Geant4-11
Public Member Functions | Protected Member Functions | Protected Attributes | Private Member Functions | Private Attributes
G4WilsonAbrasionModel Class Reference

#include <G4WilsonAbrasionModel.hh>

Inheritance diagram for G4WilsonAbrasionModel:
G4HadronicInteraction

Public Member Functions

void ActivateFor (const G4Element *anElement)
 
void ActivateFor (const G4Material *aMaterial)
 
virtual G4HadFinalState * ApplyYourself (const G4HadProjectile &, G4Nucleus &)
 
virtual void BuildPhysicsTable (const G4ParticleDefinition &)
 
void DeActivateFor (const G4Element *anElement)
 
void DeActivateFor (const G4Material *aMaterial)
 
 G4WilsonAbrasionModel (const G4WilsonAbrasionModel &right)=delete
 
 G4WilsonAbrasionModel (G4bool useAblation1=false)
 
 G4WilsonAbrasionModel (G4ExcitationHandler *)
 
G4bool GetConserveMomentum ()
 
virtual std::pair< G4double, G4double > GetEnergyMomentumCheckLevels () const
 
G4ExcitationHandler * GetExcitationHandler ()
 
virtual const std::pair< G4double, G4double > GetFatalEnergyCheckLevels () const
 
G4double GetMaxEnergy () const
 
G4double GetMaxEnergy (const G4Material *aMaterial, const G4Element *anElement) const
 
G4double GetMinEnergy () const
 
G4double GetMinEnergy (const G4Material *aMaterial, const G4Element *anElement) const
 
const G4String & GetModelName () const
 
G4double GetRecoilEnergyThreshold () const
 
G4bool GetUseAblation ()
 
G4int GetVerboseLevel () const
 
virtual void InitialiseModel ()
 
virtual G4bool IsApplicable (const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
 
G4bool IsBlocked (const G4Element *anElement) const
 
G4bool IsBlocked (const G4Material *aMaterial) const
 
virtual void ModelDescription (std::ostream &) const
 
G4bool operator!= (const G4HadronicInteraction &right) const =delete
 
const G4WilsonAbrasionModel & operator= (G4WilsonAbrasionModel &right)=delete
 
G4bool operator== (const G4HadronicInteraction &right) const =delete
 
virtual G4double SampleInvariantT (const G4ParticleDefinition *p, G4double plab, G4int Z, G4int A)
 
void SetConserveMomentum (G4bool)
 
void SetEnergyMomentumCheckLevels (G4double relativeLevel, G4double absoluteLevel)
 
void SetExcitationHandler (G4ExcitationHandler *)
 
void SetMaxEnergy (const G4double anEnergy)
 
void SetMaxEnergy (G4double anEnergy, const G4Element *anElement)
 
void SetMaxEnergy (G4double anEnergy, const G4Material *aMaterial)
 
void SetMinEnergy (G4double anEnergy)
 
void SetMinEnergy (G4double anEnergy, const G4Element *anElement)
 
void SetMinEnergy (G4double anEnergy, const G4Material *aMaterial)
 
void SetRecoilEnergyThreshold (G4double val)
 
void SetUseAblation (G4bool)
 
void SetVerboseLevel (G4int)
 
 ~G4WilsonAbrasionModel ()
 

Protected Member Functions

void Block ()
 
G4bool IsBlocked () const
 
void SetModelName (const G4String &nam)
 

Protected Attributes

G4bool isBlocked
 
G4double theMaxEnergy
 
G4double theMinEnergy
 
G4HadFinalState theParticleChange
 
G4int verboseLevel
 

Private Member Functions

G4Fragment * GetAbradedNucleons (G4int, G4double, G4double, G4double)
 
G4bool GetConserveEnergy ()
 
G4double GetNucleonInducedExcitation (G4double, G4double, G4double)
 
void PrintWelcomeMessage ()
 
void SetConserveEnergy (G4bool)
 

Private Attributes

G4double B
 
G4bool conserveEnergy
 
G4bool conserveMomentum
 
std::pair< G4double, G4double > epCheckLevels
 
G4double fradius
 
G4double npK
 
G4double r0sq
 
G4double recoilEnergyThreshold
 
G4HadronicInteractionRegistry * registry
 
G4int secID
 
G4WilsonAblationModel * theAblation
 
std::vector< const G4Material * > theBlockedList
 
std::vector< const G4Element * > theBlockedListElements
 
G4ExcitationHandler * theExcitationHandler
 
std::vector< std::pair< G4double, const G4Material * > > theMaxEnergyList
 
std::vector< std::pair< G4double, const G4Element * > > theMaxEnergyListElements
 
std::vector< std::pair< G4double, const G4Material * > > theMinEnergyList
 
std::vector< std::pair< G4double, const G4Element * > > theMinEnergyListElements
 
G4String theModelName
 
G4double third
 
G4bool useAblation
 

Detailed Description

Definition at line 77 of file G4WilsonAbrasionModel.hh.

Constructor & Destructor Documentation

◆ G4WilsonAbrasionModel() [1/3]

G4WilsonAbrasionModel::G4WilsonAbrasionModel ( G4bool  useAblation1 = false)

Definition at line 117 of file G4WilsonAbrasionModel.cc.

118 : G4HadronicInteraction("G4WilsonAbrasion"), secID(-1)
119{
120 // Send message to stdout to advise that the G4Abrasion model is being used.
122
123 // Set the default verbose level to 0 - no output.
124 verboseLevel = 0;
125 useAblation = useAblation1;
126 theAblation = nullptr;
127
128 // No de-excitation handler has been supplied - define the default handler.
129
131 if (useAblation)
132 {
136 }
137
138 // Set the minimum and maximum range for the model (despite nomanclature,
139 // this is in energy per nucleon number).
140
141 SetMinEnergy(70.0*MeV);
142 SetMaxEnergy(10.1*GeV);
143 isBlocked = false;
144
145 // npK, when mutiplied by the nuclear Fermi momentum, determines the range of
146 // momentum over which the secondary nucleon momentum is sampled.
147
148 r0sq = 0.0;
149 npK = 5.0;
150 B = 10.0 * MeV;
151 third = 1.0 / 3.0;
152 fradius = 0.99;
153 conserveEnergy = false;
154 conserveMomentum = true;
155
156 // Creator model ID for the secondaries created by this model
158}
static constexpr double GeV
Definition: G4SIunits.hh:203
static constexpr double MeV
Definition: G4SIunits.hh:200
void SetEvaporation(G4VEvaporation *ptr, G4bool isLocal=false)
void SetMinEnergy(G4double anEnergy)
G4HadronicInteraction(const G4String &modelName="HadronicModel")
const G4String & GetModelName() const
void SetMaxEnergy(const G4double anEnergy)
static G4int GetModelID(const G4int modelIndex)
G4ExcitationHandler * theExcitationHandler
G4WilsonAblationModel * theAblation

References B, conserveEnergy, conserveMomentum, fradius, G4PhysicsModelCatalog::GetModelID(), G4HadronicInteraction::GetModelName(), GeV, G4HadronicInteraction::isBlocked, MeV, npK, PrintWelcomeMessage(), r0sq, secID, G4ExcitationHandler::SetEvaporation(), G4HadronicInteraction::SetMaxEnergy(), G4HadronicInteraction::SetMinEnergy(), G4WilsonAblationModel::SetVerboseLevel(), theAblation, theExcitationHandler, third, useAblation, and G4HadronicInteraction::verboseLevel.

◆ G4WilsonAbrasionModel() [2/3]

G4WilsonAbrasionModel::G4WilsonAbrasionModel ( G4ExcitationHandler *  aExcitationHandler)

Definition at line 172 of file G4WilsonAbrasionModel.cc.

172 :
173 G4HadronicInteraction("G4WilsonAbrasion"), secID(-1)
174{
175// Send message to stdout to advise that the G4Abrasion model is being used.
176
178
179// Set the default verbose level to 0 - no output.
180
181 verboseLevel = 0;
182
183 theAblation = nullptr; //A.R. 26-Jul-2012 Coverity fix.
184 useAblation = false; //A.R. 14-Aug-2012 Coverity fix.
185
186//
187// The user is able to provide the excitation handler as well as an argument
188// which is provided in this instantiation is used to determine
189// whether the spectators of the interaction are free following the abrasion.
190//
191 theExcitationHandler = aExcitationHandler;
192//
193//
194// Set the minimum and maximum range for the model (despite nomanclature, this
195// is in energy per nucleon number).
196//
197 SetMinEnergy(70.0*MeV);
198 SetMaxEnergy(10.1*GeV);
199 isBlocked = false;
200//
201//
202// npK, when mutiplied by the nuclear Fermi momentum, determines the range of
203// momentum over which the secondary nucleon momentum is sampled.
204//
205 r0sq = 0.0;
206 npK = 5.0;
207 B = 10.0 * MeV;
208 third = 1.0 / 3.0;
209 fradius = 0.99;
210 conserveEnergy = false;
211 conserveMomentum = true;
212
213 // Creator model ID for the secondaries created by this model
215}

References B, conserveEnergy, conserveMomentum, fradius, G4PhysicsModelCatalog::GetModelID(), G4HadronicInteraction::GetModelName(), GeV, G4HadronicInteraction::isBlocked, MeV, npK, PrintWelcomeMessage(), r0sq, secID, G4HadronicInteraction::SetMaxEnergy(), G4HadronicInteraction::SetMinEnergy(), theAblation, theExcitationHandler, third, useAblation, and G4HadronicInteraction::verboseLevel.

◆ ~G4WilsonAbrasionModel()

G4WilsonAbrasionModel::~G4WilsonAbrasionModel ( )

Definition at line 218 of file G4WilsonAbrasionModel.cc.

219{
221}

References theExcitationHandler.

◆ G4WilsonAbrasionModel() [3/3]

G4WilsonAbrasionModel::G4WilsonAbrasionModel ( const G4WilsonAbrasionModel &  right)
delete

Member Function Documentation

◆ ActivateFor() [1/2]

void G4HadronicInteraction::ActivateFor ( const G4Element *  anElement)
inlineinherited

◆ ActivateFor() [2/2]

void G4HadronicInteraction::ActivateFor ( const G4Material *  aMaterial)
inlineinherited

◆ ApplyYourself()

G4HadFinalState * G4WilsonAbrasionModel::ApplyYourself ( const G4HadProjectile &  theTrack,
G4Nucleus &  theTarget 
)
virtual

Reimplemented from G4HadronicInteraction.

Definition at line 224 of file G4WilsonAbrasionModel.cc.

