Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
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G4HEAntiSigmaMinusInelastic.cc
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1//
2// ********************************************************************
3// * License and Disclaimer *
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6// * the Geant4 Collaboration. It is provided under the terms and *
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14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
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24// ********************************************************************
25//
26// $Id$
27//
28
29// G4 Process: Gheisha High Energy Collision model.
30// This includes the high energy cascading model, the two-body-resonance model
31// and the low energy two-body model. Not included are the low energy stuff
32// like nuclear reactions, nuclear fission without any cascading and all
33// processes for particles at rest.
34// First work done by J.L.Chuma and F.W.Jones, TRIUMF, June 96.
35// H. Fesefeldt, RWTH-Aachen, 23-October-1996
36
37#include "G4HEAntiSigmaMinusInelastic.hh"
38#include "globals.hh"
39#include "G4ios.hh"
40#include "G4PhysicalConstants.hh"
41#include "G4SystemOfUnits.hh"
42
43void G4HEAntiSigmaMinusInelastic::ModelDescription(std::ostream& outFile) const
44{
45 outFile << "G4HEAntiSigmaMinusInelastic is one of the High Energy\n"
46 << "Parameterized (HEP) models used to implement inelastic\n"
47 << "anti-Sigma- scattering from nuclei. It is a re-engineered\n"
48 << "version of the GHEISHA code of H. Fesefeldt. It divides the\n"
49 << "initial collision products into backward- and forward-going\n"
50 << "clusters which are then decayed into final state hadrons.\n"
51 << "The model does not conserve energy on an event-by-event\n"
52 << "basis. It may be applied to anti-Sigma- with initial\n"
53 << "energies above 20 GeV.\n";
54}
55
56
57G4HadFinalState*
58G4HEAntiSigmaMinusInelastic::ApplyYourself(const G4HadProjectile& aTrack,
59 G4Nucleus& targetNucleus)
60{
61 G4HEVector* pv = new G4HEVector[MAXPART];
62 const G4HadProjectile* aParticle = &aTrack;
63 const G4double atomicWeight = targetNucleus.GetA_asInt();
64 const G4double atomicNumber = targetNucleus.GetZ_asInt();
65 G4HEVector incidentParticle(aParticle);
66
67 G4int incidentCode = incidentParticle.getCode();
68 G4double incidentMass = incidentParticle.getMass();
69 G4double incidentTotalEnergy = incidentParticle.getEnergy();
70
71 // G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
72 // DHW 19 May 2011: variable set but not used
73
74 G4double incidentKineticEnergy = incidentTotalEnergy - incidentMass;
75
76 if (incidentKineticEnergy < 1.)
77 G4cout << "GHEAntiSigmaMinusInelastic: incident energy < 1 GeV" << G4endl;
78
79 if (verboseLevel > 1) {
80 G4cout << "G4HEAntiSigmaMinusInelastic::ApplyYourself" << G4endl;
81 G4cout << "incident particle " << incidentParticle.getName()
82 << "mass " << incidentMass
83 << "kinetic energy " << incidentKineticEnergy
84 << G4endl;
85 G4cout << "target material with (A,Z) = ("
86 << atomicWeight << "," << atomicNumber << ")" << G4endl;
87 }
88
89 G4double inelasticity = NuclearInelasticity(incidentKineticEnergy,
90 atomicWeight, atomicNumber);
91 if (verboseLevel > 1)
92 G4cout << "nuclear inelasticity = " << inelasticity << G4endl;
93
94 incidentKineticEnergy -= inelasticity;
95
96 G4double excitationEnergyGNP = 0.;
97 G4double excitationEnergyDTA = 0.;
98
99 G4double excitation = NuclearExcitation(incidentKineticEnergy,
100 atomicWeight, atomicNumber,
101 excitationEnergyGNP,
102 excitationEnergyDTA);
103 if (verboseLevel > 1)
