processes/hadronic/stopping/src/G4PiMinusStopLi.cc

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00024 // ********************************************************************
00025 //
00026 //      File name:     G4PiMinusStopLi
00027 //
00028 //      Author:        Maria Grazia Pia (pia@genova.infn.it)
00029 // 
00030 //      Creation date: 8 May 1998
00031 //
00032 // -------------------------------------------------------------------
00033 
00034 #include "G4ios.hh"
00035 
00036 #include "G4PiMinusStopLi.hh"
00037 
00038 #include <vector>
00039 
00040 #include "globals.hh"
00041 #include "Randomize.hh"
00042 #include "G4Proton.hh"
00043 #include "G4Neutron.hh"
00044 #include "G4ParticleTypes.hh"
00045 #include "G4ReactionKinematics.hh"
00046 #include "G4DynamicParticleVector.hh"
00047 #include "G4LorentzVector.hh"
00048 #include "G4NucleiPropertiesTable.hh"
00049 #include "G4PiMinusStopMaterial.hh"
00050 #include "G4DistributionGenerator.hh"
00051 
00052 // np/pp production ratio
00053 // Experimental values: 
00054 // R(np/pp) = 6.3 +- 1.4 (P.Heusi et al., Nucl. Phys. A407 (1983) 429
00055 G4double G4PiMinusStopLi::npRatio = 6.3;
00056  
00057 // Average numbers of final nucleons detected, for N-pair absorption
00058 // (P.Heusi et al., Nucl. Phys. A407 (1983) 429
00059 G4double G4PiMinusStopLi::nFinalNucleons = 1.9;
00060 
00061 // Kinetic energy (MeV) distributions measured for coincident nucleon 
00062 // emission
00063 // P. Heusi et al., Nucl. Phys. A407(1983) 429
00064 
00065 G4int G4PiMinusStopLi::eKinEntries = 21;
00066 
00067 G4double G4PiMinusStopLi::eKinData[21] = { 0.0018, 0.0025, 0.003, 0.045, 
00068                                       0.007, 0.014, 0.023, 
00069                                       0.4,  0.09,  0.18, 
00070                                       0.25,  0.3,  0.25, 0.2, 
00071                                       0.18,  0.08,  0.05, 
00072                                       0.023, 0.012,  0.007, 0.02};
00073 
00074 G4double G4PiMinusStopLi::eKin[22] = { 15., 17.5, 22.5,  27.5,  
00075                                    32.5,  37.5,  42.5,  
00076                                    47.5, 52.5,  57.5,  
00077                                    62.5, 67.5,  72.5,  77.5, 
00078                                    82.5, 87.5,  92.5,  
00079                                    97.5, 102.5, 105. };
00080 
00081 
00082 // Opening angle distributions measured for coincident nucleon emission
00083 // (P.Heusi et al., Nucl. Phys. A407 (1983) 429
00084 
00085 G4int G4PiMinusStopLi::angleEntries = 7;
00086 
00087 G4double G4PiMinusStopLi::angleData[7] = 
00088 { 0.17, 0.4, 0.7, 1.1, 1.3, 20., 70. };
00089 
00090 G4double G4PiMinusStopLi::angle[8] = { 1.308997, 1.570796, 1.832596, 2.094395, 
00091                                   2.356194, 2.617994, 2.967060, 3.1415927 };
00092 
00093 
00094 
00095 // Constructor
00096 
00097 G4PiMinusStopLi::G4PiMinusStopLi()
00098   
00099 {
00100   // Cluster size: nucleon pair, alpha, triton etc.
00101   // First implementation: interaction with nucleon pair only
00102   _clusterSize = 2;
00103 
00104   // R ratio
00105   theR = 1. / (1. + npRatio);
00106 
00107   _definitions = new std::vector<G4ParticleDefinition*>();
00108   _momenta = new std::vector<G4LorentzVector*>();
00109 
00110   std::vector<double> eKinVector;
00111   std::vector<double> eKinDataVector;
00112   int i;
00113   for (i=0; i<eKinEntries; i++)
00114     {
00115       eKinVector.push_back(eKin[i]);
00116       eKinDataVector.push_back(eKinData[i]);
00117     }
00118   eKinVector.push_back(eKin[eKinEntries]);
00119   _distributionE = new G4DistributionGenerator(eKinVector,eKinDataVector);
00120 
00121   std::vector<double> angleVector;
00122   std::vector<double> angleDataVector;
00123   for (i=0; i<angleEntries; i++)
00124     {
00125       angleVector.push_back(angle[i]);
00126       angleDataVector.push_back(angleData[i]);
00127     }
00128   angleVector.push_back(angle[angleEntries]);
00129   _distributionAngle = new G4DistributionGenerator(angleVector,angleDataVector);
00130 }
00131 
00132 
00133 // Destructor
00134 
00135 G4PiMinusStopLi::~G4PiMinusStopLi()
00136 {}
00137 
00138 G4double G4PiMinusStopLi::FinalNucleons()
00139 {
00140   return nFinalNucleons;
00141 }
00142 

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