8d2cd130 |
1 | /************************************************************************** |
2 | * Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. * |
3 | * * |
4 | * Author: The ALICE Off-line Project. * |
5 | * Contributors are mentioned in the code where appropriate. * |
6 | * * |
7 | * Permission to use, copy, modify and distribute this software and its * |
8 | * documentation strictly for non-commercial purposes is hereby granted * |
9 | * without fee, provided that the above copyright notice appears in all * |
10 | * copies and that both the copyright notice and this permission notice * |
11 | * appear in the supporting documentation. The authors make no claims * |
12 | * about the suitability of this software for any purpose. It is * |
13 | * provided "as is" without express or implied warranty. * |
14 | **************************************************************************/ |
15 | |
7cdba479 |
16 | /* $Id$ */ |
8d2cd130 |
17 | |
18 | #include "AliPythia.h" |
7cdba479 |
19 | #include "AliPythiaRndm.h" |
0f482ae4 |
20 | #include "../FASTSIM/AliFastGlauber.h" |
21 | #include "../FASTSIM/AliQuenchingWeights.h" |
22 | #include "TVector3.h" |
8d2cd130 |
23 | |
24 | ClassImp(AliPythia) |
25 | |
26 | #ifndef WIN32 |
27 | # define pyclus pyclus_ |
28 | # define pycell pycell_ |
452af8c7 |
29 | # define pyshow pyshow_ |
30 | # define pyrobo pyrobo_ |
8d2cd130 |
31 | # define type_of_call |
32 | #else |
33 | # define pyclus PYCLUS |
34 | # define pycell PYCELL |
452af8c7 |
35 | # define pyrobo PYROBO |
8d2cd130 |
36 | # define type_of_call _stdcall |
37 | #endif |
38 | |
39 | extern "C" void type_of_call pyclus(Int_t & ); |
40 | extern "C" void type_of_call pycell(Int_t & ); |
452af8c7 |
41 | extern "C" void type_of_call pyshow(Int_t &, Int_t &, Double_t &); |
42 | extern "C" void type_of_call pyrobo(Int_t &, Int_t &, Double_t &, Double_t &, Double_t &, Double_t &, Double_t &); |
8d2cd130 |
43 | |
44 | //_____________________________________________________________________________ |
45 | |
46 | AliPythia* AliPythia::fgAliPythia=NULL; |
47 | |
48 | AliPythia::AliPythia() |
49 | { |
50 | // Default Constructor |
51 | // |
52 | // Set random number |
7cdba479 |
53 | if (!AliPythiaRndm::GetPythiaRandom()) |
54 | AliPythiaRndm::SetPythiaRandom(GetRandom()); |
0f482ae4 |
55 | fGlauber = 0; |
56 | fQuenchingWeights = 0; |
8d2cd130 |
57 | } |
58 | |
59 | void AliPythia::ProcInit(Process_t process, Float_t energy, StrucFunc_t strucfunc) |
60 | { |
61 | // Initialise the process to generate |
7cdba479 |
62 | if (!AliPythiaRndm::GetPythiaRandom()) |
63 | AliPythiaRndm::SetPythiaRandom(GetRandom()); |
8d2cd130 |
64 | |
65 | fProcess = process; |
66 | fEcms = energy; |
67 | fStrucFunc = strucfunc; |
68 | // don't decay p0 |
69 | SetMDCY(Pycomp(111),1,0); |
70 | // select structure function |
71 | SetMSTP(52,2); |
72 | SetMSTP(51,strucfunc); |
73 | // |
74 | // Pythia initialisation for selected processes// |
75 | // |
76 | // Make MSEL clean |
77 | // |
78 | for (Int_t i=1; i<= 200; i++) { |
79 | SetMSUB(i,0); |
80 | } |
81 | // select charm production |
82 | switch (process) |
83 | { |
84 | case kPyCharm: |
85 | SetMSEL(4); |
86 | // |
87 | // heavy quark masses |
88 | |
89 | SetPMAS(4,1,1.2); |
90 | SetMSTU(16,2); |
91 | // |
92 | // primordial pT |
93 | SetMSTP(91,1); |
94 | SetPARP(91,1.); |
95 | SetPARP(93,5.); |
96 | // |
97 | break; |
98 | case kPyBeauty: |
99 | SetMSEL(5); |
100 | SetPMAS(5,1,4.75); |
101 | SetMSTU(16,2); |
102 | break; |
103 | case kPyJpsi: |
104 | SetMSEL(0); |
105 | // gg->J/Psi g |
106 | SetMSUB(86,1); |
107 | break; |
108 | case kPyJpsiChi: |
109 | SetMSEL(0); |
110 | // gg->J/Psi g |
111 | SetMSUB(86,1); |
112 | // gg-> chi_0c g |
113 | SetMSUB(87,1); |
114 | // gg-> chi_1c g |
115 | SetMSUB(88,1); |
116 | // gg-> chi_2c g |
117 | SetMSUB(89,1); |
118 | break; |
119 | case kPyCharmUnforced: |
120 | SetMSEL(0); |
121 | // gq->qg |
122 | SetMSUB(28,1); |
123 | // gg->qq |
124 | SetMSUB(53,1); |
125 | // gg->gg |
126 | SetMSUB(68,1); |
127 | break; |
128 | case kPyBeautyUnforced: |
129 | SetMSEL(0); |
130 | // gq->qg |
131 | SetMSUB(28,1); |
132 | // gg->qq |
133 | SetMSUB(53,1); |
134 | // gg->gg |
135 | SetMSUB(68,1); |
136 | break; |
137 | case kPyMb: |
138 | // Minimum Bias pp-Collisions |
139 | // |
140 | // |
141 | // select Pythia min. bias model |
142 | SetMSEL(0); |
511db649 |
143 | SetMSUB(92,1); // single diffraction AB-->XB |
144 | SetMSUB(93,1); // single diffraction AB-->AX |
145 | SetMSUB(94,1); // double diffraction |
146 | SetMSUB(95,1); // low pt production |
147 | |
148 | // |
149 | // ATLAS Tuning |
150 | // |
c01c4118 |
151 | |
152 | SetMSTP(51, kCTEQ5L); // CTEQ5L pdf |
511db649 |
153 | SetMSTP(81,1); // Multiple Interactions ON |
154 | SetMSTP(82,4); // Double Gaussian Model |
155 | |
