source: trunk/source/processes/hadronic/models/pre_equilibrium/exciton_model/src/G4PreCompoundNeutron.cc @ 1337

//
// ********************************************************************
// * 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: G4PreCompoundNeutron.cc,v 1.4 2009/02/11 18:06:00 vnivanch Exp $
// GEANT4 tag $Name: geant4-09-04-beta-01 $
//
// -------------------------------------------------------------------
//
// GEANT4 Class file
//
//
// File name:     G4PreCompoundNeutron
//
// Author:         V.Lara
//
// Modified:  
// 21.08.2008 J. M. Quesada add choice of options  
// 10.02.2009 J. M. Quesada set default opt3
// 

#include "G4PreCompoundNeutron.hh"

G4ReactionProduct * G4PreCompoundNeutron::GetReactionProduct() const
{
  G4ReactionProduct * theReactionProduct = 
    new G4ReactionProduct(G4Neutron::NeutronDefinition());
  theReactionProduct->SetMomentum(GetMomentum().vect());
  theReactionProduct->SetTotalEnergy(GetMomentum().e());
#ifdef PRECOMPOUND_TEST
  theReactionProduct->SetCreatorModel("G4PrecompoundModel");
#endif
  return theReactionProduct;
}

G4double G4PreCompoundNeutron::GetRj(const G4int NumberParticles, const G4int NumberCharged)
{
  G4double rj = 0.0;
  if(NumberParticles > 0) rj = static_cast<G4double>(NumberParticles - NumberCharged)/
                            static_cast<G4double>(NumberParticles);
  return rj;
}

////////////////////////////////////////////////////////////////////////////////////
//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 G4PreCompoundNeutron::CrossSection(const  G4double K)
{
  ResidualA=GetRestA();
  ResidualZ=GetRestZ(); 
  theA=GetA();
  theZ=GetZ();
  ResidualAthrd=std::pow(ResidualA,0.33333);
  FragmentA=GetA()+GetRestA();
  FragmentAthrd=std::pow(FragmentA,0.33333);

  if (OPTxs==0) return GetOpt0( K);
  else if( OPTxs==1 || OPTxs==2) return GetOpt12( K);
  else if (OPTxs==3 || OPTxs==4)  return GetOpt34( K);
  else{
    std::ostringstream errOs;
    errOs << "BAD NEUTRON CROSS SECTION OPTION !!"  <<G4endl;
    throw G4HadronicException(__FILE__, __LINE__, errOs.str());
    return 0.;
  }
}

// *********************** OPT=0 : Dostrovski's cross section  *****************************

G4double G4PreCompoundNeutron::GetOpt0(const  G4double K)
{
  
  const G4double r0 = G4PreCompoundParameters::GetAddress()->Getr0();
  // cross section is now given in mb (r0 is in mm) for the sake of consistency
  //with the rest of the options
  return 1.e+25*pi*(r0*ResidualAthrd)*(r0*ResidualAthrd)*GetAlpha()*(1.+GetBeta()/K);
}
//
//-------
//
G4double G4PreCompoundNeutron::GetAlpha()
{
  //   return 0.76+2.2/std::pow(GetRestA(),1.0/3.0);
  return 0.76+2.2/ResidualAthrd;
}
//
//------------
//
G4double G4PreCompoundNeutron::GetBeta() 
{
  //   return (2.12/std::pow(GetRestA(),2.0/3.0)-0.05)*MeV/GetAlpha();
  return (2.12/(ResidualAthrd*ResidualAthrd)-0.05)*MeV/GetAlpha();
}
//

//********************* OPT=1,2 : Chatterjee's cross section ************************ 
//(fitting to cross section from Bechetti & Greenles OM potential)

G4double G4PreCompoundNeutron::GetOpt12(const  G4double K)
{

  G4double Kc=K;

// Pramana (Bechetti & Greenles) for neutrons is chosen 

// JMQ  xsec is set constat above limit of validity
 if (K>50) Kc=50;

 G4double landa, landa0, landa1, mu, mu0, mu1,nu, nu0, nu1, nu2,xs;

 landa0 = 18.57;
 landa1 = -22.93;
 mu0 = 381.7;
 mu1 = 24.31;
 nu0 = 0.172;
 nu1 = -15.39;
 nu2 = 804.8;
 landa = landa0/ResidualAthrd + landa1;
 mu = mu0*ResidualAthrd + mu1*ResidualAthrd*ResidualAthrd;
 nu = nu0*ResidualAthrd*ResidualA + nu1*ResidualAthrd*ResidualAthrd + nu2 ;
 xs=landa*Kc + mu + nu/Kc;
 if (xs <= 0.0 ){
   std::ostringstream errOs;
   G4cout<<"WARNING:  NEGATIVE OPT=1 neutron cross section "<<G4endl;     
   errOs << "RESIDUAL: Ar=" << ResidualA << " Zr=" << ResidualZ <<G4endl;
   errOs <<"  xsec("<<Kc<<" MeV) ="<<xs <<G4endl;
   throw G4HadronicException(__FILE__, __LINE__, errOs.str());
              }
 return xs;
}


// *********** OPT=3,4 : Kalbach's cross sections (from PRECO code)*************
G4double G4PreCompoundNeutron::GetOpt34(const  G4double K)
{
  
  G4double landa, landa0, landa1, mu, mu0, mu1,nu, nu0, nu1, nu2;
  G4double p, p0, p1, p2;
  G4double flow,spill,ec,ecsq,xnulam,etest(0.),ra(0.),a,signor(1.),sig; 
  G4double b,ecut,cut,ecut2,geom,elab;

  //safety initialization
  landa0=0;
  landa1=0;
  mu0=0.;
  mu1=0.;
  nu0=0.;
  nu1=0.;
  nu2=0.;
  p0=0.;
  p1=0.;
  p2=0.;


  flow = 1.e-18;
  spill= 1.0e+18; 

  // PRECO xs for neutrons is choosen

  p0 = -312.;
  p1= 0.;
  p2 = 0.;
  landa0 = 12.10;
  landa1=  -11.27;
  mu0 = 234.1;
  mu1 = 38.26;
  nu0 = 1.55;
  nu1 = -106.1;
  nu2 = 1280.8; 

  if (ResidualA < 40.) signor=0.7+ResidualA*0.0075;
  if (ResidualA > 210.) signor = 1. + (ResidualA-210.)/250.;
  landa = landa0/ResidualAthrd + landa1;
  mu = mu0*ResidualAthrd + mu1*ResidualAthrd*ResidualAthrd;
  nu = nu0*ResidualAthrd*ResidualA + nu1*ResidualAthrd*ResidualAthrd + nu2;

  // JMQ very low energy behaviour corrected (problem  for A (apprx.)>60)
  if (nu < 0.)nu=-nu;

  ec = 0.5;
  ecsq = 0.25;
  p = p0;
  xnulam = 1.;
  etest = 32.;
  //          ** etest is the energy above which the rxn cross section is
  //          ** compared with the geometrical limit and the max taken.
  //          ** xnulam here is a dummy value to be used later.

  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<Ec 
    if (elab > ecut2)  sig = (p*elab*elab+a*elab+b) * signor;                
  }              //end for E<Ec
  else {           //start for  E>Ec
    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);

  }
  return sig;}

//   ************************** end of cross sections *******************************