Geant4 11.3.0
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//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
55//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
56
57#include "G4BetheBlochModel.hh"
58#include "Randomize.hh"
60#include "G4SystemOfUnits.hh"
61#include "G4NistManager.hh"
62#include "G4Electron.hh"
63#include "G4LossTableManager.hh"
64#include "G4EmCorrections.hh"
65#include "G4EmParameters.hh"
68#include "G4Log.hh"
69#include "G4DeltaAngle.hh"
70#include <vector>
71
72//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
73
75 const G4String& nam)
76 : G4VEmModel(nam),
77 twoln10(2.0*G4Log(10.0)),
78 fAlphaTlimit(1*CLHEP::GeV),
79 fProtonTlimit(10*CLHEP::GeV)
80{
81 theElectron = G4Electron::Electron();
84 SetLowEnergyLimit(2.0*CLHEP::MeV);
85}
86
87//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
88
90
91//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
92
94 const G4DataVector&)
95{
96 if(p != particle) { SetupParameters(p); }
97
98 // always false before the run
100
101 // initialisation once
102 if(nullptr == fParticleChange) {
103 const G4String& pname = particle->GetParticleName();
104 if(G4EmParameters::Instance()->UseICRU90Data() &&
105 (pname == "proton" || pname == "GenericIon" || pname == "alpha")) {
106 fICRU90 = nist->GetICRU90StoppingData();
107 }
108 if (pname == "GenericIon") {
109 isIon = true;
110 } else if (pname == "alpha") {
111 isAlpha = true;
112 } else if (particle->GetPDGCharge() > 1.1*CLHEP::eplus) {
113 isIon = true;
114 }
115
116 fParticleChange = GetParticleChangeForLoss();
117 if(UseAngularGeneratorFlag() && nullptr == GetAngularDistribution()) {
119 }
120 }
121 // initialisation for each new run
122 if(IsMaster() && nullptr != fICRU90) {
123 fICRU90->Initialise();
124 }
125}
126
127//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
128
130 const G4Material* mat,
131 G4double kinEnergy)
132{
133 // this method is called only for ions, so no check if it is an ion
134 if(isAlpha) { return 1.0; }
135 chargeSquare = corr->EffectiveChargeSquareRatio(p, mat, kinEnergy);
136 return chargeSquare;
137}
138
139//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
140
142 const G4Material* mat,
143 G4double kineticEnergy)
144{
145 // this method is called only for ions, so no check if it is an ion
146 return corr->GetParticleCharge(p, mat, kineticEnergy);
147}
148
149//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
150
151void G4BetheBlochModel::SetupParameters(const G4ParticleDefinition* p)
152{
153 particle = p;
154 mass = particle->GetPDGMass();
155 spin = particle->GetPDGSpin();
156 G4double q = particle->GetPDGCharge()*inveplus;
157 chargeSquare = q*q;
158 ratio = electron_mass_c2/mass;
159 constexpr G4double aMag = 1./(0.5*eplus*CLHEP::hbar_Planck*CLHEP::c_squared);
160 G4double magmom = particle->GetPDGMagneticMoment()*mass*aMag;
161 magMoment2 = magmom*magmom - 1.0;
162 formfact = 0.0;
163 tlimit = DBL_MAX;
164 if(particle->GetLeptonNumber() == 0) {
165 G4double x = 0.8426*CLHEP::GeV;
166 if(spin == 0.0 && mass < CLHEP::GeV) { x = 0.736*CLHEP::GeV; }
167 else if (mass > CLHEP::GeV) {
168 G4int iz = G4lrint(std::abs(q));
169 if(iz > 1) { x /= nist->GetA27(iz); }
170 }
171 formfact = 2.0*CLHEP::electron_mass_c2/(x*x);
172 tlimit = 2.0/formfact;
173 }
174}
175
176//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
177
183
184//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
185
188 G4double kineticEnergy,
189 G4double cut,
190 G4double maxKinEnergy)
191{
192 G4double cross = 0.0;
193 const G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
194 const G4double cutEnergy = std::min(std::min(cut,tmax), tlimit);
195 const G4double maxEnergy = std::min(tmax, maxKinEnergy);
196 if(cutEnergy < maxEnergy) {
197
