Geant4 Cross Reference

Cross-Referencing   Geant4
Geant4/processes/electromagnetic/muons/src/G4MuBetheBlochModel.cc

Version: [ ReleaseNotes ] [ 1.0 ] [ 1.1 ] [ 2.0 ] [ 3.0 ] [ 3.1 ] [ 3.2 ] [ 4.0 ] [ 4.0.p1 ] [ 4.0.p2 ] [ 4.1 ] [ 4.1.p1 ] [ 5.0 ] [ 5.0.p1 ] [ 5.1 ] [ 5.1.p1 ] [ 5.2 ] [ 5.2.p1 ] [ 5.2.p2 ] [ 6.0 ] [ 6.0.p1 ] [ 6.1 ] [ 6.2 ] [ 6.2.p1 ] [ 6.2.p2 ] [ 7.0 ] [ 7.0.p1 ] [ 7.1 ] [ 7.1.p1 ] [ 8.0 ] [ 8.0.p1 ] [ 8.1 ] [ 8.1.p1 ] [ 8.1.p2 ] [ 8.2 ] [ 8.2.p1 ] [ 8.3 ] [ 8.3.p1 ] [ 8.3.p2 ] [ 9.0 ] [ 9.0.p1 ] [ 9.0.p2 ] [ 9.1 ] [ 9.1.p1 ] [ 9.1.p2 ] [ 9.1.p3 ] [ 9.2 ] [ 9.2.p1 ] [ 9.2.p2 ] [ 9.2.p3 ] [ 9.2.p4 ] [ 9.3 ] [ 9.3.p1 ] [ 9.3.p2 ] [ 9.4 ] [ 9.4.p1 ] [ 9.4.p2 ] [ 9.4.p3 ] [ 9.4.p4 ] [ 9.5 ] [ 9.5.p1 ] [ 9.5.p2 ] [ 9.6 ] [ 9.6.p1 ] [ 9.6.p2 ] [ 9.6.p3 ] [ 9.6.p4 ] [ 10.0 ] [ 10.0.p1 ] [ 10.0.p2 ] [ 10.0.p3 ] [ 10.0.p4 ] [ 10.1 ] [ 10.1.p1 ] [ 10.1.p2 ] [ 10.1.p3 ] [ 10.2 ] [ 10.2.p1 ] [ 10.2.p2 ] [ 10.2.p3 ] [ 10.3 ] [ 10.3.p1 ] [ 10.3.p2 ] [ 10.3.p3 ] [ 10.4 ] [ 10.4.p1 ] [ 10.4.p2 ] [ 10.4.p3 ] [ 10.5 ] [ 10.5.p1 ] [ 10.6 ] [ 10.6.p1 ] [ 10.6.p2 ] [ 10.6.p3 ] [ 10.7 ] [ 10.7.p1 ] [ 10.7.p2 ] [ 10.7.p3 ] [ 10.7.p4 ] [ 11.0 ] [ 11.0.p1 ] [ 11.0.p2 ] [ 11.0.p3, ] [ 11.0.p4 ] [ 11.1 ] [ 11.1.1 ] [ 11.1.2 ] [ 11.1.3 ] [ 11.2 ] [ 11.2.1 ] [ 11.2.2 ] [ 11.3.0 ]

  1 //
  2 // ********************************************************************
  3 // * License and Disclaimer                                           *
  4 // *                                                                  *
  5 // * The  Geant4 software  is  copyright of the Copyright Holders  of *
  6 // * the Geant4 Collaboration.  It is provided  under  the terms  and *
  7 // * conditions of the Geant4 Software License,  included in the file *
  8 // * LICENSE and available at  http://cern.ch/geant4/license .  These *
  9 // * include a list of copyright holders.                             *
 10 // *                                                                  *
 11 // * Neither the authors of this software system, nor their employing *
 12 // * institutes,nor the agencies providing financial support for this *
 13 // * work  make  any representation or  warranty, express or implied, *
 14 // * regarding  this  software system or assume any liability for its *
 15 // * use.  Please see the license in the file  LICENSE  and URL above *
 16 // * for the full disclaimer and the limitation of liability.         *
 17 // *                                                                  *
 18 // * This  code  implementation is the result of  the  scientific and *
 19 // * technical work of the GEANT4 collaboration.                      *
 20 // * By using,  copying,  modifying or  distributing the software (or *
 21 // * any work based  on the software)  you  agree  to acknowledge its *
 22 // * use  in  resulting  scientific  publications,  and indicate your *
 23 // * acceptance of all terms of the Geant4 Software license.          *
 24 // ********************************************************************
 25 //
 26 //
 27 // -------------------------------------------------------------------
 28 //
 29 // GEANT4 Class header file
 30 //
 31 //
 32 // File name:     G4MuBetheBlochModel
 33 //
 34 // Author:        Vladimir Ivanchenko on base of Laszlo Urban code
 35 //
 36 // Creation date: 09.08.2002
 37 //
 38 // Modifications:
 39 //
 40 // 04-12-02 Fix problem of G4DynamicParticle constructor (V.Ivanchenko)
 41 // 23-12-02 Change interface in order to move to cut per region (V.Ivanchenko)
 42 // 27-01-03 Make models region aware (V.Ivanchenko)
 43 // 13-02-03 Add name (V.Ivanchenko)
 44 // 10-02-04 Calculation of radiative corrections using R.Kokoulin model (V.I)
 45 // 08-04-05 Major optimisation of internal interfaces (V.Ivantchenko)
 46 // 12-04-05 Add usage of G4EmCorrections (V.Ivanchenko)
 47 // 13-02-06 ComputeCrossSectionPerElectron, ComputeCrossSectionPerAtom (mma)
 48 //
 49 
 50 //