226{
227//
228//
229// The secondaries will be returned in G4HadFinalState &theParticleChange -
230// initialise this. The original track will always be discontinued and
231// secondaries followed.
232//
235//
236//
237// Get relevant information about the projectile and target (A, Z, energy/nuc,
238// momentum, etc).
239//
240 const G4ParticleDefinition *definitionP = theTrack.GetDefinition();
241 const G4double AP = definitionP->GetBaryonNumber();
242 const G4double ZP = definitionP->GetPDGCharge();
243 G4LorentzVector pP = theTrack.Get4Momentum();
244 G4double E = theTrack.GetKineticEnergy()/AP;
245 G4double AT = theTarget.GetA_asInt();
246 G4double ZT = theTarget.GetZ_asInt();
247 G4double TotalEPre = theTrack.GetTotalEnergy() +
248 theTarget.AtomicMass(AT, ZT) + theTarget.GetEnergyDeposit();
249 G4double TotalEPost = 0.0;
250//
251//
252// Determine the radii of the projectile and target nuclei.
253//
255 G4double rP = aR.GetWilsonRadius(AP);
256 G4double rT = aR.GetWilsonRadius(AT);
257 G4double rPsq = rP * rP;
258 G4double rTsq = rT * rT;
259 if (verboseLevel >= 2)
260 {
261 G4cout <<"########################################"
262 <<"########################################"
263 <<G4endl;
264 G4cout.precision(6);
265 G4cout <<"IN G4WilsonAbrasionModel" <<G4endl;
266 G4cout <<"Initial projectile A=" <<AP
267 <<", Z=" <<ZP
268 <<", radius = " <<rP/fermi <<" fm"
269 <<G4endl;
270 G4cout <<"Initial target A=" <<AT
271 <<", Z=" <<ZT
272 <<", radius = " <<rT/fermi <<" fm"
273 <<G4endl;
274 G4cout <<"Projectile momentum and Energy/nuc = " <<pP <<" ," <<E <<G4endl;
275 }
276//
277//
278// The following variables are used to determine the impact parameter in the
279// near-field (i.e. taking into consideration the electrostatic repulsion).
280//
281 G4double rm = ZP * ZT * elm_coupling / (E * AP);
282 G4double r = 0.0;
283 G4double rsq = 0.0;
284//
285//
286// Initialise some of the variables which wll be used to calculate the chord-
287// length for nucleons in the projectile and target, and hence calculate the
288// number of abraded nucleons and the excitation energy.
289//
290 G4NuclearAbrasionGeometry *theAbrasionGeometry = nullptr;
291 G4double CT = 0.0;
292 G4double F = 0.0;
293 G4int Dabr = 0;
294//
295//
296// The following loop is performed until the number of nucleons which are
297// abraded by the process is >1, i.e. an interaction MUST occur.
298//
299 G4bool skipInteraction = false; // It will be set true if the two nuclei fail to collide
300 const G4int maxNumberOfLoops = 1000;
301 G4int loopCounter = -1;
302 while (Dabr == 0 && ++loopCounter < maxNumberOfLoops) /* Loop checking, 07.08.2015, A.Ribon */
303 {
304//
305//
306// Sample the impact parameter. For the moment, this class takes account of
307// electrostatic effects on the impact parameter, but (like HZETRN AND NUCFRG2)
308// does not make any correction for the effects of nuclear-nuclear repulsion.
309//
310 G4double rPT = rP + rT;
311 G4double rPTsq = rPT * rPT;
312//
313//
314// This is a "catch" to make sure we don't go into an infinite loop because the
315// energy is too low to overcome nuclear repulsion. PRT 20091023. If the
316// value of rm < fradius * rPT then we're unlikely to sample a small enough
317// impact parameter (energy of incident particle is too low).
318//
319 if (rm >= fradius * rPT) {
320 skipInteraction = true;
321 }
322//
323//
324// Now sample impact parameter until the criterion is met that projectile
325// and target overlap, but repulsion is taken into consideration.
326//
327 G4int evtcnt = 0;
328 r = 1.1 * rPT;
329 while (r > rPT && ++evtcnt < 1000) /* Loop checking, 07.08.2015, A.Ribon */
330 {
331 G4double bsq = rPTsq * G4UniformRand();
332 r = (rm + std::sqrt(rm*rm + 4.0*bsq)) / 2.0;
333 }
334//
335//
336// We've tried to sample this 1000 times, but failed.
337//
338 if (evtcnt >= 1000) {
339 skipInteraction = true;
340 }
341
342 rsq = r * r;
343//
344//
345// Now determine the chord-length through the target nucleus.
346//
347 if (rT > rP)
348 {
349 G4double x = (rPsq + rsq - rTsq) / 2.0 / r;
350 if (x > 0.0) CT = 2.0 * std::sqrt(rTsq - x*x);
351 else CT = 2.0 * std::sqrt(rTsq - rsq);
352 }
353 else
354 {
355 G4double x = (rTsq + rsq - rPsq) / 2.0 / r;
356 if (x > 0.0) CT = 2.0 * std::sqrt(rTsq - x*x);
357 else CT = 2.0 * rT;
358 }
359//
360//
361// Determine the number of abraded nucleons. Note that the mean number of
362// abraded nucleons is used to sample the Poisson distribution. The Poisson
363// distribution is sampled only ten times with the current impact parameter,
364// and if it fails after this to find a case for which the number of abraded
365// nucleons >1, the impact parameter is re-sampled.
366//
367 delete theAbrasionGeometry;
368 theAbrasionGeometry = new G4NuclearAbrasionGeometry(AP,AT,r);
369 F = theAbrasionGeometry->F();
370 G4double lambda = 16.6*fermi / G4Pow::GetInstance()->powA(E/MeV,0.26);
371 G4double Mabr = F * AP * (1.0 - G4Exp(-CT/lambda));
372 G4long n = 0;
373 for (G4int i = 0; i<10; ++i)
374 {
375 n = G4Poisson(Mabr);
376 if (n > 0)
377 {
378 if (n>AP) Dabr = (G4int) AP;
379 else Dabr = (G4int) n;
380 break;
381 }
382 }
383 } // End of while loop
384
385 if ( loopCounter >= maxNumberOfLoops || skipInteraction ) {
386 // Assume nuclei do not collide and return unchanged primary.
390 if (verboseLevel >= 2) {
391 G4cout <<"Particle energy too low to overcome repulsion." <<G4endl;
392 G4cout <<"Event rejected and original track maintained" <<G4endl;
393 G4cout <<"########################################"
394 <<"########################################"
395 <<G4endl;
396 }
397 delete theAbrasionGeometry;
398 return &theParticleChange;
399 }
400
401 if (verboseLevel >= 2)
402 {
403 G4cout <<G4endl;
404 G4cout <<"Impact parameter = " <<r/fermi <<" fm" <<G4endl;
405 G4cout <<"# Abraded nucleons = " <<Dabr <<G4endl;
406 }
407//
408//
409// The number of abraded nucleons must be no greater than the number of
410// nucleons in either the projectile or the target. If AP - Dabr < 2 or
411// AT - Dabr < 2 then either we have only a nucleon left behind in the
412// projectile/target or we've tried to abrade too many nucleons - and Dabr
413// should be limited.
414//
415 if (AP - (G4double) Dabr < 2.0) Dabr = (G4int) AP;
416 if (AT - (G4double) Dabr < 2.0) Dabr = (G4int) AT;
417//
418//
419// Determine the abraded secondary nucleons from the projectile. *fragmentP
420// is a pointer to the prefragment from the projectile and nSecP is the number
421// of nucleons in theParticleChange which have been abraded. The total energy
422// from these is determined.
423//
424 G4ThreeVector boost = pP.findBoostToCM();
425 G4Fragment *fragmentP = GetAbradedNucleons (Dabr, AP, ZP, rP);
427 G4int i = 0;
428 for (i=0; i<nSecP; ++i)
429 {
430 TotalEPost += theParticleChange.GetSecondary(i)->
431 GetParticle()->GetTotalEnergy();
432 }
433//
434//
435// Determine the number of spectators in the interaction region for the
436// projectile.
437//
438 G4int DspcP = (G4int) (AP*F) - Dabr;
439 if (DspcP <= 0) DspcP = 0;
440 else if (DspcP > AP-Dabr) DspcP = ((G4int) AP) - Dabr;
441//
442//
443// Determine excitation energy associated with excess surface area of the
444// projectile (EsP) and the excitation due to scattering of nucleons which are
445// retained within the projectile (ExP). Add the total energy from the excited
446// nucleus to the total energy of the secondaries.
447//
448 G4bool excitationAbsorbedByProjectile = false;
449 if (fragmentP != nullptr)
450 {
451 G4double EsP = theAbrasionGeometry->GetExcitationEnergyOfProjectile();
452 G4double ExP = 0.0;
453 if (Dabr < AT)
454 excitationAbsorbedByProjectile = G4UniformRand() < 0.5;
455 if (excitationAbsorbedByProjectile)
456 ExP = GetNucleonInducedExcitation(rP, rT, r);
457 G4double xP = EsP + ExP;
458 if (xP > B*(AP-Dabr)) xP = B*(AP-Dabr);
459 G4LorentzVector lorentzVector = fragmentP->GetMomentum();
460 lorentzVector.setE(lorentzVector.e()+xP);
461 fragmentP->SetMomentum(lorentzVector);
462 TotalEPost += lorentzVector.e();
463 }
464 G4double EMassP = TotalEPost;
465//
466//
467// Determine the abraded secondary nucleons from the target. Note that it's
468// assumed that the same number of nucleons are abraded from the target as for
469// the projectile, and obviously no boost is applied to the products. *fragmentT
470// is a pointer to the prefragment from the target and nSec is the total number
471// of nucleons in theParticleChange which have been abraded. The total energy
472// from these is determined.
473//
474 G4Fragment *fragmentT = GetAbradedNucleons (Dabr, AT, ZT, rT);
476 for (i=nSecP; i<nSec; ++i)
477 {
478 TotalEPost += theParticleChange.GetSecondary(i)->
479 GetParticle()->GetTotalEnergy();
480 }
481//
482//
483// Determine the number of spectators in the interaction region for the
484// target.
485//
486 G4int DspcT = (G4int) (AT*F) - Dabr;
487 if (DspcT <= 0) DspcT = 0;
488 else if (DspcT > AP-Dabr) DspcT = ((G4int) AT) - Dabr;
489//
490//
491// Determine excitation energy associated with excess surface area of the
492// target (EsT) and the excitation due to scattering of nucleons which are
493// retained within the target (ExT). Add the total energy from the excited
494// nucleus to the total energy of the secondaries.
495//
496 if (fragmentT != nullptr)
497 {
498 G4double EsT = theAbrasionGeometry->GetExcitationEnergyOfTarget();
499 G4double ExT = 0.0;
500 if (!excitationAbsorbedByProjectile)
501 ExT = GetNucleonInducedExcitation(rT, rP, r);
502 G4double xT = EsT + ExT;
503 if (xT > B*(AT-Dabr)) xT = B*(AT-Dabr);
504 G4LorentzVector lorentzVector = fragmentT->GetMomentum();
505 lorentzVector.setE(lorentzVector.e()+xT);
506 fragmentT->SetMomentum(lorentzVector);
507 TotalEPost += lorentzVector.e();
508 }
509//
510//
511// Now determine the difference between the pre and post interaction
512// energy - this will be used to determine the Lorentz boost if conservation
513// of energy is to be imposed/attempted.
514//
515 G4double deltaE = TotalEPre - TotalEPost;
516 if (deltaE > 0.0 && conserveEnergy)
517 {
518 G4double beta = std::sqrt(1.0 - EMassP*EMassP/G4Pow::GetInstance()->powN(deltaE+EMassP,2));
519 boost = boost / boost.mag() * beta;
520 }
521//
522//
523// Now boost the secondaries from the projectile.
524//
525 G4ThreeVector pBalance = pP.vect();
526 for (i=0; i<nSecP; ++i)
527 {
529 GetParticle();
530 G4LorentzVector lorentzVector = dynamicP->Get4Momentum();
531 lorentzVector.boost(-boost);
532 dynamicP->Set4Momentum(lorentzVector);
533 pBalance -= lorentzVector.vect();
534 }
535//
536//
537// Set the boost for the projectile prefragment. This is now based on the
538// conservation of momentum. However, if the user selected momentum of the
539// prefragment is not to be conserved this simply boosted to the velocity of the
540// original projectile times the ratio of the unexcited to the excited mass
541// of the prefragment (the excitation increases the effective mass of the
542// prefragment, and therefore modifying the boost is an attempt to prevent
543// the momentum of the prefragment being excessive).
544//
545 if (fragmentP != nullptr)
546 {
547 G4LorentzVector lorentzVector = fragmentP->GetMomentum();
548 G4double fragmentM = lorentzVector.m();
550 fragmentP->SetMomentum
551 (G4LorentzVector(pBalance,std::sqrt(pBalance.mag2()+fragmentM*fragmentM+1.0*eV*eV)));
552 else
553 {
554 G4double fragmentGroundStateM = fragmentP->GetGroundStateMass();
555 fragmentP->SetMomentum(lorentzVector.boost(-boost * fragmentGroundStateM/fragmentM));
556 }
557 }
558//
559//
560// Output information to user if verbose information requested.
561//
562 if (verboseLevel >= 2)
563 {
564 G4cout <<G4endl;
565 G4cout <<"-----------------------------------" <<G4endl;
566 G4cout <<"Secondary nucleons from projectile:" <<G4endl;
567 G4cout <<"-----------------------------------" <<G4endl;
568 G4cout.precision(7);
569 for (i=0; i<nSecP; ++i)
570 {
571 G4cout <<"Particle # " <<i <<G4endl;
574 G4cout <<"New nucleon (P) " <<dyn->GetDefinition()->GetParticleName()
575 <<" : " <<dyn->Get4Momentum()
576 <<G4endl;
577 }
578 G4cout <<"---------------------------" <<G4endl;
579 G4cout <<"The projectile prefragment:" <<G4endl;
580 G4cout <<"---------------------------" <<G4endl;
581 if (fragmentP != nullptr)
582 G4cout <<*fragmentP <<G4endl;
583 else
584 G4cout <<"(No residual prefragment)" <<G4endl;
585 G4cout <<G4endl;
586 G4cout <<"-------------------------------" <<G4endl;
587 G4cout <<"Secondary nucleons from target:" <<G4endl;
588 G4cout <<"-------------------------------" <<G4endl;
589 G4cout.precision(7);
590 for (i=nSecP; i<nSec; ++i)
591 {
592 G4cout <<"Particle # " <<i <<G4endl;
595 G4cout <<"New nucleon (T) " <<dyn->GetDefinition()->GetParticleName()
596 <<" : " <<dyn->Get4Momentum()
597 <<G4endl;
598 }
599 G4cout <<"-----------------------" <<G4endl;
600 G4cout <<"The target prefragment:" <<G4endl;
601 G4cout <<"-----------------------" <<G4endl;
602 if (fragmentT != nullptr)
603 G4cout <<*fragmentT <<G4endl;
604 else
605 G4cout <<"(No residual prefragment)" <<G4endl;
606 }
607//
608//
609// Now we can decay the nuclear fragments if present. The secondaries are
610// collected and boosted as well. This is performed first for the projectile...
611//
612 if (fragmentP !=nullptr)
613 {
614 G4ReactionProductVector *products = nullptr;
615 // if (fragmentP->GetZ_asInt() != fragmentP->GetA_asInt())
616 products = theExcitationHandler->BreakItUp(*fragmentP);
617 // else
618 // products = theExcitationHandlerx->BreakItUp(*fragmentP);
619 delete fragmentP;
620 fragmentP = nullptr;
621
622 G4ReactionProductVector::iterator iter;
623 for (iter = products->begin(); iter != products->end(); ++iter)
624 {
625 G4DynamicParticle *secondary =
626 new G4DynamicParticle((*iter)->GetDefinition(),
627 (*iter)->GetTotalEnergy(), (*iter)->GetMomentum());
629 G4String particleName = (*iter)->GetDefinition()->GetParticleName();
630 delete (*iter); // get rid of leftover particle def!
631 if (verboseLevel >= 2 && particleName.find("[",0) < particleName.size())
632 {
633 G4cout <<"------------------------" <<G4endl;
634 G4cout <<"The projectile fragment:" <<G4endl;
635 G4cout <<"------------------------" <<G4endl;
636 G4cout <<" fragmentP = " <<particleName
637 <<" Energy = " <<secondary->GetKineticEnergy()
638 <<G4endl;
639 }
640 }
641 delete products;
642 }
643//
644//
645// Now decay the target nucleus - no boost is applied since in this
646// approximation it is assumed that there is negligible momentum transfer from
647// the projectile.
648//
649 if (fragmentT != nullptr)
650 {
651 G4ReactionProductVector *products = nullptr;
652 // if (fragmentT->GetZ_asInt() != fragmentT->GetA_asInt())
653 products = theExcitationHandler->BreakItUp(*fragmentT);
654 // else
655 // products = theExcitationHandlerx->BreakItUp(*fragmentT);
656 // delete fragmentT;
657 fragmentT = nullptr;
658
659 G4ReactionProductVector::iterator iter;
660 for (iter = products->begin(); iter != products->end(); ++iter)
661 {
662 G4DynamicParticle *secondary =
663 new G4DynamicParticle((*iter)->GetDefinition(),
664 (*iter)->GetTotalEnergy(), (*iter)->GetMomentum());
666 G4String particleName = (*iter)->GetDefinition()->GetParticleName();
667 delete (*iter); // get rid of leftover particle def!
668 if (verboseLevel >= 2 && particleName.find("[",0) < particleName.size())
669 {
670 G4cout <<"--------------------" <<G4endl;
671 G4cout <<"The target fragment:" <<G4endl;
672 G4cout <<"--------------------" <<G4endl;
673 G4cout <<" fragmentT = " <<particleName
674 <<" Energy = " <<secondary->GetKineticEnergy()
675 <<G4endl;
676 }
677 }
678 delete products;
679 }
680
681 if (verboseLevel >= 2)
682 G4cout <<"########################################"
683 <<"########################################"
684 <<G4endl;
685
686 delete theAbrasionGeometry;
687 return &theParticleChange;
688}
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:179
@ isAlive
@ stopAndKill
CLHEP::HepLorentzVector G4LorentzVector
G4long G4Poisson(G4double mean)
Definition: G4Poisson.hh:50
std::vector< G4ReactionProduct * > G4ReactionProductVector
static constexpr double fermi
Definition: G4SIunits.hh:83
static constexpr double eV
Definition: G4SIunits.hh:201
double G4double
Definition: G4Types.hh:83
long G4long
Definition: G4Types.hh:87
bool G4bool
Definition: G4Types.hh:86
int G4int
Definition: G4Types.hh:85
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
#define G4UniformRand()
Definition: Randomize.hh:52
Hep3Vector unit() const
double mag2() const
double mag() const
HepLorentzVector & boost(double, double, double)
Hep3Vector vect() const
Hep3Vector findBoostToCM() const
void DumpInfo(G4int mode=0) const
G4ParticleDefinition * GetDefinition() const
G4LorentzVector Get4Momentum() const
G4double GetKineticEnergy() const
void Set4Momentum(const G4LorentzVector &momentum)
G4ReactionProductVector * BreakItUp(const G4Fragment &theInitialState)
G4double GetGroundStateMass() const
Definition: G4Fragment.hh:304
const G4LorentzVector & GetMomentum() const
Definition: G4Fragment.hh:323
void SetMomentum(const G4LorentzVector &value)
Definition: G4Fragment.hh:328
void SetStatusChange(G4HadFinalStateStatus aS)
void AddSecondary(G4DynamicParticle *aP, G4int mod=-1)
std::size_t GetNumberOfSecondaries() const
void SetEnergyChange(G4double anEnergy)
G4HadSecondary * GetSecondary(size_t i)
void SetMomentumChange(const G4ThreeVector &aV)
const G4ParticleDefinition * GetDefinition() const
G4double GetKineticEnergy() const
const G4LorentzVector & Get4Momentum() const
G4double GetTotalEnergy() const
G4DynamicParticle * GetParticle()
G4int GetA_asInt() const
Definition: G4Nucleus.hh:99
G4int GetZ_asInt() const
Definition: G4Nucleus.hh:105
G4double AtomicMass(const G4double A, const G4double Z, const G4int numberOfLambdas=0) const
Definition: G4Nucleus.cc:357
G4double GetEnergyDeposit()
Definition: G4Nucleus.hh:177
G4double GetPDGCharge() const
const G4String & GetParticleName() const
static G4Pow * GetInstance()
Definition: G4Pow.cc:41
G4double powA(G4double A, G4double y) const
Definition: G4Pow.hh:230
G4Fragment * GetAbradedNucleons(G4int, G4double, G4double, G4double)
G4double GetNucleonInducedExcitation(G4double, G4double, G4double)
G4double GetWilsonRadius(G4double A)
static const G4double AP[5]
Definition: paraMaker.cc:42
int elm_coupling
Definition: hepunit.py:285