198 G4double totEnergy = kineticEnergy + mass;
199 G4double energy2 = totEnergy*totEnergy;
200 G4double beta2 = kineticEnergy*(kineticEnergy + 2.0*mass)/energy2;
201
202 cross = (maxEnergy - cutEnergy)/(cutEnergy*maxEnergy)
203 - beta2*G4Log(maxEnergy/cutEnergy)/tmax;
204
205 // +term for spin=1/2 particle
206 if( 0.0 < spin ) { cross += 0.5*(maxEnergy - cutEnergy)/energy2; }
207
208 cross *= CLHEP::twopi_mc2_rcl2*chargeSquare/beta2;
209 }
210
211 // G4cout << "BB: e= " << kineticEnergy << " tmin= " << cutEnergy
212 // << " tmax= " << tmax << " cross= " << cross << G4endl;
213
214 return cross;
215}
216
217//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
218
220 const G4ParticleDefinition* p,
221 G4double kinEnergy,
223 G4double cutEnergy,
224 G4double maxEnergy)
225{
226 return Z*ComputeCrossSectionPerElectron(p,kinEnergy,cutEnergy,maxEnergy);
227}
228
229//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
230
232 const G4Material* mat,
233 const G4ParticleDefinition* p,
234 G4double kinEnergy,
235 G4double cutEnergy,
236 G4double maxEnergy)
237{
238 G4double sigma = mat->GetElectronDensity()
239 *ComputeCrossSectionPerElectron(p,kinEnergy,cutEnergy,maxEnergy);
240 if(isAlpha) {
241 sigma *= corr->EffectiveChargeSquareRatio(p,mat,kinEnergy)/chargeSquare;
242 }
243 return sigma;
244}
245
246//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
247
249 const G4ParticleDefinition* p,
250 G4double kineticEnergy,
251 G4double cut)
252{
253 const G4double tmax = MaxSecondaryEnergy(p, kineticEnergy);
254 // projectile formfactor limit energy loss
255 const G4double cutEnergy = std::min(std::min(cut,tmax), tlimit);
256
257 G4double tau = kineticEnergy/mass;
258 G4double gam = tau + 1.0;
259 G4double bg2 = tau * (tau+2.0);
260 G4double beta2 = bg2/(gam*gam);
261 G4double xc = cutEnergy/tmax;
262
263 G4double eexc = material->GetIonisation()->GetMeanExcitationEnergy();
264 G4double eexc2 = eexc*eexc;
265
266 G4double eDensity = material->GetElectronDensity();
267
268 // added ICRU90 stopping data for limited list of materials
269 /*
270 G4cout << "### DEDX ICRI90:" << (nullptr != fICRU90)
271 << " Ekin=" << kineticEnergy
272 << " " << p->GetParticleName()
273 << " q2=" << chargeSquare
274 << " inside " << material->GetName() << G4endl;
275 */
276 if(nullptr != fICRU90 && kineticEnergy < fProtonTlimit) {
277 if(material != currentMaterial) {
278 currentMaterial = material;
279 baseMaterial = material->GetBaseMaterial()
280 ? material->GetBaseMaterial() : material;
281 iICRU90 = fICRU90->GetIndex(baseMaterial);
282 }
283 if(iICRU90 >= 0) {
284 G4double dedx = 0.0;
285 // only for alpha
286 if(isAlpha) {
287 if(kineticEnergy <= fAlphaTlimit) {
288 dedx = fICRU90->GetElectronicDEDXforAlpha(iICRU90, kineticEnergy);
289 } else {
290 const G4double e = kineticEnergy*CLHEP::proton_mass_c2/mass;
291 dedx = fICRU90->GetElectronicDEDXforProton(iICRU90, e)*chargeSquare;
292 }
293 } else {
294 dedx = fICRU90->GetElectronicDEDXforProton(iICRU90, kineticEnergy)
295 *chargeSquare;
296 }
297 dedx *= material->GetDensity();
298 if(cutEnergy < tmax) {
299 dedx += (G4Log(xc) + (1.0 - xc)*beta2)*CLHEP::twopi_mc2_rcl2
300 *(eDensity*chargeSquare/beta2);
301 }
302 //G4cout << " iICRU90=" << iICRU90 << " dedx=" << dedx << G4endl;
303 if(dedx > 0.0) { return dedx; }
304 }
305 }
306 // general Bethe-Bloch formula
307 G4double dedx = G4Log(2.0*CLHEP::electron_mass_c2*bg2*cutEnergy/eexc2)
308 - (1.0 + xc)*beta2;
309
310 if(0.0 < spin) {
311 G4double del = 0.5*cutEnergy/(kineticEnergy + mass);
312 dedx += del*del;
313 }
314
315 // density correction
316 G4double x = G4Log(bg2)/twoln10;
317 dedx -= material->GetIonisation()->DensityCorrection(x);
318
319 // shell correction
320 dedx -= 2.0*corr->ShellCorrection(p,material,kineticEnergy);
321
