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G4LCapture.cc
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27 // $Id$
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30 // G4 Model: Low-energy Neutron Capture
31 // F.W. Jones, TRIUMF, 03-DEC-96
32 //
33 // This is a prototype of a low-energy neutron capture process.
34 // Currently it is based on the GHEISHA routine CAPTUR,
35 // and conforms fairly closely to the original Fortran.
36 //
37 // HPW Capture using models now. the code comes from the
38 // original G4LCapture class.
39 //
40 // 25-JUN-98 FWJ: replaced missing Initialize for ParticleChange.
41 //
42 
43 #include <iostream>
44 
45 #include "globals.hh"
46 #include "Randomize.hh"
47 #include "G4PhysicalConstants.hh"
48 #include "G4SystemOfUnits.hh"
49 #include "G4LCapture.hh"
50 
52  : G4HadronicInteraction(name)
53 {
54  SetMinEnergy(0.0*GeV);
56  // Description();
57 }
58 
59 
61 {
63 }
64 
65 
66 void G4LCapture::ModelDescription(std::ostream& outFile) const
67 {
68  outFile << "G4LCapture is one of the Low Energy Parameterized\n"
69  << "(LEP) models used to implement neutron capture on nuclei.\n"
70  << "It is a re-engineered version of the GHEISHA code of\n"
71  << "H. Fesefeldt which simply adds the neutron mass and energy\n"
72  << "to the target nucleus, and emits gammas isotropically as\n"
73  << "long as there is sufficient excitation energy in the\n"
74  << "daughter nucleus. The model is applicable to all incident\n"
75  << "neutron energies.\n";
76 }
77 
78 
80 G4LCapture::ApplyYourself(const G4HadProjectile& aTrack, G4Nucleus& targetNucleus)
81 {
84 
85  G4double N = targetNucleus.GetA_asInt();
86  G4double Z = targetNucleus.GetZ_asInt();
87 
88  const G4LorentzVector theMom = aTrack.Get4Momentum();
89  G4double P = theMom.vect().mag()/GeV;
90  G4double Px = theMom.vect().x()/GeV;
91  G4double Py = theMom.vect().y()/GeV;
92  G4double Pz = theMom.vect().z()/GeV;
93  G4double E = theMom.e()/GeV;
94  G4double E0 = aTrack.GetDefinition()->GetPDGMass()/GeV;
95  G4double Q = aTrack.GetDefinition()->GetPDGCharge();
96  if (verboseLevel > 1) {
97  G4cout << "G4LCapture:ApplyYourself: incident particle:" << G4endl;
98  G4cout << "P " << P << " GeV/c" << G4endl;
99  G4cout << "Px " << Px << " GeV/c" << G4endl;
100  G4cout << "Py " << Py << " GeV/c" << G4endl;
101  G4cout << "Pz " << Pz << " GeV/c" << G4endl;
102  G4cout << "E " << E << " GeV" << G4endl;
103  G4cout << "mass " << E0 << " GeV" << G4endl;
104  G4cout << "charge " << Q << G4endl;
105  }
106 
107  // GHEISHA ADD operation to get total energy, mass, charge:
108 
109  if (verboseLevel > 1) {
110  G4cout << "G4LCapture:ApplyYourself: material:" << G4endl;
111  G4cout << "A " << N << G4endl;
112  G4cout << "Z " << Z << G4endl;
113  G4cout << "atomic mass " <<
114  Atomas(N, Z) << "GeV" << G4endl;
115  }
116  E = E + Atomas(N, Z);
117  G4double E02 = E*E - P*P;
118  E0 = std::sqrt(std::abs(E02));
119  if (E02 < 0) E0 = -E0;
120  Q = Q + Z;
121  if (verboseLevel > 1) {
122  G4cout << "G4LCapture:ApplyYourself: total:" << G4endl;
123  G4cout << "E " << E << " GeV" << G4endl;
124  G4cout << "mass " << E0 << " GeV" << G4endl;
125  G4cout << "charge " << Q << G4endl;
126  }
127  Px = -Px;
128  Py = -Py;
129  Pz = -Pz;
130 
131  // Make a gamma...
132 
133  G4double p;
134  if (Z == 1 && N == 1) { // special case for hydrogen
135  p = 0.0022;
136  } else {
137  G4double ran = G4RandGauss::shoot();
138  p = 0.0065 + ran*0.0010;
139  }
140 
141  G4double ran1 = G4UniformRand();
142  G4double ran2 = G4UniformRand();
143  G4double cost = -1. + 2.*ran1;
144  G4double sint = std::sqrt(std::abs(1. - cost*cost));
145  G4double phi = ran2*twopi;
146 
147  G4double px = p*sint*std::sin(phi);
148  G4double py = p*sint*std::cos(phi);
149  G4double pz = p*cost;
150  G4double e = p;
151 
152  G4double a = px*Px + py*Py + pz*Pz;
153  a = (a/(E + E0) - e)/E0;
154 
155  px = px + a*Px;
156  py = py + a*Py;
157  pz = pz + a*Pz;
158 
159  G4DynamicParticle* aGamma;
161  G4ThreeVector(px*GeV, py*GeV, pz*GeV));
163 
164  // Make another gamma if there is sufficient energy left over...
165 
166  G4double xp = 0.008 - p;
167  if (xp > 0.) {
168  if (Z > 1 || N > 1) {
169  ran1 = G4UniformRand();
170  ran2 = G4UniformRand();
171  cost = -1. + 2.*ran1;
172  sint = std::sqrt(std::abs(1. - cost*cost));
173  phi = ran2*twopi;
174 
175  px = xp*sint*std::sin(phi);
176  py = xp*sint*std::cos(phi);
177  pz = xp*cost;
178  e = xp;
179 
180  a = px*Px + py*Py + pz*Pz;
181  a = (a/(E + E0) - e)/E0;
182 
183  px = px + a*Px;
184  py = py + a*Py;
185  pz = pz + a*Pz;
186 
188  G4ThreeVector(px*GeV, py*GeV, pz*GeV));
190  }
191  }
192  return &theParticleChange;
193 }
194 
195 const std::pair<G4double, G4double> G4LCapture::GetFatalEnergyCheckLevels() const
196 {
197  // max energy non-conservation is mass of heavy nucleus
198  return std::pair<G4double, G4double>(5*perCent,250*GeV);
199 }