| 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 | // 24.11.08 V. Grichine - first implementation
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| 28 | //
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| 29 |
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| 30 | #include "G4GGNuclNuclCrossSection.hh"
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| 31 |
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| 32 | #include "G4ParticleTable.hh"
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| 33 | #include "G4IonTable.hh"
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| 34 | #include "G4ParticleDefinition.hh"
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| 35 |
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| 36 |
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| 37 |
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| 38 | ////////////////////////////////////////////////////////////////////////////////
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| 39 | //
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| 40 | //
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| 41 |
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| 42 | G4GGNuclNuclCrossSection::G4GGNuclNuclCrossSection()
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| 43 | : fUpperLimit( 100000 * GeV ),
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| 44 | fLowerLimit( 0.1 * MeV ),
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| 45 | fRadiusConst( 1.08*fermi ) // 1.1, 1.3 ?
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| 46 | {
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| 47 | theProton = G4Proton::Proton();
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| 48 | theNeutron = G4Neutron::Neutron();
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| 49 | }
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| 50 |
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| 51 | ///////////////////////////////////////////////////////////////////////////////////////
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| 52 | //
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| 53 | //
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| 54 |
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| 55 | G4GGNuclNuclCrossSection::~G4GGNuclNuclCrossSection()
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| 56 | {
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| 57 | }
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| 58 |
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| 59 |
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| 60 | ////////////////////////////////////////////////////////////////////////////////////////
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| 61 | //
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| 62 | //
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| 63 |
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| 64 |
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| 65 | G4bool
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| 66 | G4GGNuclNuclCrossSection::IsApplicable(const G4DynamicParticle* aDP,
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| 67 | const G4Element* anElement)
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| 68 | {
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| 69 | return IsZAApplicable(aDP, anElement->GetZ(), anElement->GetN());
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| 70 | }
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| 71 |
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| 72 | ////////////////////////////////////////////////////////////////////////////////////////
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| 73 | //
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| 74 | //
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| 75 |
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| 76 | G4bool
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| 77 | G4GGNuclNuclCrossSection::IsZAApplicable(const G4DynamicParticle* aDP,
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| 78 | G4double Z, G4double)
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| 79 | {
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| 80 | G4bool applicable = false;
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| 81 | // G4int baryonNumber = aDP->GetDefinition()->GetBaryonNumber();
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| 82 | G4double kineticEnergy = aDP->GetKineticEnergy();
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| 83 |
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| 84 | // const G4ParticleDefinition* theParticle = aDP->GetDefinition();
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| 85 |
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| 86 | if ( kineticEnergy >= fLowerLimit && Z > 1.5 ) applicable = true;
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| 87 |
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| 88 | return applicable;
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| 89 | }
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| 90 |
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| 91 | ////////////////////////////////////////////////////////////////////////////////////////
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| 92 | //
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| 93 | // Calculates total and inelastic Xsc, derives elastic as total - inelastic accordong to
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| 94 | // Glauber model with Gribov correction calculated in the dipole approximation on
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| 95 | // light cone. Gaussian density helps to calculate rest integrals of the model.
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| 96 | // [1] B.Z. Kopeliovich, nucl-th/0306044
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| 97 |
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| 98 |
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| 99 | G4double G4GGNuclNuclCrossSection::
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| 100 | GetCrossSection(const G4DynamicParticle* aParticle, const G4Element* anElement, G4double T)
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| 101 | {
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| 102 | return GetIsoZACrossSection(aParticle, anElement->GetZ(), anElement->GetN(), T);
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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 | // Calculates total and inelastic Xsc, derives elastic as total - inelastic accordong to
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| 108 | // Glauber model with Gribov correction calculated in the dipole approximation on
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| 109 | // light cone. Gaussian density of point-like nucleons helps to calculate rest integrals of the model.
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| 110 | // [1] B.Z. Kopeliovich, nucl-th/0306044 + simplification above
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| 111 |
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| 112 |
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| 113 |
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| 114 | G4double G4GGNuclNuclCrossSection::
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| 115 | GetIsoZACrossSection(const G4DynamicParticle* aParticle, G4double tZ, G4double tA, G4double)
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| 116 | {
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| 117 | G4double xsection, sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, cB, ratio;
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| 118 |
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| 119 | G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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| 120 | G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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| 121 |
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| 122 | G4double pTkin = aParticle->GetKineticEnergy();
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| 123 | pTkin /= pA;
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| 124 |
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| 125 | G4double pN = pA - pZ;
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| 126 | if( pN < 0. ) pN = 0.;
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| 127 |
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| 128 | G4double tN = tA - tZ;
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| 129 | if( tN < 0. ) tN = 0.;
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| 130 |
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| 131 | G4double tR = GetNucleusRadius(tA);
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| 132 | G4double pR = GetNucleusRadius(pA);
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| 133 |
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| 134 | cB = GetCoulombBarier(aParticle, tZ, tA, pR, tR);
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| 135 |
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| 136 | if(cB > 0.)