References G4HadFinalState::AddSecondary(), anonymous_namespace{paraMaker.cc}::AP, G4Nucleus::AtomicMass(), B, anonymous_namespace{G4PionRadiativeDecayChannel.cc}::beta, CLHEP::HepLorentzVector::boost(), G4ExcitationHandler::BreakItUp(), G4HadFinalState::Clear(), conserveEnergy, conserveMomentum, G4DynamicParticle::DumpInfo(), source.hepunit::elm_coupling, eV, G4NuclearAbrasionGeometry::F(), fermi, CLHEP::HepLorentzVector::findBoostToCM(), fradius, G4cout, G4endl, G4Exp(), G4Poisson(), G4UniformRand, G4DynamicParticle::Get4Momentum(), G4HadProjectile::Get4Momentum(), G4Nucleus::GetA_asInt(), GetAbradedNucleons(), G4ParticleDefinition::GetBaryonNumber(), G4DynamicParticle::GetDefinition(), G4HadProjectile::GetDefinition(), G4Nucleus::GetEnergyDeposit(), G4NuclearAbrasionGeometry::GetExcitationEnergyOfProjectile(), G4NuclearAbrasionGeometry::GetExcitationEnergyOfTarget(), G4Fragment::GetGroundStateMass(), G4Pow::GetInstance(), G4DynamicParticle::GetKineticEnergy(), G4HadProjectile::GetKineticEnergy(), G4Fragment::GetMomentum(), GetNucleonInducedExcitation(), G4HadFinalState::GetNumberOfSecondaries(), G4HadSecondary::GetParticle(), G4ParticleDefinition::GetParticleName(), G4ParticleDefinition::GetPDGCharge(), G4HadFinalState::GetSecondary(), G4HadProjectile::GetTotalEnergy(), G4WilsonRadius::GetWilsonRadius(), G4Nucleus::GetZ_asInt(), isAlive, G4InuclParticleNames::lambda, CLHEP::HepLorentzVector::m(), CLHEP::Hep3Vector::mag(), CLHEP::Hep3Vector::mag2(), MeV, CLHEP::detail::n, G4Pow::powA(), secID, G4DynamicParticle::Set4Momentum(), CLHEP::HepLorentzVector::setE(), G4HadFinalState::SetEnergyChange(), G4Fragment::SetMomentum(), G4HadFinalState::SetMomentumChange(), G4HadFinalState::SetStatusChange(), stopAndKill, theExcitationHandler, G4HadronicInteraction::theParticleChange, CLHEP::Hep3Vector::unit(), CLHEP::HepLorentzVector::vect(), and G4HadronicInteraction::verboseLevel.