156 | SetPARP(82,1.8); // [GeV] PT_min at Ref. energy |
157 | SetPARP(89,1000.); // [GeV] Ref. energy |
158 | SetPARP(90,0.16); // 2*epsilon (exponent in power law) |
159 | SetPARP(83,0.5); // Core density in proton matter distribution (def.value) |
160 | SetPARP(84,0.5); // Core radius |
161 | SetPARP(85,0.33); // Regulates gluon prod. mechanism |
162 | SetPARP(86,0.66); // Regulates gluon prod. mechanism |
163 | SetPARP(67,1); // Regulates Initial State Radiation |
164 | break; |
8d2cd130 |
165 | case kPyMbNonDiffr: |
166 | // Minimum Bias pp-Collisions |
167 | // |
168 | // |
169 | // select Pythia min. bias model |
170 | SetMSEL(0); |
511db649 |
171 | SetMSUB(95,1); // low pt production |
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172 | |
173 | // |
174 | // ATLAS Tuning |
175 | // |
511db649 |
176 | |
0f482ae4 |
177 | SetMSTP(51,7); // CTEQ5L pdf |
511db649 |
178 | SetMSTP(81,1); // Multiple Interactions ON |
179 | SetMSTP(82,4); // Double Gaussian Model |
180 | |
181 | SetPARP(82,1.8); // [GeV] PT_min at Ref. energy |
182 | SetPARP(89,1000.); // [GeV] Ref. energy |
183 | SetPARP(90,0.16); // 2*epsilon (exponent in power law) |
184 | SetPARP(83,0.5); // Core density in proton matter distribution (def.value) |
185 | SetPARP(84,0.5); // Core radius |
186 | SetPARP(85,0.33); // Regulates gluon prod. mechanism |
187 | SetPARP(86,0.66); // Regulates gluon prod. mechanism |
188 | SetPARP(67,1); // Regulates Initial State Radiation |
8d2cd130 |
189 | break; |
190 | case kPyJets: |
191 | // |
192 | // QCD Jets |
193 | // |
194 | SetMSEL(1); |
195 | break; |
196 | case kPyDirectGamma: |
197 | SetMSEL(10); |
198 | break; |
adf4d898 |
199 | case kPyCharmPbPbMNR: |
200 | case kPyD0PbPbMNR: |
8d2cd130 |
201 | // Tuning of Pythia parameters aimed to get a resonable agreement |
202 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
203 | // c-cbar single inclusive and double differential distributions. |
204 | // This parameter settings are meant to work with Pb-Pb collisions |
adf4d898 |
205 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
8d2cd130 |
206 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
207 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
208 | |
209 | // All QCD processes |
210 | SetMSEL(1); |
211 | |
212 | // No multiple interactions |
213 | SetMSTP(81,0); |
214 | SetPARP(81,0.0); |
215 | SetPARP(82,0.0); |
216 | |
217 | // Initial/final parton shower on (Pythia default) |
218 | SetMSTP(61,1); |
219 | SetMSTP(71,1); |
220 | |
221 | // 2nd order alpha_s |
222 | SetMSTP(2,2); |
223 | |
224 | // QCD scales |
225 | SetMSTP(32,2); |
226 | SetPARP(34,1.0); |
227 | |
adf4d898 |
228 | // Intrinsic <kT> |
8d2cd130 |
229 | SetMSTP(91,1); |
230 | SetPARP(91,1.304); |
231 | SetPARP(93,6.52); |
232 | |
233 | // Set c-quark mass |
234 | SetPMAS(4,1,1.2); |
235 | |
90d7b703 |
236 | break; |
237 | case kPyDPlusPbPbMNR: |
238 | // Tuning of Pythia parameters aimed to get a resonable agreement |
239 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
240 | // c-cbar single inclusive and double differential distributions. |
241 | // This parameter settings are meant to work with Pb-Pb collisions |
242 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
243 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
244 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
245 | |
246 | // All QCD processes |
247 | SetMSEL(1); |
248 | |
249 | // No multiple interactions |
250 | SetMSTP(81,0); |
251 | SetPARP(81,0.0); |
252 | SetPARP(82,0.0); |
253 | |
254 | // Initial/final parton shower on (Pythia default) |
255 | SetMSTP(61,1); |
256 | SetMSTP(71,1); |
257 | |
258 | // 2nd order alpha_s |
259 | SetMSTP(2,2); |
260 | |
261 | // QCD scales |
262 | SetMSTP(32,2); |
263 | SetPARP(34,1.0); |
264 | |
265 | // Intrinsic <kT> |
266 | SetMSTP(91,1); |
267 | SetPARP(91,1.304); |
268 | SetPARP(93,6.52); |
269 | |
270 | // Set c-quark mass |
271 | SetPMAS(4,1,1.2); |
272 | |
8d2cd130 |
273 | break; |
adf4d898 |
274 | case kPyCharmpPbMNR: |
275 | case kPyD0pPbMNR: |
276 | // Tuning of Pythia parameters aimed to get a resonable agreement |
277 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
278 | // c-cbar single inclusive and double differential distributions. |
279 | // This parameter settings are meant to work with p-Pb collisions |
280 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
281 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
282 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
283 | |
284 | // All QCD processes |
285 | SetMSEL(1); |
286 | |
287 | // No multiple interactions |
288 | SetMSTP(81,0); |
289 | SetPARP(81,0.0); |
290 | SetPARP(82,0.0); |
291 | |
292 | // Initial/final parton shower on (Pythia default) |
293 | SetMSTP(61,1); |
294 | SetMSTP(71,1); |
295 | |
296 | // 2nd order alpha_s |
297 | SetMSTP(2,2); |
298 | |
