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6b435cde | 1 | |
8d2cd130 | 2 | /************************************************************************** |
3 | * Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. * | |
4 | * * | |
5 | * Author: The ALICE Off-line Project. * | |
6 | * Contributors are mentioned in the code where appropriate. * | |
7 | * * | |
8 | * Permission to use, copy, modify and distribute this software and its * | |
9 | * documentation strictly for non-commercial purposes is hereby granted * | |
10 | * without fee, provided that the above copyright notice appears in all * | |
11 | * copies and that both the copyright notice and this permission notice * | |
12 | * appear in the supporting documentation. The authors make no claims * | |
13 | * about the suitability of this software for any purpose. It is * | |
14 | * provided "as is" without express or implied warranty. * | |
15 | **************************************************************************/ | |
16 | ||
7cdba479 | 17 | /* $Id$ */ |
8d2cd130 | 18 | |
19 | #include "AliPythia.h" | |
7cdba479 | 20 | #include "AliPythiaRndm.h" |
12cb0bc0 | 21 | #include "AliFastGlauber.h" |
22 | #include "AliQuenchingWeights.h" | |
0f482ae4 | 23 | #include "TVector3.h" |
12cb0bc0 | 24 | #include "PyquenCommon.h" |
8d2cd130 | 25 | |
26 | ClassImp(AliPythia) | |
27 | ||
28 | #ifndef WIN32 | |
29 | # define pyclus pyclus_ | |
30 | # define pycell pycell_ | |
452af8c7 | 31 | # define pyshow pyshow_ |
32 | # define pyrobo pyrobo_ | |
992f2843 | 33 | # define pyquen pyquen_ |
16a82508 | 34 | # define pyevnw pyevnw_ |
8d2cd130 | 35 | # define type_of_call |
36 | #else | |
37 | # define pyclus PYCLUS | |
38 | # define pycell PYCELL | |
452af8c7 | 39 | # define pyrobo PYROBO |
992f2843 | 40 | # define pyquen PYQUEN |
16a82508 | 41 | # define pyevnw PYEVNW |
8d2cd130 | 42 | # define type_of_call _stdcall |
43 | #endif | |
44 | ||
45 | extern "C" void type_of_call pyclus(Int_t & ); | |
46 | extern "C" void type_of_call pycell(Int_t & ); | |
452af8c7 | 47 | extern "C" void type_of_call pyshow(Int_t &, Int_t &, Double_t &); |
48 | extern "C" void type_of_call pyrobo(Int_t &, Int_t &, Double_t &, Double_t &, Double_t &, Double_t &, Double_t &); | |
992f2843 | 49 | extern "C" void type_of_call pyquen(Double_t &, Int_t &, Double_t &); |
0a2cfc0a | 50 | extern "C" void type_of_call pyevnw(){;} |
8d2cd130 | 51 | |
52 | //_____________________________________________________________________________ | |
53 | ||
54 | AliPythia* AliPythia::fgAliPythia=NULL; | |
55 | ||
e8a8adcd | 56 | AliPythia::AliPythia(): |
57 | fProcess(kPyMb), | |
58 | fEcms(0.), | |
59 | fStrucFunc(kCTEQ5L), | |
60 | fXJet(0.), | |
61 | fYJet(0.), | |
32c8e463 | 62 | fNGmax(30), |
63 | fZmax(0.97), | |
e8a8adcd | 64 | fGlauber(0), |
65 | fQuenchingWeights(0) | |
8d2cd130 | 66 | { |
67 | // Default Constructor | |
68 | // | |
69 | // Set random number | |
7cdba479 | 70 | if (!AliPythiaRndm::GetPythiaRandom()) |
71 | AliPythiaRndm::SetPythiaRandom(GetRandom()); | |
0f482ae4 | 72 | fGlauber = 0; |
73 | fQuenchingWeights = 0; | |
8d2cd130 | 74 | } |
75 | ||
e8a8adcd | 76 | AliPythia::AliPythia(const AliPythia& pythia): |
6b435cde | 77 | TPythia6(pythia), |
78 | AliRndm(pythia), | |
e8a8adcd | 79 | fProcess(kPyMb), |
80 | fEcms(0.), | |
81 | fStrucFunc(kCTEQ5L), | |
82 | fXJet(0.), | |
83 | fYJet(0.), | |
32c8e463 | 84 | fNGmax(30), |
85 | fZmax(0.97), | |
e8a8adcd | 86 | fGlauber(0), |
87 | fQuenchingWeights(0) | |
88 | { | |
89 | // Copy Constructor | |
90 | pythia.Copy(*this); | |
91 | } | |
92 | ||
8d2cd130 | 93 | void AliPythia::ProcInit(Process_t process, Float_t energy, StrucFunc_t strucfunc) |
94 | { | |
95 | // Initialise the process to generate | |
7cdba479 | 96 | if (!AliPythiaRndm::GetPythiaRandom()) |
97 | AliPythiaRndm::SetPythiaRandom(GetRandom()); | |
8d2cd130 | 98 | |
99 | fProcess = process; | |
100 | fEcms = energy; | |
101 | fStrucFunc = strucfunc; | |
1d5b1b20 | 102 | //...Switch off decay of pi0, K0S, Lambda, Sigma+-, Xi0-, Omega-. |
e2de0ce1 | 103 | SetMDCY(Pycomp(111) ,1,0); // pi0 |
104 | SetMDCY(Pycomp(310) ,1,0); // K0S | |
105 | SetMDCY(Pycomp(3122),1,0); // kLambda | |
106 | SetMDCY(Pycomp(3112),1,0); // sigma - | |
107 | SetMDCY(Pycomp(3212),1,0); // sigma 0 | |
108 | SetMDCY(Pycomp(3222),1,0); // sigma + | |
109 | SetMDCY(Pycomp(3312),1,0); // xi - | |
110 | SetMDCY(Pycomp(3322),1,0); // xi 0 | |
111 | SetMDCY(Pycomp(3334),1,0); // omega- | |
1c50ec12 | 112 | // Select structure function |
8d2cd130 | 113 | SetMSTP(52,2); |
e2de0ce1 | 114 | SetMSTP(51, AliStructFuncType::PDFsetIndex(strucfunc)); |
1c50ec12 | 115 | // Particles produced in string fragmentation point directly to either of the two endpoints |
116 | // of the string (depending in the side they were generated from). | |
117 | SetMSTU(16,2); | |
118 | ||
8d2cd130 | 119 | // |
120 | // Pythia initialisation for selected processes// | |
121 | // | |
122 | // Make MSEL clean | |
123 | // | |
124 | for (Int_t i=1; i<= 200; i++) { | |
125 | SetMSUB(i,0); | |
126 | } | |
127 | // select charm production | |
128 | switch (process) | |
129 | { | |
65f2626c | 130 | case kPyOldUEQ2ordered: //Old underlying events with Q2 ordered QCD processes |
131 | // Multiple interactions on. | |
132 | SetMSTP(81,1); | |
133 | // Double Gaussian matter distribution. | |
134 | SetMSTP(82,4); | |
135 | SetPARP(83,0.5); | |
136 | SetPARP(84,0.4); | |
137 | // pT0. | |
138 | SetPARP(82,2.0); | |
139 | // Reference energy for pT0 and energy rescaling pace. | |
140 | SetPARP(89,1800); | |
141 | SetPARP(90,0.25); | |
142 | // String drawing almost completely minimizes string length. | |
143 | SetPARP(85,0.9); | |
144 | SetPARP(86,0.95); | |
145 | // ISR and FSR activity. | |
146 | SetPARP(67,4); | |
147 | SetPARP(71,4); | |
148 | // Lambda_FSR scale. | |
149 | SetPARJ(81,0.29); | |
150 | break; | |
151 | case kPyOldUEQ2ordered2: | |
152 | // Old underlying events with Q2 ordered QCD processes | |
153 | // Multiple interactions on. | |
154 | SetMSTP(81,1); | |
155 | // Double Gaussian matter distribution. | |
156 | SetMSTP(82,4); | |
