Import Geant4 9.2.0 source tree
This commit is contained in:
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// 24.11.08 V. Grichine - first implementation
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//
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#include "G4GGNuclNuclCrossSection.hh"
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#include "G4ParticleTable.hh"
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#include "G4IonTable.hh"
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#include "G4ParticleDefinition.hh"
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////////////////////////////////////////////////////////////////////////////////
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//
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//
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G4GGNuclNuclCrossSection::G4GGNuclNuclCrossSection()
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: fUpperLimit( 100000 * GeV ),
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fLowerLimit( 0.1 * GeV ),
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fRadiusConst( 1.08*fermi ) // 1.1, 1.3 ?
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{
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theProton = G4Proton::Proton();
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theNeutron = G4Neutron::Neutron();
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}
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///////////////////////////////////////////////////////////////////////////////////////
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//
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//
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G4GGNuclNuclCrossSection::~G4GGNuclNuclCrossSection()
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{
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}
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////////////////////////////////////////////////////////////////////////////////////////
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//
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//
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G4bool
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G4GGNuclNuclCrossSection::IsApplicable(const G4DynamicParticle* aDP,
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const G4Element* anElement)
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{
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return IsZAApplicable(aDP, anElement->GetZ(), anElement->GetN());
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}
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////////////////////////////////////////////////////////////////////////////////////////
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//
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//
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G4bool
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G4GGNuclNuclCrossSection::IsZAApplicable(const G4DynamicParticle* aDP,
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G4double Z, G4double)
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{
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G4bool applicable = false;
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// G4int baryonNumber = aDP->GetDefinition()->GetBaryonNumber();
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G4double kineticEnergy = aDP->GetKineticEnergy();
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// const G4ParticleDefinition* theParticle = aDP->GetDefinition();
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if ( kineticEnergy >= fLowerLimit && Z > 1.5 ) applicable = true;
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return applicable;
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}
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////////////////////////////////////////////////////////////////////////////////////////
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//
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// Calculates total and inelastic Xsc, derives elastic as total - inelastic accordong to
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// Glauber model with Gribov correction calculated in the dipole approximation on
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// light cone. Gaussian density helps to calculate rest integrals of the model.
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// [1] B.Z. Kopeliovich, nucl-th/0306044
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G4double G4GGNuclNuclCrossSection::
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GetCrossSection(const G4DynamicParticle* aParticle, const G4Element* anElement, G4double T)
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{
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return GetIsoZACrossSection(aParticle, anElement->GetZ(), anElement->GetN(), T);
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}
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////////////////////////////////////////////////////////////////////////////////////////
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//
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// Calculates total and inelastic Xsc, derives elastic as total - inelastic accordong to
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// Glauber model with Gribov correction calculated in the dipole approximation on
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// light cone. Gaussian density of point-like nucleons helps to calculate rest integrals of the model.
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// [1] B.Z. Kopeliovich, nucl-th/0306044 + simplification above
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G4double G4GGNuclNuclCrossSection::
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GetIsoZACrossSection(const G4DynamicParticle* aParticle, G4double tZ, G4double tA, G4double)
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{
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G4double xsection, sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, ratio;
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G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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G4double pTkin = aParticle->GetKineticEnergy();
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pTkin /= pA;
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G4double pN = pA - pZ;
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if( pN < 0. ) pN = 0.;
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G4double tN = tA - tZ;
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if( tN < 0. ) tN = 0.;
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G4double tR = GetNucleusRadius(tA);
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G4double pR = GetNucleusRadius(pA);
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sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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(pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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ratio = sigma/nucleusSquare;
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xsection = nucleusSquare*std::log( 1. + ratio );
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fTotalXsc = xsection;
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fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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fElasticXsc = fTotalXsc - fInelasticXsc;
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G4double difratio = ratio/(1.+ratio);
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fDiffractionXsc = 0.5*nucleusSquare*( difratio - std::log( 1. + difratio ) );
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// production to be checked !!! edit MK xsc
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sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscMK(theProton, pTkin, theProton) +
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(pZ*tN+pN*tZ)*GetHadronNucleonXscMK(theProton, pTkin, theNeutron);