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| 137 | {
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| 138 |
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| 139 | sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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| 140 | (pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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| 141 |
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| 142 | nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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| 143 |
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| 144 | ratio = sigma/nucleusSquare;
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| 145 |
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| 146 | xsection = nucleusSquare*std::log( 1. + ratio );
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| 147 |
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| 148 | fTotalXsc = xsection;
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| 149 |
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| 150 | fTotalXsc *= cB;
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| 151 |
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| 152 | fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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| 153 |
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| 154 | fInelasticXsc *= cB;
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| 155 |
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| 156 | fElasticXsc = fTotalXsc - fInelasticXsc;
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| 157 |
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| 158 | // if (fElasticXsc < DBL_MIN) fElasticXsc = DBL_MIN;
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| 159 | /*
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| 160 | G4double difratio = ratio/(1.+ratio);
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| 161 |
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| 162 | fDiffractionXsc = 0.5*nucleusSquare*( difratio - std::log( 1. + difratio ) );
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| 163 | */
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| 164 | // production to be checked !!! edit MK xsc
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| 165 |
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| 166 | //sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscMK(theProton, pTkin, theProton) +
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| 167 | // (pZ*tN+pN*tZ)*GetHadronNucleonXscMK(theProton, pTkin, theNeutron);
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| 168 |
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| 169 | sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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| 170 | (pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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| 171 |
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| 172 | ratio = sigma/nucleusSquare;
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| 173 |
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| 174 | fProductionXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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| 175 |
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| 176 | if (fElasticXsc < 0.) fElasticXsc = 0.;
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| 177 | }
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| 178 | else
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| 179 | {
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| 180 | fInelasticXsc = 0.;
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| 181 | fTotalXsc = 0.;
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| 182 | fElasticXsc = 0.;
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| 183 | fProductionXsc = 0.;
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| 184 | }
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| 185 | return fInelasticXsc; // xsection;
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| 186 | }
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| 187 |
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| 188 | ////////////////////////////////////////////////////////////////////////////////////////
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| 189 | //
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| 190 | //
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| 191 |
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| 192 | G4double G4GGNuclNuclCrossSection::
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| 193 | GetCoulombBarier(const G4DynamicParticle* aParticle, G4double tZ, G4double tA, G4double pR, G4double tR)
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| 194 | {
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| 195 | G4double ratio;
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| 196 | G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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| 197 |
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| 198 |
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| 199 | G4double pTkin = aParticle->GetKineticEnergy();
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| 200 | // G4double pPlab = aParticle->GetTotalMomentum();
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| 201 | G4double pM = aParticle->GetDefinition()->GetPDGMass();
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| 202 | // G4double tM = tZ*proton_mass_c2 + (tA-tZ)*neutron_mass_c2; // ~ 1% accuracy
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| 203 | G4double tM = G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass( G4int(tZ), G4int(tA) );
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| 204 | G4double pElab = pTkin + pM;
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| 205 | G4double totEcm = std::sqrt(pM*pM + tM*tM + 2.*pElab*tM);
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| 206 | // G4double pPcm = pPlab*tM/totEcm;
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| 207 | // G4double pTcm = std::sqrt(pM*pM + pPcm*pPcm) - pM;
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| 208 | G4double totTcm = totEcm - pM -tM;
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| 209 |
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| 210 | G4double bC = fine_structure_const*hbarc*pZ*tZ;
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| 211 | bC /= pR + tR;
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| 212 | bC /= 2.; // 4., 2. parametrisation cof ??? vmg
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| 213 |
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| 214 | // G4cout<<"pTkin = "<<pTkin/GeV<<"; pPlab = "
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| 215 | // <<pPlab/GeV<<"; bC = "<<bC/GeV<<"; pTcm = "<<pTcm/GeV<<G4endl;
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| 216 |
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| 217 | if( totTcm <= bC ) ratio = 0.;
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| 218 | else ratio = 1. - bC/totTcm;
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| 219 |
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| 220 | // if(ratio < DBL_MIN) ratio = DBL_MIN;
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| 221 | if( ratio < 0.) ratio = 0.;
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| 222 |
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| 223 | // G4cout <<"ratio = "<<ratio<<G4endl;
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| 224 | return ratio;
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| 225 | }
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| 226 |
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| 227 |
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| 228 | //////////////////////////////////////////////////////////////////////////
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| 229 | //
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| 230 | // Return single-diffraction/inelastic cross-section ratio
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| 231 |
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| 232 | G4double G4GGNuclNuclCrossSection::
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| 233 | GetRatioSD(const G4DynamicParticle* aParticle, G4double tA, G4double tZ)
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| 234 | {
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| 235 | G4double sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, ratio;
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| 236 |
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| 237 | G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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| 238 | G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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| 239 |
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| 240 | G4double pTkin = aParticle->GetKineticEnergy();
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| 241 | pTkin /= pA;
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| 242 |
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| 243 | G4double pN = pA - pZ;
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| 244 | if( pN < 0. ) pN = 0.;
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| 245 |
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| 246 | G4double tN = tA - tZ;
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| 247 | if( tN < 0. ) tN = 0.;
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| 248 |
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| 249 | G4double tR = GetNucleusRadius(tA);
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| 250 | G4double pR = GetNucleusRadius(pA);
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| 251 |