104 G4cout << "nuclear excitation = " << excitation << excitationEnergyGNP
105 << excitationEnergyDTA << G4endl;
106
107 incidentKineticEnergy -= excitation;
108 incidentTotalEnergy = incidentKineticEnergy + incidentMass;
109 // incidentTotalMomentum = std::sqrt( (incidentTotalEnergy-incidentMass)
110 // *(incidentTotalEnergy+incidentMass));
111 // DHW 19 May 2011: variable set but not used
112
113 G4HEVector targetParticle;
114 if (G4UniformRand() < atomicNumber/atomicWeight) {
115 targetParticle.setDefinition("Proton");
116 } else {
117 targetParticle.setDefinition("Neutron");
118 }
119
120 G4double targetMass = targetParticle.getMass();
121 G4double centerOfMassEnergy = std::sqrt(incidentMass*incidentMass
122 + targetMass*targetMass
123 + 2.0*targetMass*incidentTotalEnergy);
124 G4double availableEnergy = centerOfMassEnergy - targetMass - incidentMass;
125
126 G4bool inElastic = true;
127 vecLength = 0;
128
129 if (verboseLevel > 1)
130 G4cout << "ApplyYourself: CallFirstIntInCascade for particle "
131 << incidentCode << G4endl;
132
133 G4bool successful = false;
134
135 FirstIntInCasAntiSigmaMinus(inElastic, availableEnergy, pv, vecLength,
136 incidentParticle, targetParticle, atomicWeight);
137
138 if (verboseLevel > 1)
139 G4cout << "ApplyYourself::StrangeParticlePairProduction" << G4endl;
140
141 if ((vecLength > 0) && (availableEnergy > 1.))
142 StrangeParticlePairProduction(availableEnergy, centerOfMassEnergy,
143 pv, vecLength,
144 incidentParticle, targetParticle);
145 HighEnergyCascading(successful, pv, vecLength,
146 excitationEnergyGNP, excitationEnergyDTA,
147 incidentParticle, targetParticle,
148 atomicWeight, atomicNumber);
149 if (!successful)
150 HighEnergyClusterProduction(successful, pv, vecLength,
151 excitationEnergyGNP, excitationEnergyDTA,
152 incidentParticle, targetParticle,
153 atomicWeight, atomicNumber);
154 if (!successful)
155 MediumEnergyCascading(successful, pv, vecLength,
156 excitationEnergyGNP, excitationEnergyDTA,
157 incidentParticle, targetParticle,
158 atomicWeight, atomicNumber);
159
160 if (!successful)
161 MediumEnergyClusterProduction(successful, pv, vecLength,
162 excitationEnergyGNP, excitationEnergyDTA,
163 incidentParticle, targetParticle,
164 atomicWeight, atomicNumber);
165 if (!successful)
166 QuasiElasticScattering(successful, pv, vecLength,
167 excitationEnergyGNP, excitationEnergyDTA,
168 incidentParticle, targetParticle,
169 atomicWeight, atomicNumber);
170 if (!successful)
171 ElasticScattering(successful, pv, vecLength,
172 incidentParticle,
173 atomicWeight, atomicNumber);
174
175 if (!successful)
176 G4cout << "GHEInelasticInteraction::ApplyYourself fails to produce final state particles"
177 << G4endl;
178 FillParticleChange(pv, vecLength);
179 delete [] pv;
180 theParticleChange.SetStatusChange(stopAndKill);
181 return &theParticleChange;
182}
183
184
185void
186G4HEAntiSigmaMinusInelastic::FirstIntInCasAntiSigmaMinus(G4bool& inElastic,
187 const G4double availableEnergy,
188 G4HEVector pv[],
189 G4int& vecLen,
190 const G4HEVector& incidentParticle,
191 const G4HEVector& targetParticle,
192 const G4double atomicWeight)
193
194// AntiSigma- undergoes interaction with nucleon within a nucleus. Check if it is
195// energetically possible to produce pions/kaons. In not, assume nuclear excitation
196// occurs and input particle is degraded in energy. No other particles are produced.
197// If reaction is possible, find the correct number of pions/protons/neutrons
198// produced using an interpolation to multiplicity data. Replace some pions or
199// protons/neutrons by kaons or strange baryons according to the average
200// multiplicity per inelastic reaction.