 51 // -------------------------------------------------------------------
 52 //
 53 
 54 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 55 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 56 
 57 #include "G4MuBetheBlochModel.hh"
 58 #include "G4PhysicalConstants.hh"
 59 #include "G4SystemOfUnits.hh"
 60 #include "Randomize.hh"
 61 #include "G4Electron.hh"
 62 #include "G4LossTableManager.hh"
 63 #include "G4EmCorrections.hh"
 64 #include "G4ParticleChangeForLoss.hh"
 65 #include "G4Log.hh"
 66 #include "G4Exp.hh"
 67 #include "G4DeltaAngle.hh"
 68 
 69 G4double G4MuBetheBlochModel::xgi[]={ 0.0199, 0.1017, 0.2372, 0.4083, 0.5917,
 70                                       0.7628, 0.8983, 0.9801 };
 71                                       
 72 G4double G4MuBetheBlochModel::wgi[]={ 0.0506, 0.1112, 0.1569, 0.1813, 0.1813,
 73                                       0.1569, 0.1112, 0.0506 };
 74 
 75 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 76 
 77 G4MuBetheBlochModel::G4MuBetheBlochModel(const G4ParticleDefinition* p,
 78                                          const G4String& nam)
 79   : G4VEmModel(nam),
 80     limitRadCorrection(250.*CLHEP::MeV),
 81     limitKinEnergy(100.*CLHEP::keV),
 82     logLimitKinEnergy(G4Log(limitKinEnergy)),
 83     twoln10(2.0*G4Log(10.0)),
 84     alphaprime(CLHEP::fine_structure_const/CLHEP::twopi)
 85 {
 86   theElectron = G4Electron::Electron();
 87   corr = G4LossTableManager::Instance()->EmCorrections();
 88   if(nullptr != p) { SetParticle(p); }
 89 }
 90 
 91 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
 92 
 93 G4double G4MuBetheBlochModel::MinEnergyCut(const G4ParticleDefinition*,
 94                                            const G4MaterialCutsCouple* couple)
 95 {
 96   return couple->GetMaterial()->GetIonisation()->GetMeanExcitationEnergy();
 97 }
 98 
 99 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.....
100 
101 G4double G4MuBetheBlochModel::MaxSecondaryEnergy(const G4ParticleDefinition*,
102                                                  G4double kinEnergy) 
103 {
104   G4double tau  = kinEnergy/mass;
105   G4double tmax = 2.0*CLHEP::electron_mass_c2*tau*(tau + 2.) /
106                   (1. + 2.0*(tau + 1.)*ratio + ratio*ratio);
107   return tmax;
108 }
109 
110 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
111 
112 void G4MuBetheBlochModel::SetParticle(const G4ParticleDefinition* p)
113 {
114   if(nullptr == particle) {
115     particle = p;
116     mass = particle->GetPDGMass();
117     massSquare = mass*mass;
118     ratio = CLHEP::electron_mass_c2/mass;
119   }
120 }
121 
122 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
123 
124 void G4MuBetheBlochModel::Initialise(const G4ParticleDefinition* p,
125                                      const G4DataVector&)
126 {
127   SetParticle(p);
128   if(nullptr == fParticleChange) { 
129     fParticleChange = GetParticleChangeForLoss();
130     if(UseAngularGeneratorFlag() && nullptr == GetAngularDistribution()) {
131       SetAngularDistribution(new G4DeltaAngle());
132     }
133   }
134 }
135 
136 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
137 
138 G4double G4MuBetheBlochModel::ComputeCrossSectionPerElectron(
139                                            const G4ParticleDefinition* p,
140                                                  G4double kineticEnergy,
141                                                  G4double cutEnergy,
142                                                  G4double maxKinEnergy)
143 {
144   G4double cross = 0.0;
145   G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
146   G4double maxEnergy = std::min(tmax, maxKinEnergy);
147   if(cutEnergy < maxEnergy) {
148 
149     G4double totEnergy = kineticEnergy + mass;
150     G4double energy2 = totEnergy*totEnergy;
151     G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/energy2;
152 
153     cross = 1.0/cutEnergy - 1.0/maxEnergy - 
154       beta2*G4Log(maxEnergy/cutEnergy)/tmax +