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| 252 | sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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| 253 | (pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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| 254 |
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| 255 | nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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| 256 |
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| 257 | ratio = sigma/nucleusSquare;
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| 258 |
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| 259 |
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| 260 | fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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| 261 |
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| 262 | G4double difratio = ratio/(1.+ratio);
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| 263 |
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| 264 | fDiffractionXsc = 0.5*nucleusSquare*( difratio - std::log( 1. + difratio ) );
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| 265 |
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| 266 | if (fInelasticXsc > 0.) ratio = fDiffractionXsc/fInelasticXsc;
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| 267 | else ratio = 0.;
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| 268 |
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| 269 | return ratio;
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| 270 | }
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| 271 |
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| 272 | //////////////////////////////////////////////////////////////////////////
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| 273 | //
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| 274 | // Return suasi-elastic/inelastic cross-section ratio
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| 275 |
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| 276 | G4double G4GGNuclNuclCrossSection::
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| 277 | GetRatioQE(const G4DynamicParticle* aParticle, G4double tA, G4double tZ)
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| 278 | {
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| 279 | G4double sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, ratio;
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| 280 |
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| 281 | G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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| 282 | G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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| 283 |
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| 284 | G4double pTkin = aParticle->GetKineticEnergy();
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| 285 | pTkin /= pA;
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| 286 |
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| 287 | G4double pN = pA - pZ;
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| 288 | if( pN < 0. ) pN = 0.;
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| 289 |
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| 290 | G4double tN = tA - tZ;
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| 291 | if( tN < 0. ) tN = 0.;
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| 292 |
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| 293 | G4double tR = GetNucleusRadius(tA);
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| 294 | G4double pR = GetNucleusRadius(pA);
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| 295 |
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| 296 | sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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| 297 | (pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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| 298 |
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| 299 | nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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| 300 |
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| 301 | ratio = sigma/nucleusSquare;
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| 302 |
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| 303 | fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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| 304 |
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| 305 | // sigma = GetHNinelasticXsc(aParticle, tA, tZ);
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| 306 | ratio = sigma/nucleusSquare;
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| 307 |
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| 308 | fProductionXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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| 309 |
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| 310 | if (fInelasticXsc > fProductionXsc) ratio = (fInelasticXsc-fProductionXsc)/fInelasticXsc;
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| 311 | else ratio = 0.;
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| 312 | if ( ratio < 0. ) ratio = 0.;
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| 313 |
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| 314 | return ratio;
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| 315 | }
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| 316 |
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| 317 | /////////////////////////////////////////////////////////////////////////////////////
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| 318 | //
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| 319 | // Returns hadron-nucleon Xsc according to differnt parametrisations:
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| 320 | // [2] E. Levin, hep-ph/9710546
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| 321 | // [3] U. Dersch, et al, hep-ex/9910052
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| 322 | // [4] M.J. Longo, et al, Phys.Rev.Lett. 33 (1974) 725
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| 323 |
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| 324 | G4double
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| 325 | G4GGNuclNuclCrossSection::GetHadronNucleonXsc(const G4DynamicParticle* aParticle,
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| 326 | const G4Element* anElement )
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| 327 | {
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| 328 | G4double At = anElement->GetN(); // number of nucleons
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| 329 | G4double Zt = anElement->GetZ(); // number of protons
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| 330 |
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| 331 |
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| 332 | return GetHadronNucleonXsc( aParticle, At, Zt );
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| 333 | }
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| 334 |
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| 335 |
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| 336 |
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| 337 |
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| 338 | /////////////////////////////////////////////////////////////////////////////////////
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| 339 | //
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| 340 | // Returns hadron-nucleon Xsc according to differnt parametrisations:
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| 341 | // [2] E. Levin, hep-ph/9710546
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| 342 | // [3] U. Dersch, et al, hep-ex/9910052
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| 343 | // [4] M.J. Longo, et al, Phys.Rev.Lett. 33 (1974) 725
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| 344 |
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| 345 | G4double
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| 346 | G4GGNuclNuclCrossSection::GetHadronNucleonXsc(const G4DynamicParticle* aParticle,
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| 347 | G4double At, G4double Zt )
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| 348 | {
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| 349 | G4double xsection = 0.;
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| 350 |
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| 351 |
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| 352 | G4double targ_mass = G4ParticleTable::GetParticleTable()->
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| 353 | GetIonTable()->GetIonMass( G4int(Zt+0.5) , G4int(At+0.5) );
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| 354 |
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| 355 | targ_mass = 0.939*GeV; // ~mean neutron and proton ???
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| 356 |
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| 357 | G4double proj_mass = aParticle->GetMass();
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| 358 | G4double proj_momentum = aParticle->GetMomentum().mag();
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| 359 | G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
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| 360 |
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| 361 | sMand /= GeV*GeV; // in GeV for parametrisation
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| 362 | proj_momentum /= GeV;
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| 363 |
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| 364 | const G4ParticleDefinition* pParticle = aParticle->GetDefinition();
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| 365 |
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| 366 |
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| 367 | if(pParticle == theNeutron) // as proton ???