201{
202 static const G4double expxu = 82; // upper bound for arg. of exp
203 static const G4double expxl = -expxu; // lower bound for arg. of exp
204
205 static const G4double protb = 0.7;
206 static const G4double neutb = 0.7;
207 static const G4double c = 1.25;
208
209 static const G4int numMul = 1200;
210 static const G4int numMulAn = 400;
211 static const G4int numSec = 60;
212
213 G4int neutronCode = Neutron.getCode();
214 G4int protonCode = Proton.getCode();
215
216 G4int targetCode = targetParticle.getCode();
217 G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
218
219 static G4bool first = true;
220 static G4double protmul[numMul], protnorm[numSec]; // proton constants
221 static G4double protmulAn[numMulAn],protnormAn[numSec];
222 static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
223 static G4double neutmulAn[numMulAn],neutnormAn[numSec];
224
225 // misc. local variables
226 // npos = number of pi+, nneg = number of pi-, nzero = number of pi0
227
228 G4int i, counter, nt, npos, nneg, nzero;
229
230 if( first )
231 { // compute normalization constants, this will only be done once
232 first = false;
233 for( i=0; i<numMul ; i++ ) protmul[i] = 0.0;
234 for( i=0; i<numSec ; i++ ) protnorm[i] = 0.0;
235 counter = -1;
236 for( npos=0; npos<(numSec/3); npos++ )
237 {
238 for( nneg=std::max(0,npos-2); nneg<=npos; nneg++ )
239 {
240 for( nzero=0; nzero<numSec/3; nzero++ )
241 {
242 if( ++counter < numMul )
243 {
244 nt = npos+nneg+nzero;
245 if( (nt>0) && (nt<=numSec) )
246 {
247 protmul[counter] = pmltpc(npos,nneg,nzero,nt,protb,c);
248 protnorm[nt-1] += protmul[counter];
249 }
250 }
251 }
252 }
253 }
254 for( i=0; i<numMul; i++ )neutmul[i] = 0.0;
255 for( i=0; i<numSec; i++ )neutnorm[i] = 0.0;
256 counter = -1;
257 for( npos=0; npos<numSec/3; npos++ )
258 {
259 for( nneg=std::max(0,npos-1); nneg<=(npos+1); nneg++ )
260 {
261 for( nzero=0; nzero<numSec/3; nzero++ )
262 {
263 if( ++counter < numMul )
264 {
265 nt = npos+nneg+nzero;
266 if( (nt>0) && (nt<=numSec) )
267 {
268 neutmul[counter] = pmltpc(npos,nneg,nzero,nt,neutb,c);
269 neutnorm[nt-1] += neutmul[counter];
270 }
271 }
272 }
273 }
274 }
275 for( i=0; i<numSec; i++ )
276 {
277 if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
278 if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
279 }
280 // annihilation
281 for( i=0; i<numMulAn ; i++ ) protmulAn[i] = 0.0;
282 for( i=0; i<numSec ; i++ ) protnormAn[i] = 0.0;
283 counter = -1;
284 for( npos=1; npos<(numSec/3); npos++ )
285 {
286 nneg = std::max(0,npos-2);
287 for( nzero=0; nzero<numSec/3; nzero++ )
288 {
289 if( ++counter < numMulAn )
290 {
291 nt = npos+nneg+nzero;
292 if( (nt>1) && (nt<=numSec) )
293 {
294 protmulAn[counter] = pmltpc(npos,nneg,nzero,nt,protb,c);
295 protnormAn[nt-1] += protmulAn[counter];
