source: trunk/source/processes/hadronic/models/high_energy/src/G4HEOmegaMinusInelastic.cc@ 1350

Last change on this file since 1350 was 1347, checked in by garnier, 15 years ago

geant4 tag 9.4
File size: 18.7 KB
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25//
26// $Id: G4HEOmegaMinusInelastic.cc,v 1.17 2010/11/29 05:44:44 dennis Exp $
27// GEANT4 tag $Name: geant4-09-04-ref-00 $
28//
29
30#include "globals.hh"
31#include "G4ios.hh"
32
33// G4 Process: Gheisha High Energy Collision model.
34// This includes the high energy cascading model, the two-body-resonance model
35// and the low energy two-body model. Not included are the low energy stuff
36// like nuclear reactions, nuclear fission without any cascading and all
37// processes for particles at rest.
38// First work done by J.L.Chuma and F.W.Jones, TRIUMF, June 96.
39// H. Fesefeldt, RWTH-Aachen, 23-October-1996
40// Last modified: 29-July-1998
41
42#include "G4HEOmegaMinusInelastic.hh"
43
44G4HadFinalState*
45G4HEOmegaMinusInelastic::ApplyYourself(const G4HadProjectile& aTrack,
46 G4Nucleus& targetNucleus)
47{
48 G4HEVector* pv = new G4HEVector[MAXPART];
49 const G4HadProjectile* aParticle = &aTrack;
50 const G4double A = targetNucleus.GetN();
51 const G4double Z = targetNucleus.GetZ();
52 G4HEVector incidentParticle(aParticle);
53
54 G4double atomicNumber = Z;
55 G4double atomicWeight = A;
56
57 G4int incidentCode = incidentParticle.getCode();
58 G4double incidentMass = incidentParticle.getMass();
59 G4double incidentTotalEnergy = incidentParticle.getEnergy();
60 G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
61 G4double incidentKineticEnergy = incidentTotalEnergy - incidentMass;
62
63 if (incidentKineticEnergy < 1.)
64 G4cout << "GHEOmegaMinusInelastic: incident energy < 1 GeV" << G4endl;
65
66 if (verboseLevel > 1) {
67 G4cout << "G4HEOmegaMinusInelastic::ApplyYourself" << G4endl;
68 G4cout << "incident particle " << incidentParticle.getName()
69 << "mass " << incidentMass
70 << "kinetic energy " << incidentKineticEnergy
71 << G4endl;
72 G4cout << "target material with (A,Z) = ("
73 << atomicWeight << "," << atomicNumber << ")" << G4endl;
74 }
75
76 G4double inelasticity = NuclearInelasticity(incidentKineticEnergy,
77 atomicWeight, atomicNumber);
78 if (verboseLevel > 1)
79 G4cout << "nuclear inelasticity = " << inelasticity << G4endl;
80
81 incidentKineticEnergy -= inelasticity;
82
83 G4double excitationEnergyGNP = 0.;
84 G4double excitationEnergyDTA = 0.;
85
86 G4double excitation = NuclearExcitation(incidentKineticEnergy,
87 atomicWeight, atomicNumber,
88 excitationEnergyGNP,
89 excitationEnergyDTA);
90 if (verboseLevel > 1)
91 G4cout << "nuclear excitation = " << excitation << excitationEnergyGNP
92 << excitationEnergyDTA << G4endl;
93
94 incidentKineticEnergy -= excitation;
95 incidentTotalEnergy = incidentKineticEnergy + incidentMass;
96 incidentTotalMomentum = std::sqrt( (incidentTotalEnergy-incidentMass)
97 *(incidentTotalEnergy+incidentMass));
98
99 G4HEVector targetParticle;
100 if (G4UniformRand() < atomicNumber/atomicWeight) {
101 targetParticle.setDefinition("Proton");
102 } else {
103 targetParticle.setDefinition("Neutron");
104 }
105
106 G4double targetMass = targetParticle.getMass();
107 G4double centerOfMassEnergy = std::sqrt(incidentMass*incidentMass
108 + targetMass*targetMass
109 + 2.0*targetMass*incidentTotalEnergy);
110 G4double availableEnergy = centerOfMassEnergy - targetMass - incidentMass;
111
112 G4bool inElastic = true;
113 vecLength = 0;
114
115 if (verboseLevel > 1)
116 G4cout << "ApplyYourself: CallFirstIntInCascade for particle "
117 << incidentCode << G4endl;
118
119 G4bool successful = false;
120
121 FirstIntInCasOmegaMinus(inElastic, availableEnergy, pv, vecLength,
122 incidentParticle, targetParticle, atomicWeight);
123
124 if (verboseLevel > 1)
125 G4cout << "ApplyYourself::StrangeParticlePairProduction" << G4endl;
126
127 if ((vecLength > 0) && (availableEnergy > 1.))