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| 368 | {
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| 369 | xsection = At*(21.70*std::pow(sMand,0.0808) + 56.08*std::pow(sMand,-0.4525));
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| 370 | }
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| 371 | else if(pParticle == theProton)
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| 372 | {
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| 373 | xsection = At*(21.70*std::pow(sMand,0.0808) + 56.08*std::pow(sMand,-0.4525));
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| 374 | // xsection = At*( 49.51*std::pow(sMand,-0.097) + 0.314*std::log(sMand)*std::log(sMand) );
|
|---|
| 375 | // xsection = At*( 38.4 + 0.85*std::abs(std::pow(log(sMand),1.47)) );
|
|---|
| 376 | }
|
|---|
| 377 |
|
|---|
| 378 | xsection *= millibarn;
|
|---|
| 379 | return xsection;
|
|---|
| 380 | }
|
|---|
| 381 |
|
|---|
| 382 |
|
|---|
| 383 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 384 | //
|
|---|
| 385 | // Returns hadron-nucleon Xsc according to PDG parametrisation (2005):
|
|---|
| 386 | // http://pdg.lbl.gov/2006/reviews/hadronicrpp.pdf
|
|---|
| 387 |
|
|---|
| 388 | G4double
|
|---|
| 389 | G4GGNuclNuclCrossSection::GetHadronNucleonXscPDG(const G4DynamicParticle* aParticle,
|
|---|
| 390 | const G4Element* anElement )
|
|---|
| 391 | {
|
|---|
| 392 | G4double At = anElement->GetN(); // number of nucleons
|
|---|
| 393 | G4double Zt = anElement->GetZ(); // number of protons
|
|---|
| 394 |
|
|---|
| 395 |
|
|---|
| 396 | return GetHadronNucleonXscPDG( aParticle, At, Zt );
|
|---|
| 397 | }
|
|---|
| 398 |
|
|---|
| 399 |
|
|---|
| 400 |
|
|---|
| 401 |
|
|---|
| 402 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 403 | //
|
|---|
| 404 | // Returns hadron-nucleon Xsc according to PDG parametrisation (2005):
|
|---|
| 405 | // http://pdg.lbl.gov/2006/reviews/hadronicrpp.pdf
|
|---|
| 406 | // At = number of nucleons, Zt = number of protons
|
|---|
| 407 |
|
|---|
| 408 | G4double
|
|---|
| 409 | G4GGNuclNuclCrossSection::GetHadronNucleonXscPDG(const G4DynamicParticle* aParticle,
|
|---|
| 410 | G4double At, G4double Zt )
|
|---|
| 411 | {
|
|---|
| 412 | G4double xsection = 0.;
|
|---|
| 413 |
|
|---|
| 414 | G4double Nt = At-Zt; // number of neutrons
|
|---|
| 415 | if (Nt < 0.) Nt = 0.;
|
|---|
| 416 |
|
|---|
| 417 |
|
|---|
| 418 | G4double targ_mass = G4ParticleTable::GetParticleTable()->
|
|---|
| 419 | GetIonTable()->GetIonMass( G4int(Zt+0.5) , G4int(At+0.5) );
|
|---|
| 420 |
|
|---|
| 421 | targ_mass = 0.939*GeV; // ~mean neutron and proton ???
|
|---|
| 422 |
|
|---|
| 423 | G4double proj_mass = aParticle->GetMass();
|
|---|
| 424 | G4double proj_momentum = aParticle->GetMomentum().mag();
|
|---|
| 425 |
|
|---|
| 426 | G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
|
|---|
| 427 |
|
|---|
| 428 | sMand /= GeV*GeV; // in GeV for parametrisation
|
|---|
| 429 |
|
|---|
| 430 | // General PDG fit constants
|
|---|
| 431 |
|
|---|
| 432 | G4double s0 = 5.38*5.38; // in Gev^2
|
|---|
| 433 | G4double eta1 = 0.458;
|
|---|
| 434 | G4double eta2 = 0.458;
|
|---|
| 435 | G4double B = 0.308;
|
|---|
| 436 |
|
|---|
| 437 |
|
|---|
| 438 | const G4ParticleDefinition* pParticle = aParticle->GetDefinition();
|
|---|
| 439 |
|
|---|
| 440 |
|
|---|
| 441 | if(pParticle == theNeutron) // proton-neutron fit
|
|---|
| 442 | {
|
|---|
| 443 | xsection = Zt*( 35.80 + B*std::pow(std::log(sMand/s0),2.)
|
|---|
| 444 | + 40.15*std::pow(sMand,-eta1) - 30.*std::pow(sMand,-eta2));
|
|---|
| 445 | xsection += Nt*( 35.45 + B*std::pow(std::log(sMand/s0),2.)
|
|---|
| 446 | + 42.53*std::pow(sMand,-eta1) - 33.34*std::pow(sMand,-eta2)); // pp for nn
|
|---|
| 447 | }
|
|---|
| 448 | else if(pParticle == theProton)
|
|---|
| 449 | {
|
|---|
| 450 |
|
|---|
| 451 | xsection = Zt*( 35.45 + B*std::pow(std::log(sMand/s0),2.)
|
|---|
| 452 | + 42.53*std::pow(sMand,-eta1) - 33.34*std::pow(sMand,-eta2));
|
|---|
| 453 |
|
|---|
| 454 | xsection += Nt*( 35.80 + B*std::pow(std::log(sMand/s0),2.)
