source: trunk/source/processes/hadronic/models/de_excitation/evaporation/src/G4He3EvaporationProbability.cc @ 1315

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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 "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<G4double>(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)!!"  
               <<G4endl;
         throw G4HadronicException(__FILE__, __LINE__, errOs.str());
         return 0.;}
       if( OPTxs==1 || OPTxs==2) return G4He3EvaporationProbability::GetOpt12( K);
       else if (OPTxs==3 || OPTxs==4)  return G4He3EvaporationProbability::GetOpt34( K);
       else{
         std::ostringstream errOs;
         errOs << "BAD He3's 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 G4He3EvaporationProbability::GetOpt12(const  G4double K)
{

G4double Kc=K;

// JMQ xsec is set constat above limit of validity
 if (K>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;
  
  //JMQ 13/02/09 increase of reduced radius to lower the barrier
  // ec = 1.44 * theZ * ResidualZ / (1.5*ResidualAthrd+ra);
  ec = 1.44 * theZ * ResidualZ / (1.7*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;
//JMQ 290310 for avoiding unphysical increase below minimum (at ecut)
//ecut<0 means that there is no cut with energy axis, i.e. xs is set to 0 bellow minimum
//  if (cut < 0.) ecut2 = ecut - 2.;
  if (cut < 0.) ecut2 = ecut;
  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);
  }           //end for E>Ec
  return sig;
  
}

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