128 StrangeParticlePairProduction(availableEnergy, centerOfMassEnergy,
129 pv, vecLength,
130 incidentParticle, targetParticle);
131
132 HighEnergyCascading(successful, pv, vecLength,
133 excitationEnergyGNP, excitationEnergyDTA,
134 incidentParticle, targetParticle,
135 atomicWeight, atomicNumber);
136 if (!successful)
137 HighEnergyClusterProduction(successful, pv, vecLength,
138 excitationEnergyGNP, excitationEnergyDTA,
139 incidentParticle, targetParticle,
140 atomicWeight, atomicNumber);
141 if (!successful)
142 MediumEnergyCascading(successful, pv, vecLength,
143 excitationEnergyGNP, excitationEnergyDTA,
144 incidentParticle, targetParticle,
145 atomicWeight, atomicNumber);
146
147 if (!successful)
148 MediumEnergyClusterProduction(successful, pv, vecLength,
149 excitationEnergyGNP, excitationEnergyDTA,
150 incidentParticle, targetParticle,
151 atomicWeight, atomicNumber);
152 if (!successful)
153 QuasiElasticScattering(successful, pv, vecLength,
154 excitationEnergyGNP, excitationEnergyDTA,
155 incidentParticle, targetParticle,
156 atomicWeight, atomicNumber);
157 if (!successful)
158 ElasticScattering(successful, pv, vecLength,
159 incidentParticle,
160 atomicWeight, atomicNumber);
161
162 if (!successful)
163 G4cout << "GHEInelasticInteraction::ApplyYourself fails to produce final state particles"
164 << G4endl;
165
166 FillParticleChange(pv, vecLength);
167 delete [] pv;
168 theParticleChange.SetStatusChange(stopAndKill);
169 return &theParticleChange;
170}
171
172
173void
174G4HEOmegaMinusInelastic::FirstIntInCasOmegaMinus(G4bool& inElastic,
175 const G4double availableEnergy,
176 G4HEVector pv[],
177 G4int& vecLen,
178 const G4HEVector& incidentParticle,
179 const G4HEVector& targetParticle,
180 const G4double atomicWeight)
181
182// Xi0 undergoes interaction with nucleon within a nucleus. Check if it is
183// energetically possible to produce pions/kaons. In not, assume nuclear excitation
184// occurs and input particle is degraded in energy. No other particles are produced.
185// If reaction is possible, find the correct number of pions/protons/neutrons
186// produced using an interpolation to multiplicity data. Replace some pions or
187// protons/neutrons by kaons or strange baryons according to the average
188// multiplicity per inelastic reaction.
