Geant4 11.1.1
Toolkit for the simulation of the passage of particles through matter
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G4BetheBlochModel.cc
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25//
26// -------------------------------------------------------------------
27//
28// GEANT4 Class header file
29//
30//
31// File name: G4BetheBlochModel
32//
33// Author: Vladimir Ivanchenko on base of Laszlo Urban code
34//
35// Creation date: 03.01.2002
36//
37// Modifications:
38//
39// 04-12-02 Fix problem of G4DynamicParticle constructor (V.Ivanchenko)
40// 23-12-02 Change interface in order to move to cut per region (V.Ivanchenko)
41// 27-01-03 Make models region aware (V.Ivanchenko)
42// 13-02-03 Add name (V.Ivanchenko)
43// 24-03-05 Add G4EmCorrections (V.Ivanchenko)
44// 11-04-05 Major optimisation of internal interfaces (V.Ivanchenko)
45// 11-02-06 ComputeCrossSectionPerElectron, ComputeCrossSectionPerAtom (mma)
46// 12-02-06 move G4LossTableManager::Instance()->EmCorrections()
47// in constructor (mma)
48// 12-08-08 Added methods GetParticleCharge, GetChargeSquareRatio,
49// CorrectionsAlongStep needed for ions(V.Ivanchenko)
50//
51// -------------------------------------------------------------------
52//
53
54
55//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
56//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
57
58#include "G4BetheBlochModel.hh"
59#include "Randomize.hh"
61#include "G4SystemOfUnits.hh"
62#include "G4NistManager.hh"
63#include "G4Electron.hh"
64#include "G4LossTableManager.hh"
65#include "G4EmCorrections.hh"
66#include "G4EmParameters.hh"
69#include "G4Log.hh"
70#include "G4DeltaAngle.hh"
71
72//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
73
74using namespace std;
75
77 const G4String& nam)
78 : G4VEmModel(nam),
79 twoln10(2.0*G4Log(10.0)),
80 fAlphaTlimit(1*CLHEP::GeV),
81 fProtonTlimit(10*CLHEP::GeV)
82{
83 theElectron = G4Electron::Electron();
86 SetLowEnergyLimit(2.0*CLHEP::MeV);
87}
88
89//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
90
92
93//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
94
96 const G4DataVector&)
97{
98 if(p != particle) { SetupParameters(p); }
99
100 //G4cout << "G4BetheBlochModel::Initialise for " << p->GetParticleName()
101 // << " isIon= " << isIon
102 // << G4endl;
103
104 // always false before the run
105 SetDeexcitationFlag(false);
106
107 // initialisation once
108 if(nullptr == fParticleChange) {
109 const G4String& pname = particle->GetParticleName();
110 if(IsMaster() && G4EmParameters::Instance()->UseICRU90Data() &&
111 (pname == "proton" || pname == "GenericIon" || pname == "alpha")) {
112 fICRU90 = nist->GetICRU90StoppingData();
113 fICRU90->Initialise();
114 }
115 if(particle->GetPDGCharge() > CLHEP::eplus ||
116 pname == "GenericIon") { isIon = true; }
117 if(pname == "alpha") { isAlpha = true; }
118
119 fParticleChange = GetParticleChangeForLoss();
120 if(UseAngularGeneratorFlag() && nullptr == GetAngularDistribution()) {
122 }
123 }
124}
125
126//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
127
129 const G4Material* mat,
130 G4double kineticEnergy)
131{
132 // this method is called only for ions, so no check if it is an ion
133 return
134 (!isAlpha) ? corr->EffectiveChargeSquareRatio(p,mat,kineticEnergy) : 1.0;
135}
136
137//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
138
140 const G4Material* mat,
141 G4double kineticEnergy)
142{
143 // this method is called only for ions, so no check if it is an ion
144 return corr->GetParticleCharge(p,mat,kineticEnergy);
145}
146
147//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
148
149void G4BetheBlochModel::SetupParameters(const G4ParticleDefinition* p)
150{
151 particle = p;
152 mass = particle->GetPDGMass();
153 spin = particle->GetPDGSpin();
154 G4double q = particle->GetPDGCharge()*inveplus;
