source: trunk/source/processes/hadronic/cross_sections/src/G4ProtonInelasticCrossSection.cc@ 1350

Last change on this file since 1350 was 1340, checked in by garnier, 15 years ago

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25//
26// By JPW, working, but to be cleaned up. @@@
27// G.Folger, 29-sept-2006: extend to 1TeV, using a constant above 20GeV
28// 22 Dec 2006 - DHW added isotope dependence
29// G.Folger, 25-Nov-2009: extend to 100TeV, using a constant above 20GeV
30//
31
32#include "G4ProtonInelasticCrossSection.hh"
33#include "G4HadTmpUtil.hh"
34#include "globals.hh"
35
36
37G4double G4ProtonInelasticCrossSection::
38GetCrossSection(const G4DynamicParticle* aPart,
39 const G4Element* anEle, G4double /*aTemperature*/)
40{
41 G4int nIso = anEle->GetNumberOfIsotopes();
42 G4double KE = aPart->GetKineticEnergy();
43 G4double cross_section = 0;
44
45 if (nIso) {
46 G4double psig;
47 G4IsotopeVector* isoVector = anEle->GetIsotopeVector();
48 G4double* abundVector = anEle->GetRelativeAbundanceVector();
49 G4int ZZ;
50 G4int AA;
51
52 for (G4int i = 0; i < nIso; i++) {
53 ZZ = (*isoVector)[i]->GetZ();
54 AA = (*isoVector)[i]->GetN();
55 psig = GetCrossSection(KE, AA, ZZ);
56 cross_section += psig*abundVector[i];
57 }
58
59 } else {
60 G4int ZZ = G4lrint(anEle->GetZ());
61 G4int AA = G4lrint(anEle->GetN());
62 cross_section = GetCrossSection(KE, AA, ZZ);
63 }
64
65 return cross_section;
66}
67
68
69G4double G4ProtonInelasticCrossSection::
70GetCrossSection(G4double kineticEnergy, G4int atomicNumber, G4int nOfProtons)
71{
72 if (kineticEnergy > 19.9*GeV )
73 { // constant cross section above ~20GeV.
74 return GetCrossSection(19.8*GeV,atomicNumber,nOfProtons);
75 }
76 G4int nOfNeutrons = atomicNumber-nOfProtons;
77 kineticEnergy /=GeV;
78 G4double a = atomicNumber;
79 const G4double nuleonRadius=1.36E-15;
80 const G4double pi=3.14159265;
81 G4double fac=pi*nuleonRadius*nuleonRadius;
82 G4double b0=2.247-0.915*(1-std::pow(a,-0.3333));
83 G4double fac1=b0*(1-std::pow(a,-0.3333));
84 G4double fac2=1.;
85 if(nOfNeutrons > 1) fac2=std::log((G4double(nOfNeutrons)));
86 G4double crossSection = 1E31*fac*fac2*(1+std::pow(a,0.3333)-fac1);
87
88 // high energy correction
89
90 crossSection = (1-0.15*std::exp(-kineticEnergy))*crossSection/(1.00-0.0007*a);
91 // first try on low energies: rise
92
93 G4double ff1= 0.70-0.002*a; // slope of the drop at medium energies.
94 G4double ff2= 1.00+1/a; // start of the slope.
95 G4double ff3= 0.8+18/a-0.002*a; // stephight
96 fac = 1.0;
97 if (kineticEnergy > DBL_MIN)
98 fac= 1.0 - (1.0/(1+std::exp(-8*ff1*(std::log10(kineticEnergy)+1.37*ff2))));
99 crossSection = crossSection*(1+ff3*fac);
100
101 // low energy return to zero
102
103 ff1=1.-1/a-0.001*a; // slope of the rise
104 ff2=1.17-2.7/a-0.0014*a; // start of the rise
105 fac = 0.0;
106 if (kineticEnergy > DBL_MIN) {
107 fac=-8.*ff1*(std::log10(kineticEnergy)+2.0*ff2);
108 fac=1/(1+std::exp(fac));
109 }
110 crossSection = crossSection*fac;
111 return crossSection*millibarn;
112}
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