157 | SetPARP(83,0.5); | |
158 | SetPARP(84,0.4); | |
159 | // pT0. | |
160 | SetPARP(82,2.0); | |
161 | // Reference energy for pT0 and energy rescaling pace. | |
162 | SetPARP(89,1800); | |
163 | SetPARP(90,0.16); // here is the difference with kPyOldUEQ2ordered | |
164 | // String drawing almost completely minimizes string length. | |
165 | SetPARP(85,0.9); | |
166 | SetPARP(86,0.95); | |
167 | // ISR and FSR activity. | |
168 | SetPARP(67,4); | |
169 | SetPARP(71,4); | |
170 | // Lambda_FSR scale. | |
171 | SetPARJ(81,0.29); | |
172 | break; | |
173 | case kPyOldPopcorn: | |
174 | // Old production mechanism: Old Popcorn | |
175 | SetMSEL(1); | |
176 | SetMSTJ(12,3); | |
177 | // (D=2) Like MSTJ(12)=2 but added prod ofthe 1er rank baryon | |
178 | SetMSTP(88,2); | |
179 | // (D=1)see can be used to form baryons (BARYON JUNCTION) | |
180 | SetMSTJ(1,1); | |
e0e89f40 | 181 | AtlasTuning(); |
65f2626c | 182 | break; |
8d2cd130 | 183 | case kPyCharm: |
184 | SetMSEL(4); | |
8d2cd130 | 185 | // heavy quark masses |
186 | ||
187 | SetPMAS(4,1,1.2); | |
8d2cd130 | 188 | // |
189 | // primordial pT | |
190 | SetMSTP(91,1); | |
191 | SetPARP(91,1.); | |
192 | SetPARP(93,5.); | |
193 | // | |
194 | break; | |
195 | case kPyBeauty: | |
196 | SetMSEL(5); | |
197 | SetPMAS(5,1,4.75); | |
8d2cd130 | 198 | break; |
199 | case kPyJpsi: | |
200 | SetMSEL(0); | |
201 | // gg->J/Psi g | |
202 | SetMSUB(86,1); | |
203 | break; | |
204 | case kPyJpsiChi: | |
205 | SetMSEL(0); | |
206 | // gg->J/Psi g | |
207 | SetMSUB(86,1); | |
208 | // gg-> chi_0c g | |
209 | SetMSUB(87,1); | |
210 | // gg-> chi_1c g | |
211 | SetMSUB(88,1); | |
212 | // gg-> chi_2c g | |
213 | SetMSUB(89,1); | |
214 | break; | |
215 | case kPyCharmUnforced: | |
216 | SetMSEL(0); | |
217 | // gq->qg | |
218 | SetMSUB(28,1); | |
219 | // gg->qq | |
220 | SetMSUB(53,1); | |
221 | // gg->gg | |
222 | SetMSUB(68,1); | |
223 | break; | |
224 | case kPyBeautyUnforced: | |
225 | SetMSEL(0); | |
226 | // gq->qg | |
227 | SetMSUB(28,1); | |
228 | // gg->qq | |
229 | SetMSUB(53,1); | |
230 | // gg->gg | |
231 | SetMSUB(68,1); | |
232 | break; | |
233 | case kPyMb: | |
234 | // Minimum Bias pp-Collisions | |
235 | // | |
236 | // | |
237 | // select Pythia min. bias model | |
238 | SetMSEL(0); | |
511db649 | 239 | SetMSUB(92,1); // single diffraction AB-->XB |
240 | SetMSUB(93,1); // single diffraction AB-->AX | |
241 | SetMSUB(94,1); // double diffraction | |
242 | SetMSUB(95,1); // low pt production | |
243 | ||
e0e89f40 | 244 | AtlasTuning(); |
f529e69b | 245 | break; |
04081a91 | 246 | |
247 | case kPyMbWithDirectPhoton: | |
248 | // Minimum Bias pp-Collisions with direct photon processes added | |
249 | // | |
250 | // | |
251 | // select Pythia min. bias model | |
252 | SetMSEL(0); | |
253 | SetMSUB(92,1); // single diffraction AB-->XB | |
254 | SetMSUB(93,1); // single diffraction AB-->AX | |
255 | SetMSUB(94,1); // double diffraction | |
256 | SetMSUB(95,1); // low pt production | |
257 | ||
258 | SetMSUB(14,1); // | |
259 | SetMSUB(18,1); // | |
260 | SetMSUB(29,1); // | |
261 | SetMSUB(114,1); // | |
262 | SetMSUB(115,1); // | |
263 | ||
264 | ||
265 | AtlasTuning(); | |
266 | break; | |
267 | ||
f529e69b | 268 | case kPyMbDefault: |
269 | // Minimum Bias pp-Collisions | |
270 | // | |
271 | // | |
272 | // select Pythia min. bias model | |
273 | SetMSEL(0); | |
274 | SetMSUB(92,1); // single diffraction AB-->XB | |
275 | SetMSUB(93,1); // single diffraction AB-->AX | |
276 | SetMSUB(94,1); // double diffraction | |
277 | SetMSUB(95,1); // low pt production | |
278 | ||
0a0cbcfd | 279 | break; |
280 | case kPyLhwgMb: | |
281 | // Les Houches Working Group 05 Minimum Bias pp-Collisions: hep-ph/0604120 | |
282 | // -> Pythia 6.3 or above is needed | |
283 | // | |
284 | SetMSEL(0); | |
285 | SetMSUB(92,1); // single diffraction AB-->XB | |
286 | SetMSUB(93,1); // single diffraction AB-->AX | |
287 | SetMSUB(94,1); // double diffraction | |
288 | SetMSUB(95,1); // low pt production | |
289 | ||
e2de0ce1 | 290 | SetMSTP(51,AliStructFuncType::PDFsetIndex(kCTEQ6ll)); // CTEQ6ll pdf |
0a0cbcfd | 291 | SetMSTP(52,2); |
292 | SetMSTP(68,1); | |
293 | SetMSTP(70,2); | |
294 | SetMSTP(81,1); // Multiple Interactions ON | |
295 | SetMSTP(82,4); // Double Gaussian Model | |
296 | SetMSTP(88,1); | |
297 | ||
298 | SetPARP(82,2.3); // [GeV] PT_min at Ref. energy | |
299 | SetPARP(83,0.5); // Core density in proton matter distribution (def.value) | |
300 | SetPARP(84,0.5); // Core radius | |
301 | SetPARP(85,0.9); // Regulates gluon prod. mechanism | |
302 | SetPARP(90,0.2); // 2*epsilon (exponent in power law) | |
303 | ||
511db649 | 304 | break; |
8d2cd130 | 305 | case kPyMbNonDiffr: |
306 | // Minimum Bias pp-Collisions | |
307 | // | |
308 | // | |
309 | // select Pythia min. bias model | |
310 | SetMSEL(0); | |
511db649 | 311 | SetMSUB(95,1); // low pt production |
0f482ae4 | 312 | |
d7de4a67 | 313 | AtlasTuning(); |
314 | break; | |
315 | case kPyMbMSEL1: | |
316 | ConfigHeavyFlavor(); | |
317 | // Intrinsic <kT^2> | |
318 | SetMSTP(91,1);// Width (1=gaussian) primordial kT dist. inside hadrons | |
319 | SetPARP(91,1.); // <kT^2> = PARP(91,1.)^2 | |
320 | SetPARP(93,5.); // Upper cut-off | |
321 | // Set Q-quark mass | |
322 | SetPMAS(4,1,1.2); // Charm quark mass | |
323 | SetPMAS(5,1,4.78); // Beauty quark mass | |
324 | SetPARP(71,4.); // Defaut value | |
325 | // Atlas Tuning | |
e0e89f40 | 326 | AtlasTuning(); |
8d2cd130 | 327 | break; |
328 | case kPyJets: | |
329 | // | |
330 | // QCD Jets | |
331 | // | |
332 | SetMSEL(1); | |
65f2626c | 333 | // Pythia Tune A (CDF) |
334 | // | |
4167b79f | 335 | SetPARP(67,2.5); // Regulates Initial State Radiation (value from best fit to D0 dijet analysis) |
65f2626c | 336 | SetMSTP(82,4); // Double Gaussian Model |
337 | SetPARP(82,2.0); // [GeV] PT_min at Ref. energy | |
338 | SetPARP(84,0.4); // Core radius | |
339 | SetPARP(85,0.90) ; // Regulates gluon prod. mechanism | |
340 | SetPARP(86,0.95); // Regulates gluon prod. mechanism | |
341 | SetPARP(89,1800.); // [GeV] Ref. energy | |
342 | SetPARP(90,0.25); // 2*epsilon (exponent in power law) | |