299 | // QCD scales |
300 | SetMSTP(32,2); |
301 | SetPARP(34,1.0); |
302 | |
303 | // Intrinsic <kT> |
304 | SetMSTP(91,1); |
305 | SetPARP(91,1.16); |
306 | SetPARP(93,5.8); |
307 | |
308 | // Set c-quark mass |
309 | SetPMAS(4,1,1.2); |
310 | |
90d7b703 |
311 | break; |
312 | case kPyDPluspPbMNR: |
313 | // Tuning of Pythia parameters aimed to get a resonable agreement |
314 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
315 | // c-cbar single inclusive and double differential distributions. |
316 | // This parameter settings are meant to work with p-Pb collisions |
317 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
318 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
319 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
320 | |
321 | // All QCD processes |
322 | SetMSEL(1); |
323 | |
324 | // No multiple interactions |
325 | SetMSTP(81,0); |
326 | SetPARP(81,0.0); |
327 | SetPARP(82,0.0); |
328 | |
329 | // Initial/final parton shower on (Pythia default) |
330 | SetMSTP(61,1); |
331 | SetMSTP(71,1); |
332 | |
333 | // 2nd order alpha_s |
334 | SetMSTP(2,2); |
335 | |
336 | // QCD scales |
337 | SetMSTP(32,2); |
338 | SetPARP(34,1.0); |
339 | |
340 | // Intrinsic <kT> |
341 | SetMSTP(91,1); |
342 | SetPARP(91,1.16); |
343 | SetPARP(93,5.8); |
344 | |
345 | // Set c-quark mass |
346 | SetPMAS(4,1,1.2); |
347 | |
adf4d898 |
348 | break; |
349 | case kPyCharmppMNR: |
350 | case kPyD0ppMNR: |
351 | // Tuning of Pythia parameters aimed to get a resonable agreement |
352 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
353 | // c-cbar single inclusive and double differential distributions. |
354 | // This parameter settings are meant to work with pp collisions |
355 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
356 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
357 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
358 | |
359 | // All QCD processes |
360 | SetMSEL(1); |
361 | |
362 | // No multiple interactions |
363 | SetMSTP(81,0); |
364 | SetPARP(81,0.0); |
365 | SetPARP(82,0.0); |
366 | |
367 | // Initial/final parton shower on (Pythia default) |
368 | SetMSTP(61,1); |
369 | SetMSTP(71,1); |
370 | |
371 | // 2nd order alpha_s |
372 | SetMSTP(2,2); |
373 | |
374 | // QCD scales |
375 | SetMSTP(32,2); |
376 | SetPARP(34,1.0); |
377 | |
378 | // Intrinsic <kT^2> |
379 | SetMSTP(91,1); |
380 | SetPARP(91,1.); |
381 | SetPARP(93,5.); |
382 | |
383 | // Set c-quark mass |
384 | SetPMAS(4,1,1.2); |
385 | |
90d7b703 |
386 | break; |
387 | case kPyDPlusppMNR: |
388 | // Tuning of Pythia parameters aimed to get a resonable agreement |
389 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
390 | // c-cbar single inclusive and double differential distributions. |
391 | // This parameter settings are meant to work with pp collisions |
392 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
393 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
394 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. |
395 | |
396 | // All QCD processes |
397 | SetMSEL(1); |
398 | |
399 | // No multiple interactions |
400 | SetMSTP(81,0); |
401 | SetPARP(81,0.0); |
402 | SetPARP(82,0.0); |
403 | |
404 | // Initial/final parton shower on (Pythia default) |
405 | SetMSTP(61,1); |
406 | SetMSTP(71,1); |
407 | |
408 | // 2nd order alpha_s |
409 | SetMSTP(2,2); |
410 | |
411 | // QCD scales |
412 | SetMSTP(32,2); |
413 | SetPARP(34,1.0); |
414 | |
415 | // Intrinsic <kT^2> |
416 | SetMSTP(91,1); |
417 | SetPARP(91,1.); |
418 | SetPARP(93,5.); |
419 | |
420 | // Set c-quark mass |
421 | SetPMAS(4,1,1.2); |
422 | |
adf4d898 |
423 | break; |
424 | case kPyBeautyPbPbMNR: |
8d2cd130 |
425 | // Tuning of Pythia parameters aimed to get a resonable agreement |
426 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
427 | // b-bbar single inclusive and double differential distributions. |
428 | // This parameter settings are meant to work with Pb-Pb collisions |
429 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
430 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
431 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. |
432 | |
433 | // All QCD processes |
434 | SetMSEL(1); |
435 | |
436 | // No multiple interactions |
437 | SetMSTP(81,0); |
438 | SetPARP(81,0.0); |
439 | SetPARP(82,0.0); |
440 | |
441 | // Initial/final parton shower on (Pythia default) |
442 | SetMSTP(61,1); |
443 | SetMSTP(71,1); |
444 | |
445 | // 2nd order alpha_s |
446 | SetMSTP(2,2); |
447 | |
448 | // QCD scales |
449 | SetMSTP(32,2); |
450 | SetPARP(34,1.0); |
451 | SetPARP(67,1.0); |
452 | SetPARP(71,1.0); |
453 | |
adf4d898 |
454 | // Intrinsic <kT> |
8d2cd130 |
455 | SetMSTP(91,1); |
456 | SetPARP(91,2.035); |
457 | SetPARP(93,10.17); |
458 | |
459 | // Set b-quark mass |
460 | SetPMAS(5,1,4.75); |
461 | |
adf4d898 |
462 | break; |