155       0.5*(maxEnergy - cutEnergy)/energy2;
156 
157     // radiative corrections of R. Kokoulin
158     if (maxEnergy > limitKinEnergy && kineticEnergy > limitRadCorrection) {
159 
160       G4double logtmax = G4Log(maxEnergy);
161       G4double logtmin = G4Log(std::max(cutEnergy,limitKinEnergy));
162       G4double logstep = logtmax - logtmin;
163       G4double dcross  = 0.0;
164 
165       for (G4int ll=0; ll<8; ++ll) {
166         G4double ep = G4Exp(logtmin + xgi[ll]*logstep);
167         G4double a1 = G4Log(1.0 + 2.0*ep/CLHEP::electron_mass_c2);
168         G4double a3 = G4Log(4.0*totEnergy*(totEnergy - ep)/massSquare);
169         dcross += wgi[ll]*(1.0/ep - beta2/tmax + 0.5*ep/energy2)*a1*(a3 - a1);
170       }
171       cross += dcross*logstep*alphaprime;
172     }
173     cross *= CLHEP::twopi_mc2_rcl2/beta2;
174   }
175   //  G4cout << "tmin= " << cutEnergy << " tmax= " << tmax
176   //         << " cross= " << cross << G4endl;  
177   return cross;
178 }
179 
180 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
181 
182 G4double G4MuBetheBlochModel::ComputeCrossSectionPerAtom(
183                                            const G4ParticleDefinition* p,
184                                                  G4double kineticEnergy,
185                                                  G4double Z, G4double,
186                                                  G4double cutEnergy,
187                                                  G4double maxEnergy)
188 {
189   G4double cross = Z*ComputeCrossSectionPerElectron
190                                          (p,kineticEnergy,cutEnergy,maxEnergy);
191   return cross;
192 }
193 
194 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
195 
196 G4double G4MuBetheBlochModel::CrossSectionPerVolume(
197                                            const G4Material* material,
198                                            const G4ParticleDefinition* p,
199                                                  G4double kineticEnergy,
200                                                  G4double cutEnergy,
201                                                  G4double maxEnergy)
202 {
203   G4double eDensity = material->GetElectronDensity();
204   G4double cross = eDensity*ComputeCrossSectionPerElectron
205                                          (p,kineticEnergy,cutEnergy,maxEnergy);
206   return cross;
207 }
208 
209 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
210 
211 G4double G4MuBetheBlochModel::ComputeDEDXPerVolume(const G4Material* material,
212                                                   const G4ParticleDefinition* p,
213                                                   G4double kineticEnergy,
214                                                   G4double cut)
215 {
216   G4double tmax  = MaxSecondaryEnergy(p, kineticEnergy);
217   G4double tau   = kineticEnergy/mass;
218   G4double cutEnergy = std::min(cut, tmax);
219   G4double gam   = tau + 1.0;
220   G4double bg2   = tau * (tau+2.0);
221   G4double beta2 = bg2/(gam*gam);
222 
223   G4double eexc  = material->GetIonisation()->GetMeanExcitationEnergy();
224   G4double eexc2 = eexc*eexc;
225 
226   G4double eDensity = material->GetElectronDensity();
227 
228   G4double dedx = G4Log(2.0*CLHEP::electron_mass_c2*bg2*cutEnergy/eexc2)
229                  -(1.0 + cutEnergy/tmax)*beta2;
230 
231   G4double totEnergy = kineticEnergy + mass;
232   G4double del = 0.5*cutEnergy/totEnergy;
233   dedx += del*del;
234 
235   // density correction
236   G4double x = G4Log(bg2)/twoln10;
237   dedx -= material->GetIonisation()->DensityCorrection(x);
238 
239   // shell and high order corrections
240   dedx -= 2.0*corr->ShellCorrection(p,material,kineticEnergy);
241 
242   // radiative corrections of R. Kokoulin
243   if (cutEnergy > limitKinEnergy && kineticEnergy > limitRadCorrection) {
244 
245     G4double logtmax = G4Log(cutEnergy);
246     G4double logstep = logtmax - logLimitKinEnergy;