343 | break; | |
8d2cd130 | 344 | case kPyDirectGamma: |
345 | SetMSEL(10); | |
346 | break; | |
adf4d898 | 347 | case kPyCharmPbPbMNR: |
348 | case kPyD0PbPbMNR: | |
90d7b703 | 349 | case kPyDPlusPbPbMNR: |
e0e89f40 | 350 | case kPyDPlusStrangePbPbMNR: |
90d7b703 | 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 Pb-Pb 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. | |
3dc3ec94 | 358 | ConfigHeavyFlavor(); |
90d7b703 | 359 | // Intrinsic <kT> |
360 | SetMSTP(91,1); | |
361 | SetPARP(91,1.304); | |
362 | SetPARP(93,6.52); | |
90d7b703 | 363 | // Set c-quark mass |
364 | SetPMAS(4,1,1.2); | |
8d2cd130 | 365 | break; |
adf4d898 | 366 | case kPyCharmpPbMNR: |
367 | case kPyD0pPbMNR: | |
90d7b703 | 368 | case kPyDPluspPbMNR: |
e0e89f40 | 369 | case kPyDPlusStrangepPbMNR: |
90d7b703 | 370 | // Tuning of Pythia parameters aimed to get a resonable agreement |
371 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
372 | // c-cbar single inclusive and double differential distributions. | |
373 | // This parameter settings are meant to work with p-Pb collisions | |
374 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. | |
375 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) | |
376 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. | |
3dc3ec94 | 377 | ConfigHeavyFlavor(); |
90d7b703 | 378 | // Intrinsic <kT> |
3dc3ec94 | 379 | SetMSTP(91,1); |
380 | SetPARP(91,1.16); | |
381 | SetPARP(93,5.8); | |
382 | ||
90d7b703 | 383 | // Set c-quark mass |
3dc3ec94 | 384 | SetPMAS(4,1,1.2); |
adf4d898 | 385 | break; |
386 | case kPyCharmppMNR: | |
387 | case kPyD0ppMNR: | |
90d7b703 | 388 | case kPyDPlusppMNR: |
e0e89f40 | 389 | case kPyDPlusStrangeppMNR: |
90d7b703 | 390 | // Tuning of Pythia parameters aimed to get a resonable agreement |
391 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
392 | // c-cbar single inclusive and double differential distributions. | |
393 | // This parameter settings are meant to work with pp collisions | |
394 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. | |
395 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) | |
396 | // has to be set to 2.1GeV. Example in ConfigCharmPPR.C. | |
3dc3ec94 | 397 | ConfigHeavyFlavor(); |
90d7b703 | 398 | // Intrinsic <kT^2> |
3dc3ec94 | 399 | SetMSTP(91,1); |
400 | SetPARP(91,1.); | |
401 | SetPARP(93,5.); | |
402 | ||
90d7b703 | 403 | // Set c-quark mass |
3dc3ec94 | 404 | SetPMAS(4,1,1.2); |
adf4d898 | 405 | break; |
e0e89f40 | 406 | case kPyCharmppMNRwmi: |
407 | // Tuning of Pythia parameters aimed to get a resonable agreement | |
408 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
409 | // c-cbar single inclusive and double differential distributions. | |
410 | // This parameter settings are meant to work with pp collisions | |
411 | // and with kCTEQ5L PDFs. | |
412 | // Added multiple interactions according to ATLAS tune settings. | |
413 | // To get a "reasonable" agreement with MNR results, events have to be | |
414 | // generated with the minimum ptHard (AliGenPythia::SetPtHard) | |
415 | // set to 2.76 GeV. | |
416 | // To get a "perfect" agreement with MNR results, events have to be | |
417 | // generated in four ptHard bins with the following relative | |
418 | // normalizations: | |
419 | // 2.76-3 GeV: 25% | |
420 | // 3-4 GeV: 40% | |
421 | // 4-8 GeV: 29% | |
422 | // >8 GeV: 6% | |
423 | ConfigHeavyFlavor(); | |
424 | // Intrinsic <kT^2> | |
425 | SetMSTP(91,1); | |
426 | SetPARP(91,1.); | |
427 | SetPARP(93,5.); | |
428 | ||
429 | // Set c-quark mass | |
430 | SetPMAS(4,1,1.2); | |
431 | AtlasTuning(); | |
432 | break; | |
adf4d898 | 433 | case kPyBeautyPbPbMNR: |
8d2cd130 | 434 | // Tuning of Pythia parameters aimed to get a resonable agreement |
435 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
436 | // b-bbar single inclusive and double differential distributions. | |
437 | // This parameter settings are meant to work with Pb-Pb collisions | |
438 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. | |
439 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) | |
440 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. | |
3dc3ec94 | 441 | ConfigHeavyFlavor(); |
8d2cd130 | 442 | // QCD scales |
3dc3ec94 | 443 | SetPARP(67,1.0); |
444 | SetPARP(71,1.0); | |
adf4d898 | 445 | // Intrinsic <kT> |
3dc3ec94 | 446 | SetMSTP(91,1); |
447 | SetPARP(91,2.035); | |
448 | SetPARP(93,10.17); | |
8d2cd130 | 449 | // Set b-quark mass |
3dc3ec94 | 450 | SetPMAS(5,1,4.75); |
adf4d898 | 451 | break; |
452 | case kPyBeautypPbMNR: | |
453 | // Tuning of Pythia parameters aimed to get a resonable agreement | |
454 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
455 | // b-bbar single inclusive and double differential distributions. | |
456 | // This parameter settings are meant to work with p-Pb collisions | |
457 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. | |
458 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) | |
459 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. | |
3dc3ec94 | 460 | ConfigHeavyFlavor(); |
adf4d898 | 461 | // QCD scales |
3dc3ec94 | 462 | SetPARP(67,1.0); |
463 | SetPARP(71,1.0); | |
adf4d898 | 464 | // Intrinsic <kT> |
3dc3ec94 | 465 | SetMSTP(91,1); |
466 | SetPARP(91,1.60); | |
467 | SetPARP(93,8.00); | |
adf4d898 | 468 | // Set b-quark mass |
3dc3ec94 | 469 | SetPMAS(5,1,4.75); |
adf4d898 | 470 | break; |
471 | case kPyBeautyppMNR: | |
472 | // Tuning of Pythia parameters aimed to get a resonable agreement | |
473 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
474 | // b-bbar single inclusive and double differential distributions. | |
475 | // This parameter settings are meant to work with pp collisions | |
476 | // (AliGenPythia::SetNuclei) and with kCTEQ4L PDFs. | |
477 | // To get a good agreement the minimum ptHard (AliGenPythia::SetPtHard) | |
478 | // has to be set to 2.75GeV. Example in ConfigBeautyPPR.C. | |
3dc3ec94 | 479 | ConfigHeavyFlavor(); |
adf4d898 | 480 | // QCD scales |
3dc3ec94 | 481 | SetPARP(67,1.0); |
482 | SetPARP(71,1.0); | |
483 | ||
484 | // Intrinsic <kT> | |
485 | SetMSTP(91,1); | |
486 | SetPARP(91,1.); | |