463 | case kPyBeautypPbMNR: |
464 | // Tuning of Pythia parameters aimed to get a resonable agreement |
465 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
466 | // b-bbar single inclusive and double differential distributions. |
467 | // This parameter settings are meant to work with p-Pb collisions |
468 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
469 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
470 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. |
471 | |
472 | // All QCD processes |
473 | SetMSEL(1); |
474 | |
475 | // No multiple interactions |
476 | SetMSTP(81,0); |
477 | SetPARP(81,0.0); |
478 | SetPARP(82,0.0); |
479 | |
480 | // Initial/final parton shower on (Pythia default) |
481 | SetMSTP(61,1); |
482 | SetMSTP(71,1); |
483 | |
484 | // 2nd order alpha_s |
485 | SetMSTP(2,2); |
486 | |
487 | // QCD scales |
488 | SetMSTP(32,2); |
489 | SetPARP(34,1.0); |
490 | SetPARP(67,1.0); |
491 | SetPARP(71,1.0); |
492 | |
493 | // Intrinsic <kT> |
494 | SetMSTP(91,1); |
495 | SetPARP(91,1.60); |
496 | SetPARP(93,8.00); |
497 | |
498 | // Set b-quark mass |
499 | SetPMAS(5,1,4.75); |
500 | |
501 | break; |
502 | case kPyBeautyppMNR: |
503 | // Tuning of Pythia parameters aimed to get a resonable agreement |
504 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the |
505 | // b-bbar single inclusive and double differential distributions. |
506 | // This parameter settings are meant to work with pp collisions |
507 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. |
508 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) |
509 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. |
510 | |
511 | // All QCD processes |
512 | SetMSEL(1); |
513 | |
514 | // No multiple interactions |
515 | SetMSTP(81,0); |
516 | SetPARP(81,0.0); |
517 | SetPARP(82,0.0); |
518 | |
519 | // Initial/final parton shower on (Pythia default) |
520 | SetMSTP(61,1); |
521 | SetMSTP(71,1); |
522 | |
523 | // 2nd order alpha_s |
524 | SetMSTP(2,2); |
525 | |
526 | // QCD scales |
527 | SetMSTP(32,2); |
528 | SetPARP(34,1.0); |
529 | SetPARP(67,1.0); |
530 | SetPARP(71,1.0); |
531 | |
532 | // Intrinsic <kT> |
533 | SetMSTP(91,1); |
534 | SetPARP(91,1.); |
535 | SetPARP(93,5.); |
536 | |
537 | // Set b-quark mass |
538 | SetPMAS(5,1,4.75); |
539 | |
8d2cd130 |
540 | break; |
541 | } |
542 | // |
543 | // Initialize PYTHIA |
544 | SetMSTP(41,1); // all resonance decays switched on |
545 | |
546 | Initialize("CMS","p","p",fEcms); |
547 | |
548 | } |
549 | |
550 | Int_t AliPythia::CheckedLuComp(Int_t kf) |
551 | { |
552 | // Check Lund particle code (for debugging) |
553 | Int_t kc=Pycomp(kf); |
554 | printf("\n Lucomp kf,kc %d %d",kf,kc); |
555 | return kc; |
556 | } |
557 | |
558 | void AliPythia::SetNuclei(Int_t a1, Int_t a2) |
559 | { |
560 | // Treat protons as inside nuclei with mass numbers a1 and a2 |
561 | // The MSTP array in the PYPARS common block is used to enable and |
562 | // select the nuclear structure functions. |
563 | // MSTP(52) : (D=1) choice of proton and nuclear structure-function library |
564 | // =1: internal PYTHIA acording to MSTP(51) |
565 | // =2: PDFLIB proton s.f., with MSTP(51) = 1000xNGROUP+NSET |
566 | // If the following mass number both not equal zero, nuclear corrections of the stf are used. |
567 | // MSTP(192) : Mass number of nucleus side 1 |
568 | // MSTP(193) : Mass number of nucleus side 2 |
569 | SetMSTP(52,2); |
570 | SetMSTP(192, a1); |
571 | SetMSTP(193, a2); |
572 | } |
573 | |
574 | |
575 | AliPythia* AliPythia::Instance() |
576 | { |
577 | // Set random number generator |
578 | if (fgAliPythia) { |
579 | return fgAliPythia; |
580 | } else { |
581 | fgAliPythia = new AliPythia(); |
582 | return fgAliPythia; |
583 | } |
584 | } |
585 | |
586 | void AliPythia::PrintParticles() |
587 | { |
588 | // Print list of particl properties |
589 | Int_t np = 0; |
c31f1d37 |
590 | char* name = new char[16]; |
8d2cd130 |
591 | for (Int_t kf=0; kf<1000000; kf++) { |
592 | for (Int_t c = 1; c > -2; c-=2) { |
8d2cd130 |
593 | Int_t kc = Pycomp(c*kf); |
594 | if (kc) { |
595 | Float_t mass = GetPMAS(kc,1); |
596 | Float_t width = GetPMAS(kc,2); |
597 | Float_t tau = GetPMAS(kc,4); |
c31f1d37 |
598 | |
8d2cd130 |
599 | Pyname(kf,name); |
600 | |
601 | np++; |
602 | |
603 | printf("\n mass, width, tau: %6d %s %10.3f %10.3e %10.3e", |
604 | c*kf, name, mass, width, tau); |
605 | } |
606 | } |
607 | } |
608 | printf("\n Number of particles %d \n \n", np); |
609 | } |
610 | |
611 | void AliPythia::ResetDecayTable() |
612 | { |
613 | // Set default values for pythia decay switches |
614 | Int_t i; |
615 | for (i = 1; i < 501; i++) SetMDCY(i,1,fDefMDCY[i]); |
616 | for (i = 1; i < 2001; i++) SetMDME(i,1,fDefMDME[i]); |
617 | } |
618 | |
619 | void AliPythia::SetDecayTable() |
620 | { |
621 | // Set default values for pythia decay switches |