247     G4double dloss = 0.0;
248     G4double ftot2= 0.5/(totEnergy*totEnergy);
249 
250     for (G4int ll=0; ll<8; ++ll) {
251       G4double ep = G4Exp(logLimitKinEnergy + xgi[ll]*logstep);
252       G4double a1 = G4Log(1.0 + 2.0*ep/CLHEP::electron_mass_c2);
253       G4double a3 = G4Log(4.0*totEnergy*(totEnergy - ep)/massSquare);
254       dloss += wgi[ll]*(1.0 - beta2*ep/tmax + ep*ep*ftot2)*a1*(a3 - a1);
255     }
256     dedx += dloss*logstep*alphaprime;
257   }
258   dedx *= CLHEP::twopi_mc2_rcl2*eDensity/beta2;
259 
260   //High order corrections
261   dedx += corr->HighOrderCorrections(p,material,kineticEnergy,cutEnergy);
262   dedx = std::max(dedx, 0.);
263   return dedx;
264 }
265 
266 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
267 
268 void G4MuBetheBlochModel::SampleSecondaries(
269                           std::vector<G4DynamicParticle*>* vdp,
270         const G4MaterialCutsCouple* couple,
271         const G4DynamicParticle* dp,
272         G4double minKinEnergy,
273         G4double maxEnergy)
274 {
275   G4double kineticEnergy = dp->GetKineticEnergy();
276   G4double tmax = MaxSecondaryEnergy(dp->GetDefinition(), kineticEnergy);
277   G4double maxKinEnergy = std::min(maxEnergy, tmax);
278   if(minKinEnergy >= maxKinEnergy) { return; }
279 
280   G4double totEnergy = kineticEnergy + mass;
281   G4double etot2 = totEnergy*totEnergy;
282   G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/etot2;
283  
284   G4double grej  = 1.;
285   G4bool radC = (tmax > limitKinEnergy && kineticEnergy > limitRadCorrection);
286   if(radC) {
287     G4double a0 = G4Log(2.*totEnergy/mass);
288     grej += alphaprime*a0*a0;
289   }
290 
291   G4double tkin, f;
292 
293   // sampling follows ...
294   do {
295     G4double q = G4UniformRand();
296     tkin = minKinEnergy*maxKinEnergy/(minKinEnergy*(1.0 - q) + maxKinEnergy*q);
297     f = 1.0 - beta2*tkin/tmax + 0.5*tkin*tkin/etot2;
298 
299     if(radC && tkin > limitKinEnergy) {
300       G4double a1 = G4Log(1.0 + 2.0*tkin/CLHEP::electron_mass_c2);
301       G4double a3 = G4Log(4.0*totEnergy*(totEnergy - tkin)/massSquare);
302       f *= (1. + alphaprime*a1*(a3 - a1));
303     }
304 
305     if(f > grej) {
306         G4cout << "G4MuBetheBlochModel::SampleSecondary Warning! "
307                << "Majorant " << grej << " < "
308                << f << " for edelta= " << tkin
309                << " tmin= " << minKinEnergy << " max= " << maxKinEnergy
310                << G4endl;
311     }
312     // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
313   } while( grej*G4UniformRand() > f );
314 
315   G4ThreeVector deltaDirection;
316 
317   if(UseAngularGeneratorFlag()) {
318     const G4Material* mat = couple->GetMaterial();
319     deltaDirection = GetAngularDistribution()->SampleDirection(dp, tkin,
320                      SelectRandomAtomNumber(mat), mat);
321   } else {
322  
323     G4double deltaMom = std::sqrt(tkin * (tkin + 2.0*CLHEP::electron_mass_c2));
324     G4double totalMom = totEnergy*std::sqrt(beta2);
325     G4double cost = tkin * (totEnergy + CLHEP::electron_mass_c2) /
326       (deltaMom * totalMom);
327     cost = std::min(cost, 1.0);
328     const G4double sint = std::sqrt((1.0 - cost)*(1.0 + cost));
329     const G4double phi = twopi*G4UniformRand();
330 
331     deltaDirection.set(sint*std::cos(phi),sint*std::sin(phi), cost) ;
332     deltaDirection.rotateUz(dp->GetMomentumDirection());
333   }
334   // create G4DynamicParticle object for delta ray
335   auto delta = new G4DynamicParticle(theElectron, deltaDirection, tkin);
336   vdp->push_back(delta);
337 
338   // primary change
339   kineticEnergy -= tkin;
340   G4ThreeVector dir = dp->GetMomentum() - delta->GetMomentum();
341   dir = dir.unit();
342   fParticleChange->SetProposedKineticEnergy(kineticEnergy);
343   fParticleChange->SetProposedMomentumDirection(dir);
344 }
345 
346 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
347