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G4IonsKoxCrossSection.cc
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26 // 18-Sep-2003 First version is written by T. Koi
27 // 10-Nov-2003 Bug fix at Cal. ke_per_n and D T. Koi
28 // 12-Nov-2003 Add energy check at lower side T. Koi
29 // 26-Dec-2006 Add isotope dependence D. Wright
30 // 14-Mar-2011 Moved constructor, destructor and virtual methods to source by V.Ivanchenko
31 // 19-Aug-2011 V.Ivanchenko move to new design and make x-section per element
32 
33 #include "G4IonsKoxCrossSection.hh"
34 #include "G4PhysicalConstants.hh"
35 #include "G4SystemOfUnits.hh"
36 #include "G4DynamicParticle.hh"
37 #include "G4NucleiProperties.hh"
38 #include "G4HadTmpUtil.hh"
39 #include "G4NistManager.hh"
40 
42  : G4VCrossSectionDataSet("IonsKox"), lowerLimit ( 10*MeV ),
43  r0 ( 1.1*fermi ), rc ( 1.3*fermi )
44 {}
45 
47 {}
48 
49 void
51 {
52  outFile << "G4IonsKoxCrossSection calculates the total reaction cross\n"
53  << "section for nucleus-nucleus scattering using the Kox\n"
54  << "parameterization. It is valid for projectiles and targets\n"
55  << "of all Z, at projectile energies up to 10 GeV/n. If the\n"
56  << "projectile energy is less than 10 MeV/n, a zero cross section\n"
57  << "is returned.\n";
58 }
59 
61  G4int, const G4Material*)
62 {
63  return (1 <= aDP->GetDefinition()->GetBaryonNumber());
64 }
65 
66 G4double
68  const G4DynamicParticle* aParticle, G4int ZZ, const G4Material*)
69 {
70  G4double xsection = 0.0;
71 
72  G4int Ap = aParticle->GetDefinition()->GetBaryonNumber();
73  G4int Zp = G4int(aParticle->GetDefinition()->GetPDGCharge() / eplus + 0.5);
74  G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
75 
76  // Apply energy check, if less than lower limit then 0 value is returned
77  // if ( ke_per_N < lowerLimit ) return xsection;
78 
79  G4int At = G4lrint(G4NistManager::Instance()->GetAtomicMassAmu(ZZ));
80  G4int Zt = ZZ;
81 
82  G4double one_third = 1.0 / 3.0;
83 
84  G4double cubicrAt = std::pow ( G4double(At) , G4double(one_third) );
85  G4double cubicrAp = std::pow ( G4double(Ap) , G4double(one_third) );
86 
87  // rc divide fermi
88  G4double Bc = Zt * Zp / ( (rc/fermi) * (cubicrAp+cubicrAt) );
89 
90  G4double targ_mass = G4NucleiProperties::GetNuclearMass(At, Zt);
91  G4double proj_mass = aParticle->GetMass();
92  G4double proj_momentum = aParticle->GetMomentum().mag();
93 
94  G4double Ecm = calEcm ( proj_mass , targ_mass , proj_momentum );
95  if( Ecm <= Bc) return xsection;
96 
97  G4double Rvol = r0 * ( cubicrAp + cubicrAt );
98 
99 // G4double ke_per_N = aParticle->GetKineticEnergy() / Ap;
100  G4double c = calCeValue ( ke_per_N / MeV );
101 
102  G4double a = 1.85;
103  G4double Rsurf = r0 * (a*cubicrAp * cubicrAt/(cubicrAp + cubicrAt) - c);
104  G4double D = 5.0 * ( At - 2 * Zt ) * Zp / ( Ap * At );
105  Rsurf = Rsurf + D * fermi; // multiply D by fermi
106 
107  G4double Rint = Rvol + Rsurf;
108  xsection = pi * Rint * Rint * ( 1 - Bc / ( Ecm / MeV ) );
109 
110  return xsection;
111 }
112 
113 G4double
114 G4IonsKoxCrossSection::calEcm(G4double mp, G4double mt, G4double Plab)
115 {
116  G4double Elab = std::sqrt ( mp * mp + Plab * Plab );
117  G4double Ecm = std::sqrt ( mp * mp + mt * mt + 2 * Elab * mt );
118  G4double Pcm = Plab * mt / Ecm;
119  G4double KEcm = std::sqrt ( Pcm * Pcm + mp * mp ) - mp;
120  return KEcm;
121 }
122 
123 
124 G4double G4IonsKoxCrossSection::calCeValue(const G4double ke)
125 {
126  // Calculate c value
127  // This value is indepenent from projectile and target particle
128  // ke is projectile kinetic energy per nucleon in the Lab system with MeV unit
129  // fitting function is made by T. Koi
130  // There are no data below 30 MeV/n in Kox et al.,
131 
132  G4double Ce;
133  G4double log10_ke = std::log10 ( ke );
134  if (log10_ke > 1.5)
135  {
136  Ce = - 10.0 / std::pow ( G4double(log10_ke) , G4double(5) ) + 2.0;
137  }
138  else
139  {
140  Ce = (-10.0/std::pow(G4double(1.5), G4double(5) ) + 2.0) /
141  std::pow(G4double(1.5), G4double(3)) * std::pow(G4double(log10_ke), G4double(3) );
142 
143  }
144  return Ce;
145 }
146