622 | // |
623 | Int_t i; |
624 | for (i = 1; i < 501; i++) fDefMDCY[i] = GetMDCY(i,1); |
625 | for (i = 1; i < 2001; i++) fDefMDME[i] = GetMDME(i,1); |
626 | } |
627 | |
628 | void AliPythia::Pyclus(Int_t& njet) |
629 | { |
630 | // Call Pythia clustering algorithm |
631 | // |
632 | pyclus(njet); |
633 | } |
634 | |
635 | void AliPythia::Pycell(Int_t& njet) |
636 | { |
637 | // Call Pythia jet reconstruction algorithm |
638 | // |
639 | pycell(njet); |
640 | } |
641 | |
452af8c7 |
642 | void AliPythia::Pyshow(Int_t ip1, Int_t ip2, Double_t qmax) |
643 | { |
644 | // Call Pythia jet reconstruction algorithm |
645 | // |
452af8c7 |
646 | pyshow(ip1, ip2, qmax); |
647 | } |
648 | |
649 | void AliPythia::Pyrobo(Int_t imi, Int_t ima, Double_t the, Double_t phi, Double_t bex, Double_t bey, Double_t bez) |
650 | { |
651 | pyrobo(imi, ima, the, phi, bex, bey, bez); |
652 | } |
653 | |
654 | |
655 | |
0f482ae4 |
656 | void AliPythia::InitQuenching(Float_t cMin, Float_t cMax, Float_t qTransport, Float_t maxLength, Int_t iECMethod) |
657 | { |
658 | // Initializes |
659 | // (1) The quenching model using quenching weights according to C. Salgado and U. Wiedemann |
660 | // (2) The nuclear geometry using the Glauber Model |
661 | // |
662 | |
663 | |
664 | fGlauber = new AliFastGlauber(); |
665 | fGlauber->Init(2); |
666 | fGlauber->SetCentralityClass(cMin, cMax); |
667 | |
668 | fQuenchingWeights = new AliQuenchingWeights(); |
669 | fQuenchingWeights->InitMult(); |
670 | fQuenchingWeights->SetQTransport(qTransport); |
671 | fQuenchingWeights->SetECMethod(AliQuenchingWeights::kECMethod(iECMethod)); |
672 | fQuenchingWeights->SetLengthMax(Int_t(maxLength)); |
673 | fQuenchingWeights->SampleEnergyLoss(); |
674 | |
675 | } |
676 | |
677 | |
452af8c7 |
678 | void AliPythia::Quench() |
679 | { |
680 | // |
681 | // |
682 | // Simple Jet Quenching routine: |
683 | // ============================= |
684 | // The jet formed by all final state partons radiated by the parton created |
0f482ae4 |
685 | // in the hard collisions is quenched by a factor (1-z) using light cone variables in |
686 | // the initial parton reference frame: |
452af8c7 |
687 | // (E + p_z)new = (1-z) (E + p_z)old |
688 | // |
0f482ae4 |
689 | // |
690 | // |
691 | // |
452af8c7 |
692 | // The lost momentum is first balanced by one gluon with virtuality > 0. |
693 | // Subsequently the gluon splits to yield two gluons with E = p. |
694 | // |
0f482ae4 |
695 | // |
696 | // |
4e383037 |
697 | static Float_t eMean = 0.; |
698 | static Int_t icall = 0; |
0f482ae4 |
699 | |
700 | Double_t p0[2][5]; |
701 | Double_t p1[2][5]; |
702 | Double_t p2[2][5]; |
452af8c7 |
703 | Int_t klast[2] = {-1, -1}; |
452af8c7 |
704 | |
705 | Int_t numpart = fPyjets->N; |
0f482ae4 |
706 | Double_t px = 0., py = 0., pz = 0., e = 0., m = 0., p = 0., pt = 0., theta = 0.; |
707 | Double_t pxq[2], pyq[2], pzq[2], eq[2], yq[2], mq[2], pq[2], phiq[2], thetaq[2], ptq[2]; |
708 | Bool_t quenched[2]; |
709 | Double_t phi; |
710 | Double_t zInitial[2], wjtKick[2]; |
4e383037 |
711 | Int_t nGluon[2]; |
712 | |
0f482ae4 |
713 | Int_t imo, kst, pdg; |
511db649 |
714 | // |
0f482ae4 |
715 | // Primary partons |
511db649 |
716 | // |
4e383037 |
717 | |
718 | |
0f482ae4 |
719 | |
720 | for (Int_t i = 6; i <= 7; i++) { |
721 | Int_t j = i - 6; |
452af8c7 |
722 | |
0f482ae4 |
723 | pxq[j] = fPyjets->P[0][i]; |
724 | pyq[j] = fPyjets->P[1][i]; |
725 | pzq[j] = fPyjets->P[2][i]; |
726 | eq[j] = fPyjets->P[3][i]; |
727 | mq[j] = fPyjets->P[4][i]; |
4e383037 |
728 | yq[j] = 0.5 * TMath::Log((eq[j] + pzq[j] + 1.e-14) / (eq[j] - pzq[j] + 1.e-14)); |
0f482ae4 |
729 | pq[j] = TMath::Sqrt(pxq[j] * pxq[j] + pyq[j] * pyq[j] + pzq[j] * pzq[j]); |
730 | phiq[j] = TMath::Pi()+TMath::ATan2(-pyq[j], -pxq[j]); |
731 | ptq[j] = TMath::Sqrt(pxq[j] * pxq[j] + pyq[j] * pyq[j]); |
732 | thetaq[j] = TMath::ATan2(ptq[j], pzq[j]); |
733 | phi = phiq[j]; |
734 | |
735 | // Quench only central jets |
736 | if (TMath::Abs(yq[j]) > 2.5) { |
737 | zInitial[j] = 0.; |
738 | } else { |
739 | pdg = fPyjets->K[1][i]; |
740 | |
741 | // Get length in nucleus |
742 | Double_t l; |
743 | fGlauber->GetLengthsForPythia(1, &phi, &l, -1.); |
744 | // |
745 | // Energy loss for given length and parton typr |
746 | Int_t itype = (pdg == 21) ? 2 : 1; |
4e383037 |
747 | |
0f482ae4 |
748 | Double_t eloss = fQuenchingWeights->GetELossRandom(itype, l, eq[j]); |
4e383037 |
749 | if (eq[j] > 80. && TMath::Abs(yq[j]) < 0.5) { |
750 | icall ++; |
751 | eMean += eloss; |
752 | } |
753 | |
0f482ae4 |
754 | // |
755 | // Extra pt |
4e383037 |
756 | |
0f482ae4 |
757 | wjtKick[j] = TMath::Sqrt(l * fQuenchingWeights->GetQTransport()); |
758 | // |
759 | // Fractional energy loss |
760 | zInitial[j] = eloss / eq[j]; |
761 | // |
762 | // Avoid complete loss |
763 | // |
