Geant4 Cross Reference

Cross-Referencing   Geant4
Geant4/processes/electromagnetic/highenergy/src/G4AnnihiToMuPair.cc

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  1 //
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 25 //
 26 //
 27 //
 28 //         ------------ G4AnnihiToMuPair physics process ------
 29 //         by H.Burkhardt, S. Kelner and R. Kokoulin, November 2002
 30 // -----------------------------------------------------------------------------
 31 //
 32 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......//
 33 //
 34 // 27.01.03 : first implementation (hbu)
 35 // 04.02.03 : cosmetic simplifications (mma)
 36 // 25.10.04 : migrade to new interfaces of ParticleChange (vi)
 37 // 28.02.18 : cross section now including SSS threshold factor
 38 //
 39 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 40 
 41 #include "G4AnnihiToMuPair.hh"
 42 
 43 #include "G4Exp.hh"
 44 #include "G4LossTableManager.hh"
 45 #include "G4Material.hh"
 46 #include "G4MuonMinus.hh"
 47 #include "G4MuonPlus.hh"
 48 #include "G4PhysicalConstants.hh"
 49 #include "G4Positron.hh"
 50 #include "G4Step.hh"
 51 #include "G4SystemOfUnits.hh"
 52 #include "G4TauMinus.hh"
 53 #include "G4TauPlus.hh"
 54 #include "G4ios.hh"
 55 #include "Randomize.hh"
 56 
 57 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 58 
 59 G4AnnihiToMuPair::G4AnnihiToMuPair(const G4String& processName,
 60     G4ProcessType type):G4VDiscreteProcess (processName, type)
 61 {
 62   //e+ Energy threshold
 63   if(processName == "AnnihiToTauPair") {
 64     SetProcessSubType(fAnnihilationToTauTau);
 65     part1 = G4TauPlus::TauPlus();
 66     part2 = G4TauMinus::TauMinus();
 67     fInfo = "e+e->tau+tau-";
 68   } else {
 69     SetProcessSubType(fAnnihilationToMuMu);
 70     part1 = G4MuonPlus::MuonPlus();
 71     part2 = G4MuonMinus::MuonMinus();
 72   }
 73   fMass = part1->GetPDGMass();
 74   fLowEnergyLimit = 2. * fMass * fMass / CLHEP::electron_mass_c2 - CLHEP::electron_mass_c2;
 75 
 76   // model is ok up to 1000 TeV due to neglected Z-interference
 77   fHighEnergyLimit = 1000. * TeV;
 78 
 79   fCurrentSigma = 0.0;
 80   fCrossSecFactor = 1.;
 81   fManager = G4LossTableManager::Instance();
 82   fManager->Register(this);
 83 }
 84 
 85 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 86 
 87 G4AnnihiToMuPair::~G4AnnihiToMuPair() // (empty) destructor
 88 { 
 89   fManager->DeRegister(this);
 90 }
 91 
 92 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 93 
 94 G4bool G4AnnihiToMuPair::IsApplicable(const G4ParticleDefinition& particle)
 95 {
 96   return ( &particle == G4Positron::Positron() );
 97 }
 98 
 99 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
100 
101 void G4AnnihiToMuPair::BuildPhysicsTable(const G4ParticleDefinition&)
102 {
103   PrintInfoDefinition();
104 }
105 
106 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
107 
108 void G4AnnihiToMuPair::SetCrossSecFactor(G4double fac)
109 // Set the factor to artificially increase the cross section
110 { 
111   fCrossSecFactor = fac;
112   //G4cout << "The cross section for AnnihiToMuPair is artificially "
113   //       << "increased by the CrossSecFactor=" << fCrossSecFactor << G4endl;
114 }
115 
116 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
117 
118 G4double G4AnnihiToMuPair::ComputeCrossSectionPerElectron(const G4double e)
119 // Calculates the microscopic cross section in GEANT4 internal units.
120 // It gives a good description from threshold to 1000 GeV
121 {
122   G4double rmuon = CLHEP::elm_coupling/fMass; //classical particle radius
123   G4double sig0 = CLHEP::pi*rmuon*rmuon/3.;   //constant in crossSection
124   const G4double pial = CLHEP::pi*CLHEP::fine_structure_const; // pi * alphaQED
125 
126   if (e <= fLowEnergyLimit) return 0.0;
127    
128   const G4double xi = fLowEnergyLimit/e;
129   const G4double piaxi = pial * std::sqrt(xi);
130   G4double sigma = sig0 * xi * (1. + xi*0.5);
131   //G4cout << "### xi= " << xi << " piaxi=" << piaxi << G4endl;
132 
133   // argument of the exponent below 0.1 or above 10
134   // Sigma per electron * number of electrons per atom
135   if(xi <= 1.0 - 100*piaxi*piaxi) {
136     sigma *= std::sqrt(1.0 - xi);
137   }
138   else if (xi >= 1.0 - 0.01 * piaxi * piaxi) {
139     sigma *= piaxi;
140   }
141   else {
142     sigma *= piaxi / (1. - G4Exp(-piaxi / std::sqrt(1 - xi)));
143   }
144   // G4cout << "### sigma= " << sigma << G4endl;
145   return sigma;
146 }
147 
148 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
149 
150 G4double G4AnnihiToMuPair::ComputeCrossSectionPerAtom(const G4double energy,
151                                                       const G4double Z)
152 {
153   return ComputeCrossSectionPerElectron(energy)*Z;
154 }
155 
156 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
157 
158 G4double G4AnnihiToMuPair::CrossSectionPerVolume(G4double energy, 