155 isIon = (!isAlpha && q > 1.1);
156 chargeSquare = q*q;
157 ratio = electron_mass_c2/mass;
158 static const G4double aMag = 1./(0.5*eplus*CLHEP::hbar_Planck*CLHEP::c_squared);
159 G4double magmom = particle->GetPDGMagneticMoment()*mass*aMag;
160 magMoment2 = magmom*magmom - 1.0;
161 formfact = 0.0;
162 tlimit = DBL_MAX;
163 if(particle->GetLeptonNumber() == 0) {
164 G4double x = 0.8426*CLHEP::GeV;
165 if(spin == 0.0 && mass < CLHEP::GeV) { x = 0.736*CLHEP::GeV; }
166 else if (mass > CLHEP::GeV) {
167 G4int iz = G4lrint(std::abs(q));
168 if(iz > 1) { x /= nist->GetA27(iz); }
169 }
170 formfact = 2.0*CLHEP::electron_mass_c2/(x*x);
171 tlimit = 2.0/formfact;
172 }
173}
174
175//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
176
178 const G4MaterialCutsCouple* couple)
179{
181}
182
183//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
184
187 G4double kineticEnergy,
188 G4double cutEnergy,
189 G4double maxKinEnergy)
190{
191 G4double cross = 0.0;
192 G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
193 G4double maxEnergy = std::min(tmax, maxKinEnergy);
194 if(cutEnergy < maxEnergy) {
195
196 G4double totEnergy = kineticEnergy + mass;
197 G4double energy2 = totEnergy*totEnergy;
198 G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/energy2;
199
200 cross = (maxEnergy - cutEnergy)/(cutEnergy*maxEnergy)
201 - beta2*G4Log(maxEnergy/cutEnergy)/tmax;
202
203 // +term for spin=1/2 particle
204 if( 0.0 < spin ) { cross += 0.5*(maxEnergy - cutEnergy)/energy2; }
205
206 cross *= CLHEP::twopi_mc2_rcl2*chargeSquare/beta2;
207 }
208
209 // G4cout << "BB: e= " << kineticEnergy << " tmin= " << cutEnergy
210 // << " tmax= " << tmax << " cross= " << cross << G4endl;
211
212 return cross;
213}
214
215//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
216
218 const G4ParticleDefinition* p,
219 G4double kinEnergy,
221 G4double cutEnergy,
222 G4double maxEnergy)
223{
224 return Z*ComputeCrossSectionPerElectron(p,kinEnergy,cutEnergy,maxEnergy);
225}
226
227//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
228
230 const G4Material* mat,
231 const G4ParticleDefinition* p,
232 G4double kinEnergy,
233 G4double cutEnergy,
234 G4double maxEnergy)
235{
236 G4double sigma = mat->GetElectronDensity()
237 *ComputeCrossSectionPerElectron(p,kinEnergy,cutEnergy,maxEnergy);
238 if(isAlpha) {
239 sigma *= corr->EffectiveChargeSquareRatio(p,mat,kinEnergy)/chargeSquare;
240 }
241 return sigma;
242}
243
244//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
245
247 const G4ParticleDefinition* p,
248 G4double kineticEnergy,
249 G4double cut)
250{
251 const G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
252 // projectile formfactor limit energy loss
253 const G4double cutEnergy = std::min(std::min(cut,tmax), tlimit);
254
255 G4double tau = kineticEnergy/mass;
256 G4double gam = tau + 1.0;
257 G4double bg2 = tau * (tau+2.0);
258 G4double beta2 = bg2/(gam*gam);
259 G4double xc = cutEnergy/tmax;
260
261 G4double eexc = material->GetIonisation()->GetMeanExcitationEnergy();
262 G4double eexc2 = eexc*eexc;
263
264 G4double eDensity = material->GetElectronDensity();
265
266 // added ICRU90 stopping data for limited list of materials
267 /*
268 G4cout << "### DEDX ICRI90:" << (nullptr != fICRU90)
269 << " Ekin=" << kineticEnergy
270 << " " << p->GetParticleName()
271 << " q2=" << chargeSquare
272 << " inside " << material->GetName() << G4endl;
273 */
274 if(nullptr != fICRU90 && kineticEnergy < fProtonTlimit) {
275 if(material != currentMaterial) {
276 currentMaterial = material;
277 baseMaterial = material->GetBaseMaterial()
278 ? material->GetBaseMaterial() : material;
279 iICRU90 = fICRU90->GetIndex(baseMaterial);
280 }
281 if(iICRU90 >= 0) {
282 G4double dedx = 0.0;
283 // only for alpha
284 if(isAlpha) {
285 if(kineticEnergy <= fAlphaTlimit) {
