Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4hPairProductionModel.cc
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25//
26// $Id$
27//
28// -------------------------------------------------------------------
29//
30// GEANT4 Class file
31//
32//
33// File name: G4hPairProductionModel
34//
35// Author: Vladimir Ivanchenko on base of G4MuPairProductionModel
36//
37// Creation date: 28.02.2008
38//
39// Modifications:
40//
41
42//
43// Class Description:
44//
45//
46// -------------------------------------------------------------------
47//
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50
53
54using namespace std;
55
57 const G4String& nam)
59{}
60
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62
64{}
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67
69 G4double tkin,
70 G4double Z,
71 G4double pairEnergy)
72// differential cross section
73{
74 G4double bbbtf= 183. ;
75 G4double bbbh = 202.4 ;
76 G4double g1tf = 1.95e-5 ;
77 G4double g2tf = 5.3e-5 ;
78 G4double g1h = 4.4e-5 ;
79 G4double g2h = 4.8e-5 ;
80
81 G4double totalEnergy = tkin + particleMass;
82 G4double residEnergy = totalEnergy - pairEnergy;
83 G4double massratio = particleMass/electron_mass_c2 ;
84 G4double massratio2 = massratio*massratio ;
85 G4double cross = 0.;
86
88
89 G4double c3 = 0.75*sqrte*particleMass;
90 if (residEnergy <= c3*z13) return cross;
91
92 G4double c7 = 4.*electron_mass_c2;
94 G4double alf = c7/pairEnergy;
95 G4double a3 = 1. - alf;
96 if (a3 <= 0.) return cross;
97
98 // zeta calculation
99 G4double bbb,g1,g2;
100 if( Z < 1.5 ) { bbb = bbbh ; g1 = g1h ; g2 = g2h ; }
101 else { bbb = bbbtf; g1 = g1tf; g2 = g2tf; }
102
103 G4double zeta = 0;
104 G4double zeta1 = 0.073*log(totalEnergy/(particleMass+g1*z23*totalEnergy))-0.26;
105 if ( zeta1 > 0.)
106 {
107 G4double zeta2 = 0.058*log(totalEnergy/(particleMass+g2*z13*totalEnergy))-0.14;
108 zeta = zeta1/zeta2 ;
109 }
110
111 G4double z2 = Z*(Z+zeta);
112 G4double screen0 = 2.*electron_mass_c2*sqrte*bbb/(z13*pairEnergy);
113 G4double a0 = totalEnergy*residEnergy;
114 G4double a1 = pairEnergy*pairEnergy/a0;
115 G4double bet = 0.5*a1;
116 G4double xi0 = 0.25*massratio2*a1;
117 G4double del = c8/a0;
118
119 G4double rta3 = sqrt(a3);
120 G4double tmnexp = alf/(1. + rta3) + del*rta3;
121 if(tmnexp >= 1.0) return cross;
122
123 G4double tmn = log(tmnexp);
124 G4double sum = 0.;
125
126 // Gaussian integration in ln(1-ro) ( with 8 points)
127 for (G4int i=0; i<8; i++)
128 {
129 G4double a4 = exp(tmn*xgi[i]); // a4 = (1.-asymmetry)
130 G4double a5 = a4*(2.-a4) ;
131 G4double a6 = 1.-a5 ;
132 G4double a7 = 1.+a6 ;
133 G4double a9 = 3.+a6 ;
134 G4double xi = xi0*a5 ;
135 G4double xii = 1./xi ;
136 G4double xi1 = 1.+xi ;
137 G4double screen = screen0*xi1/a5 ;
138 G4double yeu = 5.-a6+4.*bet*a7 ;
139 G4double yed = 2.*(1.+3.*bet)*log(3.+xii)-a6-a1*(2.-a6) ;
140 G4double ye1 = 1.+yeu/yed ;
141 G4double ale=log(bbb/z13*sqrt(xi1*ye1)/(1.+screen*ye1)) ;
142 G4double cre = 0.5*log(1.+2.25*z23*xi1*ye1/massratio2) ;
143 G4double be;
144
145 if (xi <= 1.e3) be = ((2.+a6)*(1.+bet)+xi*a9)*log(1.+xii)+(a5-bet)/xi1-a9;
146 else be = (3.-a6+a1*a7)/(2.*xi);
147
148 G4double fe = (ale-cre)*be;
149 if ( fe < 0.) fe = 0. ;
150
151 G4double ymu = 4.+a6 +3.*bet*a7 ;
152 G4double ymd = a7*(1.5+a1)*log(3.+xi)+1.-1.5*a6 ;
153 G4double ym1 = 1.+ymu/ymd ;
154 G4double alm_crm = log(bbb*massratio/(1.5*z23*(1.+screen*ym1)));
155 G4double a10,bm;
156 if ( xi >= 1.e-3)
157 {
158 a10 = (1.+a1)*a5 ;
159 bm = (a7*(1.+1.5*bet)-a10*xii)*log(xi1)+xi*(a5-bet)/xi1+a10;
160 } else {
161 bm = (5.-a6+bet*a9)*(xi/2.);
162 }
163
164 G4double fm = alm_crm*bm;
165 if ( fm < 0.) fm = 0. ;
166
167 sum += wgi[i]*a4*(fe+fm/massratio2);
168 }
169
170 cross = -tmn*sum*factorForCross*z2*residEnergy/(totalEnergy*pairEnergy);
171
172 return cross;
173}
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G4fissionEvent * fe
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
virtual G4double ComputeDMicroscopicCrossSection(G4double tkin, G4double Z, G4double pairEnergy)
G4hPairProductionModel(const G4ParticleDefinition *p=0, const G4String &nam="hPairProd")