source: trunk/source/processes/hadronic/cross_sections/src/G4IonsShenCrossSection.cc @ 1199

Last change on this file since 1199 was 1055, checked in by garnier, 15 years ago

maj sur la beta de geant 4.9.3

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25//
26// 18-Sep-2003 First version is written by T. Koi
27// 12-Nov-2003 Add energy check at lower side T. Koi
28// 15-Nov-2006 Above 10GeV/n Cross Section become constant T. Koi (SLAC/SCCS)
29// 23-Dec-2006 Isotope dependence adde by D. Wright
30//
31
32#include "G4IonsShenCrossSection.hh"
33#include "G4ParticleTable.hh"
34#include "G4IonTable.hh"
35
36
37G4double G4IonsShenCrossSection::
38GetIsoZACrossSection(const G4DynamicParticle* aParticle, G4double ZZ, 
39                G4double AA, G4double /*temperature*/)
40{
41   G4double xsection = 0.0;
42
43   G4int Ap = aParticle->GetDefinition()->GetBaryonNumber();
44   G4int Zp = int ( aParticle->GetDefinition()->GetPDGCharge() / eplus + 0.5 ); 
45   G4double ke_per_N = aParticle->GetKineticEnergy() / Ap; 
46   if ( ke_per_N > 10*GeV ) ke_per_N = 10*GeV;
47
48// Apply energy check, if less than lower limit then 0 value is returned
49   // if (  ke_per_N < lowerLimit ) return xsection;
50
51   G4int At = G4int(AA);
52   G4int Zt = G4int(ZZ);
53 
54   G4double one_third = 1.0 / 3.0;
55
56   G4double cubicrAt = std::pow ( G4double(At) , G4double(one_third) ); 
57   G4double cubicrAp = std::pow ( G4double(Ap) , G4double(one_third) ); 
58
59   G4double Rt = 1.12 * cubicrAt - 0.94 * ( 1.0 / cubicrAt );
60   G4double Rp = 1.12 * cubicrAp - 0.94 * ( 1.0 / cubicrAp );
61
62   G4double r = Rt + Rp + 3.2;   // in fm
63   G4double b = 1.0;   // in MeV/fm
64   G4double targ_mass = G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass( Zt , At );
65   G4double proj_mass = aParticle->GetMass();
66   G4double proj_momentum = aParticle->GetMomentum().mag();
67
68   G4double Ecm = calEcmValue ( proj_mass , targ_mass , proj_momentum ); 
69
70   G4double B = 1.44 * Zt * Zp / r - b * Rt * Rp / ( Rt + Rp ); 
71   if(Ecm <= B) return xsection;
72   //G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
73
74   G4double c = calCeValue ( ke_per_N / MeV  ); 
75
76   G4double R1 = r0 * ( cubicrAt + cubicrAp + 1.85 * cubicrAt * cubicrAp / ( cubicrAt + cubicrAp ) - c); 
77
78   G4double R2 = 1.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
79
80
81   G4double R3 = 0.176 / std::pow ( G4double(Ecm) , G4double(one_third) ) * cubicrAt * cubicrAp / ( cubicrAt + cubicrAp );
82
83   G4double R = R1 + R2 + R3;
84
85   xsection = 10 * pi * R * R * ( 1 - B / Ecm );   
86   xsection = xsection * millibarn;   // mulitply xsection by millibarn   
87 
88   return xsection; 
89}
90
91
92G4double G4IonsShenCrossSection::
93GetCrossSection(const G4DynamicParticle* aParticle, const G4Element* anElement,
94                G4double temperature)
95{
96  G4int nIso = anElement->GetNumberOfIsotopes();
97  G4double xsection = 0;
98   
99  if (nIso) {
100    G4double sig;
101    G4IsotopeVector* isoVector = anElement->GetIsotopeVector();
102    G4double* abundVector = anElement->GetRelativeAbundanceVector();
103    G4double ZZ;
104    G4double AA;
105   
106    for (G4int i = 0; i < nIso; i++) {
107      ZZ = G4double( (*isoVector)[i]->GetZ() );
108      AA = G4double( (*isoVector)[i]->GetN() );
109      sig = GetIsoZACrossSection(aParticle, ZZ, AA, temperature);
110      xsection += sig*abundVector[i];
111    }
112 
113  } else {
114    xsection =
115      GetIsoZACrossSection(aParticle, anElement->GetZ(), anElement->GetN(), 
116                           temperature);
117  }
118 
119  return xsection;
120}
121
122
123G4double G4IonsShenCrossSection::calEcmValue( const G4double mp , const G4double mt , const G4double Plab )
124{
125   G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
126   G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
127   G4double Pcm = Plab * mt / Ecm;
128   G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
129   return KEcm;
130}
131
132
133G4double G4IonsShenCrossSection::calCeValue( const G4double ke )
134{
135   // Calculate c value
136   // This value is indepenent from projectile and target particle
137   // ke is projectile kinetic energy per nucleon in the Lab system with MeV unit
138   // fitting function is made by T. Koi
139   // There are no data below 30 MeV/n in Kox et al.,
140
141   G4double Ce; 
142   G4double log10_ke = std::log10 ( ke );   
143   if ( log10_ke > 1.5 ) 
144   {
145      Ce = - 10.0 / std::pow ( G4double(log10_ke) , G4double(5) ) + 2.0;
146   }
147   else
148   {
149      Ce = ( - 10.0 / std::pow ( G4double(1.5) , G4double(5) ) + 2.0 ) / std::pow ( G4double(1.5) , G4double(3) ) * std::pow ( G4double(log10_ke) , G4double(3) );
150   }
151   return Ce;
152}
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