|
|---|
| 455 | + 40.15*std::pow(sMand,-eta1) - 30.*std::pow(sMand,-eta2));
|
|---|
| 456 | }
|
|---|
| 457 | xsection *= millibarn; // parametrised in mb
|
|---|
| 458 | return xsection;
|
|---|
| 459 | }
|
|---|
| 460 |
|
|---|
| 461 |
|
|---|
| 462 |
|
|---|
| 463 |
|
|---|
| 464 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 465 | //
|
|---|
| 466 | // Returns nucleon-nucleon cross-section based on N. Starkov parametrisation of
|
|---|
| 467 | // data from mainly http://wwwppds.ihep.su:8001/c5-6A.html database
|
|---|
| 468 | // projectile nucleon is pParticle with pTkin shooting target nucleon tParticle
|
|---|
| 469 |
|
|---|
| 470 | G4double
|
|---|
| 471 | G4GGNuclNuclCrossSection::GetHadronNucleonXscNS( G4ParticleDefinition* pParticle,
|
|---|
| 472 | G4double pTkin,
|
|---|
| 473 | G4ParticleDefinition* tParticle)
|
|---|
| 474 | {
|
|---|
| 475 | G4double xsection(0), Delta, A0, B0;
|
|---|
| 476 | G4double hpXsc(0);
|
|---|
| 477 | G4double hnXsc(0);
|
|---|
| 478 |
|
|---|
| 479 |
|
|---|
| 480 | G4double targ_mass = tParticle->GetPDGMass();
|
|---|
| 481 | G4double proj_mass = pParticle->GetPDGMass();
|
|---|
| 482 |
|
|---|
| 483 | G4double proj_energy = proj_mass + pTkin;
|
|---|
| 484 | G4double proj_momentum = std::sqrt(pTkin*(pTkin+2*proj_mass));
|
|---|
| 485 |
|
|---|
| 486 | G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
|
|---|
| 487 |
|
|---|
| 488 | sMand /= GeV*GeV; // in GeV for parametrisation
|
|---|
| 489 | proj_momentum /= GeV;
|
|---|
| 490 | proj_energy /= GeV;
|
|---|
| 491 | proj_mass /= GeV;
|
|---|
| 492 |
|
|---|
| 493 | // General PDG fit constants
|
|---|
| 494 |
|
|---|
| 495 | // G4double s0 = 5.38*5.38; // in Gev^2
|
|---|
| 496 | // G4double eta1 = 0.458;
|
|---|
| 497 | // G4double eta2 = 0.458;
|
|---|
| 498 | // G4double B = 0.308;
|
|---|
| 499 |
|
|---|
| 500 |
|
|---|
| 501 |
|
|---|
| 502 |
|
|---|
| 503 |
|
|---|
| 504 | if( proj_momentum >= 10. ) // high energy: pp = nn = np
|
|---|
| 505 | // if( proj_momentum >= 2.)
|
|---|
| 506 | {
|
|---|
| 507 | Delta = 1.;
|
|---|
| 508 |
|
|---|
| 509 | if( proj_energy < 40. ) Delta = 0.916+0.0021*proj_energy;
|
|---|
| 510 |
|
|---|
| 511 | if( proj_momentum >= 10.)
|
|---|
| 512 | {
|
|---|
| 513 | B0 = 7.5;
|
|---|
| 514 | A0 = 100. - B0*std::log(3.0e7);
|
|---|
| 515 |
|
|---|
| 516 | xsection = A0 + B0*std::log(proj_energy) - 11
|
|---|
| 517 | + 103*std::pow(2*0.93827*proj_energy + proj_mass*proj_mass+
|
|---|
| 518 | 0.93827*0.93827,-0.165); // mb
|
|---|
| 519 | }
|
|---|
| 520 | }
|
|---|
| 521 | else // low energy pp = nn != np
|
|---|
| 522 | {
|
|---|
| 523 | if(pParticle == tParticle) // pp or nn // nn to be pp
|
|---|
| 524 | {
|
|---|
| 525 | if( proj_momentum < 0.73 )
|
|---|
| 526 | {
|
|---|
| 527 | hnXsc = 23 + 50*( std::pow( std::log(0.73/proj_momentum), 3.5 ) );
|
|---|
| 528 | }
|
|---|
| 529 | else if( proj_momentum < 1.05 )
|
|---|
| 530 | {
|
|---|
| 531 | hnXsc = 23 + 40*(std::log(proj_momentum/0.73))*
|
|---|
| 532 | (std::log(proj_momentum/0.73));
|
|---|
| 533 | }
|
|---|
| 534 | else // if( proj_momentum < 10. )
|
|---|
| 535 | {
|
|---|
| 536 | hnXsc = 39.0 +
|
|---|
| 537 | 75*(proj_momentum - 1.2)/(std::pow(proj_momentum,3.0) + 0.15);
|
|---|
| 538 | }
|
|---|
| 539 | xsection = hnXsc;
|
|---|
| 540 | }
|
|---|
| 541 | else // pn to be np
|
|---|
| 542 | {
|
|---|
| 543 | if( proj_momentum < 0.8 )
|
|---|
| 544 | {
|
|---|
| 545 | hpXsc = 33+30*std::pow(std::log(proj_momentum/1.3),4.0);
|
|---|
| 546 | }
|
|---|
| 547 | else if( proj_momentum < 1.4 )
|
|---|
| 548 | {
|
|---|
| 549 | hpXsc = 33+30*std::pow(std::log(proj_momentum/0.95),2.0);
|
|---|
| 550 | }
|
|---|
| 551 | else // if( proj_momentum < 10. )
|