487 | SetPARP(93,5.); | |
488 | ||
489 | // Set b-quark mass | |
490 | SetPMAS(5,1,4.75); | |
8d2cd130 | 491 | break; |
e0e89f40 | 492 | case kPyBeautyppMNRwmi: |
493 | // Tuning of Pythia parameters aimed to get a resonable agreement | |
494 | // between with the NLO calculation by Mangano, Nason, Ridolfi for the | |
495 | // b-bbar single inclusive and double differential distributions. | |
496 | // This parameter settings are meant to work with pp collisions | |
497 | // and with kCTEQ5L PDFs. | |
498 | // Added multiple interactions according to ATLAS tune settings. | |
499 | // To get a "reasonable" agreement with MNR results, events have to be | |
500 | // generated with the minimum ptHard (AliGenPythia::SetPtHard) | |
501 | // set to 2.76 GeV. | |
502 | // To get a "perfect" agreement with MNR results, events have to be | |
503 | // generated in four ptHard bins with the following relative | |
504 | // normalizations: | |
505 | // 2.76-4 GeV: 5% | |
506 | // 4-6 GeV: 31% | |
507 | // 6-8 GeV: 28% | |
508 | // >8 GeV: 36% | |
509 | ConfigHeavyFlavor(); | |
510 | // QCD scales | |
511 | SetPARP(67,1.0); | |
512 | SetPARP(71,1.0); | |
513 | ||
514 | // Intrinsic <kT> | |
515 | SetMSTP(91,1); | |
516 | SetPARP(91,1.); | |
517 | SetPARP(93,5.); | |
518 | ||
519 | // Set b-quark mass | |
520 | SetPMAS(5,1,4.75); | |
521 | ||
522 | AtlasTuning(); | |
523 | break; | |
589380c6 | 524 | case kPyW: |
525 | ||
526 | //Inclusive production of W+/- | |
527 | SetMSEL(0); | |
528 | //f fbar -> W+ | |
529 | SetMSUB(2,1); | |
530 | // //f fbar -> g W+ | |
531 | // SetMSUB(16,1); | |
532 | // //f fbar -> gamma W+ | |
533 | // SetMSUB(20,1); | |
534 | // //f g -> f W+ | |
535 | // SetMSUB(31,1); | |
536 | // //f gamma -> f W+ | |
537 | // SetMSUB(36,1); | |
538 | ||
539 | // Initial/final parton shower on (Pythia default) | |
540 | // With parton showers on we are generating "W inclusive process" | |
541 | SetMSTP(61,1); //Initial QCD & QED showers on | |
542 | SetMSTP(71,1); //Final QCD & QED showers on | |
543 | ||
544 | break; | |
0f6ee828 | 545 | |
546 | case kPyZ: | |
547 | ||
548 | //Inclusive production of Z | |
549 | SetMSEL(0); | |
550 | //f fbar -> Z/gamma | |
551 | SetMSUB(1,1); | |
552 | ||
553 | // // f fbar -> g Z/gamma | |
554 | // SetMSUB(15,1); | |
555 | // // f fbar -> gamma Z/gamma | |
556 | // SetMSUB(19,1); | |
557 | // // f g -> f Z/gamma | |
558 | // SetMSUB(30,1); | |
559 | // // f gamma -> f Z/gamma | |
560 | // SetMSUB(35,1); | |
561 | ||
562 | //only Z included, not gamma | |
563 | SetMSTP(43,2); | |
564 | ||
565 | // Initial/final parton shower on (Pythia default) | |
566 | // With parton showers on we are generating "Z inclusive process" | |
567 | SetMSTP(61,1); //Initial QCD & QED showers on | |
568 | SetMSTP(71,1); //Final QCD & QED showers on | |
569 | ||
570 | break; | |
571 | ||
8d2cd130 | 572 | } |
573 | // | |
574 | // Initialize PYTHIA | |
575 | SetMSTP(41,1); // all resonance decays switched on | |
8d2cd130 | 576 | Initialize("CMS","p","p",fEcms); |
4167b79f | 577 | |
8d2cd130 | 578 | } |
579 | ||
580 | Int_t AliPythia::CheckedLuComp(Int_t kf) | |
581 | { | |
582 | // Check Lund particle code (for debugging) | |
583 | Int_t kc=Pycomp(kf); | |
584 | printf("\n Lucomp kf,kc %d %d",kf,kc); | |
585 | return kc; | |
586 | } | |
587 | ||
20e47f08 | 588 | void AliPythia::SetNuclei(Int_t a1, Int_t a2, Int_t pdf) |
8d2cd130 | 589 | { |
590 | // Treat protons as inside nuclei with mass numbers a1 and a2 | |
591 | // The MSTP array in the PYPARS common block is used to enable and | |
592 | // select the nuclear structure functions. | |
593 | // MSTP(52) : (D=1) choice of proton and nuclear structure-function library | |
594 | // =1: internal PYTHIA acording to MSTP(51) | |
595 | // =2: PDFLIB proton s.f., with MSTP(51) = 1000xNGROUP+NSET | |
596 | // If the following mass number both not equal zero, nuclear corrections of the stf are used. | |
597 | // MSTP(192) : Mass number of nucleus side 1 | |
598 | // MSTP(193) : Mass number of nucleus side 2 | |
20e47f08 | 599 | // MSTP(194) : Nuclear structure function: 0: EKS98 1:EPS08 |
8d2cd130 | 600 | SetMSTP(52,2); |
601 | SetMSTP(192, a1); | |
20e47f08 | 602 | SetMSTP(193, a2); |
603 | SetMSTP(194, pdf); | |
8d2cd130 | 604 | } |
605 | ||
606 | ||
607 | AliPythia* AliPythia::Instance() | |
608 | { | |
609 | // Set random number generator | |
610 | if (fgAliPythia) { | |
611 | return fgAliPythia; | |
612 | } else { | |
613 | fgAliPythia = new AliPythia(); | |
614 | return fgAliPythia; | |
615 | } | |
616 | } | |
617 | ||
618 | void AliPythia::PrintParticles() | |
619 | { | |
620 | // Print list of particl properties | |
621 | Int_t np = 0; | |
c31f1d37 | 622 | char* name = new char[16]; |
8d2cd130 | 623 | for (Int_t kf=0; kf<1000000; kf++) { |
624 | for (Int_t c = 1; c > -2; c-=2) { | |
8d2cd130 | 625 | Int_t kc = Pycomp(c*kf); |
626 | if (kc) { | |
627 | Float_t mass = GetPMAS(kc,1); | |
628 | Float_t width = GetPMAS(kc,2); | |
629 | Float_t tau = GetPMAS(kc,4); | |
c31f1d37 | 630 | |
8d2cd130 | 631 | Pyname(kf,name); |
632 | ||
633 | np++; | |
634 | ||
635 | printf("\n mass, width, tau: %6d %s %10.3f %10.3e %10.3e", | |
636 | c*kf, name, mass, width, tau); | |
637 | } | |
638 | } | |
639 | } | |
640 | printf("\n Number of particles %d \n \n", np); | |
641 | } | |
642 | ||
643 | void AliPythia::ResetDecayTable() | |
644 | { | |
645 | // Set default values for pythia decay switches | |
646 | Int_t i; | |
647 | for (i = 1; i < 501; i++) SetMDCY(i,1,fDefMDCY[i]); | |
648 | for (i = 1; i < 2001; i++) SetMDME(i,1,fDefMDME[i]); | |
649 | } | |
650 | ||
651 | void AliPythia::SetDecayTable() | |
652 | { | |
653 | // Set default values for pythia decay switches | |
654 | // | |
655 | Int_t i; | |
656 | for (i = 1; i < 501; i++) fDefMDCY[i] = GetMDCY(i,1); | |
657 | for (i = 1; i < 2001; i++) fDefMDME[i] = GetMDME(i,1); | |
658 | } | |
659 | ||
660 | void AliPythia::Pyclus(Int_t& njet) | |
661 | { | |
662 | // Call Pythia clustering algorithm | |
663 | // | |
664 | pyclus(njet); | |
665 | } | |
666 | ||
667 | void AliPythia::Pycell(Int_t& njet) | |
668 | { | |
