G4CoulombBarrier.cc

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//
//
// Hadronic Process: Nuclear De-excitations
// by V. Lara (Dec 1999)
//
// 14-11-2007 modified barrier by JMQ (test30) 
// 15-11-2010 V.Ivanchenko use G4Pow and cleanup 
 
#include "G4CoulombBarrier.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
#include "G4NuclearRadii.hh"
 
namespace
{
  constexpr G4double e0 = 2*CLHEP::MeV;
}
 
G4CoulombBarrier::G4CoulombBarrier(G4int A, G4int Z)
  : G4VCoulombBarrier(A, Z)
{
  factor = CLHEP::elm_coupling*Z;
  theRho = 0.5*G4NuclearRadii::RadiusCB(Z, A);
}
 
G4double G4CoulombBarrier::GetCoulombBarrier(
         G4int ARes, G4int ZRes, G4double U) const 
{
  G4double cb = factor*ZRes/(G4NuclearRadii::RadiusCB(ZRes,ARes) + theRho);
  cb /= (1.0 + std::sqrt( U / ((ARes + theA)*e0)));
  return cb;
}
 
G4double G4CoulombBarrier::BarrierPenetrationFactor(G4int aZ) const 
{
  // Data comes from 
  // Dostrovsky, Fraenkel and Friedlander
  // Physical Review, vol 116, num. 3 1959
  // 
  // const G4int size = 5;
  // const G4double Zlist[size] = {10.0, 20.0, 30.0, 50.0, 70.0};
  // const G4double Kprot[size] = {0.42, 0.58, 0.68, 0.77, 0.80};
  // 
  G4double res = 1.0;
  if(theZ == 1) {
    res = (aZ >= 70) ? 0.80 :
    (((0.2357e-5*aZ) - 0.42679e-3)*aZ + 0.27035e-1)*aZ + 0.19025;
    res += 0.06*(theA - 1);
 
  } else if(theZ == 2 && theA <= 4) {
    res = (aZ >= 70) ? 0.98 :
    (((0.23684e-5*aZ) - 0.42143e-3)*aZ + 0.25222e-1)*aZ + 0.46699;
    res += 0.12*(4 - theA);
  }
  return res;
}