296 }
297 }
298 }
299 }
300 for( i=0; i<numMulAn; i++ ) neutmulAn[i] = 0.0;
301 for( i=0; i<numSec; i++ ) neutnormAn[i] = 0.0;
302 counter = -1;
303 for( npos=0; npos<numSec/3; npos++ )
304 {
305 nneg = npos-1;
306 for( nzero=0; nzero<numSec/3; nzero++ )
307 {
308 if( ++counter < numMulAn )
309 {
310 nt = npos+nneg+nzero;
311 if( (nt>1) && (nt<=numSec) )
312 {
313 neutmulAn[counter] = pmltpc(npos,nneg,nzero,nt,neutb,c);
314 neutnormAn[nt-1] += neutmulAn[counter];
315 }
316 }
317 }
318 }
319 for( i=0; i<numSec; i++ )
320 {
321 if( protnormAn[i] > 0.0 )protnormAn[i] = 1.0/protnormAn[i];
322 if( neutnormAn[i] > 0.0 )neutnormAn[i] = 1.0/neutnormAn[i];
323 }
324 } // end of initialization
325
326
327 // initialize the first two places
328 // the same as beam and target
329 pv[0] = incidentParticle;
330 pv[1] = targetParticle;
331 vecLen = 2;
332
333 if( !inElastic )
334 { // some two-body reactions
335 G4double cech[] = {0.50, 0.45, 0.40, 0.35, 0.30, 0.25, 0.06, 0.04, 0.005, 0.};
336
337 G4int iplab = std::min(9, G4int( incidentTotalMomentum*2.5 ));
338 if( G4UniformRand() < cech[iplab]/std::pow(atomicWeight,0.42) )
339 {
340 G4double ran = G4UniformRand();
341
342 if ( targetCode == neutronCode)
343 {
344 if(ran < 0.2)
345 {
346 pv[0] = AntiSigmaZero;
347 pv[1] = Proton;
348 }
349 else if (ran < 0.4)
350 {
351 pv[0] = AntiLambda;
352 pv[1] = Proton;
353 }
354 else if (ran < 0.6)
355 {
356 pv[0] = Proton;
357 pv[1] = AntiLambda;
358 }
359 else if (ran < 0.8)
360 {
361 pv[0] = Proton;
362 pv[1] = AntiSigmaZero;
363 }
364 else
365 {
366 pv[0] = Neutron;
367 pv[1] = AntiSigmaMinus;
368 }
369 }
370 else
371 {
372 pv[0] = Proton;
373 pv[1] = AntiSigmaMinus;
374 }
375 }
376 return;
377 }
378 else if (availableEnergy <= PionPlus.getMass())
379 return;
380
381 // inelastic scattering
382
383 npos = 0; nneg = 0; nzero = 0;
384 G4double anhl[] = {1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 1.00, 0.97, 0.88,
385 0.85, 0.81, 0.75, 0.64, 0.64, 0.55, 0.55, 0.45, 0.47, 0.40,
386 0.39, 0.36, 0.33, 0.10, 0.01};
387 G4int iplab = G4int( incidentTotalMomentum*10.);
388 if ( iplab > 9) iplab = 10 + G4int( (incidentTotalMomentum -1.)*5. );
389 if ( iplab > 14) iplab = 15 + G4int( incidentTotalMomentum -2. );
390 if ( iplab > 22) iplab = 23 + G4int( (incidentTotalMomentum -10.)/10.);
391 iplab = std::min(24, iplab);
392
393 if (G4UniformRand() > anhl[iplab]) { // non- annihilation channels
394
395 // number of total particles vs. centre of mass Energy - 2*proton mass
396 G4double aleab = std::log(availableEnergy);
397 G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514
398 + aleab*(0.117712+0.0136912*aleab))) - 2.0;
399
400 // normalization constant for kno-distribution.
401 // calculate first the sum of all constants, check for numerical problems.