189{
190 static const G4double expxu = std::log(MAXFLOAT); // upper bound for arg. of exp
191 static const G4double expxl = -expxu; // lower bound for arg. of exp
192
193 static const G4double protb = 0.7;
194 static const G4double neutb = 0.7;
195 static const G4double c = 1.25;
196
197 static const G4int numMul = 1200;
198 static const G4int numSec = 60;
199
200 G4int protonCode = Proton.getCode();
201
202 G4int targetCode = targetParticle.getCode();
203 G4double incidentTotalMomentum = incidentParticle.getTotalMomentum();
204
205 static G4bool first = true;
206 static G4double protmul[numMul], protnorm[numSec]; // proton constants
207 static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
208
209 // misc. local variables
210 // np = number of pi+, nm = number of pi-, nz = number of pi0
211
212 G4int i, counter, nt, np, nm, nz;
213
214 if( first )
215 { // compute normalization constants, this will only be done once
216 first = false;
217 for( i=0; i<numMul; i++ )protmul[i] = 0.0;
218 for( i=0; i<numSec; i++ )protnorm[i] = 0.0;
219 counter = -1;
220 for( np=0; np<(numSec/3); np++ )
221 {
222 for( nm=std::max(0,np-1); nm<=np; nm++ )
223 {
224 for( nz=0; nz<numSec/3; nz++ )
225 {
226 if( ++counter < numMul )
227 {
228 nt = np+nm+nz;
229 if( (nt>0) && (nt<=numSec) )
230 {
231 protmul[counter] = pmltpc(np,nm,nz,nt,protb,c);
232 protnorm[nt-1] += protmul[counter];
233 }
234 }
235 }
236 }
237 }
238 for( i=0; i<numMul; i++ )neutmul[i] = 0.0;
239 for( i=0; i<numSec; i++ )neutnorm[i] = 0.0;
240 counter = -1;
241 for( np=0; np<numSec/3; np++ )
242 {
243 for( nm=np; nm<=(np+1); nm++ )
244 {
245 for( nz=0; nz<numSec/3; nz++ )
246 {
247 if( ++counter < numMul )
248 {
249 nt = np+nm+nz;
250 if( (nt>0) && (nt<=numSec) )
251 {
252 neutmul[counter] = pmltpc(np,nm,nz,nt,neutb,c);
253 neutnorm[nt-1] += neutmul[counter];
254 }
255 }
256 }
257 }
258 }
259 for( i=0; i<numSec; i++ )
260 {
261 if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
262 if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
263 }
264 } // end of initialization
265
266
267 // initialize the first two places
268 // the same as beam and target
269 pv[0] = incidentParticle;
270 pv[1] = targetParticle;
271 vecLen = 2;
272
273 if( !inElastic )
274 { // quasi-elastic scattering, no pions produced
275 G4double cech[] = {0.50, 0.45, 0.40, 0.35, 0.30, 0.25, 0.06, 0.04, 0.005, 0.};
276 G4int iplab = G4int( std::min( 9.0, incidentTotalMomentum*2.5 ) );
277 if( G4UniformRand() < cech[iplab]/std::pow(atomicWeight,0.42) )
278 {
279 G4double ran = G4UniformRand();
280 if( targetCode == protonCode)
281 {
282 if (ran < 0.2)
283 {
284 pv[0] = XiZero;
285 pv[1] = SigmaZero;
286 }
287 else if (ran < 0.4)
288 {
289 pv[0] = SigmaZero;
290 pv[1] = XiZero;
291 }
292 else if (ran < 0.6)
293 {
294 pv[0] = XiZero;
295 pv[1] = Lambda;
296 }
297 else if (ran < 0.8)
298 {
299 pv[0] = Lambda;
300 pv[1] = XiZero;
301 }
302 else
303 {
304 pv[0] = Proton;
305 pv[1] = OmegaMinus;
306 }
307 }
308 else
309 {
310 if (ran < 0.2)
311 {
312 pv[0] = Neutron;
313 pv[1] = OmegaMinus;
314 }
315 else if (ran < 0.4)
316 {
317 pv[0] = XiZero;
318 pv[1] = SigmaMinus;
319 }
320 else if (ran < 0.6)
321 {
322 pv[0] = SigmaMinus;
323 pv[1] = XiZero;
324 }
325 else if (ran < 0.8)
326 {
327 pv[0] = XiMinus;
328 pv[1] = Lambda;
329 }
330 else
331 {
332 pv[0] = Lambda;
333 pv[1] = XiMinus;
334 }
335 }
336 }
337 return;
338 }
339 else if (availableEnergy <= PionPlus.getMass())
340 return;
341
342 // inelastic scattering
343
344 np = 0; nm = 0; nz = 0;
345
346// number of total particles vs. centre of mass Energy - 2*proton mass
347
348 G4double aleab = std::log(availableEnergy);
349 G4double n = 3.62567+aleab*(0.665843+aleab*(0.336514
350 + aleab*(0.117712+0.0136912*aleab))) - 2.0;
351
352// normalization constant for kno-distribution.
