// // ******************************************************************** // * 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. * // ******************************************************************** // // $Id: G4HETCFragment.cc,v 1.4 2010/08/28 15:16:55 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-03-ref-09 $ // // by V. Lara // // Modified: // 23.08.2010 V.Ivanchenko general cleanup, move constructor and destructor // the source, use G4Pow #include "G4HETCFragment.hh" #include "G4PreCompoundParameters.hh" G4HETCFragment:: G4HETCFragment(const G4ParticleDefinition* part, G4VCoulombBarrier* aCoulombBarrier) : G4VPreCompoundFragment(part, aCoulombBarrier) { G4double r0 = theParameters->Getr0(); r2norm = r0*r0/(CLHEP::pi*CLHEP::hbarc*CLHEP::hbarc*CLHEP::hbarc); } G4HETCFragment::~G4HETCFragment() {} G4double G4HETCFragment:: CalcEmissionProbability(const G4Fragment & aFragment) { if (GetEnergyThreshold() <= 0.0) { theEmissionProbability = 0.0; return 0.0; } // Coulomb barrier is the lower limit // of integration over kinetic energy G4double LowerLimit = theCoulombBarrier; // Excitation energy of nucleus after fragment emission is the upper limit // of integration over kinetic energy G4double UpperLimit = GetMaximalKineticEnergy(); theEmissionProbability = IntegrateEmissionProbability(LowerLimit,UpperLimit,aFragment); return theEmissionProbability; } G4double G4HETCFragment:: IntegrateEmissionProbability(const G4double & Low, const G4double & Up, const G4Fragment & aFragment) { if ( !IsItPossible(aFragment) ) { return 0.0; } G4double U = aFragment.GetExcitationEnergy(); G4int P = aFragment.GetNumberOfParticles(); G4int H = aFragment.GetNumberOfHoles(); G4int N = P + H; G4int Pb = P - GetA(); G4int Nb = Pb + H; if (Nb <= 0.0) { return 0.0; } G4double g = (6.0/pi2)*aFragment.GetA()*theParameters->GetLevelDensity(); G4double gb = (6.0/pi2)*GetRestA()*theParameters->GetLevelDensity(); G4double A = G4double(P*P+H*H+P-3*H)/(4.0*g); G4double Ab = G4double(Pb*Pb+H*H+Pb-3*H)/(4.0*gb); U = std::max(U-A,0.0); if (U <= 0.0) { return 0.0; } G4int Pf = P; G4int Hf = H; G4int Nf = N-1; for (G4int i = 1; i < GetA(); ++i) { Pf *= (P-i); Hf *= (H-i); Nf *= (N-1-i); } G4double X = std::max(Up - Ab + GetBeta(),0.0); G4double Y = std::max(Up - Ab - Low, 0.0); G4double Probability = r2norm*GetSpinFactor()*GetReducedMass()*GetAlpha() *g4pow->Z23(GetRestA())*Pf*Hf*Nf*K(aFragment)*(X/Nb - Y/(Nb+1)) *U*g4pow->powN(g*gb,Nb)/g4pow->powN(g*U,N); // G4double Probability = GetSpinFactor()/(pi*hbarc*hbarc*hbarc) // * GetReducedMass() * GetAlpha() * // r0 * r0 * std::pow->Z23(GetRestA())/std::pow->pow(U,G4double(N-1)) * // (std::pow->(gb,Nb)/std::pow(g,N)) * Pf * Hf * Nf * K(aFragment) * // std::pow(Y,Nb) * (X/Nb - Y/(Nb+1)); return Probability; }