source: trunk/source/processes/hadronic/cross_sections/src/G4IonsShenCrossSection.cc @ 1355

Last change on this file since 1355 was 1347, checked in by garnier, 14 years ago

geant4 tag 9.4

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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#include "G4HadTmpUtil.hh"
36
37
38G4double G4IonsShenCrossSection::
39GetZandACrossSection(const G4DynamicParticle* aParticle, G4int ZZ, 
40                     G4int AA, G4double /*temperature*/)
41{
42   G4double xsection = 0.0;
43
44   G4int Ap = aParticle->GetDefinition()->GetBaryonNumber();
45   G4int Zp = G4int(aParticle->GetDefinition()->GetPDGCharge()/eplus + 0.5 ); 
46   G4double ke_per_N = aParticle->GetKineticEnergy() / Ap; 
47   if ( ke_per_N > 10*GeV ) ke_per_N = 10*GeV;
48
49// Apply energy check, if less than lower limit then 0 value is returned
50   // if (  ke_per_N < lowerLimit ) return xsection;
51
52   G4int At = AA;
53   G4int Zt = 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   G4double targ_mass =
66     G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass(Zt, At);
67   G4double proj_mass = aParticle->GetMass();
68   G4double proj_momentum = aParticle->GetMomentum().mag();
69
70   G4double Ecm = calEcmValue (proj_mass, targ_mass, proj_momentum); 
71
72   G4double B = 1.44 * Zt * Zp / r - b * Rt * Rp / ( Rt + Rp ); 
73   if(Ecm <= B) return xsection;
74   //G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
75
76   G4double c = calCeValue ( ke_per_N / MeV  ); 
77
78   G4double R1 = r0 * (cubicrAt + cubicrAp + 1.85*cubicrAt*cubicrAp/(cubicrAt + cubicrAp) - c); 
79
80   G4double R2 = 1.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
81
82
83   G4double R3 = 0.176 / std::pow(G4double(Ecm), G4double(one_third)) * cubicrAt * cubicrAp /(cubicrAt + cubicrAp);
84
85   G4double R = R1 + R2 + R3;
86
87   xsection = 10 * pi * R * R * ( 1 - B / Ecm );   
88   xsection = xsection * millibarn;   // mulitply xsection by millibarn
89
90   return xsection; 
91}
92
93
94G4double G4IonsShenCrossSection::
95GetCrossSection(const G4DynamicParticle* aParticle, const G4Element* anElement,
96                G4double temperature)
97{
98  G4int nIso = anElement->GetNumberOfIsotopes();
99  G4double xsection = 0;
100   
101  if (nIso) {
102    G4double sig;
103    G4IsotopeVector* isoVector = anElement->GetIsotopeVector();
104    G4double* abundVector = anElement->GetRelativeAbundanceVector();
105    G4int ZZ;
106    G4int AA;
107   
108    for (G4int i = 0; i < nIso; i++) {
109      ZZ = (*isoVector)[i]->GetZ();
110      AA = (*isoVector)[i]->GetN();
111      sig = GetZandACrossSection(aParticle, ZZ, AA, temperature);
112      xsection += sig*abundVector[i];
113    }
114 
115  } else {
116    G4int ZZ = G4lrint(anElement->GetZ());
117    G4int AA = G4lrint(anElement->GetN());
118    xsection = GetZandACrossSection(aParticle, ZZ, AA, temperature);
119  }
120 
121  return xsection;
122}
123
124
125G4double
126G4IonsShenCrossSection::calEcmValue(const G4double mp, const G4double mt,
127                                    const G4double Plab)
128{
129   G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
130   G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
131   G4double Pcm = Plab * mt / Ecm;
132   G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
133   return KEcm;
134}
135
136
137G4double G4IonsShenCrossSection::calCeValue(const G4double ke)
138{
139  // Calculate c value
140  // This value is indepenent from projectile and target particle
141  // ke is projectile kinetic energy per nucleon in the Lab system
142  // with MeV unit
143  // fitting function is made by T. Koi
144  // There are no data below 30 MeV/n in Kox et al.,
145
146   G4double Ce; 
147   G4double log10_ke = std::log10 ( ke );   
148   if (log10_ke > 1.5) 
149   {
150     Ce = -10.0/std::pow(G4double(log10_ke), G4double(5)) + 2.0;
151   }
152   else
153   {
154     Ce = (-10.0/std::pow(G4double(1.5), G4double(5) ) + 2.0) /
155         std::pow(G4double(1.5) , G4double(3)) * std::pow(G4double(log10_ke), G4double(3));
156   }
157   return Ce;
158}
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