source: trunk/source/processes/electromagnetic/lowenergy/src/G4CrossSectionExcitationEmfietzoglouPartial.cc @ 846

Last change on this file since 846 was 819, checked in by garnier, 16 years ago

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26//
27// $Id: G4CrossSectionExcitationEmfietzoglouPartial.cc,v 1.2 2007/12/10 16:31:26 gunter Exp $
28// GEANT4 tag $Name:  $
29//
30// Contact Author: Maria Grazia Pia (Maria.Grazia.Pia@cern.ch)
31//
32// Reference: TNS Geant4-DNA paper
33// Reference for implementation model: NIM. 155, pp. 145-156, 1978
34
35// History:
36// -----------
37// Date         Name              Modification
38// 28 Apr 2007  M.G. Pia          Created in compliance with design described in TNS paper
39//
40// -------------------------------------------------------------------
41
42// Class description:
43// Geant4-DNA Cross total cross section for electron elastic scattering in water
44// Reference: TNS Geant4-DNA paper
45// S. Chauvie et al., Geant4 physics processes for microdosimetry simulation:
46// design foundation and implementation of the first set of models,
47// IEEE Trans. Nucl. Sci., vol. 54, no. 6, Dec. 2007.
48// Further documentation available from http://www.ge.infn.it/geant4/dna
49
50// -------------------------------------------------------------------
51
52
53#include "G4CrossSectionExcitationEmfietzoglouPartial.hh"
54#include "G4Track.hh"
55#include "G4DynamicParticle.hh"
56#include "G4ParticleDefinition.hh"
57#include "G4Electron.hh"
58
59#include "Randomize.hh"
60
61#include <deque>
62
63G4CrossSectionExcitationEmfietzoglouPartial::G4CrossSectionExcitationEmfietzoglouPartial()
64{
65
66  nLevels = waterExcitation.NumberOfLevels();
67  //G4cout << "Water excitation energy: number of levels = " << nLevels << G4endl;
68}
69
70
71G4CrossSectionExcitationEmfietzoglouPartial::~G4CrossSectionExcitationEmfietzoglouPartial()
72{ }
73 
74G4double G4CrossSectionExcitationEmfietzoglouPartial::CrossSection(G4double t, G4int level)
75{
76  //                 Aj                        T
77  // Sigma(T) = ------------- (Bj /  T) ln(Cj ---) [1 - Bj / T]^Pj
78  //             2 pi alpha0                   R
79  //
80  // Sigma is the macroscopic cross section = N sigma, where N = number of target particles per unit volume
81  // and sigma is the microscopic cross section
82  // T      is the incoming electron kinetic energy
83  // alpha0 is the Bohr Radius (Bohr_radius)
84  // Aj, Bj, Cj & Pj are parameters that can be found in Emfietzoglou's papers
85  //
86  //
87  // From Phys. Med. Biol. 48 (2003) 2355-2371, D.Emfietzoglou,
88  // Monte Carlo Simulation of the energy loss of low energy electrons in liquid Water
89 
90  // Scaling for macroscopic cross section: number of water moleculs per unit volume
91  // (capra) const G4double sigma0 = (10. / 3.343e22) * cm2;
92  const G4double density = 3.34192e+19 * mm3;
93
94  const G4double aj[]={0.0205, 0.0209, 0.0130, 0.0026, 0.0025};
95  const G4double cj[]={4.9801, 3.3850, 2.8095, 1.9242, 3.4624};
96  const G4double pj[]={0.4757, 0.3483, 0.4443, 0.3429, 0.4379};
97  const G4double r = 13.6 * eV;
98 
99  G4double sigma = 0.;
100 
101  G4double exc = waterExcitation.ExcitationEnergy(level);
102  // G4cout << "Water excitation energy " << exc/keV << " level = " << level << G4endl;
103
104  if (t >= exc)
105    {
106      G4double excitationSigma = ( aj[level] / (2.*pi*Bohr_radius)) 
107        * (exc / t) 
108        * std::log(cj[level]*(t/r)) 
109        * std::pow((1.- (exc/t)), pj[level]);
110      sigma = excitationSigma / density;
111    }
112  return sigma;
113}
114
115G4int G4CrossSectionExcitationEmfietzoglouPartial::RandomSelect(G4double k)
116{
117  G4int i = nLevels;
118  G4double value = 0.;
119  std::deque<double> values;
120 
121  // ---- MGP ---- The following algorithm is wrong: it works is the cross section
122  // is a monotone increasing function.
123  // The algorithm should be corrected by building the cumulative function
124  // of the cross section and comparing a random number in the range 0-1 against
125  // the cumulative value at each bin
126
127  while (i > 0)
128    {
129      i--;
130      G4double partial = CrossSection(k,i);
131      values.push_front(partial);
132      value += partial;
133    }
134
135    value *= G4UniformRand();
136   
137    i = nLevels;
138
139    while (i > 0)
140      {
141        i--;
142        if (values[i] > value) return i;
143        value -= values[i];
144      }
145   
146    return 0;
147}
148
149G4double G4CrossSectionExcitationEmfietzoglouPartial::Sum(G4double k)
150{
151  G4double totalCrossSection = 0.;
152
153  for (G4int i=0; i<nLevels; i++)
154    {
155      totalCrossSection += CrossSection(k,i);
156    }
157  return totalCrossSection;
158}
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