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| 33 | #include "G4IonTable.hh"
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| 34 |
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| 35 | G4double G4IonsKoxCrossSection::
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| 36 | GetIsoZACrossSection(const G4DynamicParticle* aParticle, G4double ZZ,
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| 37 | G4double AA, G4double /*temperature*/)
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| 38 | {
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| 39 | G4double xsection = 0.0;
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| 40 |
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| 41 | G4int Ap = aParticle->GetDefinition()->GetBaryonNumber();
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| 42 | G4int Zp = int ( aParticle->GetDefinition()->GetPDGCharge() / eplus + 0.5);
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| 43 | G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
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| 44 |
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| 45 | // Apply energy check, if less than lower limit then 0 value is returned
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| 46 | if ( ke_per_N < lowerLimit )
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| 47 | return xsection;
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| 48 |
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| 49 | G4int At = int (AA + 0.5);
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| 50 | G4int Zt = int (ZZ + 0.5 );
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| 51 |
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| 52 | G4double one_third = 1.0 / 3.0;
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| 53 |
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| 54 | G4double cubicrAt = std::pow ( G4double(At) , G4double(one_third) );
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| 55 | G4double cubicrAp = std::pow ( G4double(Ap) , G4double(one_third) );
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| 56 |
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| 57 |
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| 58 | G4double Bc = Zt * Zp / ( ( rc / fermi ) * ( cubicrAp + cubicrAt ) ); // rc divide fermi
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| 59 |
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| 60 | G4double Rvol = r0 * ( cubicrAp + cubicrAt );
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| 61 |
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| 62 | // G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
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| 63 | G4double c = calCeValue ( ke_per_N / MeV );
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| 64 |
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| 65 | G4double a = 1.85;
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| 66 | G4double Rsurf = r0 * ( a * cubicrAp * cubicrAt / ( cubicrAp + cubicrAt ) - c);
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| 67 | G4double D = 5.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
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| 68 | Rsurf = Rsurf + D * fermi; // multiply D by fermi
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| 69 |
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| 70 | G4double Rint = Rvol + Rsurf;
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| 71 |
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| 72 | G4double targ_mass = G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass( Zt , At );
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| 73 | G4double proj_mass = aParticle->GetMass();
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| 74 | G4double proj_momentum = aParticle->GetMomentum().mag();
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| 75 |
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| 76 | G4double Ecm = calEcm ( proj_mass , targ_mass , proj_momentum );
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| 77 |
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| 78 | xsection = pi * Rint * Rint * ( 1 - Bc / ( Ecm / MeV ) );
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| 79 |
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| 80 | return xsection;
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| 81 | }
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| 82 |
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| 83 | G4double G4IonsKoxCrossSection::
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| 84 | GetCrossSection(const G4DynamicParticle* aParticle,
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| 85 | const G4Element* anElement, G4double temperature)
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| 86 | {
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| 87 | G4int nIso = anElement->GetNumberOfIsotopes();
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| 88 | G4double xsection = 0;
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| 89 |
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| 90 | if (nIso) {
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| 91 | G4double sig;
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| 92 | G4IsotopeVector* isoVector = anElement->GetIsotopeVector();
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| 93 | G4double* abundVector = anElement->GetRelativeAbundanceVector();
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| 94 | G4double ZZ;
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| 95 | G4double AA;
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| 96 |
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| 97 | for (G4int i = 0; i < nIso; i++) {
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| 98 | ZZ = G4double( (*isoVector)[i]->GetZ() );
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| 99 | AA = G4double( (*isoVector)[i]->GetN() );
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| 100 | sig = GetIsoZACrossSection(aParticle, ZZ, AA, temperature);
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| 101 | xsection += sig*abundVector[i];
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| 102 | }
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| 103 |
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| 104 | } else {
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| 105 | xsection =
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| 106 | GetIsoZACrossSection(aParticle, anElement->GetZ(), anElement->GetN(),
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| 107 | temperature);
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| 108 | }
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| 109 |
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| 110 | return xsection;
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| 111 | }
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| 112 |
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| 113 |
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| 114 | G4double G4IonsKoxCrossSection::calEcm ( G4double mp , G4double mt , G4double Plab )
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| 115 | {
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| 116 | G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
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| 117 | G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
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| 118 | G4double Pcm = Plab * mt / Ecm;
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| 119 | G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
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| 120 | return KEcm;
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| 121 | }
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| 122 |
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| 123 |
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| 124 | G4double G4IonsKoxCrossSection::calCeValue( const G4double ke )
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| 125 | {
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| 126 | // Calculate c value
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| 127 | // This value is indepenent from projectile and target particle
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| 128 | // ke is projectile kinetic energy per nucleon in the Lab system with MeV unit
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| 129 | // fitting function is made by T. Koi
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| 130 | // There are no data below 30 MeV/n in Kox et al.,
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| 131 |
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| 132 | G4double Ce;
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| 133 | G4double log10_ke = std::log10 ( ke );
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| 134 | if ( log10_ke > 1.5 )
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| 135 | {
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| 136 | Ce = - 10.0 / std::pow ( G4double(log10_ke) , G4double(5) ) + 2.0;
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| 137 | }
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| 138 | else
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| 139 | {
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| 140 | Ce = ( - 10.0 / std::pow ( G4double(1.5) , G4double(5) ) + 2.0 ) / std::pow ( G4double(1.5) , G4double(3) ) * std::pow ( G4double(log10_ke) , G4double(3) );
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| 141 |
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| 142 | }
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| 143 | return Ce;
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| 144 | }
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