// // ******************************************************************** // * 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. * // ******************************************************************** // //J.M. Quesada (August2008). Based on: // // Hadronic Process: Nuclear De-excitations // by V. Lara (Oct 1998) // // Modif (03 September 2008) by J. M. Quesada for external choice of inverse // cross section option #include "G4He3EvaporationProbability.hh" G4He3EvaporationProbability::G4He3EvaporationProbability() : G4EvaporationProbability(3,2,2,&theCoulombBarrier) // A,Z,Gamma,&theCoulombBarrier { } G4He3EvaporationProbability::G4He3EvaporationProbability(const G4He3EvaporationProbability &) : G4EvaporationProbability() { throw G4HadronicException(__FILE__, __LINE__, "G4He3EvaporationProbability::copy_constructor meant to not be accessable"); } const G4He3EvaporationProbability & G4He3EvaporationProbability:: operator=(const G4He3EvaporationProbability &) { throw G4HadronicException(__FILE__, __LINE__, "G4He3EvaporationProbability::operator= meant to not be accessable"); return *this; } G4bool G4He3EvaporationProbability::operator==(const G4He3EvaporationProbability &) const { return false; } G4bool G4He3EvaporationProbability::operator!=(const G4He3EvaporationProbability &) const { return true; } G4double G4He3EvaporationProbability::CalcAlphaParam(const G4Fragment & fragment) { return 1.0 + CCoeficient(static_cast(fragment.GetZ()-GetZ()));} G4double G4He3EvaporationProbability::CalcBetaParam(const G4Fragment & ) { return 0.0; } G4double G4He3EvaporationProbability::CCoeficient(const G4double aZ) { // Data comes from // Dostrovsky, Fraenkel and Friedlander // Physical Review, vol 116, num. 3 1959 // // const G4int size = 5; // G4double Zlist[5] = { 10.0, 20.0, 30.0, 50.0, 70.0}; // G4double Calpha[5] = { 0.10, 0.10, 0.10, 0.08, 0.06}; // C for He3 is equal to C for alpha times 4/3 G4double C = 0.0; if (aZ <= 30) { C = 0.10; } else if (aZ <= 50) { C = 0.1 + -((aZ-50.)/20.)*0.02; } else if (aZ < 70) { C = 0.08 + -((aZ-70.)/20.)*0.02; } else { C = 0.06; } return C*(4.0/3.0); } /////////////////////////////////////////////////////////////////////////////////// //J. M. Quesada (Dec 2007-June 2008): New inverse reaction cross sections //OPT=0 Dostrovski's parameterization //OPT=1,2 Chatterjee's paramaterization //OPT=3,4 Kalbach's parameterization // G4double G4He3EvaporationProbability::CrossSection(const G4Fragment & fragment, const G4double K) { theA=GetA(); theZ=GetZ(); ResidualA=fragment.GetA()-theA; ResidualZ=fragment.GetZ()-theZ; ResidualAthrd=std::pow(ResidualA,0.33333); FragmentA=fragment.GetA(); FragmentAthrd=std::pow(FragmentA,0.33333); if (OPTxs==0) {std::ostringstream errOs; errOs << "We should'n be here (OPT =0) at evaporation cross section calculation (He3's)!!" <50) Kc=50; G4double landa ,mu ,nu ,p , Ec,q,r,ji,xs; G4double p0 = -3.06; G4double p1 = 278.5; G4double p2 = -1389.; G4double landa0 = -0.00535; G4double landa1 = -11.16; G4double mu0 = 555.5; G4double mu1 = 0.40; G4double nu0 = 687.4; G4double nu1 = -476.3; G4double nu2 = 0.509; G4double delta=1.2; Ec = 1.44*theZ*ResidualZ/(1.5*ResidualAthrd+delta); p = p0 + p1/Ec + p2/(Ec*Ec); landa = landa0*ResidualA + landa1; mu = mu0*std::pow(ResidualA,mu1); nu = std::pow(ResidualA,mu1)*(nu0 + nu1*Ec + nu2*(Ec*Ec)); q = landa - nu/(Ec*Ec) - 2*p*Ec; r = mu + 2*nu/Ec + p*(Ec*Ec); ji=std::max(Kc,Ec); if(Kc < Ec) { xs = p*Kc*Kc + q*Kc + r;} else {xs = p*(Kc - ji)*(Kc - ji) + landa*Kc + mu + nu*(2 - Kc/ji)/ji ;} if (xs <0.0) {xs=0.0;} return xs; } // *********** OPT=3,4 : Kalbach's cross sections (from PRECO code)************* G4double G4He3EvaporationProbability::GetOpt34(const G4double K) //c ** 3he from o.m. of gibson et al { G4double landa, mu, nu, p , signor(1.),sig; G4double ec,ecsq,xnulam,etest(0.),a; G4double b,ecut,cut,ecut2,geom,elab; G4double flow = 1.e-18; G4double spill= 1.e+18; G4double p0 = -2.88; G4double p1 = 205.6; G4double p2 = -1487.; G4double landa0 = 0.00459; G4double landa1 = -8.93; G4double mu0 = 611.2; G4double mu1 = 0.35; G4double nu0 = 473.8; G4double nu1 = -468.2; G4double nu2 = -2.225; G4double ra=0.80; ec = 1.44 * theZ * ResidualZ / (1.5*ResidualAthrd+ra); ecsq = ec * ec; p = p0 + p1/ec + p2/ecsq; landa = landa0*ResidualA + landa1; a = std::pow(ResidualA,mu1); mu = mu0 * a; nu = a* (nu0+nu1*ec+nu2*ecsq); xnulam = nu / landa; if (xnulam > spill) xnulam=0.; if (xnulam >= flow) etest = 1.2 *std::sqrt(xnulam); a = -2.*p*ec + landa - nu/ecsq; b = p*ecsq + mu + 2.*nu/ec; ecut = 0.; cut = a*a - 4.*p*b; if (cut > 0.) ecut = std::sqrt(cut); ecut = (ecut-a) / (p+p); ecut2 = ecut; if (cut < 0.) ecut2 = ecut - 2.; elab = K * FragmentA / ResidualA; sig = 0.; if (elab <= ec) { //start for E ecut2) sig = (p*elab*elab+a*elab+b) * signor; } //end for EEc sig = (landa*elab+mu+nu/elab) * signor; geom = 0.; if (xnulam < flow || elab < etest) return sig; geom = std::sqrt(theA*K); geom = 1.23*ResidualAthrd + ra + 4.573/geom; geom = 31.416 * geom * geom; sig = std::max(geom,sig); } //end for E>Ec return sig; } // ************************** end of cross sections *******************************