◆ Block()

void G4HadronicInteraction::Block ( )
inlineprotectedinherited

◆ BuildPhysicsTable()

void G4HadronicInteraction::BuildPhysicsTable ( const G4ParticleDefinition &  )
virtualinherited

◆ DeActivateFor() [1/2]

void G4HadronicInteraction::DeActivateFor ( const G4Element *  anElement)
inherited

Definition at line 186 of file G4HadronicInteraction.cc.

187{
188 Block();
189 theBlockedListElements.push_back(anElement);
190}
std::vector< const G4Element * > theBlockedListElements

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theBlockedListElements.

◆ DeActivateFor() [2/2]

void G4HadronicInteraction::DeActivateFor ( const G4Material *  aMaterial)
inherited

Definition at line 180 of file G4HadronicInteraction.cc.

181{
182 Block();
183 theBlockedList.push_back(aMaterial);
184}
std::vector< const G4Material * > theBlockedList

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theBlockedList.

Referenced by G4HadronHElasticPhysics::ConstructProcess().

◆ GetAbradedNucleons()

G4Fragment * G4WilsonAbrasionModel::GetAbradedNucleons ( G4int  Dabr,
G4double  A,
G4double  Z,
G4double  r 
)
private

Definition at line 691 of file G4WilsonAbrasionModel.cc.

693{
694//
695//
696// Initialise variables. tau is the Fermi radius of the nucleus. The variables
697// p..., C... and gamma are used to help sample the secondary nucleon
698// spectrum.
699//
700
701 G4double pK = hbarc * G4Pow::GetInstance()->A13(9.0 * pi / 4.0 * A) / (1.29 * r);
702 if (A <= 24.0) pK *= -0.229*G4Pow::GetInstance()->A13(A) + 1.62;
703 G4double pKsq = pK * pK;
704 G4double p1sq = 2.0/5.0 * pKsq;
705 G4double p2sq = 6.0/5.0 * pKsq;
706 G4double p3sq = 500.0 * 500.0;
707 G4double C1 = 1.0;
708 G4double C2 = 0.03;
709 G4double C3 = 0.0002;
710 G4double gamma = 90.0 * MeV;
711 G4double maxn = C1 + C2 + C3;
712//
713//
714// initialise the number of secondary nucleons abraded to zero, and initially set
715// the type of nucleon abraded to proton ... just for now.
716//
717 G4double Aabr = 0.0;
718 G4double Zabr = 0.0;
720 G4DynamicParticle *dynamicNucleon = nullptr;
721 G4ParticleMomentum pabr(0.0, 0.0, 0.0);
722//
723//
724// Now go through each abraded nucleon and sample type, spectrum and angle.
725//
726 G4bool isForLoopExitAnticipated = false;
727 for (G4int i=0; i<Dabr; ++i)
728 {
729//
730//
731// Sample the nucleon momentum distribution by simple rejection techniques. We
732// reject values of p == 0.0 since this causes bad behaviour in the sinh term.
733//
734 G4double p = 0.0;
735 G4bool found = false;
736 const G4int maxNumberOfLoops = 100000;
737 G4int loopCounter = -1;
738 while (!found && ++loopCounter < maxNumberOfLoops) /* Loop checking, 07.08.2015, A.Ribon */
739 {
740 while (p <= 0.0) p = npK * pK * G4UniformRand(); /* Loop checking, 07.08.2015, A.Ribon */
741 G4double psq = p * p;
742 found = maxn * G4UniformRand() < C1*G4Exp(-psq/p1sq/2.0) +
743 C2*G4Exp(-psq/p2sq/2.0) + C3*G4Exp(-psq/p3sq/2.0) + p/gamma/(0.5*(G4Exp(p/gamma)-G4Exp(-p/gamma)));
744 }
745 if ( loopCounter >= maxNumberOfLoops )
746 {
747 isForLoopExitAnticipated = true;
748 break;
749 }
750//
751//
752// Determine the type of particle abraded. Can only be proton or neutron,
753// and the probability is determine to be proportional to the ratio as found
754// in the nucleus at each stage.
755//
756 G4double prob = (Z-Zabr)/(A-Aabr);
757 if (G4UniformRand()<prob)
758 {
759 Zabr++;
760 typeNucleon = G4Proton::ProtonDefinition();
761 }
762 else
763 typeNucleon = G4Neutron::NeutronDefinition();
764 Aabr++;
765//
766//
767// The angular distribution of the secondary nucleons is approximated to an
768// isotropic distribution in the rest frame of the nucleus (this will be Lorentz
769// boosted later.
770//
771 G4double costheta = 2.*G4UniformRand()-1.0;
772 G4double sintheta = std::sqrt((1.0 - costheta)*(1.0 + costheta));
773 G4double phi = 2.0*pi*G4UniformRand()*rad;
774 G4ThreeVector direction(sintheta*std::cos(phi),sintheta*std::sin(phi),costheta);
775 G4double nucleonMass = typeNucleon->GetPDGMass();
776 G4double E = std::sqrt(p*p + nucleonMass*nucleonMass)-nucleonMass;
777 dynamicNucleon = new G4DynamicParticle(typeNucleon,direction,E);
778 theParticleChange.AddSecondary (dynamicNucleon, secID);
779 pabr += p*direction;
780 }
781//
782//
783// Next determine the details of the nuclear prefragment .. that is if there
784// is one or more protons in the residue. (Note that the 1 eV in the total
785// energy is a safety factor to avoid any possibility of negative rest mass
786// energy.)
787//
788 G4Fragment *fragment = nullptr;
789 if ( ! isForLoopExitAnticipated && Z-Zabr>=1.0 )
790 {
792 GetIonMass(G4lrint(Z-Zabr),G4lrint(A-Aabr));
793 G4double E = std::sqrt(pabr.mag2() + ionMass*ionMass);
794 G4LorentzVector lorentzVector = G4LorentzVector(-pabr, E + 1.0*eV);
795 fragment =
796 new G4Fragment((G4int) (A-Aabr), (G4int) (Z-Zabr), lorentzVector);
797 }
798
799 return fragment;
800}
static constexpr double rad
Definition: G4SIunits.hh:129
static constexpr double pi
Definition: G4SIunits.hh:55
const G4int Z[17]
const G4double A[17]
const double C2
const double C1
#define C3
static G4Neutron * NeutronDefinition()
Definition: G4Neutron.cc:98
G4IonTable * GetIonTable() const
static G4ParticleTable * GetParticleTable()
G4double A13(G4double A) const
Definition: G4Pow.cc:120
static G4Proton * ProtonDefinition()
Definition: G4Proton.cc:87
float hbarc
Definition: hepunit.py:264
int G4lrint(double ad)
Definition: templates.hh:134

References A, G4Pow::A13(), G4HadFinalState::AddSecondary(), C1, C2, C3, eV, G4Exp(), G4lrint(), G4UniformRand, G4Pow::GetInstance(), G4ParticleTable::GetIonTable(), G4ParticleTable::GetParticleTable(), G4ParticleDefinition::GetPDGMass(), source.hepunit::hbarc, CLHEP::Hep3Vector::mag2(), MeV, G4Neutron::NeutronDefinition(), npK, pi, G4Proton::ProtonDefinition(), rad, secID, G4HadronicInteraction::theParticleChange, and Z.

Referenced by ApplyYourself().

◆ GetConserveEnergy()

G4bool G4WilsonAbrasionModel::GetConserveEnergy ( )
inlineprivate

Definition at line 132 of file G4WilsonAbrasionModel.hh.

133 {return conserveEnergy;}

References conserveEnergy.

◆ GetConserveMomentum()

G4bool G4WilsonAbrasionModel::GetConserveMomentum ( )
inline

Definition at line 138 of file G4WilsonAbrasionModel.hh.

139 {return conserveMomentum;}

References conserveMomentum.

◆ GetEnergyMomentumCheckLevels()

std::pair< G4double, G4double > G4HadronicInteraction::GetEnergyMomentumCheckLevels ( ) const
virtualinherited

◆ GetExcitationHandler()

G4ExcitationHandler * G4WilsonAbrasionModel::GetExcitationHandler ( )
inline

Definition at line 123 of file G4WilsonAbrasionModel.hh.