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ratio = sigma/nucleusSquare;
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fProductionXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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if (fElasticXsc < 0.) fElasticXsc = 0.;
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return xsection;
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}
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//////////////////////////////////////////////////////////////////////////
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//
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// Return single-diffraction/inelastic cross-section ratio
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G4double G4GGNuclNuclCrossSection::
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GetRatioSD(const G4DynamicParticle* aParticle, G4double tA, G4double tZ)
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{
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G4double sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, ratio;
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G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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G4double pTkin = aParticle->GetKineticEnergy();
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pTkin /= pA;
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G4double pN = pA - pZ;
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if( pN < 0. ) pN = 0.;
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G4double tN = tA - tZ;
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if( tN < 0. ) tN = 0.;
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G4double tR = GetNucleusRadius(tA);
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G4double pR = GetNucleusRadius(pA);
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sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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(pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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ratio = sigma/nucleusSquare;
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fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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G4double difratio = ratio/(1.+ratio);
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fDiffractionXsc = 0.5*nucleusSquare*( difratio - std::log( 1. + difratio ) );
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if (fInelasticXsc > 0.) ratio = fDiffractionXsc/fInelasticXsc;
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else ratio = 0.;
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return ratio;
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}
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//////////////////////////////////////////////////////////////////////////
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//
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// Return suasi-elastic/inelastic cross-section ratio
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G4double G4GGNuclNuclCrossSection::
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GetRatioQE(const G4DynamicParticle* aParticle, G4double tA, G4double tZ)
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{
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G4double sigma, cofInelastic = 2.4, cofTotal = 2.0, nucleusSquare, ratio;
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G4double pZ = aParticle->GetDefinition()->GetPDGCharge();
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G4double pA = aParticle->GetDefinition()->GetBaryonNumber();
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G4double pTkin = aParticle->GetKineticEnergy();
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pTkin /= pA;
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G4double pN = pA - pZ;
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if( pN < 0. ) pN = 0.;
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G4double tN = tA - tZ;
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if( tN < 0. ) tN = 0.;
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G4double tR = GetNucleusRadius(tA);
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G4double pR = GetNucleusRadius(pA);
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sigma = (pZ*tZ+pN*tN)*GetHadronNucleonXscNS(theProton, pTkin, theProton) +
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(pZ*tN+pN*tZ)*GetHadronNucleonXscNS(theProton, pTkin, theNeutron);
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nucleusSquare = cofTotal*pi*( pR*pR + tR*tR ); // basically 2piRR
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ratio = sigma/nucleusSquare;
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fInelasticXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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// sigma = GetHNinelasticXsc(aParticle, tA, tZ);
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ratio = sigma/nucleusSquare;
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fProductionXsc = nucleusSquare*std::log( 1. + cofInelastic*ratio )/cofInelastic;
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if (fInelasticXsc > fProductionXsc) ratio = (fInelasticXsc-fProductionXsc)/fInelasticXsc;
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else ratio = 0.;
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if ( ratio < 0. ) ratio = 0.;
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return ratio;
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}
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/////////////////////////////////////////////////////////////////////////////////////
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//
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// Returns hadron-nucleon Xsc according to differnt parametrisations:
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// [2] E. Levin, hep-ph/9710546
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// [3] U. Dersch, et al, hep-ex/9910052
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// [4] M.J. Longo, et al, Phys.Rev.Lett. 33 (1974) 725
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G4double
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G4GGNuclNuclCrossSection::GetHadronNucleonXsc(const G4DynamicParticle* aParticle,
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const G4Element* anElement )
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{
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G4double At = anElement->GetN(); // number of nucleons
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G4double Zt = anElement->GetZ(); // number of protons
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return GetHadronNucleonXsc( aParticle, At, Zt );
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}
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/////////////////////////////////////////////////////////////////////////////////////
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//
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// Returns hadron-nucleon Xsc according to differnt parametrisations:
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// [2] E. Levin, hep-ph/9710546
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// [3] U. Dersch, et al, hep-ex/9910052
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// [4] M.J. Longo, et al, Phys.Rev.Lett. 33 (1974) 725
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G4double
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G4GGNuclNuclCrossSection::GetHadronNucleonXsc(const G4DynamicParticle* aParticle,
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G4double At, G4double Zt )
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{
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G4double xsection = 0.;
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G4double targ_mass = G4ParticleTable::GetParticleTable()->
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GetIonTable()->GetIonMass( G4int(Zt+0.5) , G4int(At+0.5) );
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targ_mass = 0.939*GeV; // ~mean neutron and proton ???