286 dedx = fICRU90->GetElectronicDEDXforAlpha(iICRU90, kineticEnergy);
287 } else {
288 const G4double e = kineticEnergy*CLHEP::proton_mass_c2/mass;
289 dedx = fICRU90->GetElectronicDEDXforProton(iICRU90, e)*chargeSquare;
290 }
291 } else {
292 dedx = fICRU90->GetElectronicDEDXforProton(iICRU90, kineticEnergy)
293 *chargeSquare;
294 }
295 dedx *= material->GetDensity();
296 if(cutEnergy < tmax) {
297 dedx += (G4Log(xc) + (1.0 - xc)*beta2)*CLHEP::twopi_mc2_rcl2
298 *(eDensity*chargeSquare/beta2);
299 }
300 //G4cout << " iICRU90=" << iICRU90 << " dedx=" << dedx << G4endl;
301 if(dedx > 0.0) { return dedx; }
302 }
303 }
304 // general Bethe-Bloch formula
305 G4double dedx = G4Log(2.0*CLHEP::electron_mass_c2*bg2*cutEnergy/eexc2)
306 - (1.0 + xc)*beta2;
307
308 if(0.0 < spin) {
309 G4double del = 0.5*cutEnergy/(kineticEnergy + mass);
310 dedx += del*del;
311 }
312
313 // density correction
314 G4double x = G4Log(bg2)/twoln10;
315 dedx -= material->GetIonisation()->DensityCorrection(x);
316
317 // shell correction
318 dedx -= 2.0*corr->ShellCorrection(p,material,kineticEnergy);
319
320 // now compute the total ionization loss
321 dedx *= CLHEP::twopi_mc2_rcl2*chargeSquare*eDensity/beta2;
322
323 //High order correction different for hadrons and ions
324 if(isIon) {
325 dedx += corr->IonBarkasCorrection(p,material,kineticEnergy);
326 } else {
327 dedx += corr->HighOrderCorrections(p,material,kineticEnergy,cutEnergy);
328 }
329
330 dedx = std::max(dedx, 0.0);
331 /*
332 G4cout << "E(MeV)= " << kineticEnergy/CLHEP::MeV << " dedx= " << dedx
333 << " " << material->GetName() << G4endl;
334 */
335 return dedx;
336}
337
338//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
339
341 const G4DynamicParticle* dp,
342 const G4double& /*length*/,
343 G4double& eloss)
344{
345 // no correction for alpha
346 if(isAlpha) { return; }
347
348 // no correction at the last step or at small step
349 const G4double preKinEnergy = dp->GetKineticEnergy();
350 if(eloss >= preKinEnergy || eloss < preKinEnergy*0.05) { return; }
351
352 // corrections for all charged particles with Q > 1
353 const G4ParticleDefinition* p = dp->GetDefinition();
354 if(p != particle) { SetupParameters(p); }
355 if(!isIon) { return; }
356
357 // effective energy and charge at a step
358 const G4double e = std::max(preKinEnergy - eloss*0.5, preKinEnergy*0.5);
359 const G4Material* mat = couple->GetMaterial();
360 const G4double q20 = corr->EffectiveChargeSquareRatio(p, mat, preKinEnergy);
361 const G4double q2 = corr->EffectiveChargeSquareRatio(p, mat, e);
362 const G4double qfactor = q2/q20;
363
364 /*
365 G4cout << "G4BetheBlochModel::CorrectionsAlongStep: Epre(MeV)="
366 << preKinEnergy << " Eeff(MeV)=" << e
367 << " eloss=" << eloss << " elossnew=" << eloss*qfactor
368 << " qfactor=" << qfactor << " Qpre=" << q20
369 << p->GetParticleName() <<G4endl;
370 */
371 eloss *= qfactor;
372}
373
374//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
375
376void G4BetheBlochModel::SampleSecondaries(vector<G4DynamicParticle*>* vdp,
377 const G4MaterialCutsCouple* couple,
378 const G4DynamicParticle* dp,
379 G4double minKinEnergy,
380 G4double maxEnergy)
381{
382 G4double kineticEnergy = dp->GetKineticEnergy();
383 const G4double tmax = MaxSecondaryEnergy(dp->GetDefinition(),kineticEnergy);
384 const G4double maxKinEnergy = std::min(maxEnergy,tmax);
385 if(minKinEnergy >= maxKinEnergy) { return; }
386
387 //G4cout << "G4BetheBlochModel::SampleSecondaries Emin= " << minKinEnergy
388 // << " Emax= " << maxKinEnergy << G4endl;
389
390 const G4double totEnergy = kineticEnergy + mass;
391 const G4double etot2 = totEnergy*totEnergy;
392 const G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/etot2;
393
394 G4double deltaKinEnergy, f;
395 G4double f1 = 0.0;
396 G4double fmax = 1.0;
397 if( 0.0 < spin ) { fmax += 0.5*maxKinEnergy*maxKinEnergy/etot2; }