124 {return theExcitationHandler;}

References theExcitationHandler.

◆ GetFatalEnergyCheckLevels()

const std::pair< G4double, G4double > G4HadronicInteraction::GetFatalEnergyCheckLevels ( ) const
virtualinherited

Reimplemented in G4FissLib, G4LFission, G4LENDFission, G4ParticleHPCapture, G4ParticleHPElastic, G4ParticleHPFission, G4ParticleHPInelastic, and G4ParticleHPThermalScattering.

Definition at line 210 of file G4HadronicInteraction.cc.

211{
212 // default level of Check
213 return std::pair<G4double, G4double>(2.*perCent, 1. * GeV);
214}
static constexpr double perCent
Definition: G4SIunits.hh:325

References GeV, and perCent.

Referenced by G4HadronicProcess::CheckResult().

◆ GetMaxEnergy() [1/2]

G4double G4HadronicInteraction::GetMaxEnergy ( ) const
inlineinherited

◆ GetMaxEnergy() [2/2]

G4double G4HadronicInteraction::GetMaxEnergy ( const G4Material *  aMaterial,
const G4Element *  anElement 
) const
inherited

Definition at line 131 of file G4HadronicInteraction.cc.

133{
134 if(!IsBlocked()) { return theMaxEnergy; }
135 if( IsBlocked(aMaterial) || IsBlocked(anElement) ) { return 0.0; }
136 if(!theMaxEnergyListElements.empty()) {
137 for(auto const& elmlist : theMaxEnergyListElements) {
138 if( anElement == elmlist.second )
139 { return elmlist.first; }
140 }
141 }
142 if(!theMaxEnergyList.empty()) {
143 for(auto const& matlist : theMaxEnergyList) {
144 if( aMaterial == matlist.second )
145 { return matlist.first; }
146 }
147 }
148 return theMaxEnergy;
149}
std::vector< std::pair< G4double, const G4Material * > > theMaxEnergyList
std::vector< std::pair< G4double, const G4Element * > > theMaxEnergyListElements

References G4HadronicInteraction::IsBlocked(), G4HadronicInteraction::theMaxEnergy, G4HadronicInteraction::theMaxEnergyList, and G4HadronicInteraction::theMaxEnergyListElements.

◆ GetMinEnergy() [1/2]

G4double G4HadronicInteraction::GetMinEnergy ( ) const
inlineinherited

◆ GetMinEnergy() [2/2]

G4double G4HadronicInteraction::GetMinEnergy ( const G4Material *  aMaterial,
const G4Element *  anElement 
) const
inherited

Definition at line 81 of file G4HadronicInteraction.cc.

83{
84 if(!IsBlocked()) { return theMinEnergy; }
85 if( IsBlocked(aMaterial) || IsBlocked(anElement) ) { return DBL_MAX; }
86 if(!theMinEnergyListElements.empty()) {
87 for(auto const& elmlist : theMinEnergyListElements) {
88 if( anElement == elmlist.second )
89 { return elmlist.first; }
90 }
91 }
92 if(!theMinEnergyList.empty()) {
93 for(auto const & matlist : theMinEnergyList) {
94 if( aMaterial == matlist.second )
95 { return matlist.first; }
96 }
97 }
98 return theMinEnergy;
99}
std::vector< std::pair< G4double, const G4Element * > > theMinEnergyListElements
std::vector< std::pair< G4double, const G4Material * > > theMinEnergyList
#define DBL_MAX
Definition: templates.hh:62

References DBL_MAX, G4HadronicInteraction::IsBlocked(), G4HadronicInteraction::theMinEnergy, G4HadronicInteraction::theMinEnergyList, and G4HadronicInteraction::theMinEnergyListElements.

◆ GetModelName()

const G4String & G4HadronicInteraction::GetModelName ( ) const
inlineinherited

Definition at line 115 of file G4HadronicInteraction.hh.

116 { return theModelName; }

References G4HadronicInteraction::theModelName.

Referenced by G4MuMinusCapturePrecompound::ApplyYourself(), G4HadronElastic::ApplyYourself(), G4INCLXXInterface::ApplyYourself(), G4TheoFSGenerator::ApplyYourself(), G4HadronStoppingProcess::AtRestDoIt(), G4VHadronPhysics::BuildModel(), G4HadronicProcess::CheckEnergyMomentumConservation(), G4HadronicProcess::CheckResult(), G4ChargeExchangePhysics::ConstructProcess(), G4MuonicAtomDecay::DecayIt(), G4LENDModel::DumpLENDTargetInfo(), G4AblaInterface::G4AblaInterface(), G4ElectroVDNuclearModel::G4ElectroVDNuclearModel(), G4EMDissociation::G4EMDissociation(), G4ExcitedStringDecay::G4ExcitedStringDecay(), G4LEHadronProtonElastic::G4LEHadronProtonElastic(), G4LENDModel::G4LENDModel(), G4LENDorBERTModel::G4LENDorBERTModel(), G4LEnp::G4LEnp(), G4LEpp::G4LEpp(), G4LFission::G4LFission(), G4LowEGammaNuclearModel::G4LowEGammaNuclearModel(), G4LowEIonFragmentation::G4LowEIonFragmentation(), G4MuonVDNuclearModel::G4MuonVDNuclearModel(), G4NeutrinoElectronCcModel::G4NeutrinoElectronCcModel(), G4NeutrinoNucleusModel::G4NeutrinoNucleusModel(), G4WilsonAbrasionModel(), G4INCLXXInterface::GetDeExcitationModelName(), G4EnergyRangeManager::GetHadronicInteraction(), G4VHighEnergyGenerator::GetProjectileNucleus(), G4NeutronRadCapture::InitialiseModel(), G4BinaryCascade::ModelDescription(), G4LMsdGenerator::ModelDescription(), G4VPartonStringModel::ModelDescription(), G4TheoFSGenerator::ModelDescription(), G4VHadronPhysics::NewModel(), G4NeutrinoElectronProcess::PostStepDoIt(), G4HadronicProcess::PostStepDoIt(), G4ElNeutrinoNucleusProcess::PostStepDoIt(), G4HadronElasticProcess::PostStepDoIt(), G4MuNeutrinoNucleusProcess::PostStepDoIt(), G4HadronicProcessStore::PrintModelHtml(), G4BinaryCascade::PropagateModelDescription(), G4HadronicProcessStore::RegisterInteraction(), and G4LENDModel::returnUnchanged().

◆ GetNucleonInducedExcitation()

G4double G4WilsonAbrasionModel::GetNucleonInducedExcitation ( G4double  rP,
G4double  rT,
G4double  r 
)
private

Definition at line 803 of file G4WilsonAbrasionModel.cc.

805{
806//
807//
808// Initialise variables.
809//
810 G4double Cl = 0.0;
811 G4double rPsq = rP * rP;
812 G4double rTsq = rT * rT;
813 G4double rsq = r * r;
814//
815//
816// Depending upon the impact parameter, a different form of the chord length is
817// is used.
818//
819 if (r > rT) Cl = 2.0*std::sqrt(rPsq + 2.0*r*rT - rsq - rTsq);
820 else Cl = 2.0*rP;
821//
822//
823// The next lines have been changed to include a "catch" to make sure if the
824// projectile and target are too close, Ct is set to twice rP or twice rT.
825// Otherwise the standard Wilson algorithm should work fine.
826// PRT 20091023.
827//
828 G4double Ct = 0.0;
829 if (rT > rP && rsq < rTsq - rPsq) Ct = 2.0 * rP;
830 else if (rP > rT && rsq < rPsq - rTsq) Ct = 2.0 * rT;
831 else {
832 G4double bP = (rPsq+rsq-rTsq)/2.0/r;
833 G4double x = rPsq - bP*bP;
834 if (x < 0.0) {
835 G4cerr <<"########################################"
836 <<"########################################"
837 <<G4endl;
838 G4cerr <<"ERROR IN G4WilsonAbrasionModel::GetNucleonInducedExcitation"
839 <<G4endl;
840 G4cerr <<"rPsq - bP*bP < 0.0 and cannot be square-rooted" <<G4endl;
841 G4cerr <<"Set to zero instead" <<G4endl;
842 G4cerr <<"########################################"
843 <<"########################################"
844 <<G4endl;
845 }
846 Ct = 2.0*std::sqrt(x);
847 }
848
849 G4double Ex = 13.0 * Cl / fermi;
850 if (Ct > 1.5*fermi)
851 Ex += 13.0 * Cl / fermi /3.0 * (Ct/fermi - 1.5);
852
853 return Ex;
854}
G4GLOB_DLL std::ostream G4cerr

References fermi, G4cerr, and G4endl.

Referenced by ApplyYourself().

◆ GetRecoilEnergyThreshold()

G4double G4HadronicInteraction::GetRecoilEnergyThreshold ( ) const
inlineinherited

◆ GetUseAblation()

G4bool G4WilsonAbrasionModel::GetUseAblation ( )
inline

Definition at line 126 of file G4WilsonAbrasionModel.hh.

127 {return useAblation;}

References useAblation.

◆ GetVerboseLevel()

G4int G4HadronicInteraction::GetVerboseLevel ( ) const
inlineinherited

Definition at line 109 of file G4HadronicInteraction.hh.

110 { return verboseLevel; }

References G4HadronicInteraction::verboseLevel.

◆ InitialiseModel()

void G4HadronicInteraction::InitialiseModel ( )
virtualinherited

◆ IsApplicable()

G4bool G4HadronicInteraction::IsApplicable ( const G4HadProjectile &  aTrack,
G4Nucleus &  targetNucleus 
)
virtualinherited

◆ IsBlocked() [1/3]

G4bool G4HadronicInteraction::IsBlocked ( ) const
inlineprotectedinherited

◆ IsBlocked() [2/3]

G4bool G4HadronicInteraction::IsBlocked ( const G4Element *  anElement) const
inherited

Definition at line 202 of file G4HadronicInteraction.cc.

203{
204 for (auto const& elm : theBlockedListElements) {
205 if (anElement == elm) return true;
206 }
207 return false;
208}

References G4HadronicInteraction::theBlockedListElements.

◆ IsBlocked() [3/3]

G4bool G4HadronicInteraction::IsBlocked ( const G4Material *  aMaterial) const
inherited

Definition at line 193 of file G4HadronicInteraction.cc.

194{
195 for (auto const& mat : theBlockedList) {
196 if (aMaterial == mat) return true;
197 }
198 return false;
199}

References G4HadronicInteraction::theBlockedList.