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G4double proj_mass = aParticle->GetMass();
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G4double proj_momentum = aParticle->GetMomentum().mag();
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G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
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sMand /= GeV*GeV; // in GeV for parametrisation
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proj_momentum /= GeV;
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const G4ParticleDefinition* pParticle = aParticle->GetDefinition();
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if(pParticle == theNeutron) // as proton ???
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{
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xsection = At*(21.70*std::pow(sMand,0.0808) + 56.08*std::pow(sMand,-0.4525));
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}
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else if(pParticle == theProton)
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{
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xsection = At*(21.70*std::pow(sMand,0.0808) + 56.08*std::pow(sMand,-0.4525));
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// xsection = At*( 49.51*std::pow(sMand,-0.097) + 0.314*std::log(sMand)*std::log(sMand) );
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// xsection = At*( 38.4 + 0.85*std::abs(std::pow(log(sMand),1.47)) );
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}
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xsection *= millibarn;
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return xsection;
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}
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/////////////////////////////////////////////////////////////////////////////////////
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//
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// Returns hadron-nucleon Xsc according to PDG parametrisation (2005):
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// http://pdg.lbl.gov/2006/reviews/hadronicrpp.pdf
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G4double
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G4GGNuclNuclCrossSection::GetHadronNucleonXscPDG(const G4DynamicParticle* aParticle,
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const G4Element* anElement )
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{
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G4double At = anElement->GetN(); // number of nucleons
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G4double Zt = anElement->GetZ(); // number of protons
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return GetHadronNucleonXscPDG( aParticle, At, Zt );
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}
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/////////////////////////////////////////////////////////////////////////////////////
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//
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// Returns hadron-nucleon Xsc according to PDG parametrisation (2005):
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// http://pdg.lbl.gov/2006/reviews/hadronicrpp.pdf
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// At = number of nucleons, Zt = number of protons
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G4double
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G4GGNuclNuclCrossSection::GetHadronNucleonXscPDG(const G4DynamicParticle* aParticle,
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G4double At, G4double Zt )
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{
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G4double xsection = 0.;
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G4double Nt = At-Zt; // number of neutrons
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if (Nt < 0.) Nt = 0.;
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G4double targ_mass = G4ParticleTable::GetParticleTable()->
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GetIonTable()->GetIonMass( G4int(Zt+0.5) , G4int(At+0.5) );
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targ_mass = 0.939*GeV; // ~mean neutron and proton ???
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G4double proj_mass = aParticle->GetMass();
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G4double proj_momentum = aParticle->GetMomentum().mag();
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G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
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sMand /= GeV*GeV; // in GeV for parametrisation
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// General PDG fit constants
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G4double s0 = 5.38*5.38; // in Gev^2
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G4double eta1 = 0.458;
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G4double eta2 = 0.458;
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G4double B = 0.308;
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const G4ParticleDefinition* pParticle = aParticle->GetDefinition();
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if(pParticle == theNeutron) // proton-neutron fit
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{
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xsection = Zt*( 35.80 + B*std::pow(std::log(sMand/s0),2.)
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+ 40.15*std::pow(sMand,-eta1) - 30.*std::pow(sMand,-eta2));
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xsection += Nt*( 35.45 + B*std::pow(std::log(sMand/s0),2.)
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+ 42.53*std::pow(sMand,-eta1) - 33.34*std::pow(sMand,-eta2)); // pp for nn
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}
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else if(pParticle == theProton)
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{
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xsection = Zt*( 35.45 + B*std::pow(std::log(sMand/s0),2.)
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+ 42.53*std::pow(sMand,-eta1) - 33.34*std::pow(sMand,-eta2));
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xsection += Nt*( 35.80 + B*std::pow(std::log(sMand/s0),2.)