669 | // Call Pythia jet reconstruction algorithm | |
670 | // | |
671 | pycell(njet); | |
672 | } | |
673 | ||
452af8c7 | 674 | void AliPythia::Pyshow(Int_t ip1, Int_t ip2, Double_t qmax) |
675 | { | |
676 | // Call Pythia jet reconstruction algorithm | |
677 | // | |
452af8c7 | 678 | pyshow(ip1, ip2, qmax); |
679 | } | |
680 | ||
681 | void AliPythia::Pyrobo(Int_t imi, Int_t ima, Double_t the, Double_t phi, Double_t bex, Double_t bey, Double_t bez) | |
682 | { | |
683 | pyrobo(imi, ima, the, phi, bex, bey, bez); | |
684 | } | |
685 | ||
686 | ||
687 | ||
32c8e463 | 688 | void AliPythia::InitQuenching(Float_t cMin, Float_t cMax, Float_t k, Int_t iECMethod, Float_t zmax, Int_t ngmax) |
0f482ae4 | 689 | { |
690 | // Initializes | |
691 | // (1) The quenching model using quenching weights according to C. Salgado and U. Wiedemann | |
692 | // (2) The nuclear geometry using the Glauber Model | |
693 | // | |
6b435cde | 694 | |
18b7a4a1 | 695 | fGlauber = AliFastGlauber::Instance(); |
0f482ae4 | 696 | fGlauber->Init(2); |
697 | fGlauber->SetCentralityClass(cMin, cMax); | |
698 | ||
699 | fQuenchingWeights = new AliQuenchingWeights(); | |
700 | fQuenchingWeights->InitMult(); | |
86b6ad68 | 701 | fQuenchingWeights->SetK(k); |
0f482ae4 | 702 | fQuenchingWeights->SetECMethod(AliQuenchingWeights::kECMethod(iECMethod)); |
32c8e463 | 703 | fNGmax = ngmax; |
704 | fZmax = zmax; | |
705 | ||
0f482ae4 | 706 | } |
707 | ||
708 | ||
452af8c7 | 709 | void AliPythia::Quench() |
710 | { | |
711 | // | |
712 | // | |
713 | // Simple Jet Quenching routine: | |
714 | // ============================= | |
715 | // The jet formed by all final state partons radiated by the parton created | |
0f482ae4 | 716 | // in the hard collisions is quenched by a factor (1-z) using light cone variables in |
717 | // the initial parton reference frame: | |
452af8c7 | 718 | // (E + p_z)new = (1-z) (E + p_z)old |
719 | // | |
0f482ae4 | 720 | // |
721 | // | |
722 | // | |
452af8c7 | 723 | // The lost momentum is first balanced by one gluon with virtuality > 0. |
724 | // Subsequently the gluon splits to yield two gluons with E = p. | |
725 | // | |
0f482ae4 | 726 | // |
727 | // | |
4e383037 | 728 | static Float_t eMean = 0.; |
729 | static Int_t icall = 0; | |
0f482ae4 | 730 | |
c2c598a3 | 731 | Double_t p0[4][5]; |
732 | Double_t p1[4][5]; | |
733 | Double_t p2[4][5]; | |
734 | Int_t klast[4] = {-1, -1, -1, -1}; | |
452af8c7 | 735 | |
736 | Int_t numpart = fPyjets->N; | |
86b6ad68 | 737 | Double_t px = 0., py = 0., pz = 0., e = 0., m = 0., p = 0., pt = 0., theta = 0., phi = 0.; |
c2c598a3 | 738 | Double_t pxq[4], pyq[4], pzq[4], eq[4], yq[4], mq[4], pq[4], phiq[4], thetaq[4], ptq[4]; |
739 | Bool_t quenched[4]; | |
b280c4cc | 740 | Double_t wjtKick[4]; |
c2c598a3 | 741 | Int_t nGluon[4]; |
86b6ad68 | 742 | Int_t qPdg[4]; |
0f482ae4 | 743 | Int_t imo, kst, pdg; |
b280c4cc | 744 | |
511db649 | 745 | // |
c2c598a3 | 746 | // Sore information about Primary partons |
747 | // | |
748 | // j = | |
749 | // 0, 1 partons from hard scattering | |
750 | // 2, 3 partons from initial state radiation | |
751 | // | |
752 | for (Int_t i = 2; i <= 7; i++) { | |
753 | Int_t j = 0; | |
754 | // Skip gluons that participate in hard scattering | |
755 | if (i == 4 || i == 5) continue; | |
756 | // Gluons from hard Scattering | |
757 | if (i == 6 || i == 7) { | |
758 | j = i - 6; | |
759 | pxq[j] = fPyjets->P[0][i]; | |
760 | pyq[j] = fPyjets->P[1][i]; | |
761 | pzq[j] = fPyjets->P[2][i]; | |
762 | eq[j] = fPyjets->P[3][i]; | |
763 | mq[j] = fPyjets->P[4][i]; | |
764 | } else { | |
765 | // Gluons from initial state radiation | |
766 | // | |
767 | // Obtain 4-momentum vector from difference between original parton and parton after gluon | |
768 | // radiation. Energy is calculated independently because initial state radition does not | |
769 | // conserve strictly momentum and energy for each partonic system independently. | |
770 | // | |
771 | // Not very clean. Should be improved ! | |
772 | // | |
773 | // | |
774 | j = i; | |
775 | pxq[j] = fPyjets->P[0][i] - fPyjets->P[0][i+2]; | |
776 | pyq[j] = fPyjets->P[1][i] - fPyjets->P[1][i+2]; | |
777 | pzq[j] = fPyjets->P[2][i] - fPyjets->P[2][i+2]; | |
778 | mq[j] = fPyjets->P[4][i]; | |
779 | eq[j] = TMath::Sqrt(pxq[j] * pxq[j] + pyq[j] * pyq[j] + pzq[j] * pzq[j] + mq[j] * mq[j]); | |
780 | } | |
781 | // | |
782 | // Calculate some kinematic variables | |
511db649 | 783 | // |
4e383037 | 784 | yq[j] = 0.5 * TMath::Log((eq[j] + pzq[j] + 1.e-14) / (eq[j] - pzq[j] + 1.e-14)); |
0f482ae4 | 785 | pq[j] = TMath::Sqrt(pxq[j] * pxq[j] + pyq[j] * pyq[j] + pzq[j] * pzq[j]); |
786 | phiq[j] = TMath::Pi()+TMath::ATan2(-pyq[j], -pxq[j]); | |
787 | ptq[j] = TMath::Sqrt(pxq[j] * pxq[j] + pyq[j] * pyq[j]); | |
788 | thetaq[j] = TMath::ATan2(ptq[j], pzq[j]); | |
86b6ad68 | 789 | qPdg[j] = fPyjets->K[1][i]; |
790 | } | |
791 | ||
792 | Double_t int0[4]; | |
793 | Double_t int1[4]; | |
86b6ad68 | 794 | |
b280c4cc | 795 | fGlauber->GetI0I1ForPythiaAndXY(4, phiq, int0, int1, fXJet, fYJet, 15.); |
796 | ||
86b6ad68 | 797 | for (Int_t j = 0; j < 4; j++) { |
c2c598a3 | 798 | // |
799 | // Quench only central jets and with E > 10. | |
800 | // | |
86b6ad68 | 801 | |
802 | ||
803 | Int_t itype = (qPdg[j] == 21) ? 2 : 1; | |
804 | Double_t eloss = fQuenchingWeights->GetELossRandomKFast(itype, int0[j], int1[j], eq[j]); | |
805 | ||
c2c598a3 | 806 | if (TMath::Abs(yq[j]) > 2.5 || eq[j] < 10.) { |
b280c4cc | 807 | fZQuench[j] = 0.; |
0f482ae4 | 808 | } else { |
c2c598a3 | 809 | if (eq[j] > 40. && TMath::Abs(yq[j]) < 0.5) { |
4e383037 | 810 | icall ++; |
811 | eMean += eloss; | |
812 | } | |
0f482ae4 | 813 | // |
814 | // Extra pt | |
86b6ad68 | 815 | Double_t l = fQuenchingWeights->CalcLk(int0[j], int1[j]); |
816 | wjtKick[j] = TMath::Sqrt(l * fQuenchingWeights->CalcQk(int0[j], int1[j])); | |
0f482ae4 | 817 | // |
818 | // Fractional energy loss | |
b280c4cc | 819 | fZQuench[j] = eloss / eq[j]; |
0f482ae4 | 820 | // |
821 | // Avoid complete loss | |
822 | // | |
1044c4d8 | 823 | if (fZQuench[j] > fZmax) fZQuench[j] = fZmax; |
0f482ae4 | 824 | // |
825 | // Some debug printing | |