402 G4double test, dum, anpn = 0.0;
403
404 for (nt=1; nt<=numSec; nt++) {
405 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
406 dum = pi*nt/(2.0*n*n);
407 if (std::fabs(dum) < 1.0) {
408 if( test >= 1.0e-10 )anpn += dum*test;
409 } else {
410 anpn += dum*test;
411 }
412 }
413
414 G4double ran = G4UniformRand();
415 G4double excs = 0.0;
416 if (targetCode == protonCode) {
417 counter = -1;
418 for (npos = 0; npos < numSec/3; npos++) {
419 for (nneg = std::max(0,npos-2); nneg <= npos; nneg++) {
420 for (nzero = 0; nzero < numSec/3; nzero++) {
421 if (++counter < numMul) {
422 nt = npos+nneg+nzero;
423 if ((nt > 0) && (nt <= numSec) ) {
424 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
425 dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
426 if (std::fabs(dum) < 1.0) {
427 if( test >= 1.0e-10 )excs += dum*test;
428 } else {
429 excs += dum*test;
430 }
431
432 if (ran < excs) goto outOfLoop; //----------------------->
433 }
434 }
435 }
436 }
437 }
438 // 3 previous loops continued to the end
439 inElastic = false; // quasi-elastic scattering
440 return;
441 } else { // target must be a neutron
442 counter = -1;
443 for( npos=0; npos<numSec/3; npos++ )
444 {
445 for( nneg=std::max(0,npos-1); nneg<=(npos+1); nneg++ )
446 {
447 for( nzero=0; nzero<numSec/3; nzero++ )
448 {
449 if( ++counter < numMul )
450 {
451 nt = npos+nneg+nzero;
452 if ( (nt>0) && (nt<=numSec) ) {
453 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
454 dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
455 if (std::fabs(dum) < 1.0) {
456 if( test >= 1.0e-10 )excs += dum*test;
457 } else {
458 excs += dum*test;
459 }
460
461 if (ran < excs) goto outOfLoop; // -------------------------->
462 }
463 }
464 }
465 }
466 }
467 // 3 previous loops continued to the end
468 inElastic = false; // quasi-elastic scattering.
469 return;
470 }
471
472 outOfLoop: // <------------------------------------------------------------------------
473
474 ran = G4UniformRand();
475
476 if( targetCode == protonCode)
477 {
478 if( npos == nneg)
479 {
480 }
481 else if (npos == (nneg+1))
482 {
483 if( ran < 0.50)
484 {
485 pv[1] = Neutron;
486 }
487 else if (ran < 0.75)
488 {
489 pv[0] = AntiSigmaZero;
490 }
491 else
492 {
493 pv[0] = AntiLambda;
494 }
495 }
496 else
497 {
498 if (ran < 0.5)
499 {
500 pv[0] = AntiSigmaZero;
501 pv[1] = Neutron;
502 }
503 else
504 {
505 pv[0] = AntiLambda;
506 pv[1] = Neutron;
507 }
508 }
509 }
510 else
511 {
512 if( npos == nneg)
513 {
514 if (ran < 0.5)
515 {
516 }
517 else if(ran < 0.75)
518 {
519 pv[0] = AntiSigmaZero;
520 pv[1] = Proton;
521 }
522 else
523 {
524 pv[0] = AntiLambda;
525 pv[1] = Proton;
526 }
527 }
528 else if ( npos == (nneg+1))
529 {
530 if (ran < 0.5)
531 {
532 pv[0] = AntiSigmaZero;
533 }
534 else
535 {
536 pv[0] = AntiLambda;
537 }
538 }
539 else
540 {
541 pv[1] = Proton;
542 }
543 }
544
545 }
546 else // annihilation
547 {
548 if ( availableEnergy > 2. * PionPlus.getMass() )
549 {
550
551 G4double aleab = std::log(availableEnergy);
552 G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514
553 + aleab*(0.117712+0.0136912*aleab))) - 2.0;
554
555 // normalization constant for kno-distribution.
556 // calculate first the sum of all constants, check for numerical problems.
557 G4double test, dum, anpn = 0.0;
558
559 for (nt=2; nt<=numSec; nt++) {
560 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
561 dum = pi*nt/(2.0*n*n);
562 if (std::fabs(dum) < 1.0) {
563 if( test >= 1.0e-10 )anpn += dum*test;
564 } else {
565 anpn += dum*test;
566 }
567 }
568
569 G4double ran = G4UniformRand();
570 G4double excs = 0.0;
571 if( targetCode == protonCode )
572 {
573 counter = -1;
574 for( npos=2; npos<numSec/3; npos++ )
575 {
576 nneg = npos-2;
577 for( nzero=0; nzero<numSec/3; nzero++ )
578 {
579 if( ++counter < numMulAn )
580 {
581 nt = npos+nneg+nzero;
582 if ( (nt>1) && (nt<=numSec) ) {
583 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
584 dum = (pi/anpn)*nt*protmulAn[counter]*protnormAn[nt-1]/(2.0*n*n);
585 if (std::fabs(dum) < 1.0) {
586 if( test >= 1.0e-10 )excs += dum*test;
587 } else {
588 excs += dum*test;
589 }
590
591 if (ran < excs) goto outOfLoopAn; //----------------------->
592 }
593 }
594 }
595 }
596 // 3 previous loops continued to the end
597 inElastic = false; // quasi-elastic scattering
598 return;
599 }
600 else
601 { // target must be a neutron
602 counter = -1;
603 for( npos=1; npos<numSec/3; npos++ )
604 {
605 nneg = npos-1;
606 for( nzero=0; nzero<numSec/3; nzero++ )
607 {
608 if (++counter < numMulAn) {
609 nt = npos+nneg+nzero;
610 if ( (nt>1) && (nt<=numSec) ) {
611 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
612 dum = (pi/anpn)*nt*neutmulAn[counter]*neutnormAn[nt-1]/(2.0*n*n);
613 if (std::fabs(dum) < 1.0) {
614 if( test >= 1.0e-10 )excs += dum*test;
615 } else {
616 excs += dum*test;
617 }
618
619 if (ran < excs) goto outOfLoopAn; // -------------------------->
620 }
621 }
622 }
623 }
624 inElastic = false; // quasi-elastic scattering.