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+ 40.15*std::pow(sMand,-eta1) - 30.*std::pow(sMand,-eta2));
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}
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xsection *= millibarn; // parametrised in mb
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return xsection;
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}
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||||
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||||
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/////////////////////////////////////////////////////////////////////////////////////
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//
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// Returns nucleon-nucleon cross-section based on N. Starkov parametrisation of
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// data from mainly http://wwwppds.ihep.su:8001/c5-6A.html database
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// projectile nucleon is pParticle with pTkin shooting target nucleon tParticle
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G4double
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G4GGNuclNuclCrossSection::GetHadronNucleonXscNS( G4ParticleDefinition* pParticle,
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G4double pTkin,
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G4ParticleDefinition* tParticle)
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{
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G4double xsection(0), Delta, A0, B0;
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G4double hpXsc(0);
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G4double hnXsc(0);
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G4double targ_mass = tParticle->GetPDGMass();
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G4double proj_mass = pParticle->GetPDGMass();
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G4double proj_energy = proj_mass + pTkin;
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G4double proj_momentum = std::sqrt(pTkin*(pTkin+2*proj_mass));
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G4double sMand = CalcMandelstamS ( proj_mass , targ_mass , proj_momentum );
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sMand /= GeV*GeV; // in GeV for parametrisation
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proj_momentum /= GeV;
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||||
proj_energy /= GeV;
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proj_mass /= GeV;
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||||
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||||
// General PDG fit constants
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||||
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||||
// G4double s0 = 5.38*5.38; // in Gev^2
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||||
// G4double eta1 = 0.458;
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||||
// G4double eta2 = 0.458;
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||||
// G4double B = 0.308;
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||||
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||||
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||||
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||||
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||||