86b6ad68 | 826 | |
827 | ||
bf9bb016 | 828 | // 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", |
829 | // j, itype, eq[j], phiq[j], l, eloss, wjtKick[j], eMean / Float_t(icall+1), yq[j]); | |
4e383037 | 830 | |
b280c4cc | 831 | // fZQuench[j] = 0.8; |
832 | // while (fZQuench[j] >= 0.95) fZQuench[j] = gRandom->Exp(0.2); | |
0f482ae4 | 833 | } |
4e383037 | 834 | |
b280c4cc | 835 | quenched[j] = (fZQuench[j] > 0.01); |
4e383037 | 836 | } // primary partons |
c2c598a3 | 837 | |
b280c4cc | 838 | |
839 | ||
6e90ad26 | 840 | Double_t pNew[1000][4]; |
841 | Int_t kNew[1000]; | |
842 | Int_t icount = 0; | |
b280c4cc | 843 | Double_t zquench[4]; |
844 | ||
6e90ad26 | 845 | // |
4e383037 | 846 | // System Loop |
c2c598a3 | 847 | for (Int_t isys = 0; isys < 4; isys++) { |
6e90ad26 | 848 | // Skip to next system if not quenched. |
4e383037 | 849 | if (!quenched[isys]) continue; |
850 | ||
b280c4cc | 851 | nGluon[isys] = 1 + Int_t(fZQuench[isys] / (1. - fZQuench[isys])); |
32c8e463 | 852 | if (nGluon[isys] > fNGmax) nGluon[isys] = fNGmax; |
b280c4cc | 853 | zquench[isys] = 1. - TMath::Power(1. - fZQuench[isys], 1./Double_t(nGluon[isys])); |
4e383037 | 854 | wjtKick[isys] = wjtKick[isys] / TMath::Sqrt(Double_t(nGluon[isys])); |
0f482ae4 | 855 | |
4e383037 | 856 | |
857 | ||
858 | Int_t igMin = -1; | |
859 | Int_t igMax = -1; | |
860 | Double_t pg[4] = {0., 0., 0., 0.}; | |
861 | ||
862 | // | |
863 | // Loop on radiation events | |
864 | ||
865 | for (Int_t iglu = 0; iglu < nGluon[isys]; iglu++) { | |
6e90ad26 | 866 | while (1) { |
867 | icount = 0; | |
868 | for (Int_t k = 0; k < 4; k++) | |
869 | { | |
870 | p0[isys][k] = 0.; | |
871 | p1[isys][k] = 0.; | |
872 | p2[isys][k] = 0.; | |
873 | } | |
874 | // Loop over partons | |
875 | for (Int_t i = 0; i < numpart; i++) | |
876 | { | |
877 | imo = fPyjets->K[2][i]; | |
878 | kst = fPyjets->K[0][i]; | |
879 | pdg = fPyjets->K[1][i]; | |
880 | ||
881 | ||
882 | ||
0f482ae4 | 883 | // Quarks and gluons only |
6e90ad26 | 884 | if (pdg != 21 && TMath::Abs(pdg) > 6) continue; |
0f482ae4 | 885 | // Particles from hard scattering only |
c2c598a3 | 886 | |
6e90ad26 | 887 | if (imo > 8 && imo < 1000) imo = fPyjets->K[2][imo - 1]; |
c2c598a3 | 888 | Int_t imom = imo % 1000; |
889 | if ((isys == 0 || isys == 1) && ((imom != (isys + 7)))) continue; | |
890 | if ((isys == 2 || isys == 3) && ((imom != (isys + 1)))) continue; | |
891 | ||
6e90ad26 | 892 | |
0f482ae4 | 893 | // Skip comment lines |
6e90ad26 | 894 | if (kst != 1 && kst != 2) continue; |
0f482ae4 | 895 | // |
896 | // Parton kinematic | |
6e90ad26 | 897 | px = fPyjets->P[0][i]; |
898 | py = fPyjets->P[1][i]; | |
899 | pz = fPyjets->P[2][i]; | |
900 | e = fPyjets->P[3][i]; | |
901 | m = fPyjets->P[4][i]; | |
902 | pt = TMath::Sqrt(px * px + py * py); | |
903 | p = TMath::Sqrt(px * px + py * py + pz * pz); | |
904 | phi = TMath::Pi() + TMath::ATan2(-py, -px); | |
905 | theta = TMath::ATan2(pt, pz); | |
906 | ||
0f482ae4 | 907 | // |
c2c598a3 | 908 | // Save 4-momentum sum for balancing |
909 | Int_t index = isys; | |
6e90ad26 | 910 | |
911 | p0[index][0] += px; | |
912 | p0[index][1] += py; | |
913 | p0[index][2] += pz; | |
914 | p0[index][3] += e; | |
6e90ad26 | 915 | |
916 | klast[index] = i; | |
917 | ||
0f482ae4 | 918 | // |
919 | // Fractional energy loss | |
b280c4cc | 920 | Double_t z = zquench[index]; |
4e383037 | 921 | |
c2c598a3 | 922 | |
4e383037 | 923 | // Don't fully quench radiated gluons |
924 | // | |
925 | if (imo > 1000) { | |
926 | // This small factor makes sure that the gluons are not too close in phase space to avoid recombination | |
927 | // | |
928 | ||
c2c598a3 | 929 | z = 0.02; |
4e383037 | 930 | } |
c2c598a3 | 931 | // printf("z: %d %f\n", imo, z); |
932 | ||
4e383037 | 933 | |
934 | // | |
6e90ad26 | 935 | |
936 | // | |
937 | // | |
938 | // Transform into frame in which initial parton is along z-axis | |
939 | // | |
940 | TVector3 v(px, py, pz); | |
941 | v.RotateZ(-phiq[index]); v.RotateY(-thetaq[index]); | |
942 | Double_t pxs = v.X(); Double_t pys = v.Y(); Double_t pl = v.Z(); | |
943 | ||
944 | Double_t jt = TMath::Sqrt(pxs * pxs + pys * pys); | |
945 | Double_t mt2 = jt * jt + m * m; | |
946 | Double_t zmax = 1.; | |
947 | // | |
948 | // Kinematic limit on z | |
949 | // | |
4e383037 | 950 | if (m > 0.) zmax = 1. - m / TMath::Sqrt(m * m + jt * jt); |
6e90ad26 | 951 | // |
952 | // Change light-cone kinematics rel. to initial parton | |
953 | // | |
954 | Double_t eppzOld = e + pl; | |
955 | Double_t empzOld = e - pl; | |
956 | ||
957 | Double_t eppzNew = (1. - z) * eppzOld; | |
958 | Double_t empzNew = empzOld - mt2 * z / eppzOld; | |
959 | Double_t eNew = 0.5 * (eppzNew + empzNew); | |
960 | Double_t plNew = 0.5 * (eppzNew - empzNew); | |
961 | ||
962 | Double_t jtNew; | |
963 | // | |
964 | // if mt very small (or sometimes even < 0 for numerical reasons) set it to 0 | |
965 | Double_t mt2New = eppzNew * empzNew; | |
966 | if (mt2New < 1.e-8) mt2New = 0.; | |
4e383037 | 967 | if (z < zmax) { |
968 | if (m * m > mt2New) { | |
969 | // | |
970 | // This should not happen | |
971 | // | |
972 | Fatal("Quench()", "This should never happen %e %e %e!", m, eppzNew, empzNew); | |
973 | jtNew = 0; | |
974 | } else { | |
975 | jtNew = TMath::Sqrt(mt2New - m * m); | |
976 | } | |
6e90ad26 | 977 | } else { |
4e383037 | 978 | // If pT is to small (probably a leading massive particle) we scale only the energy |
979 | // This can cause negative masses of the radiated gluon | |
980 | // Let's hope for the best ... | |
981 | jtNew = jt; | |
982 | eNew = TMath::Sqrt(plNew * plNew + mt2); | |
983 | ||
6e90ad26 | 984 | } |
6e90ad26 | 985 | // |
986 | // Calculate new px, py | |
987 | // | |
b07be423 | 988 | Double_t pxNew = 0; |
989 | Double_t pyNew = 0; | |
6e90ad26 | 990 | |
b07be423 | 991 | if (jt>0) { |
6b118b3c | 992 | pxNew = jtNew / jt * pxs; |
993 | pyNew = jtNew / jt * pys; | |
b07be423 | 994 | } |
6e90ad26 | 995 | // Double_t dpx = pxs - pxNew; |
996 | // Double_t dpy = pys - pyNew; | |
997 | // Double_t dpz = pl - plNew; | |
998 | // Double_t de = e - eNew; | |
