source: trunk/source/processes/hadronic/cross_sections/src/G4IonsShenCrossSection.cc @ 819

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

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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 )
50      return xsection;
51
52   G4int At = G4int(AA);
53   G4int Zt = G4int(ZZ);
54 
55   G4double one_third = 1.0 / 3.0;
56
57   G4double cubicrAt = std::pow ( G4double(At) , G4double(one_third) ); 
58   G4double cubicrAp = std::pow ( G4double(Ap) , G4double(one_third) ); 
59
60   G4double Rt = 1.12 * cubicrAt - 0.94 * ( 1.0 / cubicrAt );
61   G4double Rp = 1.12 * cubicrAp - 0.94 * ( 1.0 / cubicrAp );
62
63   G4double r = Rt + Rp + 3.2;   // in fm
64   G4double b = 1.0;   // in MeV/fm
65
66   G4double B = 1.44 * Zt * Zp / r - b * Rt * Rp / ( Rt + Rp ); 
67
68   //G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
69
70   G4double c = calCeValue ( ke_per_N / MeV  ); 
71
72   G4double R1 = r0 * ( cubicrAt + cubicrAp + 1.85 * cubicrAt * cubicrAp / ( cubicrAt + cubicrAp ) - c); 
73
74   G4double R2 = 1.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
75
76   G4double targ_mass = G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass( Zt , At );
77   G4double proj_mass = aParticle->GetMass();
78   G4double proj_momentum = aParticle->GetMomentum().mag();
79
80   G4double Ecm = calEcmValue ( proj_mass , targ_mass , proj_momentum ); 
81
82   G4double R3 = 0.176 / std::pow ( G4double(Ecm) , G4double(one_third) ) * cubicrAt * cubicrAp / ( cubicrAt + cubicrAp );
83
84   G4double R = R1 + R2 + R3;
85
86   xsection = 10 * pi * R * R * ( 1 - B / Ecm );   
87   xsection = xsection * millibarn;   // mulitply xsection by millibarn   
88 
89   return xsection; 
90}
91
92
93G4double G4IonsShenCrossSection::
94GetCrossSection(const G4DynamicParticle* aParticle, const G4Element* anElement,
95                G4double temperature)
96{
97  G4int nIso = anElement->GetNumberOfIsotopes();
98  G4double xsection = 0;
99   
100  if (nIso) {
101    G4double sig;
102    G4IsotopeVector* isoVector = anElement->GetIsotopeVector();
103    G4double* abundVector = anElement->GetRelativeAbundanceVector();
104    G4double ZZ;
105    G4double AA;
106   
107    for (G4int i = 0; i < nIso; i++) {
108      ZZ = G4double( (*isoVector)[i]->GetZ() );
109      AA = G4double( (*isoVector)[i]->GetN() );
110      sig = GetIsoZACrossSection(aParticle, ZZ, AA, temperature);
111      xsection += sig*abundVector[i];
112    }
113 
114  } else {
115    xsection =
116      GetIsoZACrossSection(aParticle, anElement->GetZ(), anElement->GetN(), 
117                           temperature);
118  }
119 
120  return xsection;
121}
122
123
124G4double G4IonsShenCrossSection::calEcmValue( const G4double mp , const G4double mt , const G4double Plab )
125{
126   G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
127   G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
128   G4double Pcm = Plab * mt / Ecm;
129   G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
130   return KEcm;
131}
132
133
134G4double G4IonsShenCrossSection::calCeValue( const G4double ke )
135{
136   // Calculate c value
137   // This value is indepenent from projectile and target particle
138   // ke is projectile kinetic energy per nucleon in the Lab system with MeV unit
139   // fitting function is made by T. Koi
140   // There are no data below 30 MeV/n in Kox et al.,
141
142   G4double Ce; 
143   G4double log10_ke = std::log10 ( ke );   
144   if ( log10_ke > 1.5 ) 
145   {
146      Ce = - 10.0 / std::pow ( G4double(log10_ke) , G4double(5) ) + 2.0;
147   }
148   else
149   {
150      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) );
151   }
152   return Ce;
153}
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