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if( proj_momentum >= 10. ) // high energy: pp = nn = np
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// if( proj_momentum >= 2.)
|
||||
{
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||||
Delta = 1.;
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||||
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||||
if( proj_energy < 40. ) Delta = 0.916+0.0021*proj_energy;
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||||
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||||
if( proj_momentum >= 10.)
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||||
{
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||||
B0 = 7.5;
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||||
A0 = 100. - B0*std::log(3.0e7);
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||||
|
||||
xsection = A0 + B0*std::log(proj_energy) - 11
|
||||
+ 103*std::pow(2*0.93827*proj_energy + proj_mass*proj_mass+
|
||||
0.93827*0.93827,-0.165); // mb
|
||||
}
|
||||
}
|
||||
else // low energy pp = nn != np
|
||||
{
|
||||
if(pParticle == tParticle) // pp or nn // nn to be pp
|
||||
{
|
||||
if( proj_momentum < 0.73 )
|
||||
{
|
||||
hnXsc = 23 + 50*( std::pow( std::log(0.73/proj_momentum), 3.5 ) );
|
||||
}
|
||||
else if( proj_momentum < 1.05 )
|
||||
{
|
||||
hnXsc = 23 + 40*(std::log(proj_momentum/0.73))*
|
||||
(std::log(proj_momentum/0.73));
|
||||
}
|
||||
else // if( proj_momentum < 10. )
|
||||
{
|
||||
hnXsc = 39.0 +
|
||||
75*(proj_momentum - 1.2)/(std::pow(proj_momentum,3.0) + 0.15);
|
||||
}
|
||||
xsection = hnXsc;
|
||||
}
|
||||
else // pn to be np
|
||||
{
|
||||
if( proj_momentum < 0.8 )
|
||||
{
|
||||
hpXsc = 33+30*std::pow(std::log(proj_momentum/1.3),4.0);
|
||||
}
|
||||
else if( proj_momentum < 1.4 )
|
||||
{
|
||||
hpXsc = 33+30*std::pow(std::log(proj_momentum/0.95),2.0);
|
||||
}
|
||||
else // if( proj_momentum < 10. )
|
||||
{
|
||||
hpXsc = 33.3+
|
||||
20.8*(std::pow(proj_momentum,2.0)-1.35)/
|
||||
(std::pow(proj_momentum,2.50)+0.95);
|
||||
}
|
||||
xsection = hpXsc;
|
||||
}
|
||||
}
|
||||
xsection *= millibarn; // parametrised in mb
|
||||
return xsection;
|
||||
}
|
||||
|
||||
/*
|
||||
/////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
// Returns hadron-nucleon inelastic cross-section based on proper parametrisation
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetHNinelasticXsc(const G4DynamicParticle* aParticle,
|
||||
const G4Element* anElement )
|
||||
{
|
||||
G4double At = anElement->GetN(); // number of nucleons
|
||||
G4double Zt = anElement->GetZ(); // number of protons
|
||||
|
||||
|
||||
return GetHNinelasticXsc( aParticle, At, Zt );
|
||||
}
|
||||
|
||||
/////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
// Returns hadron-nucleon inelastic cross-section based on FTF-parametrisation
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetHNinelasticXsc(const G4DynamicParticle* aParticle,
|
||||
G4double At, G4double Zt )
|
||||
{
|
||||
// G4ParticleDefinition* hadron = aParticle->GetDefinition();
|
||||
G4double sumInelastic, Nt = At - Zt;
|
||||
|
||||
if(Nt < 0.) Nt = 0.;
|
||||
|
||||
sumInelastic = Zt*GetHadronNucleonXscMK(aParticle, theProton);
|
||||
sumInelastic += Nt*GetHadronNucleonXscMK(aParticle, theNeutron);
|
||||
|
||||
return sumInelastic;
|
||||
}
|
||||
*/
|
||||
|
||||
/////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
// Returns hadron-nucleon inelastic cross-section based on FTF-parametrisation