|---|
| 552 | {
|
|---|
| 553 | hpXsc = 33.3+
|
|---|
| 554 | 20.8*(std::pow(proj_momentum,2.0)-1.35)/
|
|---|
| 555 | (std::pow(proj_momentum,2.50)+0.95);
|
|---|
| 556 | }
|
|---|
| 557 | xsection = hpXsc;
|
|---|
| 558 | }
|
|---|
| 559 | }
|
|---|
| 560 | xsection *= millibarn; // parametrised in mb
|
|---|
| 561 | return xsection;
|
|---|
| 562 | }
|
|---|
| 563 |
|
|---|
| 564 | /*
|
|---|
| 565 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 566 | //
|
|---|
| 567 | // Returns hadron-nucleon inelastic cross-section based on proper parametrisation
|
|---|
| 568 |
|
|---|
| 569 | G4double
|
|---|
| 570 | G4GGNuclNuclCrossSection::GetHNinelasticXsc(const G4DynamicParticle* aParticle,
|
|---|
| 571 | const G4Element* anElement )
|
|---|
| 572 | {
|
|---|
| 573 | G4double At = anElement->GetN(); // number of nucleons
|
|---|
| 574 | G4double Zt = anElement->GetZ(); // number of protons
|
|---|
| 575 |
|
|---|
| 576 |
|
|---|
| 577 | return GetHNinelasticXsc( aParticle, At, Zt );
|
|---|
| 578 | }
|
|---|
| 579 |
|
|---|
| 580 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 581 | //
|
|---|
| 582 | // Returns hadron-nucleon inelastic cross-section based on FTF-parametrisation
|
|---|
| 583 |
|
|---|
| 584 | G4double
|
|---|
| 585 | G4GGNuclNuclCrossSection::GetHNinelasticXsc(const G4DynamicParticle* aParticle,
|
|---|
| 586 | G4double At, G4double Zt )
|
|---|
| 587 | {
|
|---|
| 588 | // G4ParticleDefinition* hadron = aParticle->GetDefinition();
|
|---|
| 589 | G4double sumInelastic, Nt = At - Zt;
|
|---|
| 590 |
|
|---|
| 591 | if(Nt < 0.) Nt = 0.;
|
|---|
| 592 |
|
|---|
| 593 | sumInelastic = Zt*GetHadronNucleonXscNS(aParticle, theProton);
|
|---|
| 594 | sumInelastic += Nt*GetHadronNucleonXscNS(aParticle, theNeutron);
|
|---|
| 595 |
|
|---|
| 596 | return sumInelastic;
|
|---|
| 597 | }
|
|---|
| 598 | */
|
|---|
| 599 |
|
|---|
| 600 | /////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 601 | //
|
|---|
| 602 | // Returns hadron-nucleon inelastic cross-section based on FTF-parametrisation
|
|---|
| 603 |
|
|---|
| 604 | G4double
|
|---|
| 605 | G4GGNuclNuclCrossSection::GetHNinelasticXscVU(const G4DynamicParticle* aParticle,
|
|---|
| 606 | G4double At, G4double Zt )
|
|---|
| 607 | {
|
|---|
| 608 | G4int PDGcode = aParticle->GetDefinition()->GetPDGEncoding();
|
|---|
| 609 | G4int absPDGcode = std::abs(PDGcode);
|
|---|
| 610 |
|
|---|
| 611 | G4double Elab = aParticle->GetTotalEnergy();
|
|---|
| 612 | // (s - 2*0.88*GeV*GeV)/(2*0.939*GeV)/GeV;
|
|---|
| 613 | G4double Plab = aParticle->GetMomentum().mag();
|
|---|
| 614 | // std::sqrt(Elab * Elab - 0.88);
|
|---|
| 615 |
|
|---|
| 616 | Elab /= GeV;
|
|---|
| 617 | Plab /= GeV;
|
|---|
| 618 |
|
|---|
| 619 | G4double LogPlab = std::log( Plab );
|
|---|
| 620 | G4double sqrLogPlab = LogPlab * LogPlab;
|
|---|
| 621 |
|
|---|
| 622 | //G4cout<<"Plab = "<<Plab<<G4endl;
|
|---|
| 623 |
|
|---|
| 624 | G4double NumberOfTargetProtons = Zt;
|
|---|
| 625 | G4double NumberOfTargetNucleons = At;
|
|---|
| 626 | G4double NumberOfTargetNeutrons = NumberOfTargetNucleons - NumberOfTargetProtons;
|
|---|
| 627 |
|
|---|
| 628 | if(NumberOfTargetNeutrons < 0.) NumberOfTargetNeutrons = 0.;
|
|---|
| 629 |
|
|---|
| 630 | G4double Xtotal = 0., Xelastic = 0., Xinelastic =0.;
|
|---|
| 631 |
|
|---|
| 632 | if( absPDGcode > 1000 ) //------Projectile is baryon --------
|
|---|
| 633 | {
|
|---|
| 634 | G4double XtotPP = 48.0 + 0. *std::pow(Plab, 0. ) +
|
|---|
| 635 | 0.522*sqrLogPlab - 4.51*LogPlab;
|
|---|
| 636 |
|
|---|
| 637 | G4double XtotPN = 47.3 + 0. *std::pow(Plab, 0. ) +
|
|---|
| 638 | 0.513*sqrLogPlab - 4.27*LogPlab;
|
|---|
| 639 |
|
|---|
| 640 | G4double XelPP = 11.9 + 26.9*std::pow(Plab,-1.21) +