764 | if (zInitial[j] == 1.) zInitial[j] = 0.95; |
765 | // |
766 | // Some debug printing |
4e383037 |
767 | printf("Initial parton # %3d, Type %3d Energy %10.3f Phi %10.3f Length %10.3f Loss %10.3f Kick %10.3f Mean: %10.3f %10.3f\n", |
768 | j, itype, eq[j], phi, l, eloss, wjtKick[j], eMean / Float_t(icall+1), yq[j]); |
769 | |
770 | zInitial[j] = 1.; |
771 | while (zInitial[j] >= 0.95) zInitial[j] = gRandom->Exp(0.2); |
0f482ae4 |
772 | } |
4e383037 |
773 | |
0f482ae4 |
774 | quenched[j] = (zInitial[j] > 0.01); |
4e383037 |
775 | } // primary partons |
0f482ae4 |
776 | |
6e90ad26 |
777 | Double_t pNew[1000][4]; |
778 | Int_t kNew[1000]; |
779 | Int_t icount = 0; |
780 | // |
4e383037 |
781 | // System Loop |
782 | for (Int_t isys = 0; isys < 2; isys++) { |
6e90ad26 |
783 | // Skip to next system if not quenched. |
4e383037 |
784 | if (!quenched[isys]) continue; |
785 | |
786 | nGluon[isys] = 1 + Int_t(zInitial[isys] / (1. - zInitial[isys])); |
787 | if (nGluon[isys] > 6) nGluon[isys] = 6; |
788 | zInitial[isys] = 1. - TMath::Power(1. - zInitial[isys], 1./Double_t(nGluon[isys])); |
789 | wjtKick[isys] = wjtKick[isys] / TMath::Sqrt(Double_t(nGluon[isys])); |
0f482ae4 |
790 | |
4e383037 |
791 | |
792 | |
793 | Int_t igMin = -1; |
794 | Int_t igMax = -1; |
795 | Double_t pg[4] = {0., 0., 0., 0.}; |
796 | |
797 | // |
798 | // Loop on radiation events |
799 | |
800 | for (Int_t iglu = 0; iglu < nGluon[isys]; iglu++) { |
6e90ad26 |
801 | Double_t zHeavy = zInitial[isys]; |
6e90ad26 |
802 | // |
4e383037 |
803 | |
6e90ad26 |
804 | while (1) { |
805 | icount = 0; |
806 | for (Int_t k = 0; k < 4; k++) |
807 | { |
808 | p0[isys][k] = 0.; |
809 | p1[isys][k] = 0.; |
810 | p2[isys][k] = 0.; |
811 | } |
812 | // Loop over partons |
813 | for (Int_t i = 0; i < numpart; i++) |
814 | { |
815 | imo = fPyjets->K[2][i]; |
816 | kst = fPyjets->K[0][i]; |
817 | pdg = fPyjets->K[1][i]; |
818 | |
819 | |
820 | |
0f482ae4 |
821 | // Quarks and gluons only |
6e90ad26 |
822 | if (pdg != 21 && TMath::Abs(pdg) > 6) continue; |
0f482ae4 |
823 | // Particles from hard scattering only |
6e90ad26 |
824 | if (imo > 8 && imo < 1000) imo = fPyjets->K[2][imo - 1]; |
4e383037 |
825 | if (imo != (isys + 7) && (imo % 1000) != (isys + 7)) continue; |
6e90ad26 |
826 | |
0f482ae4 |
827 | // Skip comment lines |
6e90ad26 |
828 | if (kst != 1 && kst != 2) continue; |
0f482ae4 |
829 | // |
830 | // Parton kinematic |
6e90ad26 |
831 | px = fPyjets->P[0][i]; |
832 | py = fPyjets->P[1][i]; |
833 | pz = fPyjets->P[2][i]; |
834 | e = fPyjets->P[3][i]; |
835 | m = fPyjets->P[4][i]; |
836 | pt = TMath::Sqrt(px * px + py * py); |
837 | p = TMath::Sqrt(px * px + py * py + pz * pz); |
838 | phi = TMath::Pi() + TMath::ATan2(-py, -px); |
839 | theta = TMath::ATan2(pt, pz); |
840 | |
0f482ae4 |
841 | // |
842 | // Save 4-momentum sum for balancing |
6e90ad26 |
843 | Int_t index = imo - 7; |
4e383037 |
844 | if (index >= 1000) index = imo % 1000 - 7; |
6e90ad26 |
845 | |
846 | p0[index][0] += px; |
847 | p0[index][1] += py; |
848 | p0[index][2] += pz; |
849 | p0[index][3] += e; |
6e90ad26 |
850 | |
851 | klast[index] = i; |
852 | |
0f482ae4 |
853 | // |
854 | // Fractional energy loss |
6e90ad26 |
855 | Double_t z = zInitial[index]; |
4e383037 |
856 | |
857 | // Don't fully quench radiated gluons |
858 | // |
859 | if (imo > 1000) { |
860 | // This small factor makes sure that the gluons are not too close in phase space to avoid recombination |
861 | // |
862 | |
863 | z = 0.05; |
864 | } |
865 | |
866 | // |
867 | |
6e90ad26 |
868 | if (m > 0.) z = zHeavy; |
869 | |
870 | // |
871 | // |
872 | // Transform into frame in which initial parton is along z-axis |
873 | // |
874 | TVector3 v(px, py, pz); |
875 | v.RotateZ(-phiq[index]); v.RotateY(-thetaq[index]); |
876 | Double_t pxs = v.X(); Double_t pys = v.Y(); Double_t pl = v.Z(); |
877 | |
878 | Double_t jt = TMath::Sqrt(pxs * pxs + pys * pys); |
879 | Double_t mt2 = jt * jt + m * m; |
880 | Double_t zmax = 1.; |
881 | // |
882 | // Kinematic limit on z |
883 | // |
4e383037 |
884 | if (m > 0.) zmax = 1. - m / TMath::Sqrt(m * m + jt * jt); |
6e90ad26 |
885 | // |
886 | // Change light-cone kinematics rel. to initial parton |
887 | // |
888 | Double_t eppzOld = e + pl; |
889 | Double_t empzOld = e - pl; |
890 | |
891 | Double_t eppzNew = (1. - z) * eppzOld; |
892 | Double_t empzNew = empzOld - mt2 * z / eppzOld; |
893 | Double_t eNew = 0.5 * (eppzNew + empzNew); |
894 | Double_t plNew = 0.5 * (eppzNew - empzNew); |
895 | |
896 | Double_t jtNew; |
897 | // |
898 | // if mt very small (or sometimes even < 0 for numerical reasons) set it to 0 |
899 | Double_t mt2New = eppzNew * empzNew; |
900 | if (mt2New < 1.e-8) mt2New = 0.; |
4e383037 |
901 | if (z < zmax) { |
902 | if (m * m > mt2New) { |
903 | // |
904 | // This should not happen |
905 | // |