625 return;
626 }
627 outOfLoopAn: // <------------------------------------------------------------------
628 vecLen = 0;
629 }
630 }
631
632 nt = npos + nneg + nzero;
633 while ( nt > 0)
634 {
635 G4double ran = G4UniformRand();
636 if ( ran < (G4double)npos/nt)
637 {
638 if( npos > 0 )
639 { pv[vecLen++] = PionPlus;
640 npos--;
641 }
642 }
643 else if ( ran < (G4double)(npos+nneg)/nt)
644 {
645 if( nneg > 0 )
646 {
647 pv[vecLen++] = PionMinus;
648 nneg--;
649 }
650 }
651 else
652 {
653 if( nzero > 0 )
654 {
655 pv[vecLen++] = PionZero;
656 nzero--;
657 }
658 }
659 nt = npos + nneg + nzero;
660 }
661 if (verboseLevel > 1)
662 {
663 G4cout << "Particles produced: " ;
664 G4cout << pv[0].getName() << " " ;
665 G4cout << pv[1].getName() << " " ;
666 for (i=2; i < vecLen; i++)
667 {
668 G4cout << pv[i].getName() << " " ;
669 }
670 G4cout << G4endl;
671 }
672 return;
673 }
674
675
676
677
678
679
680
681
682
683
stopAndKill
@ stopAndKill
Definition: G4HadFinalState.hh:42
neutronCode
@ neutronCode
Definition: G4SmartTrackStack.cc:105
G4double
double G4double
Definition: G4Types.hh:64
G4int
int G4int
Definition: G4Types.hh:66
G4bool
bool G4bool
Definition: G4Types.hh:67
G4endl
#define G4endl
Definition: G4ios.hh:52
G4cout
G4DLLIMPORT std::ostream G4cout
G4UniformRand
#define G4UniformRand()
Definition: Randomize.hh:53
G4HEAntiSigmaMinusInelastic::ModelDescription
virtual void ModelDescription(std::ostream &) const
Definition: G4HEAntiSigmaMinusInelastic.cc:43
G4HEAntiSigmaMinusInelastic::ApplyYourself
G4HadFinalState * ApplyYourself(const G4HadProjectile &aTrack, G4Nucleus &targetNucleus)
Definition: G4HEAntiSigmaMinusInelastic.cc:58
G4HEAntiSigmaMinusInelastic::FirstIntInCasAntiSigmaMinus
void FirstIntInCasAntiSigmaMinus(G4bool &inElastic, const G4double availableEnergy, G4HEVector pv[], G4int &vecLen, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, const G4double atomicWeight)
Definition: G4HEAntiSigmaMinusInelastic.cc:186
G4HEInelastic::PionPlus
G4HEVector PionPlus
Definition: G4HEInelastic.hh:215
G4HEInelastic::AntiSigmaZero
G4HEVector AntiSigmaZero
Definition: G4HEInelastic.hh:234
G4HEInelastic::pmltpc
G4double pmltpc(G4int np, G4int nm, G4int nz, G4int n, G4double b, G4double c)
Definition: G4HEInelastic.cc:233
G4HEInelastic::MediumEnergyClusterProduction
void MediumEnergyClusterProduction(G4bool &successful, G4HEVector pv[], G4int &vecLen, G4double &excitationEnergyGNP, G4double &excitationEnergyDTA, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:4036
G4HEInelastic::ElasticScattering
void ElasticScattering(G4bool &successful, G4HEVector pv[], G4int &vecLen, const G4HEVector &incidentParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:5183
G4HEInelastic::QuasiElasticScattering
void QuasiElasticScattering(G4bool &successful, G4HEVector pv[], G4int &vecLen, G4double &excitationEnergyGNP, G4double &excitationEnergyDTA, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:4892