|
|---|
| 641 | 0.169*sqrLogPlab - 1.85*LogPlab;
|
|---|
| 642 |
|
|---|
| 643 | G4double XelPN = 11.9 + 26.9*std::pow(Plab,-1.21) +
|
|---|
| 644 | 0.169*sqrLogPlab - 1.85*LogPlab;
|
|---|
| 645 |
|
|---|
| 646 | Xtotal = ( NumberOfTargetProtons * XtotPP +
|
|---|
| 647 | NumberOfTargetNeutrons * XtotPN );
|
|---|
| 648 |
|
|---|
| 649 | Xelastic = ( NumberOfTargetProtons * XelPP +
|
|---|
| 650 | NumberOfTargetNeutrons * XelPN );
|
|---|
| 651 | }
|
|---|
| 652 | Xinelastic = Xtotal - Xelastic;
|
|---|
| 653 |
|
|---|
| 654 | if(Xinelastic < 0.) Xinelastic = 0.;
|
|---|
| 655 |
|
|---|
| 656 | return Xinelastic*= millibarn;
|
|---|
| 657 | }
|
|---|
| 658 |
|
|---|
| 659 | ////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 660 | //
|
|---|
| 661 | //
|
|---|
| 662 |
|
|---|
| 663 | G4double
|
|---|
| 664 | G4GGNuclNuclCrossSection::GetNucleusRadius( const G4DynamicParticle* ,
|
|---|
| 665 | const G4Element* anElement)
|
|---|
| 666 | {
|
|---|
| 667 | G4double At = anElement->GetN();
|
|---|
| 668 | G4double oneThird = 1.0/3.0;
|
|---|
| 669 | G4double cubicrAt = std::pow (At, oneThird);
|
|---|
| 670 |
|
|---|
| 671 |
|
|---|
| 672 | G4double R; // = fRadiusConst*cubicrAt;
|
|---|
| 673 | /*
|
|---|
| 674 | G4double tmp = std::pow( cubicrAt-1., 3.);
|
|---|
| 675 | tmp += At;
|
|---|
| 676 | tmp *= 0.5;
|
|---|
| 677 |
|
|---|
| 678 | if (At > 20.) // 20.
|
|---|
| 679 | {
|
|---|
| 680 | R = fRadiusConst*std::pow (tmp, oneThird);
|
|---|
| 681 | }
|
|---|
| 682 | else
|
|---|
| 683 | {
|
|---|
| 684 | R = fRadiusConst*cubicrAt;
|
|---|
| 685 | }
|
|---|
| 686 | */
|
|---|
| 687 |
|
|---|
| 688 | R = fRadiusConst*cubicrAt;
|
|---|
| 689 |
|
|---|
| 690 | // return R; // !!!!
|
|---|
| 691 |
|
|---|
| 692 |
|
|---|
| 693 |
|
|---|
| 694 | G4double meanA = 21.;
|
|---|
| 695 |
|
|---|
| 696 | G4double tauA1 = 40.;
|
|---|
| 697 | G4double tauA2 = 10.;
|
|---|
| 698 | G4double tauA3 = 5.;
|
|---|
| 699 |
|
|---|
| 700 | G4double a1 = 0.85;
|
|---|
| 701 | G4double b1 = 1. - a1;
|
|---|
| 702 |
|
|---|
| 703 | G4double b2 = 0.3;
|
|---|
| 704 | G4double b3 = 4.;
|
|---|
| 705 |
|
|---|
| 706 | if (At > 20.) // 20.
|
|---|
| 707 | {
|
|---|
| 708 | R *= ( a1 + b1*std::exp( -(At - meanA)/tauA1) );
|
|---|
| 709 | }
|
|---|
| 710 | else if (At > 3.5)
|
|---|
| 711 | {
|
|---|
| 712 | R *= ( 1.0 + b2*( 1. - std::exp( (At - meanA)/tauA2) ) );
|
|---|
| 713 | }
|
|---|
| 714 | else
|
|---|
| 715 | {
|
|---|
| 716 | R *= ( 1.0 + b3*( 1. - std::exp( (At - meanA)/tauA3) ) );
|
|---|
| 717 | }
|
|---|
| 718 | return R;
|
|---|
| 719 |
|
|---|
| 720 | }
|
|---|
| 721 |
|
|---|
| 722 | ////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 723 | //
|
|---|
| 724 | //
|
|---|
| 725 |
|
|---|
| 726 | G4double
|
|---|
| 727 | G4GGNuclNuclCrossSection::GetNucleusRadius(G4double At)
|
|---|
| 728 | {
|
|---|
| 729 | G4double R;
|
|---|
| 730 |
|
|---|
| 731 | // R = GetNucleusRadiusGG(At);
|
|---|
| 732 |
|
|---|
| 733 | R = GetNucleusRadiusDE(At);
|
|---|
| 734 |
|
|---|
| 735 | return R;
|
|---|
| 736 | }
|
|---|
| 737 |
|
|---|
| 738 | ///////////////////////////////////////////////////////////////////
|
|---|
| 739 |
|
|---|
| 740 | G4double
|
|---|
| 741 | G4GGNuclNuclCrossSection::GetNucleusRadiusGG(G4double At)
|
|---|
| 742 | {
|
|---|
| 743 |
|
|---|
| 744 | G4double oneThird = 1.0/3.0;
|
|---|
| 745 | G4double cubicrAt = std::pow (At, oneThird);
|
|---|
| 746 |
|
|---|
| 747 |
|
|---|
| 748 | G4double R; // = fRadiusConst*cubicrAt;
|
|---|
| 749 |
|
|---|
| 750 | /*
|
|---|
| 751 | G4double tmp = std::pow( cubicrAt-1., 3.);
|
|---|
| 752 | tmp += At;
|
|---|
| 753 | tmp *= 0.5;
|
|---|
| 754 |
|
|---|
| 755 | if (At > 20.)
