source: trunk/source/processes/hadronic/models/de_excitation/evaporation/src/G4NeutronEvaporationProbability.cc @ 1316

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//
//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 "G4NeutronEvaporationProbability.hh"

G4NeutronEvaporationProbability::G4NeutronEvaporationProbability() :
    G4EvaporationProbability(1,0,2,&theCoulombBarrier) // A,Z,Gamma,&theCoulombBarrier
{
  
}


G4NeutronEvaporationProbability::G4NeutronEvaporationProbability(const G4NeutronEvaporationProbability &) : G4EvaporationProbability()
{
    throw G4HadronicException(__FILE__, __LINE__, "G4NeutronEvaporationProbability::copy_constructor meant to not be accessable");
}




const G4NeutronEvaporationProbability & G4NeutronEvaporationProbability::
operator=(const G4NeutronEvaporationProbability &)
{
    throw G4HadronicException(__FILE__, __LINE__, "G4NeutronEvaporationProbability::operator= meant to not be accessable");
    return *this;
}


G4bool G4NeutronEvaporationProbability::operator==(const G4NeutronEvaporationProbability &) const
{
    return false;
}

G4bool G4NeutronEvaporationProbability::operator!=(const G4NeutronEvaporationProbability &) const
{
    return true;
}

 G4double G4NeutronEvaporationProbability::CalcAlphaParam(const G4Fragment & fragment) 
  { return 0.76+2.2/std::pow(static_cast<G4double>(fragment.GetA()-GetA()),1.0/3.0);}

        
  G4double G4NeutronEvaporationProbability::CalcBetaParam(const G4Fragment &  fragment) 
  { return (2.12/std::pow(static_cast<G4double>(fragment.GetA()-GetA()),2.0/3.0) - 0.05)*MeV/
      CalcAlphaParam(fragment); }


////////////////////////////////////////////////////////////////////////////////////
//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 G4NeutronEvaporationProbability::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 (neutrons)!!"  <<G4endl;
    throw G4HadronicException(__FILE__, __LINE__, errOs.str());
    return 0.;}
  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 AT EVAPORATION!!"  <<G4endl;
    throw G4HadronicException(__FILE__, __LINE__, errOs.str());
    return 0.;
  }
}






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

G4double G4NeutronEvaporationProbability::GetOpt12(const  G4double K)
{

  G4double Kc=K;

// 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 G4NeutronEvaporationProbability::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 *******************************