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetHNinelasticXscVU(const G4DynamicParticle* aParticle,
|
||||
G4double At, G4double Zt )
|
||||
{
|
||||
G4int PDGcode = aParticle->GetDefinition()->GetPDGEncoding();
|
||||
G4int absPDGcode = std::abs(PDGcode);
|
||||
|
||||
G4double Elab = aParticle->GetTotalEnergy();
|
||||
// (s - 2*0.88*GeV*GeV)/(2*0.939*GeV)/GeV;
|
||||
G4double Plab = aParticle->GetMomentum().mag();
|
||||
// std::sqrt(Elab * Elab - 0.88);
|
||||
|
||||
Elab /= GeV;
|
||||
Plab /= GeV;
|
||||
|
||||
G4double LogPlab = std::log( Plab );
|
||||
G4double sqrLogPlab = LogPlab * LogPlab;
|
||||
|
||||
//G4cout<<"Plab = "<<Plab<<G4endl;
|
||||
|
||||
G4double NumberOfTargetProtons = Zt;
|
||||
G4double NumberOfTargetNucleons = At;
|
||||
G4double NumberOfTargetNeutrons = NumberOfTargetNucleons - NumberOfTargetProtons;
|
||||
|
||||
if(NumberOfTargetNeutrons < 0.) NumberOfTargetNeutrons = 0.;
|
||||
|
||||
G4double Xtotal = 0., Xelastic = 0., Xinelastic =0.;
|
||||
|
||||
if( absPDGcode > 1000 ) //------Projectile is baryon --------
|
||||
{
|
||||
G4double XtotPP = 48.0 + 0. *std::pow(Plab, 0. ) +
|
||||
0.522*sqrLogPlab - 4.51*LogPlab;
|
||||
|
||||
G4double XtotPN = 47.3 + 0. *std::pow(Plab, 0. ) +
|
||||
0.513*sqrLogPlab - 4.27*LogPlab;
|
||||
|
||||
G4double XelPP = 11.9 + 26.9*std::pow(Plab,-1.21) +
|
||||
0.169*sqrLogPlab - 1.85*LogPlab;
|
||||
|
||||
G4double XelPN = 11.9 + 26.9*std::pow(Plab,-1.21) +
|
||||
0.169*sqrLogPlab - 1.85*LogPlab;
|
||||
|
||||
Xtotal = ( NumberOfTargetProtons * XtotPP +
|
||||
NumberOfTargetNeutrons * XtotPN );
|
||||
|
||||
Xelastic = ( NumberOfTargetProtons * XelPP +
|
||||
NumberOfTargetNeutrons * XelPN );
|
||||
}
|
||||
Xinelastic = Xtotal - Xelastic;
|
||||
|
||||
if(Xinelastic < 0.) Xinelastic = 0.;
|
||||
|
||||
return Xinelastic*= millibarn;
|
||||
}
|
||||
|
||||
/////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
// Returns hadron-nucleon cross-section based on Mikhail Kossov CHIPS parametrisation of
|
||||
// data from G4QuasiFreeRatios class
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetHadronNucleonXscMK(G4ParticleDefinition* pParticle, G4double pTkin,
|
||||
G4ParticleDefinition* nucleon )
|
||||
{
|
||||
G4int I = -1;
|
||||
G4int PDG = pParticle->GetPDGEncoding();
|
||||
G4double totalXsc = 0;
|
||||
G4double elasticXsc = 0;
|
||||
G4double inelasticXsc;
|
||||
// G4int absPDG = std::abs(PDG);
|
||||
|
||||
G4double pM = pParticle->GetPDGMass();
|
||||
G4double p = std::sqrt(pTkin*(pTkin+2*pM))/GeV;
|
||||
|
||||
G4bool F = false;
|
||||
if(nucleon == theProton) F = true;
|
||||
else if(nucleon == theNeutron) F = false;
|
||||
else
|
||||
{
|
||||
G4cout << "nucleon is not proton or neutron, return xsc for proton" << G4endl;
|
||||
F = true;
|
||||
}
|
||||
|
||||
G4bool kfl = true; // Flag of K0/aK0 oscillation
|
||||
G4bool kf = false;
|
||||
|
||||
if( PDG == 130 || PDG == 310 )
|
||||
{
|
||||
kf = true;
|
||||
if( G4UniformRand() > .5 ) kfl = false;
|
||||
}
|
||||
if ( (PDG == 2212 && F) || (PDG == 2112 && !F) ) I = 0; // pp/nn
|
||||
else if( (PDG == 2112 && F) || (PDG == 2212 && !F) ) I = 1; // np/pn
|
||||
else
|
||||
{
|
||||
G4cout<<"MK PDG = "<<PDG
|
||||
<<", while it is defined only for p,n,hyperons,anti-baryons,pi,K/antiK"<<G4endl;
|
||||
G4Exception("G4QuasiFreeRatio::FetchElTot:","22",FatalException,"CHIPScrash");
|
||||
}
|
||||
|
||||
// Each parameter set can have not more than nPoints = 128 parameters
