source: trunk/source/processes/hadronic/cross_sections/src/G4IonsShenCrossSection.cc@ 1340

Last change on this file since 1340 was 1340, checked in by garnier, 15 years ago

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[819]1//
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24// ********************************************************************
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"
[1340]35#include "G4HadTmpUtil.hh"
[819]36
37
38G4double G4IonsShenCrossSection::
[1340]39GetZandACrossSection(const G4DynamicParticle* aParticle, G4int ZZ,
40 G4int AA, G4double /*temperature*/)
[819]41{
42 G4double xsection = 0.0;
43
44 G4int Ap = aParticle->GetDefinition()->GetBaryonNumber();
[1340]45 G4int Zp = G4int(aParticle->GetDefinition()->GetPDGCharge()/eplus + 0.5 );
[819]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
[1055]50 // if ( ke_per_N < lowerLimit ) return xsection;
[819]51
[1340]52 G4int At = AA;
53 G4int Zt = ZZ;
[819]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
[1340]65 G4double targ_mass =
66 G4ParticleTable::GetParticleTable()->GetIonTable()->GetIonMass(Zt, At);
[1055]67 G4double proj_mass = aParticle->GetMass();
68 G4double proj_momentum = aParticle->GetMomentum().mag();
[819]69
[1340]70 G4double Ecm = calEcmValue (proj_mass, targ_mass, proj_momentum);
[1055]71
[819]72 G4double B = 1.44 * Zt * Zp / r - b * Rt * Rp / ( Rt + Rp );
[1055]73 if(Ecm <= B) return xsection;
[819]74 //G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
75
76 G4double c = calCeValue ( ke_per_N / MeV );
77
[1340]78 G4double R1 = r0 * (cubicrAt + cubicrAp + 1.85*cubicrAt*cubicrAp/(cubicrAt + cubicrAp) - c);
[819]79
80 G4double R2 = 1.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
81
82
[1340]83 G4double R3 = 0.176 / std::pow(G4double(Ecm), G4double(one_third)) * cubicrAt * cubicrAp /(cubicrAt + cubicrAp);
[819]84
85 G4double R = R1 + R2 + R3;
86
87 xsection = 10 * pi * R * R * ( 1 - B / Ecm );
[1340]88 xsection = xsection * millibarn; // mulitply xsection by millibarn
89
[819]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();
[1340]105 G4int ZZ;
106 G4int AA;
[819]107
108 for (G4int i = 0; i < nIso; i++) {
[1340]109 ZZ = (*isoVector)[i]->GetZ();
110 AA = (*isoVector)[i]->GetN();
[819]111 sig = GetIsoZACrossSection(aParticle, ZZ, AA, temperature);
112 xsection += sig*abundVector[i];
113 }
114
115 } else {
[1340]116 G4int ZZ = G4lrint(anElement->GetZ());
117 G4int AA = G4lrint(anElement->GetN());
118 xsection = GetIsoZACrossSection(aParticle, ZZ, AA, temperature);
[819]119 }
120
121 return xsection;
122}
123
124
[1340]125G4double
126G4IonsShenCrossSection::calEcmValue(const G4double mp, const G4double mt,
127 const G4double Plab)
[819]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
[1340]137G4double G4IonsShenCrossSection::calCeValue(const G4double ke)
[819]138{
[1340]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.,
[819]145
146 G4double Ce;
147 G4double log10_ke = std::log10 ( ke );
[1340]148 if (log10_ke > 1.5)
[819]149 {
[1340]150 Ce = -10.0/std::pow(G4double(log10_ke), G4double(5)) + 2.0;
[819]151 }
152 else
153 {
[1340]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));
[819]156 }
157 return Ce;
158}
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