353// calculate first the sum of all constants, check for numerical problems.
354 G4double test, dum, anpn = 0.0;
355
356 for (nt=1; nt<=numSec; nt++) {
357 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
358 dum = pi*nt/(2.0*n*n);
359 if (std::fabs(dum) < 1.0) {
360 if( test >= 1.0e-10 )anpn += dum*test;
361 } else {
362 anpn += dum*test;
363 }
364 }
365
366 G4double ran = G4UniformRand();
367 G4double excs = 0.0;
368 if( targetCode == protonCode )
369 {
370 counter = -1;
371 for( np=0; np<numSec/3; np++ )
372 {
373 for( nm=std::max(0,np-1); nm<=np; nm++ )
374 {
375 for( nz=0; nz<numSec/3; nz++ )
376 {
377 if( ++counter < numMul )
378 {
379 nt = np+nm+nz;
380 if ( (nt>0) && (nt<=numSec) ) {
381 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
382 dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
383 if (std::fabs(dum) < 1.0) {
384 if( test >= 1.0e-10 )excs += dum*test;
385 } else {
386 excs += dum*test;
387 }
388 if (ran < excs) goto outOfLoop; //----------------------->
389 }
390 }
391 }
392 }
393 }
394
395 // 3 previous loops continued to the end
396 inElastic = false; // quasi-elastic scattering
397 return;
398 }
399 else
400 { // target must be a neutron
401 counter = -1;
402 for( np=0; np<numSec/3; np++ )
403 {
404 for( nm=np; nm<=(np+1); nm++ )
405 {
406 for( nz=0; nz<numSec/3; nz++ )
407 {
408 if( ++counter < numMul )
409 {
410 nt = np+nm+nz;
411 if ( (nt>=1) && (nt<=numSec) ) {
412 test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
413 dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
414 if (std::fabs(dum) < 1.0) {
415 if( test >= 1.0e-10 )excs += dum*test;
416 } else {
417 excs += dum*test;
418 }
419 if (ran < excs) goto outOfLoop; // -------------------------->
420 }
421 }
422 }
423 }
424 }
425 // 3 previous loops continued to the end
426 inElastic = false; // quasi-elastic scattering.
427 return;
428 }
429
430 outOfLoop: // <------------------------------------------------------------------------
431
432 // in the following we do not consider
433 ran = G4UniformRand(); // strangeness transfer in high multiplicity
434 if( targetCode == protonCode) // events. YK combinations are added in
435 { // StrangeParticlePairProduction
436 if( np == nm)
437 {
438 }
439 else
440 {
441 pv[1] = Neutron;
442 }
443 }
444 else
445 {
446 if (np == nm)
447 {
448 }
449 else
450 {
451 pv[1] = Proton;
452 }
453 }
454
455
456 nt = np + nm + nz;
457 while ( nt > 0)
458 {
459 G4double ran = G4UniformRand();
460 if ( ran < (G4double)np/nt)
461 {
462 if( np > 0 )
463 { pv[vecLen++] = PionPlus;
464 np--;
465 }
466 }
467 else if ( ran < (G4double)(np+nm)/nt)
468 {
469 if( nm > 0 )
470 {
471 pv[vecLen++] = PionMinus;
472 nm--;
473 }
474 }
475 else
476 {
477 if( nz > 0 )
478 {
479 pv[vecLen++] = PionZero;
480 nz--;
481 }
482 }
483 nt = np + nm + nz;
484 }
485 if (verboseLevel > 1)
486 {
487 G4cout << "Particles produced: " ;
488 G4cout << pv[0].getName() << " " ;
489 G4cout << pv[1].getName() << " " ;
490 for (i=2; i < vecLen; i++)
491 {
492 G4cout << pv[i].getName() << " " ;
493 }
494 G4cout << G4endl;
495 }
496 return;
497 }
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