G4HEInelastic::Neutron
G4HEVector Neutron
Definition: G4HEInelastic.hh:226
G4HEInelastic::FillParticleChange
void FillParticleChange(G4HEVector pv[], G4int aVecLength)
Definition: G4HEInelastic.cc:57
G4HEInelastic::PionMinus
G4HEVector PionMinus
Definition: G4HEInelastic.hh:217
G4HEInelastic::HighEnergyClusterProduction
void HighEnergyClusterProduction(G4bool &successful, G4HEVector pv[], G4int &vecLen, G4double &excitationEnergyGNP, G4double &excitationEnergyDTA, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:2097
G4HEInelastic::PionZero
G4HEVector PionZero
Definition: G4HEInelastic.hh:216
G4HEInelastic::NuclearExcitation
G4double NuclearExcitation(G4double incidentKineticEnergy, G4double atomicWeight, G4double atomicNumber, G4double &excitationEnergyCascade, G4double &excitationEnergyEvaporation)
Definition: G4HEInelastic.cc:179
G4HEInelastic::AntiSigmaMinus
G4HEVector AntiSigmaMinus
Definition: G4HEInelastic.hh:235
G4HEInelastic::AntiLambda
G4HEVector AntiLambda
Definition: G4HEInelastic.hh:229
G4HEInelastic::Proton
G4HEVector Proton
Definition: G4HEInelastic.hh:224
G4HEInelastic::MediumEnergyCascading
void MediumEnergyCascading(G4bool &successful, G4HEVector pv[], G4int &vecLen, G4double &excitationEnergyGNP, G4double &excitationEnergyDTA, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:2970
G4HEInelastic::NuclearInelasticity
G4double NuclearInelasticity(G4double incidentKineticEnergy, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:149
G4HEInelastic::StrangeParticlePairProduction
void StrangeParticlePairProduction(const G4double availableEnergy, const G4double centerOfMassEnergy, G4HEVector pv[], G4int &vecLen, const G4HEVector &incidentParticle, const G4HEVector &targetParticle)
Definition: G4HEInelastic.cc:329
G4HEInelastic::HighEnergyCascading
void HighEnergyCascading(G4bool &successful, G4HEVector pv[], G4int &vecLen, G4double &excitationEnergyGNP, G4double &excitationEnergyDTA, const G4HEVector &incidentParticle, const G4HEVector &targetParticle, G4double atomicWeight, G4double atomicNumber)
Definition: G4HEInelastic.cc:598
G4HEVector::getEnergy
G4double getEnergy() const
Definition: G4HEVector.cc:313
G4HEVector::getMass
G4double getMass() const
Definition: G4HEVector.cc:361
G4HEVector::getCode
G4int getCode() const
Definition: G4HEVector.cc:426
G4HEVector::getTotalMomentum
G4double getTotalMomentum() const
Definition: G4HEVector.cc:166
G4HEVector::getName
G4String getName() const
Definition: G4HEVector.cc:431
G4HEVector::setDefinition
void setDefinition(G4String name)
Definition: G4HEVector.cc:812
G4HadFinalState::SetStatusChange
void SetStatusChange(G4HadFinalStateStatus aS)
Definition: G4HadFinalState.cc:81
G4Nucleus::GetA_asInt
G4int GetA_asInt() const
Definition: G4Nucleus.hh:109
G4Nucleus::GetZ_asInt
G4int GetZ_asInt() const
Definition: G4Nucleus.hh:115