322 // now compute the total ionization loss
323 dedx *= CLHEP::twopi_mc2_rcl2*chargeSquare*eDensity/beta2;
324
325 //High order correction different for hadrons and ions
326 if(isIon) {
327 dedx += corr->IonBarkasCorrection(p,material,kineticEnergy);
328 } else {
329 dedx += corr->HighOrderCorrections(p,material,kineticEnergy,cutEnergy);
330 }
331
332 dedx = std::max(dedx, 0.0);
333 /*
334 G4cout << "E(MeV)= " << kineticEnergy/CLHEP::MeV << " dedx= " << dedx
335 << " " << material->GetName() << G4endl;
336 */
337 return dedx;
338}
339
340//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
341
343 const G4DynamicParticle* dp,
344 const G4double& /*length*/,
345 G4double& eloss)
346{
347 // no correction for alpha
348 if(isAlpha) { return; }
349
350 // no correction at the last step or at small step
351 const G4double preKinEnergy = dp->GetKineticEnergy();
352 if(eloss >= preKinEnergy || eloss < preKinEnergy*0.05) { return; }
353
354 // corrections for all charged particles with Q > 1
355 const G4ParticleDefinition* p = dp->GetDefinition();
356 if(p != particle) { SetupParameters(p); }
357 if(!isIon) { return; }
358
359 // effective energy and charge at a step
360 const G4double e = std::max(preKinEnergy - eloss*0.5, preKinEnergy*0.5);
361 const G4Material* mat = couple->GetMaterial();
362 const G4double q20 = corr->EffectiveChargeSquareRatio(p, mat, preKinEnergy);
363 const G4double q2 = corr->EffectiveChargeSquareRatio(p, mat, e);
364 const G4double qfactor = q2/q20;
365
366 /*
367 G4cout << "G4BetheBlochModel::CorrectionsAlongStep: Epre(MeV)="
368 << preKinEnergy << " Eeff(MeV)=" << e
369 << " eloss=" << eloss << " elossnew=" << eloss*qfactor
370 << " qfactor=" << qfactor << " Qpre=" << q20
371 << p->GetParticleName() <<G4endl;
372 */
373 eloss *= qfactor;
374}
375
376//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
377
378void G4BetheBlochModel::SampleSecondaries(std::vector<G4DynamicParticle*>* vdp,
379 const G4MaterialCutsCouple* couple,
380 const G4DynamicParticle* dp,
381 G4double cut,
382 G4double maxEnergy)
383{
384 G4double kinEnergy = dp->GetKineticEnergy();
385 const G4double tmax = MaxSecondaryEnergy(dp->GetDefinition(), kinEnergy);
386 const G4double minKinEnergy = std::min(cut, tmax);
387 const G4double maxKinEnergy = std::min(maxEnergy, tmax);
388 if(minKinEnergy >= maxKinEnergy) { return; }
389
390 //G4cout << "G4BetheBlochModel::SampleSecondaries Emin= " << minKinEnergy
391 // << " Emax= " << maxKinEnergy << G4endl;
392
393 const G4double totEnergy = kinEnergy + mass;
394 const G4double etot2 = totEnergy*totEnergy;
395 const G4double beta2 = kinEnergy*(kinEnergy + 2.0*mass)/etot2;
396
397 G4double deltaKinEnergy, f;
398 G4double f1 = 0.0;
399 G4double fmax = 1.0;
400 if( 0.0 < spin ) { fmax += 0.5*maxKinEnergy*maxKinEnergy/etot2; }
401
402 CLHEP::HepRandomEngine* rndmEngineMod = G4Random::getTheEngine();
403 G4double rndm[2];
404
405 // sampling without nuclear size effect
406 do {
407 rndmEngineMod->flatArray(2, rndm);
408 deltaKinEnergy = minKinEnergy*maxKinEnergy
409 /(minKinEnergy*(1.0 - rndm[0]) + maxKinEnergy*rndm[0]);
410
411 f = 1.0 - beta2*deltaKinEnergy/tmax;
412 if( 0.0 < spin ) {
413 f1 = 0.5*deltaKinEnergy*deltaKinEnergy/etot2;
414 f += f1;
415 }
416
417 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
418 } while( fmax*rndm[1] > f);
419
420 // projectile formfactor - suppresion of high energy
421 // delta-electron production at high energy
422
423 G4double x = formfact*deltaKinEnergy;
424 if(x > 1.e-6) {
425
426 G4double x1 = 1.0 + x;
427 G4double grej = 1.0/(x1*x1);
428 if( 0.0 < spin ) {
429 G4double x2 = 0.5*electron_mass_c2*deltaKinEnergy/(mass*mass);
430 grej *= (1.0 + magMoment2*(x2 - f1/f)/(1.0 + x2));
431 }
432 if(grej > 1.1) {
433 G4cout << "### G4BetheBlochModel WARNING: grej= " << grej