◆ ModelDescription()

void G4WilsonAbrasionModel::ModelDescription ( std::ostream &  outFile) const
virtual

Reimplemented from G4HadronicInteraction.

Definition at line 160 of file G4WilsonAbrasionModel.cc.

161{
162 outFile << "G4WilsonAbrasionModel is a macroscopic treatment of\n"
163 << "nucleus-nucleus collisions using simple geometric arguments.\n"
164 << "The smaller projectile nucleus gouges out a part of the larger\n"
165 << "target nucleus, leaving a residual nucleus and a fireball\n"
166 << "region where the projectile and target intersect. The fireball"
167 << "is then treated as a highly excited nuclear fragment. This\n"
168 << "model is based on the NUCFRG2 model and is valid for all\n"
169 << "projectile energies between 70 MeV/n and 10.1 GeV/n. \n";
170}

◆ operator!=()

G4bool G4HadronicInteraction::operator!= ( const G4HadronicInteraction &  right) const
deleteinherited

◆ operator=()

const G4WilsonAbrasionModel & G4WilsonAbrasionModel::operator= ( G4WilsonAbrasionModel &  right)
delete

◆ operator==()

G4bool G4HadronicInteraction::operator== ( const G4HadronicInteraction &  right) const
deleteinherited

◆ PrintWelcomeMessage()

void G4WilsonAbrasionModel::PrintWelcomeMessage ( )
private

Definition at line 879 of file G4WilsonAbrasionModel.cc.

880{
881 G4cout <<G4endl;
882 G4cout <<" *****************************************************************"
883 <<G4endl;
884 G4cout <<" Nuclear abrasion model for nuclear-nuclear interactions activated"
885 <<G4endl;
886 G4cout <<" (Written by QinetiQ Ltd for the European Space Agency)"
887 <<G4endl;
888 G4cout <<" *****************************************************************"
889 <<G4endl;
890 G4cout << G4endl;
891
892 return;
893}

References G4cout, and G4endl.

Referenced by G4WilsonAbrasionModel().

◆ SampleInvariantT()

G4double G4HadronicInteraction::SampleInvariantT ( const G4ParticleDefinition *  p,
G4double  plab,
G4int  Z,
G4int  A 
)
virtualinherited

◆ SetConserveEnergy()

void G4WilsonAbrasionModel::SetConserveEnergy ( G4bool  conserveEnergy1)
inlineprivate

Definition at line 129 of file G4WilsonAbrasionModel.hh.

130 {conserveEnergy = conserveEnergy1;}

References conserveEnergy.

◆ SetConserveMomentum()

void G4WilsonAbrasionModel::SetConserveMomentum ( G4bool  conserveMomentum1)
inline

Definition at line 135 of file G4WilsonAbrasionModel.hh.

136 {conserveMomentum = conserveMomentum1;}

References conserveMomentum.

◆ SetEnergyMomentumCheckLevels()

void G4HadronicInteraction::SetEnergyMomentumCheckLevels ( G4double  relativeLevel,
G4double  absoluteLevel 
)
inlineinherited

Definition at line 149 of file G4HadronicInteraction.hh.

150 { epCheckLevels.first = relativeLevel;
151 epCheckLevels.second = absoluteLevel; }

References G4HadronicInteraction::epCheckLevels.

Referenced by G4BinaryCascade::G4BinaryCascade(), G4CascadeInterface::G4CascadeInterface(), and G4FTFModel::G4FTFModel().

◆ SetExcitationHandler()

void G4WilsonAbrasionModel::SetExcitationHandler ( G4ExcitationHandler *  aExcitationHandler)
inline

Definition at line 120 of file G4WilsonAbrasionModel.hh.

121 {theExcitationHandler = aExcitationHandler;}

References theExcitationHandler.

◆ SetMaxEnergy() [1/3]

void G4HadronicInteraction::SetMaxEnergy ( const G4double  anEnergy)
inlineinherited

Definition at line 102 of file G4HadronicInteraction.hh.

103 { theMaxEnergy = anEnergy; }

References G4HadronicInteraction::theMaxEnergy.

Referenced by G4HadronicInteraction::ActivateFor(), G4IonINCLXXPhysics::AddProcess(), G4BertiniElectroNuclearBuilder::Build(), G4LENDBertiniGammaElectroNuclearBuilder::Build(), G4NeutronLENDBuilder::Build(), G4NeutronPHPBuilder::Build(), G4AlphaPHPBuilder::Build(), G4BertiniKaonBuilder::Build(), G4BertiniNeutronBuilder::Build(), G4BertiniPiKBuilder::Build(), G4BertiniPionBuilder::Build(), G4BertiniProtonBuilder::Build(), G4BinaryAlphaBuilder::Build(), G4BinaryDeuteronBuilder::Build(), G4BinaryHe3Builder::Build(), G4BinaryNeutronBuilder::Build(), G4BinaryPiKBuilder::Build(), G4BinaryPionBuilder::Build(), G4BinaryProtonBuilder::Build(), G4BinaryTritonBuilder::Build(), G4DeuteronPHPBuilder::Build(), G4FTFBinaryKaonBuilder::Build(), G4FTFBinaryNeutronBuilder::Build(), G4FTFBinaryPionBuilder::Build(), G4FTFBinaryProtonBuilder::Build(), G4FTFPAntiBarionBuilder::Build(), G4FTFPKaonBuilder::Build(), G4FTFPNeutronBuilder::Build(), G4FTFPPiKBuilder::Build(), G4FTFPPionBuilder::Build(), G4FTFPProtonBuilder::Build(), G4He3PHPBuilder::Build(), G4HyperonFTFPBuilder::Build(), G4HyperonQGSPBuilder::Build(), G4INCLXXNeutronBuilder::Build(), G4INCLXXPionBuilder::Build(), G4INCLXXProtonBuilder::Build(), G4PrecoNeutronBuilder::Build(), G4PrecoProtonBuilder::Build(), G4ProtonPHPBuilder::Build(), G4QGSBinaryKaonBuilder::Build(), G4QGSBinaryNeutronBuilder::Build(), G4QGSBinaryPiKBuilder::Build(), G4QGSBinaryPionBuilder::Build(), G4QGSBinaryProtonBuilder::Build(), G4QGSPAntiBarionBuilder::Build(), G4QGSPKaonBuilder::Build(), G4QGSPLundStrFragmProtonBuilder::Build(), G4QGSPNeutronBuilder::Build(), G4QGSPPiKBuilder::Build(), G4QGSPPionBuilder::Build(), G4TritonPHPBuilder::Build(), G4QGSPProtonBuilder::Build(), G4HadronicBuilder::BuildFTFP_BERT(), G4HadronicBuilder::BuildFTFQGSP_BERT(), G4QGSBuilder::BuildModel(), G4VHadronPhysics::BuildModel(), G4HadronicBuilder::BuildQGSP_FTFP_BERT(), G4EmExtraPhysics::ConstructGammaElectroNuclear(), LBE::ConstructHad(), G4EmExtraPhysics::ConstructLENDGammaNuclear(), G4HadronDElasticPhysics::ConstructProcess(), G4HadronElasticPhysics::ConstructProcess(), G4HadronHElasticPhysics::ConstructProcess(), G4IonINCLXXPhysics::ConstructProcess(), G4IonPhysics::ConstructProcess(), G4IonPhysicsPHP::ConstructProcess(), G4IonQMDPhysics::ConstructProcess(), G4ANuElNucleusNcModel::G4ANuElNucleusNcModel(), G4ANuMuNucleusNcModel::G4ANuMuNucleusNcModel(), G4BertiniKaonBuilder::G4BertiniKaonBuilder(), G4BertiniPiKBuilder::G4BertiniPiKBuilder(), G4BertiniPionBuilder::G4BertiniPionBuilder(), G4BinaryCascade::G4BinaryCascade(), G4BinaryPiKBuilder::G4BinaryPiKBuilder(), G4BinaryPionBuilder::G4BinaryPionBuilder(), G4ChargeExchange::G4ChargeExchange(), G4DiffuseElastic::G4DiffuseElastic(), G4DiffuseElasticV2::G4DiffuseElasticV2(), G4ElectroVDNuclearModel::G4ElectroVDNuclearModel(), G4EMDissociation::G4EMDissociation(), G4FissLib::G4FissLib(), G4FTFBinaryKaonBuilder::G4FTFBinaryKaonBuilder(), G4FTFBinaryNeutronBuilder::G4FTFBinaryNeutronBuilder(), G4FTFBinaryPiKBuilder::G4FTFBinaryPiKBuilder(), G4FTFBinaryPionBuilder::G4FTFBinaryPionBuilder(), G4FTFBinaryProtonBuilder::G4FTFBinaryProtonBuilder(), G4FTFPAntiBarionBuilder::G4FTFPAntiBarionBuilder(), G4FTFPKaonBuilder::G4FTFPKaonBuilder(), G4FTFPNeutronBuilder::G4FTFPNeutronBuilder(), G4FTFPPiKBuilder::G4FTFPPiKBuilder(), G4FTFPPionBuilder::G4FTFPPionBuilder(), G4FTFPProtonBuilder::G4FTFPProtonBuilder(), G4HadronElastic::G4HadronElastic(), G4HadronicAbsorptionFritiof::G4HadronicAbsorptionFritiof(), G4HadronicAbsorptionFritiofWithBinaryCascade::G4HadronicAbsorptionFritiofWithBinaryCascade(), G4hhElastic::G4hhElastic(), G4HyperonFTFPBuilder::G4HyperonFTFPBuilder(), G4HyperonQGSPBuilder::G4HyperonQGSPBuilder(), G4INCLXXPionBuilder::G4INCLXXPionBuilder(), G4LEHadronProtonElastic::G4LEHadronProtonElastic(), G4LENDModel::G4LENDModel(), G4LEnp::G4LEnp(), G4LEpp::G4LEpp(), G4LFission::G4LFission(), G4LowEGammaNuclearModel::G4LowEGammaNuclearModel(), G4MuonVDNuclearModel::G4MuonVDNuclearModel(), G4NeutrinoElectronCcModel::G4NeutrinoElectronCcModel(), G4NeutrinoElectronNcModel::G4NeutrinoElectronNcModel(), G4NeutrinoNucleusModel::G4NeutrinoNucleusModel(), G4NeutronElectronElModel::G4NeutronElectronElModel(), G4NeutronRadCapture::G4NeutronRadCapture(), G4NuclNuclDiffuseElastic::G4NuclNuclDiffuseElastic(), G4NuElNucleusNcModel::G4NuElNucleusNcModel(), G4NuMuNucleusNcModel::G4NuMuNucleusNcModel(), G4ParticleHPCapture::G4ParticleHPCapture(), G4ParticleHPElastic::G4ParticleHPElastic(), G4ParticleHPFission::G4ParticleHPFission(), G4ParticleHPInelastic::G4ParticleHPInelastic(), G4ParticleHPThermalScattering::G4ParticleHPThermalScattering(), G4QGSPAntiBarionBuilder::G4QGSPAntiBarionBuilder(), G4WilsonAbrasionModel(), G4HadronPhysicsFTFP_BERT_HP::Neutron(), G4HadronPhysicsINCLXX::Neutron(), G4HadronPhysicsQGSP_BERT_HP::Neutron(), G4HadronPhysicsQGSP_BIC_HP::Neutron(), G4HadronPhysicsShielding::Neutron(), and G4VHadronPhysics::NewModel().