906 | Fatal("Quench()", "This should never happen %e %e %e!", m, eppzNew, empzNew); |
907 | jtNew = 0; |
908 | } else { |
909 | jtNew = TMath::Sqrt(mt2New - m * m); |
910 | } |
6e90ad26 |
911 | } else { |
4e383037 |
912 | // If pT is to small (probably a leading massive particle) we scale only the energy |
913 | // This can cause negative masses of the radiated gluon |
914 | // Let's hope for the best ... |
915 | jtNew = jt; |
916 | eNew = TMath::Sqrt(plNew * plNew + mt2); |
917 | |
6e90ad26 |
918 | } |
6e90ad26 |
919 | // |
920 | // Calculate new px, py |
921 | // |
922 | Double_t pxNew = jtNew / jt * pxs; |
923 | Double_t pyNew = jtNew / jt * pys; |
924 | |
925 | // Double_t dpx = pxs - pxNew; |
926 | // Double_t dpy = pys - pyNew; |
927 | // Double_t dpz = pl - plNew; |
928 | // Double_t de = e - eNew; |
929 | // Double_t dmass2 = de * de - dpx * dpx - dpy * dpy - dpz * dpz; |
930 | // printf("New mass (1) %e %e %e %e %e %e %e \n", dmass2, jt, jtNew, pl, plNew, e, eNew); |
931 | // printf("New mass (2) %e %e \n", pxNew, pyNew); |
932 | // |
933 | // Rotate back |
934 | // |
935 | TVector3 w(pxNew, pyNew, plNew); |
936 | w.RotateY(thetaq[index]); w.RotateZ(phiq[index]); |
937 | pxNew = w.X(); pyNew = w.Y(); plNew = w.Z(); |
938 | |
939 | p1[index][0] += pxNew; |
940 | p1[index][1] += pyNew; |
941 | p1[index][2] += plNew; |
942 | p1[index][3] += eNew; |
943 | // |
944 | // Updated 4-momentum vectors |
945 | // |
946 | pNew[icount][0] = pxNew; |
947 | pNew[icount][1] = pyNew; |
948 | pNew[icount][2] = plNew; |
949 | pNew[icount][3] = eNew; |
950 | kNew[icount] = i; |
951 | icount++; |
952 | } // parton loop |
0f482ae4 |
953 | // |
6e90ad26 |
954 | // Check if there was phase-space for quenching |
0f482ae4 |
955 | // |
0f482ae4 |
956 | |
6e90ad26 |
957 | if (icount == 0) quenched[isys] = kFALSE; |
958 | if (!quenched[isys]) break; |
959 | |
960 | for (Int_t j = 0; j < 4; j++) |
961 | { |
962 | p2[isys][j] = p0[isys][j] - p1[isys][j]; |
963 | } |
964 | p2[isys][4] = p2[isys][3] * p2[isys][3] - p2[isys][0] * p2[isys][0] - p2[isys][1] * p2[isys][1] - p2[isys][2] * p2[isys][2]; |
6e90ad26 |
965 | if (p2[isys][4] > 0.) { |
966 | p2[isys][4] = TMath::Sqrt(p2[isys][4]); |
967 | break; |
968 | } else { |
969 | printf("Warning negative mass squared in system %d %f ! \n", isys, zInitial[isys]); |
4e383037 |
970 | printf("4-Momentum: %10.3e %10.3e %10.3e %10.3e %10.3e \n", p2[isys][0], p2[isys][1], p2[isys][2], p2[isys][3], p2[isys][4]); |
6e90ad26 |
971 | if (p2[isys][4] < -0.01) { |
4e383037 |
972 | printf("Negative mass squared !\n"); |
973 | // Here we have to put the gluon back to mass shell |
974 | // This will lead to a small energy imbalance |
975 | p2[isys][4] = 0.; |
976 | p2[isys][3] = TMath::Sqrt(p2[isys][0] * p2[isys][0] + p2[isys][1] * p2[isys][1] + p2[isys][2] * p2[isys][2]); |
977 | break; |
6e90ad26 |
978 | } else { |
979 | p2[isys][4] = 0.; |
980 | break; |
981 | } |
982 | } |
6e90ad26 |
983 | /* |
6e90ad26 |
984 | zHeavy *= 0.98; |
985 | printf("zHeavy lowered to %f\n", zHeavy); |
986 | if (zHeavy < 0.01) { |
987 | printf("No success ! \n"); |
988 | icount = 0; |
989 | quenched[isys] = kFALSE; |
990 | break; |
991 | } |
4e383037 |
992 | */ |
993 | } // iteration on z (while) |
994 | |
6e90ad26 |
995 | // Update event record |
996 | for (Int_t k = 0; k < icount; k++) { |
997 | // printf("%6d %6d %10.3e %10.3e %10.3e %10.3e\n", k, kNew[k], pNew[k][0],pNew[k][1], pNew[k][2], pNew[k][3] ); |
998 | fPyjets->P[0][kNew[k]] = pNew[k][0]; |
999 | fPyjets->P[1][kNew[k]] = pNew[k][1]; |
1000 | fPyjets->P[2][kNew[k]] = pNew[k][2]; |
1001 | fPyjets->P[3][kNew[k]] = pNew[k][3]; |
0f482ae4 |
1002 | } |
4e383037 |
1003 | // |
1004 | // Add the gluons |
1005 | // |
1006 | Int_t ish = 0; |
1837e95c |
1007 | Int_t iGlu; |
4e383037 |
1008 | if (!quenched[isys]) continue; |
0f482ae4 |
1009 | // |
1010 | // Last parton from shower i |
4e383037 |
1011 | Int_t in = klast[isys]; |
0f482ae4 |
1012 | // |
1013 | // Continue if no parton in shower i selected |
1014 | if (in == -1) continue; |
1015 | // |
1016 | // If this is the second initial parton and it is behind the first move pointer by previous ish |
4e383037 |
1017 | if (isys == 1 && klast[1] > klast[0]) in += ish; |
0f482ae4 |
1018 | // |
1019 | // Starting index |
452af8c7 |
1020 | |
4e383037 |
1021 | // jmin = in - 1; |
0f482ae4 |
1022 | // How many additional gluons will be generated |
1023 | ish = 1; |
4e383037 |
1024 | if (p2[isys][4] > 0.05) ish = 2; |
0f482ae4 |
1025 | // |
1026 | // Position of gluons |
4e383037 |
1027 | iGlu = numpart; |
1028 | if (iglu == 0) igMin = iGlu; |
1029 | igMax = iGlu; |
0f482ae4 |
1030 | numpart += ish; |
1031 | (fPyjets->N) += ish; |
4e383037 |
1032 | |
0f482ae4 |
1033 | if (ish == 1) { |
4e383037 |
1034 | fPyjets->P[0][iGlu] = p2[isys][0]; |
1035 | fPyjets->P[1][iGlu] = p2[isys][1]; |