999 | // Double_t dmass2 = de * de - dpx * dpx - dpy * dpy - dpz * dpz; | |
1000 | // printf("New mass (1) %e %e %e %e %e %e %e \n", dmass2, jt, jtNew, pl, plNew, e, eNew); | |
1001 | // printf("New mass (2) %e %e \n", pxNew, pyNew); | |
1002 | // | |
1003 | // Rotate back | |
1004 | // | |
1005 | TVector3 w(pxNew, pyNew, plNew); | |
1006 | w.RotateY(thetaq[index]); w.RotateZ(phiq[index]); | |
1007 | pxNew = w.X(); pyNew = w.Y(); plNew = w.Z(); | |
1008 | ||
1009 | p1[index][0] += pxNew; | |
1010 | p1[index][1] += pyNew; | |
1011 | p1[index][2] += plNew; | |
1012 | p1[index][3] += eNew; | |
1013 | // | |
1014 | // Updated 4-momentum vectors | |
1015 | // | |
1016 | pNew[icount][0] = pxNew; | |
1017 | pNew[icount][1] = pyNew; | |
1018 | pNew[icount][2] = plNew; | |
1019 | pNew[icount][3] = eNew; | |
1020 | kNew[icount] = i; | |
1021 | icount++; | |
1022 | } // parton loop | |
0f482ae4 | 1023 | // |
6e90ad26 | 1024 | // Check if there was phase-space for quenching |
0f482ae4 | 1025 | // |
0f482ae4 | 1026 | |
6e90ad26 | 1027 | if (icount == 0) quenched[isys] = kFALSE; |
1028 | if (!quenched[isys]) break; | |
1029 | ||
1030 | for (Int_t j = 0; j < 4; j++) | |
1031 | { | |
1032 | p2[isys][j] = p0[isys][j] - p1[isys][j]; | |
1033 | } | |
1034 | 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 | 1035 | if (p2[isys][4] > 0.) { |
1036 | p2[isys][4] = TMath::Sqrt(p2[isys][4]); | |
1037 | break; | |
1038 | } else { | |
b280c4cc | 1039 | printf("Warning negative mass squared in system %d %f ! \n", isys, zquench[isys]); |
4e383037 | 1040 | 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 | 1041 | if (p2[isys][4] < -0.01) { |
4e383037 | 1042 | printf("Negative mass squared !\n"); |
1043 | // Here we have to put the gluon back to mass shell | |
1044 | // This will lead to a small energy imbalance | |
1045 | p2[isys][4] = 0.; | |
1046 | p2[isys][3] = TMath::Sqrt(p2[isys][0] * p2[isys][0] + p2[isys][1] * p2[isys][1] + p2[isys][2] * p2[isys][2]); | |
1047 | break; | |
6e90ad26 | 1048 | } else { |
1049 | p2[isys][4] = 0.; | |
1050 | break; | |
1051 | } | |
1052 | } | |
6e90ad26 | 1053 | /* |
6e90ad26 | 1054 | zHeavy *= 0.98; |
1055 | printf("zHeavy lowered to %f\n", zHeavy); | |
1056 | if (zHeavy < 0.01) { | |
1057 | printf("No success ! \n"); | |
1058 | icount = 0; | |
1059 | quenched[isys] = kFALSE; | |
1060 | break; | |
1061 | } | |
4e383037 | 1062 | */ |
1063 | } // iteration on z (while) | |
1064 | ||
6e90ad26 | 1065 | // Update event record |
1066 | for (Int_t k = 0; k < icount; k++) { | |
1067 | // 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] ); | |
1068 | fPyjets->P[0][kNew[k]] = pNew[k][0]; | |
1069 | fPyjets->P[1][kNew[k]] = pNew[k][1]; | |
1070 | fPyjets->P[2][kNew[k]] = pNew[k][2]; | |
1071 | fPyjets->P[3][kNew[k]] = pNew[k][3]; | |
0f482ae4 | 1072 | } |
4e383037 | 1073 | // |
1074 | // Add the gluons | |
1075 | // | |
1076 | Int_t ish = 0; | |
1837e95c | 1077 | Int_t iGlu; |
4e383037 | 1078 | if (!quenched[isys]) continue; |
0f482ae4 | 1079 | // |
1080 | // Last parton from shower i | |
4e383037 | 1081 | Int_t in = klast[isys]; |
0f482ae4 | 1082 | // |
1083 | // Continue if no parton in shower i selected | |
1084 | if (in == -1) continue; | |
1085 | // | |
1086 | // If this is the second initial parton and it is behind the first move pointer by previous ish | |
4e383037 | 1087 | if (isys == 1 && klast[1] > klast[0]) in += ish; |
0f482ae4 | 1088 | // |
1089 | // Starting index | |
452af8c7 | 1090 | |
4e383037 | 1091 | // jmin = in - 1; |
0f482ae4 | 1092 | // How many additional gluons will be generated |
1093 | ish = 1; | |
4e383037 | 1094 | if (p2[isys][4] > 0.05) ish = 2; |
0f482ae4 | 1095 | // |
1096 | // Position of gluons | |
4e383037 | 1097 | iGlu = numpart; |
1098 | if (iglu == 0) igMin = iGlu; | |
1099 | igMax = iGlu; | |
0f482ae4 | 1100 | numpart += ish; |
1101 | (fPyjets->N) += ish; | |
4e383037 | 1102 | |
0f482ae4 | 1103 | if (ish == 1) { |
4e383037 | 1104 | fPyjets->P[0][iGlu] = p2[isys][0]; |
1105 | fPyjets->P[1][iGlu] = p2[isys][1]; | |
1106 | fPyjets->P[2][iGlu] = p2[isys][2]; | |
1107 | fPyjets->P[3][iGlu] = p2[isys][3]; | |
1108 | fPyjets->P[4][iGlu] = p2[isys][4]; | |
0f482ae4 | 1109 | |
4e383037 | 1110 | fPyjets->K[0][iGlu] = 1; |
1111 | if (iglu == nGluon[isys] - 1) fPyjets->K[0][iGlu] = 1; | |
0f482ae4 | 1112 | fPyjets->K[1][iGlu] = 21; |
4e383037 | 1113 | fPyjets->K[2][iGlu] = fPyjets->K[2][in] + 1000; |
0f482ae4 | 1114 | fPyjets->K[3][iGlu] = -1; |
1115 | fPyjets->K[4][iGlu] = -1; | |
4e383037 | 1116 | |
1117 | pg[0] += p2[isys][0]; | |
1118 | pg[1] += p2[isys][1]; | |
1119 | pg[2] += p2[isys][2]; | |
1120 | pg[3] += p2[isys][3]; | |
0f482ae4 | 1121 | } else { |
1122 | // | |
1123 | // Split gluon in rest frame. | |
1124 | // | |
4e383037 | 1125 | Double_t bx = p2[isys][0] / p2[isys][3]; |
1126 | Double_t by = p2[isys][1] / p2[isys][3]; | |
1127 | Double_t bz = p2[isys][2] / p2[isys][3]; | |
1128 | Double_t pst = p2[isys][4] / 2.; | |
0f482ae4 | 1129 | // |
1130 | // Isotropic decay ???? | |
1131 | Double_t cost = 2. * gRandom->Rndm() - 1.; | |
60e55aee | 1132 | Double_t sint = TMath::Sqrt((1.-cost)*(1.+cost)); |
2ab330c9 | 1133 | Double_t phis = 2. * TMath::Pi() * gRandom->Rndm(); |
0f482ae4 | 1134 | |
1135 | Double_t pz1 = pst * cost; | |
1136 | Double_t pz2 = -pst * cost; | |
1137 | Double_t pt1 = pst * sint; | |
1138 | Double_t pt2 = -pst * sint; | |
2ab330c9 | 1139 | Double_t px1 = pt1 * TMath::Cos(phis); |
1140 | Double_t py1 = pt1 * TMath::Sin(phis); | |
1141 | Double_t px2 = pt2 * TMath::Cos(phis); | |
1142 | Double_t py2 = pt2 * TMath::Sin(phis); | |
0f482ae4 | 1143 | |
1144 | fPyjets->P[0][iGlu] = px1; | |
1145 | fPyjets->P[1][iGlu] = py1; | |
1146 | fPyjets->P[2][iGlu] = pz1; | |
1147 | fPyjets->P[3][iGlu] = pst; | |
1148 | fPyjets->P[4][iGlu] = 0.; | |
1149 | ||
4e383037 | 1150 | fPyjets->K[0][iGlu] = 1 ; |
0f482ae4 | 1151 | fPyjets->K[1][iGlu] = 21; |
4e383037 | 1152 | fPyjets->K[2][iGlu] = fPyjets->K[2][in] + 1000; |
0f482ae4 | 1153 | fPyjets->K[3][iGlu] = -1; |
1154 | fPyjets->K[4][iGlu] = -1; | |
1155 | ||
1156 | fPyjets->P[0][iGlu+1] = px2; | |
1157 | fPyjets->P[1][iGlu+1] = py2; | |