434 << " " << dp->GetDefinition()->GetParticleName()
435 << " Ekin(MeV)= " << kinEnergy
436 << " delEkin(MeV)= " << deltaKinEnergy
437 << G4endl;
438 }
439 if(rndmEngineMod->flat() > grej) { return; }
440 }
441
442 G4ThreeVector deltaDirection;
443
445 const G4Material* mat = couple->GetMaterial();
446 deltaDirection =
447 GetAngularDistribution()->SampleDirection(dp, deltaKinEnergy,
449 mat);
450 } else {
451
452 G4double deltaMomentum =
453 std::sqrt(deltaKinEnergy * (deltaKinEnergy + 2.0*electron_mass_c2));
454 G4double cost = deltaKinEnergy * (totEnergy + electron_mass_c2) /
455 (deltaMomentum * dp->GetTotalMomentum());
456 cost = std::min(cost, 1.0);
457 const G4double sint = std::sqrt((1.0 - cost)*(1.0 + cost));
458 const G4double phi = twopi*rndmEngineMod->flat();
459
460 deltaDirection.set(sint*std::cos(phi),sint*std::sin(phi), cost) ;
461 deltaDirection.rotateUz(dp->GetMomentumDirection());
462 }
463 /*
464 G4cout << "### G4BetheBlochModel "
465 << dp->GetDefinition()->GetParticleName()
466 << " Ekin(MeV)= " << kinEnergy
467 << " delEkin(MeV)= " << deltaKinEnergy
468 << " tmin(MeV)= " << minKinEnergy
469 << " tmax(MeV)= " << maxKinEnergy
470 << " dir= " << dp->GetMomentumDirection()
471 << " dirDelta= " << deltaDirection
472 << G4endl;
473 */
474 // create G4DynamicParticle object for delta ray
475 auto delta = new G4DynamicParticle(theElectron,deltaDirection,deltaKinEnergy);
476
477 vdp->push_back(delta);
478
479 // Change kinematics of primary particle
480 kinEnergy -= deltaKinEnergy;
481 G4ThreeVector finalP = dp->GetMomentum() - delta->GetMomentum();
482 finalP = finalP.unit();
483
484 fParticleChange->SetProposedKineticEnergy(kinEnergy);
485 fParticleChange->SetProposedMomentumDirection(finalP);
486}
487
488//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
489
491 G4double kinEnergy)
492{
493 // here particle type is checked for the case,
494 // when this model is shared between particles
495 if(pd != particle) { SetupParameters(pd); }
496 G4double tau = kinEnergy/mass;
497 return 2.0*CLHEP::electron_mass_c2*tau*(tau + 2.) /
498 (1. + 2.0*(tau + 1.)*ratio + ratio*ratio);
499}
500
501//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
G4double G4Log(G4double x)
Definition G4Log.hh:227
CLHEP::Hep3Vector G4ThreeVector
double G4double
Definition G4Types.hh:83
int G4int
Definition G4Types.hh:85
#define G4endl
Definition G4ios.hh:67
G4GLOB_DLL std::ostream G4cout
Hep3Vector unit() const
void set(double x, double y, double z)
Hep3Vector & rotateUz(const Hep3Vector &)
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:91
static G4EmParameters * Instance()
G4double DensityCorrection(G4double x) const
G4double GetMeanExcitationEnergy() const
static G4LossTableManager * Instance()
G4EmCorrections * EmCorrections()
const G4Material * GetMaterial() const
G4double GetDensity() const
const G4Material * GetBaseMaterial() const
G4IonisParamMat * GetIonisation() const
G4double GetElectronDensity() const
std::size_t GetIndex() const
static G4NistManager * Instance()
G4double GetPDGMagneticMoment() const
const G4String & GetParticleName() const
virtual G4ThreeVector & SampleDirection(const G4DynamicParticle *dp, G4double finalTotalEnergy, G4int Z, const G4Material *)=0
G4VEmAngularDistribution * GetAngularDistribution()
G4double inveplus
G4int SelectRandomAtomNumber(const G4Material *) const
G4bool IsMaster() const
void SetLowEnergyLimit(G4double)
void SetDeexcitationFlag(G4bool val)
G4VEmModel(const G4String &nam)
Definition G4VEmModel.cc:67
void SetAngularDistribution(G4VEmAngularDistribution *)
G4bool UseAngularGeneratorFlag() const
G4ParticleChangeForLoss * GetParticleChangeForLoss()
int G4lrint(double ad)
Definition templates.hh:134
#define DBL_MAX
Definition templates.hh:62