1036 | fPyjets->P[2][iGlu] = p2[isys][2]; |
1037 | fPyjets->P[3][iGlu] = p2[isys][3]; |
1038 | fPyjets->P[4][iGlu] = p2[isys][4]; |
0f482ae4 |
1039 | |
4e383037 |
1040 | fPyjets->K[0][iGlu] = 1; |
1041 | if (iglu == nGluon[isys] - 1) fPyjets->K[0][iGlu] = 1; |
0f482ae4 |
1042 | fPyjets->K[1][iGlu] = 21; |
4e383037 |
1043 | fPyjets->K[2][iGlu] = fPyjets->K[2][in] + 1000; |
0f482ae4 |
1044 | fPyjets->K[3][iGlu] = -1; |
1045 | fPyjets->K[4][iGlu] = -1; |
4e383037 |
1046 | |
1047 | pg[0] += p2[isys][0]; |
1048 | pg[1] += p2[isys][1]; |
1049 | pg[2] += p2[isys][2]; |
1050 | pg[3] += p2[isys][3]; |
0f482ae4 |
1051 | } else { |
1052 | // |
1053 | // Split gluon in rest frame. |
1054 | // |
4e383037 |
1055 | Double_t bx = p2[isys][0] / p2[isys][3]; |
1056 | Double_t by = p2[isys][1] / p2[isys][3]; |
1057 | Double_t bz = p2[isys][2] / p2[isys][3]; |
1058 | Double_t pst = p2[isys][4] / 2.; |
0f482ae4 |
1059 | // |
1060 | // Isotropic decay ???? |
1061 | Double_t cost = 2. * gRandom->Rndm() - 1.; |
1062 | Double_t sint = TMath::Sqrt(1. - cost * cost); |
1063 | Double_t phi = 2. * TMath::Pi() * gRandom->Rndm(); |
1064 | |
1065 | Double_t pz1 = pst * cost; |
1066 | Double_t pz2 = -pst * cost; |
1067 | Double_t pt1 = pst * sint; |
1068 | Double_t pt2 = -pst * sint; |
1069 | Double_t px1 = pt1 * TMath::Cos(phi); |
1070 | Double_t py1 = pt1 * TMath::Sin(phi); |
1071 | Double_t px2 = pt2 * TMath::Cos(phi); |
1072 | Double_t py2 = pt2 * TMath::Sin(phi); |
1073 | |
1074 | fPyjets->P[0][iGlu] = px1; |
1075 | fPyjets->P[1][iGlu] = py1; |
1076 | fPyjets->P[2][iGlu] = pz1; |
1077 | fPyjets->P[3][iGlu] = pst; |
1078 | fPyjets->P[4][iGlu] = 0.; |
1079 | |
4e383037 |
1080 | fPyjets->K[0][iGlu] = 1 ; |
0f482ae4 |
1081 | fPyjets->K[1][iGlu] = 21; |
4e383037 |
1082 | fPyjets->K[2][iGlu] = fPyjets->K[2][in] + 1000; |
0f482ae4 |
1083 | fPyjets->K[3][iGlu] = -1; |
1084 | fPyjets->K[4][iGlu] = -1; |
1085 | |
1086 | fPyjets->P[0][iGlu+1] = px2; |
1087 | fPyjets->P[1][iGlu+1] = py2; |
1088 | fPyjets->P[2][iGlu+1] = pz2; |
1089 | fPyjets->P[3][iGlu+1] = pst; |
1090 | fPyjets->P[4][iGlu+1] = 0.; |
1091 | |
4e383037 |
1092 | fPyjets->K[0][iGlu+1] = 1; |
1093 | if (iglu == nGluon[isys] - 1) fPyjets->K[0][iGlu+1] = 1; |
0f482ae4 |
1094 | fPyjets->K[1][iGlu+1] = 21; |
4e383037 |
1095 | fPyjets->K[2][iGlu+1] = fPyjets->K[2][in] + 1000; |
0f482ae4 |
1096 | fPyjets->K[3][iGlu+1] = -1; |
1097 | fPyjets->K[4][iGlu+1] = -1; |
1098 | SetMSTU(1,0); |
1099 | SetMSTU(2,0); |
1100 | // |
1101 | // Boost back |
1102 | // |
1103 | Pyrobo(iGlu + 1, iGlu + 2, 0., 0., bx, by, bz); |
1104 | } |
4e383037 |
1105 | /* |
1106 | for (Int_t ig = iGlu; ig < iGlu+ish; ig++) { |
1107 | Double_t px, py, pz; |
1108 | px = fPyjets->P[0][ig]; |
1109 | py = fPyjets->P[1][ig]; |
1110 | pz = fPyjets->P[2][ig]; |
1111 | TVector3 v(px, py, pz); |
1112 | v.RotateZ(-phiq[isys]); |
1113 | v.RotateY(-thetaq[isys]); |
1114 | Double_t pxs = v.X(); Double_t pys = v.Y(); Double_t pzs = v.Z(); |
1115 | Double_t r = AliPythiaRndm::GetPythiaRandom()->Rndm(); |
1116 | Double_t jtKick = 0.3 * TMath::Sqrt(-TMath::Log(r)); |
1117 | if (ish == 2) jtKick = wjtKick[i] * TMath::Sqrt(-TMath::Log(r)) / TMath::Sqrt(2.); |
1118 | Double_t phiKick = 2. * TMath::Pi() * AliPythiaRndm::GetPythiaRandom()->Rndm(); |
1119 | pxs += jtKick * TMath::Cos(phiKick); |
1120 | pys += jtKick * TMath::Sin(phiKick); |
1121 | TVector3 w(pxs, pys, pzs); |
1122 | w.RotateY(thetaq[isys]); |
1123 | w.RotateZ(phiq[isys]); |
1124 | fPyjets->P[0][ig] = w.X(); |
1125 | fPyjets->P[1][ig] = w.Y(); |
1126 | fPyjets->P[2][ig] = w.Z(); |
1127 | fPyjets->P[2][ig] = w.Mag(); |
1128 | } |
1129 | */ |
1130 | } // kGluon |
1131 | |
6e90ad26 |
1132 | |
4e383037 |
1133 | // Check energy conservation |
0f482ae4 |
1134 | Double_t pxs = 0.; |
1135 | Double_t pys = 0.; |
1136 | Double_t pzs = 0.; |
1137 | Double_t es = 14000.; |
1138 | |
1139 | for (Int_t i = 0; i < numpart; i++) |
1140 | { |
1141 | kst = fPyjets->K[0][i]; |
1142 | if (kst != 1 && kst != 2) continue; |
1143 | pxs += fPyjets->P[0][i]; |
1144 | pys += fPyjets->P[1][i]; |
1145 | pzs += fPyjets->P[2][i]; |
1146 | es -= fPyjets->P[3][i]; |
1147 | } |
1148 | if (TMath::Abs(pxs) > 1.e-2 || |
1149 | TMath::Abs(pys) > 1.e-2 || |
1150 | TMath::Abs(pzs) > 1.e-1) { |
1151 | printf("%e %e %e %e\n", pxs, pys, pzs, es); |
4e383037 |
1152 | // Fatal("Quench()", "4-Momentum non-conservation"); |
452af8c7 |
1153 | } |
4e383037 |
1154 | |
1155 | } // end quenching loop (systems) |
6e90ad26 |
1156 | // Clean-up |
0f482ae4 |
1157 | for (Int_t i = 0; i < numpart; i++) |
1158 | { |
4e383037 |
1159 | imo = fPyjets->K[2][i]; |
1160 | if (imo > 1000) { |
1161 | fPyjets->K[2][i] = fPyjets->K[2][i] % 1000; |
1162 | } |
0f482ae4 |
1163 | } |
4e383037 |
1164 | // this->Pylist(1); |
0f482ae4 |
1165 | } // end quench |
90d7b703 |
1166 | |