1158 | fPyjets->P[2][iGlu+1] = pz2; | |
1159 | fPyjets->P[3][iGlu+1] = pst; | |
1160 | fPyjets->P[4][iGlu+1] = 0.; | |
1161 | ||
4e383037 | 1162 | fPyjets->K[0][iGlu+1] = 1; |
1163 | if (iglu == nGluon[isys] - 1) fPyjets->K[0][iGlu+1] = 1; | |
0f482ae4 | 1164 | fPyjets->K[1][iGlu+1] = 21; |
4e383037 | 1165 | fPyjets->K[2][iGlu+1] = fPyjets->K[2][in] + 1000; |
0f482ae4 | 1166 | fPyjets->K[3][iGlu+1] = -1; |
1167 | fPyjets->K[4][iGlu+1] = -1; | |
1168 | SetMSTU(1,0); | |
1169 | SetMSTU(2,0); | |
1170 | // | |
1171 | // Boost back | |
1172 | // | |
1173 | Pyrobo(iGlu + 1, iGlu + 2, 0., 0., bx, by, bz); | |
1174 | } | |
4e383037 | 1175 | /* |
1176 | for (Int_t ig = iGlu; ig < iGlu+ish; ig++) { | |
1177 | Double_t px, py, pz; | |
1178 | px = fPyjets->P[0][ig]; | |
1179 | py = fPyjets->P[1][ig]; | |
1180 | pz = fPyjets->P[2][ig]; | |
1181 | TVector3 v(px, py, pz); | |
1182 | v.RotateZ(-phiq[isys]); | |
1183 | v.RotateY(-thetaq[isys]); | |
1184 | Double_t pxs = v.X(); Double_t pys = v.Y(); Double_t pzs = v.Z(); | |
1185 | Double_t r = AliPythiaRndm::GetPythiaRandom()->Rndm(); | |
1186 | Double_t jtKick = 0.3 * TMath::Sqrt(-TMath::Log(r)); | |
1187 | if (ish == 2) jtKick = wjtKick[i] * TMath::Sqrt(-TMath::Log(r)) / TMath::Sqrt(2.); | |
1188 | Double_t phiKick = 2. * TMath::Pi() * AliPythiaRndm::GetPythiaRandom()->Rndm(); | |
1189 | pxs += jtKick * TMath::Cos(phiKick); | |
1190 | pys += jtKick * TMath::Sin(phiKick); | |
1191 | TVector3 w(pxs, pys, pzs); | |
1192 | w.RotateY(thetaq[isys]); | |
1193 | w.RotateZ(phiq[isys]); | |
1194 | fPyjets->P[0][ig] = w.X(); | |
1195 | fPyjets->P[1][ig] = w.Y(); | |
1196 | fPyjets->P[2][ig] = w.Z(); | |
1197 | fPyjets->P[2][ig] = w.Mag(); | |
1198 | } | |
1199 | */ | |
1200 | } // kGluon | |
1201 | ||
6e90ad26 | 1202 | |
4e383037 | 1203 | // Check energy conservation |
0f482ae4 | 1204 | Double_t pxs = 0.; |
1205 | Double_t pys = 0.; | |
1206 | Double_t pzs = 0.; | |
1207 | Double_t es = 14000.; | |
1208 | ||
1209 | for (Int_t i = 0; i < numpart; i++) | |
1210 | { | |
1211 | kst = fPyjets->K[0][i]; | |
1212 | if (kst != 1 && kst != 2) continue; | |
1213 | pxs += fPyjets->P[0][i]; | |
1214 | pys += fPyjets->P[1][i]; | |
1215 | pzs += fPyjets->P[2][i]; | |
1216 | es -= fPyjets->P[3][i]; | |
1217 | } | |
1218 | if (TMath::Abs(pxs) > 1.e-2 || | |
1219 | TMath::Abs(pys) > 1.e-2 || | |
1220 | TMath::Abs(pzs) > 1.e-1) { | |
1221 | printf("%e %e %e %e\n", pxs, pys, pzs, es); | |
4e383037 | 1222 | // Fatal("Quench()", "4-Momentum non-conservation"); |
452af8c7 | 1223 | } |
4e383037 | 1224 | |
1225 | } // end quenching loop (systems) | |
6e90ad26 | 1226 | // Clean-up |
0f482ae4 | 1227 | for (Int_t i = 0; i < numpart; i++) |
1228 | { | |
4e383037 | 1229 | imo = fPyjets->K[2][i]; |
1230 | if (imo > 1000) { | |
1231 | fPyjets->K[2][i] = fPyjets->K[2][i] % 1000; | |
1232 | } | |
0f482ae4 | 1233 | } |
4e383037 | 1234 | // this->Pylist(1); |
0f482ae4 | 1235 | } // end quench |
90d7b703 | 1236 | |
992f2843 | 1237 | |
1238 | void AliPythia::Pyquen(Double_t a, Int_t ibf, Double_t b) | |
1239 | { | |
1240 | // Igor Lokthine's quenching routine | |
12cb0bc0 | 1241 | // http://lokhtin.web.cern.ch/lokhtin/pyquen/pyquen.txt |
1242 | ||
992f2843 | 1243 | pyquen(a, ibf, b); |
1244 | } | |
b280c4cc | 1245 | |
12cb0bc0 | 1246 | void AliPythia::SetPyquenParameters(Double_t t0, Double_t tau0, Int_t nf, Int_t iengl, Int_t iangl) |
1247 | { | |
1248 | // Set the parameters for the PYQUEN package. | |
1249 | // See comments in PyquenCommon.h | |
1250 | ||
1251 | ||
1252 | PYQPAR.t0 = t0; | |
1253 | PYQPAR.tau0 = tau0; | |
1254 | PYQPAR.nf = nf; | |
1255 | PYQPAR.iengl = iengl; | |
1256 | PYQPAR.iangl = iangl; | |
1257 | } | |
1258 | ||
1259 | ||
16a82508 | 1260 | void AliPythia::Pyevnw() |
1261 | { | |
1262 | // New multiple interaction scenario | |
1263 | pyevnw(); | |
1264 | } | |
1265 | ||
b280c4cc | 1266 | void AliPythia::GetQuenchingParameters(Double_t& xp, Double_t& yp, Double_t z[4]) |
1267 | { | |
1268 | // Return event specific quenching parameters | |
1269 | xp = fXJet; | |
1270 | yp = fYJet; | |
1271 | for (Int_t i = 0; i < 4; i++) z[i] = fZQuench[i]; | |
1272 | ||
1273 | } | |
1274 | ||
3dc3ec94 | 1275 | void AliPythia::ConfigHeavyFlavor() |
1276 | { | |
1277 | // | |
1278 | // Default configuration for Heavy Flavor production | |
1279 | // | |
1280 | // All QCD processes | |
1281 | // | |
1282 | SetMSEL(1); | |
1283 | ||
1284 | // No multiple interactions | |
1285 | SetMSTP(81,0); | |
39c2e610 | 1286 | SetPARP(81, 0.); |
1287 | SetPARP(82, 0.); | |
3dc3ec94 | 1288 | // Initial/final parton shower on (Pythia default) |
1289 | SetMSTP(61,1); | |
1290 | SetMSTP(71,1); | |
1291 | ||
1292 | // 2nd order alpha_s | |
1293 | SetMSTP(2,2); | |
1294 | ||
1295 | // QCD scales | |
1296 | SetMSTP(32,2); | |
1297 | SetPARP(34,1.0); | |
1298 | } | |
e0e89f40 | 1299 | |
1300 | void AliPythia::AtlasTuning() | |
1301 | { | |
1302 | // | |
1303 | // Configuration for the ATLAS tuning | |
e2de0ce1 | 1304 | SetMSTP(51, AliStructFuncType::PDFsetIndex(kCTEQ5L)); // CTEQ5L pdf |
e0e89f40 | 1305 | SetMSTP(81,1); // Multiple Interactions ON |
1306 | SetMSTP(82,4); // Double Gaussian Model | |
39c2e610 | 1307 | SetPARP(81,1.9); // Min. pt for multiple interactions (default in 6.2-14) |
e0e89f40 | 1308 | SetPARP(82,1.8); // [GeV] PT_min at Ref. energy |
1309 | SetPARP(89,1000.); // [GeV] Ref. energy | |
1310 | SetPARP(90,0.16); // 2*epsilon (exponent in power law) | |
1311 | SetPARP(83,0.5); // Core density in proton matter distribution (def.value) | |
1312 | SetPARP(84,0.5); // Core radius | |
1313 | SetPARP(85,0.33); // Regulates gluon prod. mechanism | |
1314 | SetPARP(86,0.66); // Regulates gluon prod. mechanism | |
1315 | SetPARP(67,1); // Regulates Initial State Radiation | |
1316 | } | |
e8a8adcd | 1317 | |
1318 | AliPythia& AliPythia::operator=(const AliPythia& rhs) | |
1319 | { | |
1320 | // Assignment operator | |
1321 | rhs.Copy(*this); | |
1322 | return *this; | |
1323 | } | |
1324 | ||
1325 | void AliPythia::Copy(TObject&) const | |
1326 | { | |
1327 | // | |
1328 | // Copy | |
1329 | // | |
1330 | Fatal("Copy","Not implemented!\n"); | |
1331 | } |