// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // By JPW, working, but to be cleaned up. @@@ // G.Folger, 29-sept-2006: extend to 1TeV, using a constant above 20GeV // 22 Dec 2006 - DHW added isotope dependence // G.Folger, 25-Nov-2009: extend to 100TeV, using a constant above 20GeV // #include "G4ProtonInelasticCrossSection.hh" #include "globals.hh" G4double G4ProtonInelasticCrossSection:: GetCrossSection(const G4DynamicParticle* aPart, const G4Element* anEle, G4double /*aTemperature*/) { G4int nIso = anEle->GetNumberOfIsotopes(); G4double KE = aPart->GetKineticEnergy(); G4double cross_section = 0; if (nIso) { G4double psig; G4IsotopeVector* isoVector = anEle->GetIsotopeVector(); G4double* abundVector = anEle->GetRelativeAbundanceVector(); G4double ZZ; G4double AA; for (G4int i = 0; i < nIso; i++) { ZZ = G4double( (*isoVector)[i]->GetZ() ); AA = G4double( (*isoVector)[i]->GetN() ); psig = GetCrossSection(KE, AA, ZZ); cross_section += psig*abundVector[i]; } } else { cross_section = GetCrossSection(KE, anEle->GetN(), anEle->GetZ()); } return cross_section; } G4double G4ProtonInelasticCrossSection:: GetCrossSection(G4double kineticEnergy, G4double atomicNumber, G4double nOfProtons) { if (kineticEnergy > 19.9*GeV ) { // constant cross section above ~20GeV. return GetCrossSection(19.8*GeV,atomicNumber,nOfProtons); } G4double nOfNeutrons = atomicNumber-nOfProtons; kineticEnergy /=GeV; G4double a = atomicNumber; const G4double nuleonRadius=1.36E-15; const G4double pi=3.14159265; G4double fac=pi*nuleonRadius*nuleonRadius; G4double b0=2.247-0.915*(1-std::pow(a,-0.3333)); G4double fac1=b0*(1-std::pow(a,-0.3333)); G4double fac2=1.; if(nOfNeutrons>1.5) fac2=std::log((nOfNeutrons)); G4double crossSection = 1E31*fac*fac2*(1+std::pow(a,0.3333)-fac1); // high energy correction crossSection = (1-0.15*std::exp(-kineticEnergy))*crossSection/(1.00-0.0007*a); // first try on low energies: rise G4double ff1= 0.70-0.002*a; // slope of the drop at medium energies. G4double ff2= 1.00+1/a; // start of the slope. G4double ff3= 0.8+18/a-0.002*a; // stephight fac = 1.0; if (kineticEnergy > DBL_MIN) fac= 1.0 - (1.0/(1+std::exp(-8*ff1*(std::log10(kineticEnergy)+1.37*ff2)))); crossSection = crossSection*(1+ff3*fac); // low energy return to zero ff1=1.-1/a-0.001*a; // slope of the rise ff2=1.17-2.7/a-0.0014*a; // start of the rise fac = 0.0; if (kineticEnergy > DBL_MIN) { fac=-8.*ff1*(std::log10(kineticEnergy)+2.0*ff2); fac=1/(1+std::exp(fac)); } crossSection = crossSection*fac; return crossSection*millibarn; }