source: trunk/source/processes/electromagnetic/lowenergy/test/testGryzinski.cc@ 1314

Last change on this file since 1314 was 1199, checked in by garnier, 16 years ago

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1//
2// ********************************************************************
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4// * *
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18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
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24// ********************************************************************
25//
26//Ho preso la struttura dal test AtomicDexecitation.cc
27
28#include "globals.hh"
29#include "G4ios.hh"
30#include <vector>
31#include <iostream>
32#include <fstream>
33#include "G4VhShellCrossSection.hh"
34#include "G4hShellCrossSection.hh"
35#include "G4AtomicTransitionManager.hh"
36#include "G4Proton.hh"
37
38int main()
39{
40 G4int Z;
41 G4double incidentEnergy;
42 G4double mass;
43 G4double deltaEnergy;
44 size_t shellNumber;
45
46 G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance();
47 G4VhShellCrossSection* shell = new G4hShellCrossSection;
48
49 //massa del protone in Kg
50 //mass = 1.67262158e-27 * kg;
51
52 G4Proton* aProtone = G4Proton::Proton();
53 mass = aProtone->GetPDGMass();
54
55 std::vector<G4double> energies;
56
57 energies.push_back(0.005); // 5 KeV
58 energies.push_back(0.010);
59 energies.push_back(0.050);
60 energies.push_back(0.100);
61 energies.push_back(0.500);
62 energies.push_back(1.000);
63 energies.push_back(5.000);
64 energies.push_back(10.00);
65 energies.push_back(15.00);
66 energies.push_back(50.00); // 50 MeV
67
68
69 G4cout << "Enter shell number: " << G4endl;
70 G4cin >> shellNumber;
71
72
73 //Z is the atomic number
74 for (Z = 1; Z<=92; Z++)
75 {
76 G4cout << "Z = " << Z << G4endl;
77
78 //Cross section for each incident energy
79 for (G4int k=0; k<10;k++)
80 {
81 incidentEnergy = energies[k]*MeV;
82
83 // *************************************************************** //
84 // From Grizinsky, Phys.Rev. 138,2A, A305 & A322, deltaEnergy //
85 // is the maximum energy of the delta ray emitted. So, deltaEnergy //
86 // will be proton energy - biding energy of the selected shell. //
87 // *************************************************************** //
88
89 G4double bindingEnergy = transitionManager->Shell(Z,shellNumber)->BindingEnergy();
90
91 deltaEnergy = incidentEnergy - bindingEnergy;
92
93 std::vector<G4double> CS = shell->Probabilities(Z,incidentEnergy,mass,deltaEnergy);
94
95 //Volendo scrivere sullo schermo
96 G4cout << " Incident Energy : " << incidentEnergy/MeV << " MeV -- ";
97 G4cout << "Cross Section = " << CS[shellNumber]/barn <<" barn " << G4endl;
98
99
100 //Volendo scrivere i risultati in un file.
101
102 // ofstream outfile( "mytest.out");
103 // outfile << CS[1]/barn << " Barn" << G4endl;
104 // outfile.close();
105
106 // ofstream outfile( "mytest.out", std::ios::out );
107 // fOut.write((G4double) (CS[1]), sizeof (G4int));
108 // //Per verificare che il file si apra.
109 // if( ! outfile) {
110 // G4cerr << "Sorry! We anable to open the file.out!" << G4endl;
111 // break;
112 // // return -1;
113 // }
114 // mytest.out << "Cross Section = " << CS[1]/barn << "Barn" << G4endl;
115 }
116 }
117 delete shell;
118
119 G4cout<<"END OF THE MAIN PROGRAM"<<G4endl;
120}
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