|
||||
|
||||
static const G4double lmi = 3.5; // min of (lnP-lmi)^2 parabola
|
||||
static const G4double pbe = .0557; // elastic (lnP-lmi)^2 parabola coefficient
|
||||
static const G4double pbt = .3; // total (lnP-lmi)^2 parabola coefficient
|
||||
static const G4double pmi = .1; // Below that fast LE calculation is made
|
||||
static const G4double pma = 1000.; // Above that fast HE calculation is made
|
||||
|
||||
if( p <= 0.)
|
||||
{
|
||||
G4cout<<" p = "<<p<<" is zero or negative"<<G4endl;
|
||||
|
||||
elasticXsc = 0.;
|
||||
inelasticXsc = 0.;
|
||||
totalXsc = 0.;
|
||||
|
||||
return totalXsc;
|
||||
}
|
||||
if (!I) // pp/nn
|
||||
{
|
||||
if( p < pmi )
|
||||
{
|
||||
G4double p2 = p*p;
|
||||
elasticXsc = 1./(.00012 + p2*.2);
|
||||
totalXsc = elasticXsc;
|
||||
}
|
||||
else if(p>pma)
|
||||
{
|
||||
G4double lp = std::log(p)-lmi;
|
||||
G4double lp2 = lp*lp;
|
||||
elasticXsc = pbe*lp2 + 6.72;
|
||||
totalXsc = pbt*lp2 + 38.2;
|
||||
}
|
||||
else
|
||||
{
|
||||
G4double p2 = p*p;
|
||||
G4double LE = 1./( .00012 + p2*.2);
|
||||
G4double lp = std::log(p) - lmi;
|
||||
G4double lp2 = lp*lp;
|
||||
G4double rp2 = 1./p2;
|
||||
elasticXsc = LE + ( pbe*lp2 + 6.72+32.6/p)/( 1. + rp2/p);
|
||||
totalXsc = LE + ( pbt*lp2 + 38.2+52.7*rp2)/( 1. + 2.72*rp2*rp2);
|
||||
}
|
||||
}
|
||||
else if( I==1 ) // np/pn
|
||||
{
|
||||
if( p < pmi )
|
||||
{
|
||||
G4double p2 = p*p;
|
||||
elasticXsc = 1./( .00012 + p2*( .051 + .1*p2));
|
||||
totalXsc = elasticXsc;
|
||||
}
|
||||
else if( p > pma )
|
||||
{
|
||||
G4double lp = std::log(p) - lmi;
|
||||
G4double lp2 = lp*lp;
|
||||
elasticXsc = pbe*lp2 + 6.72;
|
||||
totalXsc = pbt*lp2 + 38.2;
|
||||
}
|
||||
else
|
||||
{
|
||||
G4double p2 = p*p;
|
||||
G4double LE = 1./( .00012 + p2*( .051 + .1*p2 ) );
|
||||
G4double lp = std::log(p) - lmi;
|
||||
G4double lp2 = lp*lp;
|
||||
G4double rp2 = 1./p2;
|
||||
elasticXsc = LE + (pbe*lp2 + 6.72 + 30./p)/( 1. + .49*rp2/p);
|
||||
totalXsc = LE + (pbt*lp2 + 38.2)/( 1. + .54*rp2*rp2);
|
||||
}
|
||||
}
|
||||
else
|
||||
{
|
||||
G4cout<<"PDG incoding = "<<I<<" is not defined (0-1)"<<G4endl;
|
||||
|
||||
}
|
||||
if( elasticXsc > totalXsc ) elasticXsc = totalXsc;
|
||||
|
||||
totalXsc *= millibarn;
|
||||
elasticXsc *= millibarn;
|
||||
inelasticXsc = totalXsc - elasticXsc;
|
||||
if (inelasticXsc < 0.) inelasticXsc = 0.;
|
||||
|
||||
return inelasticXsc;
|
||||
}
|
||||
|
||||
////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
//
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetNucleusRadius( const G4DynamicParticle* ,
|
||||
const G4Element* anElement)
|
||||
{
|
||||
G4double At = anElement->GetN();
|
||||
G4double oneThird = 1.0/3.0;
|
||||
G4double cubicrAt = std::pow (At, oneThird);
|
||||
|
||||
|
||||
G4double R; // = fRadiusConst*cubicrAt;
|
||||
/*
|
||||
G4double tmp = std::pow( cubicrAt-1., 3.);
|
||||
tmp += At;
|
||||
tmp *= 0.5;
|
||||
|
||||
if (At > 20.) // 20.
|
||||
{
|
||||
R = fRadiusConst*std::pow (tmp, oneThird);
|
||||
}
|
||||
else
|
||||
{
|
||||
R = fRadiusConst*cubicrAt;
|
||||
}
|
||||
*/
|
||||
|
||||
R = fRadiusConst*cubicrAt;
|
||||
|
||||
// return R; // !!!!
|
||||
|
||||
|
||||
|
||||
G4double meanA = 21.;
|
||||
|
||||
G4double tauA1 = 40.;
|
||||
G4double tauA2 = 10.;
|
||||
G4double tauA3 = 5.;
|
||||
|
||||
G4double a1 = 0.85;
|
||||
G4double b1 = 1. - a1;
|
||||
|
||||
G4double b2 = 0.3;
|
||||
G4double b3 = 4.;
|
||||
|
||||
if (At > 20.) // 20.
