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

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