159              const G4Material* aMaterial)
160 {
161   return ComputeCrossSectionPerElectron(energy)*aMaterial->GetTotNbOfElectPerVolume();
162 }
163 
164 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
165 
166 G4double G4AnnihiToMuPair::GetMeanFreePath(const G4Track& aTrack,
167                                            G4double, G4ForceCondition*)
168 // returns the positron mean free path in GEANT4 internal units
169 {
170   const G4DynamicParticle* aDynamicPositron = aTrack.GetDynamicParticle();
171   G4double energy = aDynamicPositron->GetTotalEnergy();
172   const G4Material* aMaterial = aTrack.GetMaterial();
173 
174   // cross section before step
175   fCurrentSigma = CrossSectionPerVolume(energy, aMaterial);
176 
177   // increase the CrossSection by CrossSecFactor (default 1)
178   return (fCurrentSigma > 0.0) ? 1.0/(fCurrentSigma*fCrossSecFactor) : DBL_MAX;
179 }
180 
181 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
182 
183 G4VParticleChange* G4AnnihiToMuPair::PostStepDoIt(const G4Track& aTrack,
184                                                   const G4Step&  aStep)
185 //
186 // generation of e+e- -> mu+mu-
187 //
188 {
189   aParticleChange.Initialize(aTrack);
190 
191   // current Positron energy and direction, return if energy too low
192   const G4DynamicParticle *aDynamicPositron = aTrack.GetDynamicParticle();
193   const G4double Mele = CLHEP::electron_mass_c2;
194   G4double Epos = aDynamicPositron->GetTotalEnergy();
195   G4double xs = CrossSectionPerVolume(Epos, aTrack.GetMaterial());
196 
197   // test of cross section
198   if(xs > 0.0 && fCurrentSigma*G4UniformRand() > xs) {
199     return G4VDiscreteProcess::PostStepDoIt(aTrack,aStep);
200   }
201 
202   const G4ThreeVector PosiDirection = aDynamicPositron->GetMomentumDirection();
203   G4double xi = fLowEnergyLimit/Epos; // xi is always less than 1,
204                                       // goes to 0 at high Epos
205 
206   // generate cost; probability function 1+cost**2 at high Epos
207   //
208   G4double cost;
209   do { cost = 2.*G4UniformRand()-1.; }
210   // Loop checking, 07-Aug-2015, Vladimir Ivanchenko
211   while (2.*G4UniformRand() > 1.+xi+cost*cost*(1.-xi) ); 
212   G4double sint = std::sqrt(1.-cost*cost);
213 
214   // generate phi
215   //
216   G4double phi = 2.*CLHEP::pi*G4UniformRand();
217 
218   G4double Ecm   = std::sqrt(0.5*Mele*(Epos+Mele));
219   G4double Pcm   = std::sqrt(Ecm*Ecm - fMass*fMass);
220   G4double beta  = std::sqrt((Epos-Mele)/(Epos+Mele));
221   G4double gamma = Ecm/Mele;
222   G4double Pt    = Pcm*sint;
223   
224   // energy and momentum of the muons in the Lab
225   //
226   G4double EmuPlus   = gamma*(Ecm + cost*beta*Pcm);
227   G4double EmuMinus  = gamma*(Ecm - cost*beta*Pcm);
228   G4double PmuPlusZ  = gamma*(beta*Ecm + cost*Pcm);
229   G4double PmuMinusZ = gamma*(beta*Ecm - cost*Pcm);
230   G4double PmuPlusX  = Pt*std::cos(phi);
231   G4double PmuPlusY  = Pt*std::sin(phi);
232   G4double PmuMinusX =-PmuPlusX;
233   G4double PmuMinusY =-PmuPlusY;
234   // absolute momenta
235   G4double PmuPlus  = std::sqrt(Pt*Pt+PmuPlusZ *PmuPlusZ );
236   G4double PmuMinus = std::sqrt(Pt*Pt+PmuMinusZ*PmuMinusZ);
237 
238   // mu+ mu- directions for Positron in z-direction
239   //
240   G4ThreeVector MuPlusDirection(PmuPlusX / PmuPlus, PmuPlusY / PmuPlus, PmuPlusZ / PmuPlus);
241   G4ThreeVector MuMinusDirection(PmuMinusX / PmuMinus, PmuMinusY / PmuMinus, PmuMinusZ / PmuMinus);
242 
243   // rotate to actual Positron direction
244   //
245   MuPlusDirection.rotateUz(PosiDirection);
246   MuMinusDirection.rotateUz(PosiDirection);
247 
248   aParticleChange.SetNumberOfSecondaries(2);
249 
250   // create G4DynamicParticle object for the particle1
251   auto aParticle1 = new G4DynamicParticle(part1, MuPlusDirection, EmuPlus - fMass);
252   aParticleChange.AddSecondary(aParticle1);
253   // create G4DynamicParticle object for the particle2
254   auto aParticle2 = new G4DynamicParticle(part2, MuMinusDirection, EmuMinus - fMass);
255   aParticleChange.AddSecondary(aParticle2);
256 
257   // Kill the incident positron 
258   //
259   aParticleChange.ProposeEnergy(0.); 
260   aParticleChange.ProposeTrackStatus(fStopAndKill);
261 
262   return &aParticleChange;
263 }
264 
265 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
266 
267 void G4AnnihiToMuPair::PrintInfoDefinition()
268 {
269   G4String comments = fInfo + " annihilation, atomic e- at rest, SubType=";
270   G4cout << G4endl << GetProcessName() << ":  " << comments << GetProcessSubType() << G4endl;
271   G4cout << "        threshold at " << fLowEnergyLimit / CLHEP::GeV << " GeV"
272          << " good description up to " << fHighEnergyLimit / CLHEP::TeV << " TeV for all Z."
273          << G4endl;
274 }
275 
276 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
277