|
||||
{
|
||||
R *= ( a1 + b1*std::exp( -(At - meanA)/tauA1) );
|
||||
}
|
||||
else if (At > 3.5)
|
||||
{
|
||||
R *= ( 1.0 + b2*( 1. - std::exp( (At - meanA)/tauA2) ) );
|
||||
}
|
||||
else
|
||||
{
|
||||
R *= ( 1.0 + b3*( 1. - std::exp( (At - meanA)/tauA3) ) );
|
||||
}
|
||||
return R;
|
||||
|
||||
}
|
||||
|
||||
////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
//
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetNucleusRadius(G4double At)
|
||||
{
|
||||
G4double R;
|
||||
|
||||
// R = GetNucleusRadiusGG(At);
|
||||
|
||||
R = GetNucleusRadiusDE(At);
|
||||
|
||||
return R;
|
||||
}
|
||||
|
||||
///////////////////////////////////////////////////////////////////
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetNucleusRadiusGG(G4double At)
|
||||
{
|
||||
|
||||
G4double oneThird = 1.0/3.0;
|
||||
G4double cubicrAt = std::pow (At, oneThird);
|
||||
|
||||
|
||||
G4double R; // = fRadiusConst*cubicrAt;
|
||||
|
||||
/*
|
||||
G4double tmp = std::pow( cubicrAt-1., 3.);
|
||||
tmp += At;
|
||||
tmp *= 0.5;
|
||||
|
||||
if (At > 20.)
|
||||
{
|
||||
R = fRadiusConst*std::pow (tmp, oneThird);
|
||||
}
|
||||
else
|
||||
{
|
||||
R = fRadiusConst*cubicrAt;
|
||||
}
|
||||
*/
|
||||
|
||||
R = fRadiusConst*cubicrAt;
|
||||
|
||||
G4double meanA = 20.;
|
||||
G4double tauA = 20.;
|
||||
|
||||
if ( At > 20.) // 20.
|
||||
{
|
||||
R *= ( 0.8 + 0.2*std::exp( -(At - meanA)/tauA) );
|
||||
}
|
||||
else
|
||||
{
|
||||
R *= ( 1.0 + 0.1*( 1. - std::exp( (At - meanA)/tauA) ) );
|
||||
}
|
||||
|
||||
return R;
|
||||
|
||||
}
|
||||
|
||||
|
||||
G4double
|
||||
G4GGNuclNuclCrossSection::GetNucleusRadiusDE(G4double A)
|
||||
{
|
||||
|
||||
// algorithm from diffuse-elastic
|
||||
|
||||
G4double R, r0, a11, a12, a13, a2, a3;
|
||||
|
||||
a11 = 1.26; // 1.08, 1.16
|
||||
a12 = 1.; // 1.08, 1.16
|
||||
a13 = 1.12; // 1.08, 1.16
|
||||
a2 = 1.1;
|
||||
a3 = 1.;
|
||||
|
||||
|
||||
if( A < 50. )
|
||||
{
|
||||
if( 10 < A && A <= 15. ) r0 = a11*( 1 - std::pow(A, -2./3.) )*fermi; // 1.08*fermi;
|
||||
else if( 15 < A && A <= 20 ) r0 = a12*( 1 - std::pow(A, -2./3.) )*fermi;
|
||||
else if( 20 < A && A <= 30 ) r0 = a13*( 1 - std::pow(A, -2./3.) )*fermi;
|
||||
else r0 = a2*fermi;
|
||||
|
||||
R = r0*std::pow( A, 1./3. );
|
||||
}
|
||||
else
|
||||
{
|
||||
r0 = a3*fermi;
|
||||
|
||||
R = r0*std::pow(A, 0.27);
|
||||
}
|
||||
return R;
|
||||
|
||||
|
||||
|
||||
}
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
|
||||
////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
//
|
||||
|
||||
G4double G4GGNuclNuclCrossSection::CalculateEcmValue( const G4double mp ,
|
||||
const G4double mt ,
|
||||
const G4double Plab )
|
||||
{
|
||||
G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
|
||||
G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
|
||||
// G4double Pcm = Plab * mt / Ecm;
|
||||
// G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
|
||||
|
||||
return Ecm ; // KEcm;
|
||||
}
|
||||
|
||||
|
||||
////////////////////////////////////////////////////////////////////////////////////
|
||||
//
|
||||
//
|
||||
|
||||
G4double G4GGNuclNuclCrossSection::CalcMandelstamS( const G4double mp ,
|
||||
const G4double mt ,
|
||||
const G4double Plab )
|
||||
{
|
||||
G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
|
||||
G4double sMand = mp*mp + mt*mt + 2*Elab*mt ;
|
||||
|
||||
return sMand;
|
||||
}
|
||||
|
||||
|
||||
//
|
||||
//
|
||||
///////////////////////////////////////////////////////////////////////////////////////
|
||||
Reference in New Issue
Block a user