source: trunk/source/processes/electromagnetic/lowenergy/src/G4CrossSectionExcitationEmfietzoglouPartial.cc @ 1315

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// $Id: G4CrossSectionExcitationEmfietzoglouPartial.cc,v 1.4 2009/06/10 13:32:36 mantero Exp $
// GEANT4 tag $Name: geant4-09-04-beta-cand-01 $

#include "G4CrossSectionExcitationEmfietzoglouPartial.hh"

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G4CrossSectionExcitationEmfietzoglouPartial::G4CrossSectionExcitationEmfietzoglouPartial()
{
  nLevels = waterExcitation.NumberOfLevels();
}

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G4CrossSectionExcitationEmfietzoglouPartial::~G4CrossSectionExcitationEmfietzoglouPartial()
{}
 
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G4double G4CrossSectionExcitationEmfietzoglouPartial::CrossSection(G4double t, G4int level)
{
  //                 Aj                        T
  // Sigma(T) = ------------- (Bj /  T) ln(Cj ---) [1 - Bj / T]^Pj
  //             2 pi alpha0                   R
  //
  // Sigma is the macroscopic cross section = N sigma, where N = number of target particles per unit volume
  // and sigma is the microscopic cross section
  // T      is the incoming electron kinetic energy
  // alpha0 is the Bohr Radius (Bohr_radius)
  // Aj, Bj, Cj & Pj are parameters that can be found in Emfietzoglou's papers
  //
  // From Phys. Med. Biol. 48 (2003) 2355-2371, D.Emfietzoglou,
  // Monte Carlo Simulation of the energy loss of low energy electrons in liquid Water
  //
  // Scaling for macroscopic cross section: number of water moleculs per unit volume
  // const G4double sigma0 = (10. / 3.343e22) * cm2;

  const G4double density = 3.34192e+19 * mm3;

  const G4double aj[]={0.0205, 0.0209, 0.0130, 0.0026, 0.0025};
  const G4double cj[]={4.9801, 3.3850, 2.8095, 1.9242, 3.4624};
  const G4double pj[]={0.4757, 0.3483, 0.4443, 0.3429, 0.4379};
  const G4double r = 13.6 * eV;
  
  G4double sigma = 0.;
  
  G4double exc = waterExcitation.ExcitationEnergy(level);
  
  if (t >= exc)
    {
      G4double excitationSigma = ( aj[level] / (2.*pi*Bohr_radius)) 
        * (exc / t) 
        * std::log(cj[level]*(t/r)) 
        * std::pow((1.- (exc/t)), pj[level]);
      sigma = excitationSigma / density;
    }
  return sigma;
}

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G4int G4CrossSectionExcitationEmfietzoglouPartial::RandomSelect(G4double k)
{
  G4int i = nLevels;
  G4double value = 0.;
  std::deque<double> values;
  
  // ---- MGP ---- The following algorithm is wrong: it works if the cross section 
  // is a monotone increasing function.
  // The algorithm should be corrected by building the cumulative function 
  // of the cross section and comparing a random number in the range 0-1 against
  // the cumulative value at each bin 

  while (i > 0)
  {
    i--;
    G4double partial = CrossSection(k,i);
    values.push_front(partial);
    value += partial;
  }

  value *= G4UniformRand();
    
  i = nLevels;

  while (i > 0)
  {
    i--;
    if (values[i] > value) return i;
    value -= values[i];
  }
    
  return 0;
}

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G4double G4CrossSectionExcitationEmfietzoglouPartial::Sum(G4double k)
{
  G4double totalCrossSection = 0.;

  for (G4int i=0; i<nLevels; i++)
  {
    totalCrossSection += CrossSection(k,i);
  }
  return totalCrossSection;
}