◆ SetMaxEnergy() [2/3]

void G4HadronicInteraction::SetMaxEnergy ( G4double  anEnergy,
const G4Element *  anElement 
)
inherited

Definition at line 151 of file G4HadronicInteraction.cc.

153{
154 Block();
155 if(!theMaxEnergyListElements.empty()) {
156 for(auto & elmlist : theMaxEnergyListElements) {
157 if( anElement == elmlist.second ) {
158 elmlist.first = anEnergy;
159 return;
160 }
161 }
162 }
163 theMaxEnergyListElements.push_back(std::pair<G4double, const G4Element *>(anEnergy, anElement));
164}

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theMaxEnergyListElements.

◆ SetMaxEnergy() [3/3]

void G4HadronicInteraction::SetMaxEnergy ( G4double  anEnergy,
const G4Material *  aMaterial 
)
inherited

Definition at line 166 of file G4HadronicInteraction.cc.

167{
168 Block();
169 if(!theMaxEnergyList.empty()) {
170 for(auto & matlist: theMaxEnergyList) {
171 if( aMaterial == matlist.second ) {
172 matlist.first = anEnergy;
173 return;
174 }
175 }
176 }
177 theMaxEnergyList.push_back(std::pair<G4double, const G4Material *>(anEnergy, aMaterial));
178}

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theMaxEnergyList.

◆ SetMinEnergy() [1/3]

void G4HadronicInteraction::SetMinEnergy ( G4double  anEnergy)
inlineinherited

Definition at line 89 of file G4HadronicInteraction.hh.

90 { theMinEnergy = anEnergy; }

References G4HadronicInteraction::theMinEnergy.

Referenced by G4HadronicInteraction::ActivateFor(), G4BertiniElectroNuclearBuilder::Build(), G4LENDBertiniGammaElectroNuclearBuilder::Build(), G4NeutronLENDBuilder::Build(), G4NeutronPHPBuilder::Build(), G4AlphaPHPBuilder::Build(), G4BertiniKaonBuilder::Build(), G4BertiniNeutronBuilder::Build(), G4BertiniPiKBuilder::Build(), G4BertiniPionBuilder::Build(), G4BertiniProtonBuilder::Build(), G4BinaryAlphaBuilder::Build(), G4BinaryDeuteronBuilder::Build(), G4BinaryHe3Builder::Build(), G4BinaryNeutronBuilder::Build(), G4BinaryPiKBuilder::Build(), G4BinaryPionBuilder::Build(), G4BinaryProtonBuilder::Build(), G4BinaryTritonBuilder::Build(), G4DeuteronPHPBuilder::Build(), G4FTFBinaryKaonBuilder::Build(), G4FTFBinaryNeutronBuilder::Build(), G4FTFBinaryPiKBuilder::Build(), G4FTFBinaryPionBuilder::Build(), G4FTFBinaryProtonBuilder::Build(), G4FTFPAntiBarionBuilder::Build(), G4FTFPKaonBuilder::Build(), G4FTFPNeutronBuilder::Build(), G4FTFPPiKBuilder::Build(), G4FTFPPionBuilder::Build(), G4FTFPProtonBuilder::Build(), G4He3PHPBuilder::Build(), G4HyperonFTFPBuilder::Build(), G4HyperonQGSPBuilder::Build(), G4INCLXXNeutronBuilder::Build(), G4INCLXXPionBuilder::Build(), G4INCLXXProtonBuilder::Build(), G4PrecoNeutronBuilder::Build(), G4PrecoProtonBuilder::Build(), G4ProtonPHPBuilder::Build(), G4QGSBinaryKaonBuilder::Build(), G4QGSBinaryNeutronBuilder::Build(), G4QGSBinaryPiKBuilder::Build(), G4QGSBinaryPionBuilder::Build(), G4QGSBinaryProtonBuilder::Build(), G4QGSPAntiBarionBuilder::Build(), G4QGSPKaonBuilder::Build(), G4QGSPLundStrFragmProtonBuilder::Build(), G4QGSPNeutronBuilder::Build(), G4QGSPPiKBuilder::Build(), G4QGSPPionBuilder::Build(), G4TritonPHPBuilder::Build(), G4QGSPProtonBuilder::Build(), G4QGSBuilder::BuildModel(), G4VHadronPhysics::BuildModel(), G4EmExtraPhysics::ConstructGammaElectroNuclear(), LBE::ConstructHad(), G4EmExtraPhysics::ConstructLENDGammaNuclear(), G4HadronElasticPhysicsHP::ConstructProcess(), G4HadronElasticPhysicsLEND::ConstructProcess(), G4HadronElasticPhysicsPHP::ConstructProcess(), G4HadronDElasticPhysics::ConstructProcess(), G4HadronElasticPhysics::ConstructProcess(), G4HadronHElasticPhysics::ConstructProcess(), G4IonElasticPhysics::ConstructProcess(), G4IonINCLXXPhysics::ConstructProcess(), G4IonPhysics::ConstructProcess(), G4IonPhysicsPHP::ConstructProcess(), G4IonQMDPhysics::ConstructProcess(), G4ANuElNucleusNcModel::G4ANuElNucleusNcModel(), G4ANuMuNucleusNcModel::G4ANuMuNucleusNcModel(), G4BertiniKaonBuilder::G4BertiniKaonBuilder(), G4BertiniPiKBuilder::G4BertiniPiKBuilder(), G4BertiniPionBuilder::G4BertiniPionBuilder(), G4BinaryCascade::G4BinaryCascade(), G4BinaryPiKBuilder::G4BinaryPiKBuilder(), G4BinaryPionBuilder::G4BinaryPionBuilder(), G4ChargeExchange::G4ChargeExchange(), G4DiffuseElastic::G4DiffuseElastic(), G4DiffuseElasticV2::G4DiffuseElasticV2(), G4ElectroVDNuclearModel::G4ElectroVDNuclearModel(), G4EMDissociation::G4EMDissociation(), G4FissLib::G4FissLib(), G4FTFBinaryKaonBuilder::G4FTFBinaryKaonBuilder(), G4FTFBinaryNeutronBuilder::G4FTFBinaryNeutronBuilder(), G4FTFBinaryPiKBuilder::G4FTFBinaryPiKBuilder(), G4FTFBinaryPionBuilder::G4FTFBinaryPionBuilder(), G4FTFBinaryProtonBuilder::G4FTFBinaryProtonBuilder(), G4FTFPAntiBarionBuilder::G4FTFPAntiBarionBuilder(), G4FTFPKaonBuilder::G4FTFPKaonBuilder(), G4FTFPNeutronBuilder::G4FTFPNeutronBuilder(), G4FTFPPiKBuilder::G4FTFPPiKBuilder(), G4FTFPPionBuilder::G4FTFPPionBuilder(), G4FTFPProtonBuilder::G4FTFPProtonBuilder(), G4HadronElastic::G4HadronElastic(), G4HadronicAbsorptionBertini::G4HadronicAbsorptionBertini(), G4HadronicAbsorptionFritiof::G4HadronicAbsorptionFritiof(), G4HadronicAbsorptionFritiofWithBinaryCascade::G4HadronicAbsorptionFritiofWithBinaryCascade(), G4hhElastic::G4hhElastic(), G4HyperonFTFPBuilder::G4HyperonFTFPBuilder(), G4HyperonQGSPBuilder::G4HyperonQGSPBuilder(), G4INCLXXPionBuilder::G4INCLXXPionBuilder(), G4LEHadronProtonElastic::G4LEHadronProtonElastic(), G4LENDModel::G4LENDModel(), G4LEnp::G4LEnp(), G4LEpp::G4LEpp(), G4LFission::G4LFission(), G4LowEGammaNuclearModel::G4LowEGammaNuclearModel(), G4MuonVDNuclearModel::G4MuonVDNuclearModel(), G4NeutrinoElectronCcModel::G4NeutrinoElectronCcModel(), G4NeutrinoElectronNcModel::G4NeutrinoElectronNcModel(), G4NeutrinoNucleusModel::G4NeutrinoNucleusModel(), G4NeutronElectronElModel::G4NeutronElectronElModel(), G4NeutronRadCapture::G4NeutronRadCapture(), G4NuclNuclDiffuseElastic::G4NuclNuclDiffuseElastic(), G4NuElNucleusNcModel::G4NuElNucleusNcModel(), G4NuMuNucleusNcModel::G4NuMuNucleusNcModel(), G4ParticleHPCapture::G4ParticleHPCapture(), G4ParticleHPElastic::G4ParticleHPElastic(), G4ParticleHPFission::G4ParticleHPFission(), G4ParticleHPInelastic::G4ParticleHPInelastic(), G4ParticleHPThermalScattering::G4ParticleHPThermalScattering(), G4QGSPAntiBarionBuilder::G4QGSPAntiBarionBuilder(), G4WilsonAbrasionModel(), G4NeutrinoElectronCcModel::IsApplicable(), G4HadronPhysicsFTFP_BERT_HP::Neutron(), G4HadronPhysicsINCLXX::Neutron(), G4HadronPhysicsQGSP_BERT_HP::Neutron(), G4HadronPhysicsQGSP_BIC_HP::Neutron(), G4HadronPhysicsShielding::Neutron(), and G4VHadronPhysics::NewModel().

◆ SetMinEnergy() [2/3]

void G4HadronicInteraction::SetMinEnergy ( G4double  anEnergy,
const G4Element *  anElement 
)
inherited

Definition at line 101 of file G4HadronicInteraction.cc.

103{
104 Block();
105 if(!theMinEnergyListElements.empty()) {
106 for(auto & elmlist : theMinEnergyListElements) {
107 if( anElement == elmlist.second ) {
108 elmlist.first = anEnergy;
109 return;
110 }
111 }
112 }
113 theMinEnergyListElements.push_back(std::pair<G4double, const G4Element *>(anEnergy, anElement));
114}

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theMinEnergyListElements.