398
399 CLHEP::HepRandomEngine* rndmEngineMod = G4Random::getTheEngine();
400 G4double rndm[2];
401
402 // sampling without nuclear size effect
403 do {
404 rndmEngineMod->flatArray(2, rndm);
405 deltaKinEnergy = minKinEnergy*maxKinEnergy
406 /(minKinEnergy*(1.0 - rndm[0]) + maxKinEnergy*rndm[0]);
407
408 f = 1.0 - beta2*deltaKinEnergy/tmax;
409 if( 0.0 < spin ) {
410 f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2;
411 f += f1;
412 }
413
414 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
415 } while( fmax*rndm[1] > f);
416
417 // projectile formfactor - suppresion of high energy
418 // delta-electron production at high energy
419
420 G4double x = formfact*deltaKinEnergy;
421 if(x > 1.e-6) {
422
423 G4double x1 = 1.0 + x;
424 G4double grej = 1.0/(x1*x1);
425 if( 0.0 < spin ) {
426 G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass);
427 grej *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2));
428 }
429 if(grej > 1.1) {
430 G4cout << "### G4BetheBlochModel WARNING: grej= " << grej
431 << " " << dp->GetDefinition()->GetParticleName()
432 << " Ekin(MeV)= " << kineticEnergy
433 << " delEkin(MeV)= " << deltaKinEnergy
434 << G4endl;
435 }
436 if(rndmEngineMod->flat() > grej) { return; }
437 }
438
439 G4ThreeVector deltaDirection;
440
442 const G4Material* mat = couple->GetMaterial();
443 deltaDirection =
444 GetAngularDistribution()->SampleDirection(dp, deltaKinEnergy,
446 mat);
447 } else {
448
449 G4double deltaMomentum =
450 sqrt(deltaKinEnergy * (deltaKinEnergy + 2.0*electron_mass_c2));
451 G4double cost = deltaKinEnergy * (totEnergy + electron_mass_c2) /
452 (deltaMomentum * dp->GetTotalMomentum());
453 cost = std::min(cost, 1.0);
454 const G4double sint = std::sqrt((1.0 - cost)*(1.0 + cost));
455 const G4double phi = twopi*rndmEngineMod->flat();
456
457 deltaDirection.set(sint*std::cos(phi),sint*std::sin(phi), cost) ;
458 deltaDirection.rotateUz(dp->GetMomentumDirection());
459 }
460 /*
461 G4cout << "### G4BetheBlochModel "
462 << dp->GetDefinition()->GetParticleName()
463 << " Ekin(MeV)= " << kineticEnergy
464 << " delEkin(MeV)= " << deltaKinEnergy
465 << " tmin(MeV)= " << minKinEnergy
466 << " tmax(MeV)= " << maxKinEnergy
467 << " dir= " << dp->GetMomentumDirection()
468 << " dirDelta= " << deltaDirection
469 << G4endl;
470 */
471 // create G4DynamicParticle object for delta ray
472 auto delta = new G4DynamicParticle(theElectron,deltaDirection,deltaKinEnergy);
473
474 vdp->push_back(delta);
475
476 // Change kinematics of primary particle
477 kineticEnergy -= deltaKinEnergy;
478 G4ThreeVector finalP = dp->GetMomentum() - delta->GetMomentum();
479 finalP = finalP.unit();
480
481 fParticleChange->SetProposedKineticEnergy(kineticEnergy);
482 fParticleChange->SetProposedMomentumDirection(finalP);
483}
484
485//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
486
488 G4double kinEnergy)
489{
490 // here particle type is checked for the case,
491 // when this model is shared between particles
492 if(pd != particle) { SetupParameters(pd); }
493 G4double tau = kinEnergy/mass;
494 return 2.0*CLHEP::electron_mass_c2*tau*(tau + 2.) /
495 (1. + 2.0*(tau + 1.)*ratio + ratio*ratio);
496}
497
498//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4Log(G4double x)
Definition: G4Log.hh:227
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
const G4int Z[17]
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
Hep3Vector unit() const
void set(double x, double y, double z)
Hep3Vector & rotateUz(const Hep3Vector &)
Definition: ThreeVector.cc:33
virtual double flat()=0
virtual void flatArray(const int size, double *vect)=0
void CorrectionsAlongStep(const G4MaterialCutsCouple *couple, const G4DynamicParticle *dp, const G4double &length, G4double &eloss) override
void Initialise(const G4ParticleDefinition *, const G4DataVector &) override
G4double ComputeDEDXPerVolume(const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy) override
virtual G4double ComputeCrossSectionPerElectron(const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy, G4double maxEnergy)
void SampleSecondaries(std::vector< G4DynamicParticle * > *, const G4MaterialCutsCouple *, const G4DynamicParticle *, G4double tmin, G4double maxEnergy) override
G4double GetParticleCharge(const G4ParticleDefinition *p, const G4Material *mat, G4double kineticEnergy) override
G4double GetChargeSquareRatio() const
~G4BetheBlochModel() override
G4double MinEnergyCut(const G4ParticleDefinition *, const G4MaterialCutsCouple *couple) override
G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition *, G4double kineticEnergy, G4double Z, G4double A, G4double cutEnergy, G4double maxEnergy) override
G4double MaxSecondaryEnergy(const G4ParticleDefinition *, G4double kinEnergy) override
G4double CrossSectionPerVolume(const G4Material *, const G4ParticleDefinition *, G4double kineticEnergy, G4double cutEnergy, G4double maxEnergy) override
G4BetheBlochModel(const G4ParticleDefinition *p=nullptr, const G4String &nam="BetheBloch")
const G4ThreeVector & GetMomentumDirection() const
G4ParticleDefinition * GetDefinition() const
G4double GetKineticEnergy() const
G4ThreeVector GetMomentum() const
G4double GetTotalMomentum() const
static G4Electron * Electron()
Definition: G4Electron.cc:93
G4double EffectiveChargeSquareRatio(const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
G4double IonBarkasCorrection(const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
G4double HighOrderCorrections(const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy, G4double cutEnergy)
G4double ShellCorrection(const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
G4double GetParticleCharge(const G4ParticleDefinition *, const G4Material *, G4double kineticEnergy)
static G4EmParameters * Instance()
G4double GetElectronicDEDXforProton(const G4Material *, G4double kinEnergy) const
G4int GetIndex(const G4Material *) const
G4double GetElectronicDEDXforAlpha(const G4Material *, G4double scaledKinEnergy) const
G4double DensityCorrection(G4double x) const
G4double GetMeanExcitationEnergy() const
static G4LossTableManager * Instance()
G4EmCorrections * EmCorrections()
const G4Material * GetMaterial() const
G4double GetDensity() const
Definition: G4Material.hh:175
const G4Material * GetBaseMaterial() const
Definition: G4Material.hh:228
G4IonisParamMat * GetIonisation() const
Definition: G4Material.hh:221
G4double GetElectronDensity() const
Definition: G4Material.hh:212
G4ICRU90StoppingData * GetICRU90StoppingData()
G4double GetA27(G4int Z) const
static G4NistManager * Instance()
void SetProposedKineticEnergy(G4double proposedKinEnergy)
void SetProposedMomentumDirection(const G4ThreeVector &dir)
G4double GetPDGMagneticMoment() const
G4double GetPDGCharge() const
const G4String & GetParticleName() const
virtual G4ThreeVector & SampleDirection(const G4DynamicParticle *dp, G4double finalTotalEnergy, G4int Z, const G4Material *)=0
G4VEmAngularDistribution * GetAngularDistribution()
Definition: G4VEmModel.hh:600
G4double inveplus
Definition: G4VEmModel.hh:427
G4int SelectRandomAtomNumber(const G4Material *) const
Definition: G4VEmModel.cc:253
G4bool IsMaster() const
Definition: G4VEmModel.hh:725
void SetLowEnergyLimit(G4double)
Definition: G4VEmModel.hh:753
void SetDeexcitationFlag(G4bool val)
Definition: G4VEmModel.hh:802
void SetAngularDistribution(G4VEmAngularDistribution *)
Definition: G4VEmModel.hh:607
G4bool UseAngularGeneratorFlag() const
Definition: G4VEmModel.hh:697
G4ParticleChangeForLoss * GetParticleChangeForLoss()
Definition: G4VEmModel.cc:109
Definition: DoubConv.h:17
int G4lrint(double ad)
Definition: templates.hh:134
#define DBL_MAX
Definition: templates.hh:62