|
|---|
| 756 | {
|
|---|
| 757 | R = fRadiusConst*std::pow (tmp, oneThird);
|
|---|
| 758 | }
|
|---|
| 759 | else
|
|---|
| 760 | {
|
|---|
| 761 | R = fRadiusConst*cubicrAt;
|
|---|
| 762 | }
|
|---|
| 763 | */
|
|---|
| 764 |
|
|---|
| 765 | R = fRadiusConst*cubicrAt;
|
|---|
| 766 |
|
|---|
| 767 | G4double meanA = 20.;
|
|---|
| 768 | G4double tauA = 20.;
|
|---|
| 769 |
|
|---|
| 770 | if ( At > 20.) // 20.
|
|---|
| 771 | {
|
|---|
| 772 | R *= ( 0.8 + 0.2*std::exp( -(At - meanA)/tauA) );
|
|---|
| 773 | }
|
|---|
| 774 | else
|
|---|
| 775 | {
|
|---|
| 776 | R *= ( 1.0 + 0.1*( 1. - std::exp( (At - meanA)/tauA) ) );
|
|---|
| 777 | }
|
|---|
| 778 |
|
|---|
| 779 | return R;
|
|---|
| 780 |
|
|---|
| 781 | }
|
|---|
| 782 |
|
|---|
| 783 |
|
|---|
| 784 | G4double
|
|---|
| 785 | G4GGNuclNuclCrossSection::GetNucleusRadiusDE(G4double A)
|
|---|
| 786 | {
|
|---|
| 787 |
|
|---|
| 788 | // algorithm from diffuse-elastic
|
|---|
| 789 |
|
|---|
| 790 | G4double R, r0, a11, a12, a13, a2, a3;
|
|---|
| 791 |
|
|---|
| 792 | a11 = 1.26; // 1.08, 1.16
|
|---|
| 793 | a12 = 1.; // 1.08, 1.16
|
|---|
| 794 | a13 = 1.12; // 1.08, 1.16
|
|---|
| 795 | a2 = 1.1;
|
|---|
| 796 | a3 = 1.;
|
|---|
| 797 |
|
|---|
| 798 |
|
|---|
| 799 | if( A < 50. )
|
|---|
| 800 | {
|
|---|
| 801 | if( 10 < A && A <= 15. ) r0 = a11*( 1 - std::pow(A, -2./3.) )*fermi; // 1.08*fermi;
|
|---|
| 802 | else if( 15 < A && A <= 20 ) r0 = a12*( 1 - std::pow(A, -2./3.) )*fermi;
|
|---|
| 803 | else if( 20 < A && A <= 30 ) r0 = a13*( 1 - std::pow(A, -2./3.) )*fermi;
|
|---|
| 804 | else r0 = a2*fermi;
|
|---|
| 805 |
|
|---|
| 806 | R = r0*std::pow( A, 1./3. );
|
|---|
| 807 | }
|
|---|
| 808 | else
|
|---|
| 809 | {
|
|---|
| 810 | r0 = a3*fermi;
|
|---|
| 811 |
|
|---|
| 812 | R = r0*std::pow(A, 0.27);
|
|---|
| 813 | }
|
|---|
| 814 | return R;
|
|---|
| 815 | }
|
|---|
| 816 |
|
|---|
| 817 |
|
|---|
| 818 | ////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 819 | //
|
|---|
| 820 | //
|
|---|
| 821 |
|
|---|
| 822 | G4double G4GGNuclNuclCrossSection::CalculateEcmValue( const G4double mp ,
|
|---|
| 823 | const G4double mt ,
|
|---|
| 824 | const G4double Plab )
|
|---|
| 825 | {
|
|---|
| 826 | G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
|
|---|
| 827 | G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
|
|---|
| 828 | // G4double Pcm = Plab * mt / Ecm;
|
|---|
| 829 | // G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
|
|---|
| 830 |
|
|---|
| 831 | return Ecm ; // KEcm;
|
|---|
| 832 | }
|
|---|
| 833 |
|
|---|
| 834 |
|
|---|
| 835 | ////////////////////////////////////////////////////////////////////////////////////
|
|---|
| 836 | //
|
|---|
| 837 | //
|
|---|
| 838 |
|
|---|
| 839 | G4double G4GGNuclNuclCrossSection::CalcMandelstamS( const G4double mp ,
|
|---|
| 840 | const G4double mt ,
|
|---|
| 841 | const G4double Plab )
|
|---|
| 842 | {
|
|---|
| 843 | G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
|
|---|
| 844 | G4double sMand = mp*mp + mt*mt + 2*Elab*mt ;
|
|---|
| 845 |
|
|---|
| 846 | return sMand;
|
|---|
| 847 | }
|
|---|
| 848 |
|
|---|
| 849 |
|
|---|
| 850 | //
|
|---|
| 851 | //
|
|---|
| 852 | ///////////////////////////////////////////////////////////////////////////////////////
|
|---|