◆ SetMinEnergy() [3/3]

void G4HadronicInteraction::SetMinEnergy ( G4double  anEnergy,
const G4Material *  aMaterial 
)
inherited

Definition at line 116 of file G4HadronicInteraction.cc.

118{
119 Block();
120 if(!theMinEnergyList.empty()) {
121 for(auto & matlist : theMinEnergyList) {
122 if( aMaterial == matlist.second ) {
123 matlist.first = anEnergy;
124 return;
125 }
126 }
127 }
128 theMinEnergyList.push_back(std::pair<G4double, const G4Material *>(anEnergy, aMaterial));
129}

References G4HadronicInteraction::Block(), and G4HadronicInteraction::theMinEnergyList.

◆ SetModelName()

void G4HadronicInteraction::SetModelName ( const G4String &  nam)
inlineprotectedinherited

◆ SetRecoilEnergyThreshold()

void G4HadronicInteraction::SetRecoilEnergyThreshold ( G4double  val)
inlineinherited

◆ SetUseAblation()

void G4WilsonAbrasionModel::SetUseAblation ( G4bool  useAblation1)

◆ SetVerboseLevel()

void G4WilsonAbrasionModel::SetVerboseLevel ( G4int  verboseLevel1)
inline

Field Documentation

◆ B

G4double G4WilsonAbrasionModel::B
private

Definition at line 113 of file G4WilsonAbrasionModel.hh.

Referenced by ApplyYourself(), and G4WilsonAbrasionModel().

◆ conserveEnergy

G4bool G4WilsonAbrasionModel::conserveEnergy
private

◆ conserveMomentum

G4bool G4WilsonAbrasionModel::conserveMomentum
private

◆ epCheckLevels

std::pair<G4double, G4double> G4HadronicInteraction::epCheckLevels
privateinherited

◆ fradius

G4double G4WilsonAbrasionModel::fradius
private

Definition at line 115 of file G4WilsonAbrasionModel.hh.

Referenced by ApplyYourself(), and G4WilsonAbrasionModel().

◆ isBlocked

G4bool G4HadronicInteraction::isBlocked
protectedinherited

◆ npK

G4double G4WilsonAbrasionModel::npK
private

Definition at line 107 of file G4WilsonAbrasionModel.hh.

Referenced by G4WilsonAbrasionModel(), and GetAbradedNucleons().

◆ r0sq

G4double G4WilsonAbrasionModel::r0sq
private

Definition at line 106 of file G4WilsonAbrasionModel.hh.

Referenced by G4WilsonAbrasionModel().

◆ recoilEnergyThreshold

G4double G4HadronicInteraction::recoilEnergyThreshold
privateinherited

◆ registry

G4HadronicInteractionRegistry* G4HadronicInteraction::registry
privateinherited

◆ secID

G4int G4WilsonAbrasionModel::secID
private

◆ theAblation

G4WilsonAblationModel* G4WilsonAbrasionModel::theAblation
private

◆ theBlockedList

std::vector<const G4Material *> G4HadronicInteraction::theBlockedList
privateinherited

◆ theBlockedListElements

std::vector<const G4Element *> G4HadronicInteraction::theBlockedListElements
privateinherited

◆ theExcitationHandler

G4ExcitationHandler* G4WilsonAbrasionModel::theExcitationHandler
private

◆ theMaxEnergy

G4double G4HadronicInteraction::theMaxEnergy
protectedinherited

◆ theMaxEnergyList

std::vector<std::pair<G4double, const G4Material *> > G4HadronicInteraction::theMaxEnergyList
privateinherited

◆ theMaxEnergyListElements

std::vector<std::pair<G4double, const G4Element *> > G4HadronicInteraction::theMaxEnergyListElements
privateinherited

◆ theMinEnergy

G4double G4HadronicInteraction::theMinEnergy
protectedinherited

◆ theMinEnergyList

std::vector<std::pair<G4double, const G4Material *> > G4HadronicInteraction::theMinEnergyList
privateinherited

◆ theMinEnergyListElements

std::vector<std::pair<G4double, const G4Element *> > G4HadronicInteraction::theMinEnergyListElements
privateinherited

◆ theModelName

G4String G4HadronicInteraction::theModelName
privateinherited

◆ theParticleChange

G4HadFinalState G4HadronicInteraction::theParticleChange
protectedinherited

Definition at line 172 of file G4HadronicInteraction.hh.

Referenced by ApplyYourself(), G4EMDissociation::ApplyYourself(), G4LENDCapture::ApplyYourself(), G4LENDElastic::ApplyYourself(), G4LENDFission::ApplyYourself(), G4LENDInelastic::ApplyYourself(), G4ElectroVDNuclearModel::ApplyYourself(), G4ParticleHPThermalScattering::ApplyYourself(), G4NeutrinoElectronNcModel::ApplyYourself(), G4NeutronElectronElModel::ApplyYourself(), G4LFission::ApplyYourself(), G4ANuElNucleusCcModel::ApplyYourself(), G4ANuElNucleusNcModel::ApplyYourself(), G4ANuMuNucleusCcModel::ApplyYourself(), G4ANuMuNucleusNcModel::ApplyYourself(), G4MuonVDNuclearModel::ApplyYourself(), G4NeutrinoElectronCcModel::ApplyYourself(), G4NuElNucleusCcModel::ApplyYourself(), G4NuElNucleusNcModel::ApplyYourself(), G4NuMuNucleusCcModel::ApplyYourself(), G4NuMuNucleusNcModel::ApplyYourself(), G4QMDReaction::ApplyYourself(), G4NeutronRadCapture::ApplyYourself(), G4LowEGammaNuclearModel::ApplyYourself(), G4ChargeExchange::ApplyYourself(), G4HadronElastic::ApplyYourself(), G4LEHadronProtonElastic::ApplyYourself(), G4LEnp::ApplyYourself(), G4LEpp::ApplyYourself(), G4BinaryCascade::ApplyYourself(), G4CascadeInterface::ApplyYourself(), G4LMsdGenerator::ApplyYourself(), G4ElectroVDNuclearModel::CalculateEMVertex(), G4MuonVDNuclearModel::CalculateEMVertex(), G4ElectroVDNuclearModel::CalculateHadronicVertex(), G4MuonVDNuclearModel::CalculateHadronicVertex(), G4NeutrinoNucleusModel::CoherentPion(), G4CascadeInterface::copyOutputToHadronicResult(), G4BinaryCascade::DebugEpConservation(), G4BinaryCascade::DebugFinalEpConservation(), G4NeutrinoNucleusModel::FinalBarion(), G4NeutrinoNucleusModel::FinalMeson(), GetAbradedNucleons(), G4CascadeInterface::NoInteraction(), G4CascadeInterface::Propagate(), G4NeutrinoNucleusModel::RecoilDeexcitation(), G4LEHadronProtonElastic::~G4LEHadronProtonElastic(), G4LEnp::~G4LEnp(), and G4LFission::~G4LFission().

◆ third

G4double G4WilsonAbrasionModel::third
private

Definition at line 114 of file G4WilsonAbrasionModel.hh.

Referenced by G4WilsonAbrasionModel().

◆ useAblation

G4bool G4WilsonAbrasionModel::useAblation
private

◆ verboseLevel

G4int G4HadronicInteraction::verboseLevel
protectedinherited

Definition at line 177 of file G4HadronicInteraction.hh.

Referenced by ApplyYourself(), G4EMDissociation::ApplyYourself(), G4LFission::ApplyYourself(), G4MuMinusCapturePrecompound::ApplyYourself(), G4NeutronRadCapture::ApplyYourself(), G4LowEGammaNuclearModel::ApplyYourself(), G4ChargeExchange::ApplyYourself(), G4HadronElastic::ApplyYourself(), G4LEHadronProtonElastic::ApplyYourself(), G4LEnp::ApplyYourself(), G4LEpp::ApplyYourself(), G4CascadeInterface::ApplyYourself(), G4CascadeInterface::checkFinalResult(), G4CascadeInterface::copyOutputToHadronicResult(), G4CascadeInterface::copyOutputToReactionProducts(), G4LENDModel::create_used_target_map(), G4CascadeInterface::createBullet(), G4CascadeInterface::createTarget(), G4ElasticHadrNucleusHE::DefineHadronValues(), G4ElasticHadrNucleusHE::FillData(), G4ElasticHadrNucleusHE::FillFq2(), G4DiffuseElastic::G4DiffuseElastic(), G4DiffuseElasticV2::G4DiffuseElasticV2(), G4ElasticHadrNucleusHE::G4ElasticHadrNucleusHE(), G4EMDissociation::G4EMDissociation(), G4hhElastic::G4hhElastic(), G4NuclNuclDiffuseElastic::G4NuclNuclDiffuseElastic(), G4WilsonAbrasionModel(), G4ElasticHadrNucleusHE::GetFt(), G4ElasticHadrNucleusHE::GetLightFq2(), G4ElasticHadrNucleusHE::GetQ2_2(), G4HadronicInteraction::GetVerboseLevel(), G4ElasticHadrNucleusHE::HadronNucleusQ2_2(), G4ElasticHadrNucleusHE::HadronProtonQ2(), G4LFission::init(), G4DiffuseElastic::Initialise(), G4DiffuseElasticV2::Initialise(), G4NuclNuclDiffuseElastic::Initialise(), G4DiffuseElastic::InitialiseOnFly(), G4DiffuseElasticV2::InitialiseOnFly(), G4NuclNuclDiffuseElastic::InitialiseOnFly(), G4CascadeInterface::makeDynamicParticle(), G4CascadeInterface::NoInteraction(), G4CascadeInterface::Propagate(), G4ElasticHadrNucleusHE::SampleInvariantT(), G4AntiNuclElastic::SampleThetaCMS(), G4DiffuseElastic::SampleThetaLab(), G4NuclNuclDiffuseElastic::SampleThetaLab(), G4AntiNuclElastic::SampleThetaLab(), SetUseAblation(), G4HadronicInteraction::SetVerboseLevel(), SetVerboseLevel(), G4DiffuseElastic::ThetaCMStoThetaLab(), G4DiffuseElasticV2::ThetaCMStoThetaLab(), G4NuclNuclDiffuseElastic::ThetaCMStoThetaLab(), G4DiffuseElastic::ThetaLabToThetaCMS(), G4DiffuseElasticV2::ThetaLabToThetaCMS(), and G4NuclNuclDiffuseElastic::ThetaLabToThetaCMS().


The documentation for this class was generated from the following files: