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2c890605 | 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 | ||
16 | /* $Id$ */ | |
17 | ||
18 | // Class to generate correlated Heavy Flavor hadron pairs (one or several pairs | |
19 | // per event) using paramtrized kinematics of quark pairs from some generator | |
20 | // and quark fragmentation functions. | |
21 | // Is a generalisation of AliGenParam class for correlated pairs of hadrons. | |
22 | // In this version quark pairs and fragmentation functions are obtained from | |
b44c3901 | 23 | // Pythia6.124 using 100K events generated with kCharmppMNRwmi&kBeautyppMNRwmi |
2c890605 | 24 | // in pp collisions at 14 TeV. |
25 | // Decays are performed by Pythia. Used AliRoot version: v4-04-Release | |
26 | // Author: S. Grigoryan, LPC Clermont-Fd & YerPhI, Smbat.Grigoryan@cern.ch | |
b44c3901 | 27 | // July 07: added quarks in the stack (B. Vulpescu) |
2c890605 | 28 | //------------------------------------------------------------------------- |
29 | // How it works (for the given flavor): | |
30 | // | |
31 | // 1) Reads QQbar kinematical grid from the Input file and generates | |
32 | // quark pairs according to the weights of the cells. | |
33 | // It is a 5D grid in y1,y2,pt1,pt2 and deltaphi, with occupancy weights | |
34 | // of the cells obtained from Pythia (see details in GetQuarkPair). | |
35 | // 2) Reads "soft" and "hard" fragmentation functions (12 2D-histograms each, | |
36 | // for 12 pt bins) from the Input file, applies to quarks and produces hadrons | |
37 | // (only lower states, with proportions of species obtained from Pythia). | |
38 | // Fragmentation functions are the same for all hadron species and depend | |
39 | // on 2 variables - light cone energy-momentum fractions: | |
40 | // z1=(E_H + Pz_H)/(E_Q + Pz_Q), z2=(E_H - Pz_H)/(E_Q - Pz_Q). | |
41 | // "soft" & "hard" FFs correspond to "slower" & "faster" quark of a pair | |
42 | // (see details in GetHadronPair). | |
43 | // 3) Decays the hadrons and saves all the particles in the event stack in the | |
44 | // following order: HF hadron from Q, then its decay products, then HF hadron | |
45 | // from Qbar, then its decay productes, then next HF hadon pair (if any) | |
46 | // in the same way, etc... | |
47 | // 4) It is fast, e.g., generates the same number of events with a beauty pair | |
48 | // ~15 times faster than AliGenPythia with kBeautyppMNRwmi (w/o tracking) | |
49 | // | |
50 | // An Input file for each quark flavor is included in EVGEN/dataCorrHF/ | |
51 | // One can use also user-defined Input files. | |
52 | // | |
53 | // More details could be found in my presentation at DiMuonNet Workshop, Dec 2006: | |
54 | // http://www-dapnia.cea.fr/Sphn/Alice/DiMuonNet | |
55 | // and will be published in an Internal Note. | |
56 | // | |
57 | //------------------------------------------------------------------------- | |
58 | // How to use it: | |
59 | // | |
60 | // add the following typical lines in Config.C | |
61 | /* | |
62 | if (!strcmp(option,"corr")) { | |
63 | // Example for correlated charm or beauty hadron pair production | |
64 | ||
65 | // AliGenCorrHF *gener = new AliGenCorrHF(1, 4); // for charm, 1 pair per event | |
66 | AliGenCorrHF *gener = new AliGenCorrHF(1, 5); // for beauty, 1 pair per event | |
67 | ||
68 | gener->SetMomentumRange(0,9999); | |
69 | gener->SetCutOnChild(0); // 1/0 means cuts on children enable/disable | |
70 | gener->SetChildThetaRange(171.0,178.0); | |
71 | gener->SetOrigin(0,0,0); //vertex position | |
72 | gener->SetSigma(0,0,0); //Sigma in (X,Y,Z) (cm) on IP position | |
73 | gener->SetForceDecay(kSemiMuonic); | |
74 | gener->SetTrackingFlag(0); | |
75 | gener->Init(); | |
76 | } | |
77 | */ | |
78 | // and in aliroot do e.g. gAlice->Run(10,"Config.C") to produce 10 events. | |
79 | // One can include AliGenCorrHF in an AliGenCocktail generator. | |
80 | //-------------------------------------------------------------------------- | |
81 | ||
7ca4655f | 82 | #include <Riostream.h> |
83 | #include <TCanvas.h> | |
84 | #include <TClonesArray.h> | |
85 | #include <TDatabasePDG.h> | |
2c890605 | 86 | #include <TFile.h> |
2c890605 | 87 | #include <TH2F.h> |
2c890605 | 88 | #include <TLorentzVector.h> |
7ca4655f | 89 | #include <TMath.h> |
2c890605 | 90 | #include <TParticle.h> |
91 | #include <TParticlePDG.h> | |
7ca4655f | 92 | #include <TROOT.h> |
93 | #include <TRandom.h> | |
94 | #include <TTree.h> | |
2c890605 | 95 | #include <TVirtualMC.h> |
b44c3901 | 96 | #include <TVector3.h> |
2c890605 | 97 | |
98 | #include "AliGenCorrHF.h" | |
99 | #include "AliLog.h" | |
100 | #include "AliConst.h" | |
101 | #include "AliDecayer.h" | |
102 | #include "AliMC.h" | |
103 | #include "AliRun.h" | |
84555c93 | 104 | #include "AliGenEventHeader.h" |
2c890605 | 105 | |
106 | ClassImp(AliGenCorrHF) | |
107 | ||
108 | //Begin_Html | |
109 | /* | |
110 | <img src="picts/AliGenCorrHF.gif"> | |
111 | */ | |
112 | //End_Html | |
113 | ||
114 | Double_t AliGenCorrHF::fgdph[19] = {0, 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 160, 170, 180}; | |
115 | Double_t AliGenCorrHF::fgy[31] = {-10,-7, -6.5, -6, -5.5, -5, -4.5, -4, -3.5, -3, -2.5, -2,- 1.5, -1, -0.5, 0, 0.5, 1, 1.5, 2, 2.5, 3, 3.5, 4, 4.5, 5, 5.5, 6, 6.5, 7, 10}; | |
116 | Double_t AliGenCorrHF::fgpt[33] = {0, 0.5, 1, 1.5, 2, 2.5, 3, 3.5, 4, 4.5, 5, 5.5, 6, 6.6, 7.2, 7.8, 8.4, 9, 9.6, 10.3, 11.1, 12, 13.1, 14.3, 15.6, 17.1, 19, 21, 24, 28, 35, 50, 100}; | |
117 | Int_t AliGenCorrHF::fgnptbins = 12; | |
118 | Double_t AliGenCorrHF::fgptbmin[12] = {0, 0.5, 1, 1.5, 2, 2.5, 3, 4, 5, 6, 7, 9}; | |
119 | Double_t AliGenCorrHF::fgptbmax[12] = {0.5, 1, 1.5, 2, 2.5, 3, 4, 5, 6, 7, 9, 100}; | |
120 | ||
121 | Double_t* AliGenCorrHF::fgIntegral = 0; | |
122 | ||
123 | //____________________________________________________________ | |
124 | AliGenCorrHF::AliGenCorrHF(): | |
125 | fFileName(0), | |
126 | fFile(0), | |
127 | fQuark(0), | |
128 | fBias(0.), | |
129 | fTrials(0), | |
130 | fDecayer(0) | |
131 | { | |
132 | // Default constructor | |
133 | } | |
134 | ||
135 | //____________________________________________________________ | |
136 | AliGenCorrHF::AliGenCorrHF(Int_t npart, Int_t param): | |
137 | AliGenMC(npart), | |
138 | fFileName(0), | |
139 | fFile(0), | |
140 | fQuark(param), | |
141 | fBias(0.), | |
142 | fTrials(0), | |
143 | // fDecayer(new AliDecayerPythia()) | |
144 | fDecayer(0) | |
145 | { | |
146 | // Constructor using number of particles, quark type & default InputFile | |
147 | // | |
148 | if (fQuark != 5) fQuark = 4; | |
149 | fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmppMNRwmiCorr100K.root"; | |
150 | if (fQuark == 5) fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyppMNRwmiCorr100K.root"; | |
151 | ||
152 | fName = "Default"; | |
153 | fTitle= "Generator for correlated pairs of HF hadrons"; | |
154 | ||
155 | fChildSelect.Set(5); | |
156 | for (Int_t i=0; i<5; i++) fChildSelect[i]=0; | |
157 | SetForceDecay(); | |
158 | SetCutOnChild(); | |
159 | SetChildMomentumRange(); | |
160 | SetChildPtRange(); | |
161 | SetChildPhiRange(); | |
162 | SetChildThetaRange(); | |
163 | } | |
164 | ||
165 | //___________________________________________________________________ | |
166 | AliGenCorrHF::AliGenCorrHF(char* tname, Int_t npart, Int_t param): | |
167 | AliGenMC(npart), | |
168 | fFileName(tname), | |
169 | fFile(0), | |
170 | fQuark(param), | |
171 | fBias(0.), | |
172 | fTrials(0), | |
173 | // fDecayer(new AliDecayerPythia()) | |
174 | fDecayer(0) | |
175 | { | |
176 | // Constructor using number of particles, quark type & user-defined InputFile | |
177 | // | |
178 | if (fQuark != 5) fQuark = 4; | |
179 | fName = "UserDefined"; | |
180 | fTitle= "Generator for correlated pairs of HF hadrons"; | |
181 | ||
182 | fChildSelect.Set(5); | |
183 | for (Int_t i=0; i<5; i++) fChildSelect[i]=0; | |
184 | SetForceDecay(); | |
185 | SetCutOnChild(); | |
186 | SetChildMomentumRange(); | |
187 | SetChildPtRange(); | |
188 | SetChildPhiRange(); | |
189 | SetChildThetaRange(); | |
190 | } | |
191 | ||
2c890605 | 192 | //____________________________________________________________ |
193 | AliGenCorrHF::~AliGenCorrHF() | |
194 | { | |
195 | // Destructor | |
196 | delete fFile; | |
197 | } | |
198 | ||
199 | //____________________________________________________________ | |
200 | void AliGenCorrHF::Init() | |
201 | { | |
202 | // Initialisation | |
203 | ||
204 | AliInfo(Form(" QQbar kinematics and fragm. functions from: %s",fFileName.Data() )); | |
205 | fFile = TFile::Open(fFileName.Data()); | |
206 | if(!fFile->IsOpen()){ | |
207 | AliError(Form("Could not open file %s",fFileName.Data() )); | |
208 | } | |
209 | ||
210 | ComputeIntegral(fFile); | |
b44c3901 | 211 | |
2c890605 | 212 | fParentWeight = 1./fNpart; // fNpart is number of HF-hadron pairs |
213 | ||
214 | // particle decay related initialization | |
215 | ||
216 | if (gMC) fDecayer = gMC->GetDecayer(); | |
217 | fDecayer->SetForceDecay(fForceDecay); | |
218 | fDecayer->Init(); | |
219 | ||
220 | // | |
221 | AliGenMC::Init(); | |
222 | } | |
2c890605 | 223 | //____________________________________________________________ |
224 | void AliGenCorrHF::Generate() | |
225 | { | |
226 | // | |
84555c93 | 227 | // Generate 'npart' of light and heavy mesons (J/Psi, upsilon or phi, Pion, |
228 | // Kaons, Etas, Omegas) and Baryons (proton, antiprotons, neutrons and | |
229 | // antineutrons in the the desired theta, phi and momentum windows; | |
2c890605 | 230 | // Gaussian smearing on the vertex is done if selected. |
84555c93 | 231 | // The decay of heavy mesons is done using lujet, |
2c890605 | 232 | // and the childern particle are tracked by GEANT |
233 | // However, light mesons are directly tracked by GEANT | |
234 | // setting fForceDecay = nodecay (SetForceDecay(nodecay)) | |
235 | // | |
84555c93 | 236 | // |
237 | // Reinitialize decayer | |
2c890605 | 238 | |
84555c93 | 239 | fDecayer->SetForceDecay(fForceDecay); |
240 | fDecayer->Init(); | |
241 | ||
242 | // | |
2c890605 | 243 | Float_t polar[3]= {0,0,0}; // Polarisation of the parent particle (for GEANT tracking) |
244 | Float_t origin0[3]; // Origin of the generated parent particle (for GEANT tracking) | |
245 | Float_t pt, pl, ptot; // Transverse, logitudinal and total momenta of the parent particle | |
246 | Float_t phi, theta; // Phi and theta spherical angles of the parent particle momentum | |
247 | Float_t p[3], pc[3], och[3];// Momentum, polarisation and origin of the children particles from lujet | |
84555c93 | 248 | Int_t nt, i, j, ipa, ihadron[2], iquark[2]; |
249 | Float_t wgtp, wgtch, random[6]; | |
250 | Float_t pq[2][3]; // Momenta of the two quarks | |
251 | Int_t ntq[2] = {-1, -1}; | |
252 | Float_t tanhy, qm; | |
2c890605 | 253 | |
b44c3901 | 254 | Double_t dphi=0, ptq[2], yq[2], pth[2], plh[2], ph[2], phih[2], phiq[2]; |
2c890605 | 255 | for (i=0; i<2; i++) { |
b44c3901 | 256 | ptq[i] =0; |
257 | yq[i] =0; | |
258 | pth[i] =0; | |
259 | plh[i] =0; | |
260 | phih[i] =0; | |
261 | phiq[i] =0; | |
2c890605 | 262 | ihadron[i] =0; |
84555c93 | 263 | iquark[i] =0; |
2c890605 | 264 | } |
265 | ||
266 | static TClonesArray *particles; | |
267 | // | |
268 | if(!particles) particles = new TClonesArray("TParticle",1000); | |
269 | ||
84555c93 | 270 | TDatabasePDG *pDataBase = TDatabasePDG::Instance(); |
271 | // | |
272 | ||
273 | // Calculating vertex position per event | |
2c890605 | 274 | for (j=0;j<3;j++) origin0[j]=fOrigin[j]; |
275 | if(fVertexSmear==kPerEvent) { | |
84555c93 | 276 | Vertex(); |
277 | for (j=0;j<3;j++) origin0[j]=fVertex[j]; | |
2c890605 | 278 | } |
279 | ||
84555c93 | 280 | ipa=0; |
281 | ||
282 | // Generating fNpart particles | |
283 | fNprimaries = 0; | |
284 | ||
285 | while (ipa<2*fNpart) { | |
286 | ||
287 | GetQuarkPair(fFile, fgIntegral, yq[0], yq[1], ptq[0], ptq[1], dphi); | |
288 | ||
289 | GetHadronPair(fFile, fQuark, yq[0], yq[1], ptq[0], ptq[1], ihadron[0], ihadron[1], plh[0], plh[1], pth[0], pth[1]); | |
290 | ||
291 | // Cuts from AliGenerator | |
292 | ||
293 | // Cut on theta | |
294 | theta=TMath::ATan2(pth[0],plh[0]); | |
295 | if(theta<fThetaMin || theta>fThetaMax) continue; | |
296 | theta=TMath::ATan2(pth[1],plh[1]); | |
297 | if(theta<fThetaMin || theta>fThetaMax) continue; | |
298 | ||
299 | // Cut on momentum | |
300 | ph[0]=TMath::Sqrt(pth[0]*pth[0]+plh[0]*plh[0]); | |
301 | if (ph[0]<fPMin || ph[0]>fPMax) continue; | |
302 | ph[1]=TMath::Sqrt(pth[1]*pth[1]+plh[1]*plh[1]); | |
303 | if (ph[1]<fPMin || ph[1]>fPMax) continue; | |
304 | ||
305 | // Add the quarks in the stack | |
306 | ||
307 | phiq[0] = Rndm()*k2PI; | |
308 | if (Rndm() < 0.5) { | |
b44c3901 | 309 | phiq[1] = phiq[0] + dphi*kDegrad; |
84555c93 | 310 | } else { |
311 | phiq[1] = phiq[0] - dphi*kDegrad; | |
312 | } | |
313 | if (phiq[1] > k2PI) phiq[1] -= k2PI; | |
314 | if (phiq[1] < 0 ) phiq[1] += k2PI; | |
315 | ||
316 | // quarks pdg | |
317 | iquark[0] = +fQuark; | |
318 | iquark[1] = -fQuark; | |
319 | ||
320 | // px and py | |
321 | TVector2 qvect1 = TVector2(); | |
322 | TVector2 qvect2 = TVector2(); | |
323 | qvect1.SetMagPhi(ptq[0],phiq[0]); | |
324 | qvect2.SetMagPhi(ptq[1],phiq[1]); | |
325 | pq[0][0] = qvect1.Px(); | |
326 | pq[0][1] = qvect1.Py(); | |
327 | pq[1][0] = qvect2.Px(); | |
328 | pq[1][1] = qvect2.Py(); | |
329 | ||
330 | // pz | |
331 | tanhy = TMath::TanH(yq[0]); | |
332 | qm = pDataBase->GetParticle(iquark[0])->Mass(); | |
333 | pq[0][2] = TMath::Sqrt((ptq[0]*ptq[0]+qm*qm)*tanhy/(1-tanhy)); | |
334 | tanhy = TMath::TanH(yq[1]); | |
335 | qm = pDataBase->GetParticle(iquark[1])->Mass(); | |
336 | pq[1][2] = TMath::Sqrt((ptq[1]*ptq[1]+qm*qm)*tanhy/(1-tanhy)); | |
337 | ||
338 | // set special value shift to have a signature of this generator | |
339 | pq[0][0] += 1000000.0; | |
340 | pq[0][1] += 1000000.0; | |
341 | pq[0][2] += 1000000.0; | |
342 | pq[1][0] += 1000000.0; | |
343 | pq[1][1] += 1000000.0; | |
344 | pq[1][2] += 1000000.0; | |
345 | ||
346 | // Here we assume that |phi_H1 - phi_H2| = |phi_Q1 - phi_Q2| = dphi | |
347 | // which is a good approximation for heavy flavors in Pythia | |
348 | // ... moreover, same phi angles as for the quarks ... | |
349 | ||
350 | phih[0] = phiq[0]; | |
351 | phih[1] = phiq[1]; | |
b44c3901 | 352 | |
84555c93 | 353 | for (Int_t ihad = 0; ihad < 2; ihad++) { |
354 | while(1) { | |
355 | // | |
356 | // particle type | |
357 | Int_t iPart = ihadron[ihad]; | |
358 | fChildWeight=(fDecayer->GetPartialBranchingRatio(iPart))*fParentWeight; | |
359 | wgtp=fParentWeight; | |
360 | wgtch=fChildWeight; | |
361 | TParticlePDG *particle = pDataBase->GetParticle(iPart); | |
362 | Float_t am = particle->Mass(); | |
363 | phi = phih[ihad]; | |
364 | pt = pth[ihad]; | |
365 | pl = plh[ihad]; | |
366 | ptot=TMath::Sqrt(pt*pt+pl*pl); | |
367 | ||
368 | p[0]=pt*TMath::Cos(phi); | |
369 | p[1]=pt*TMath::Sin(phi); | |
370 | p[2]=pl; | |
b44c3901 | 371 | |
2c890605 | 372 | if(fVertexSmear==kPerTrack) { |
84555c93 | 373 | Rndm(random,6); |
374 | for (j=0;j<3;j++) { | |
375 | origin0[j]= | |
376 | fOrigin[j]+fOsigma[j]*TMath::Cos(2*random[2*j]*TMath::Pi())* | |
377 | TMath::Sqrt(-2*TMath::Log(random[2*j+1])); | |
2c890605 | 378 | } |
379 | } | |
84555c93 | 380 | |
381 | // Looking at fForceDecay : | |
382 | // if fForceDecay != none Primary particle decays using | |
383 | // AliPythia and children are tracked by GEANT | |
384 | // | |
385 | // if fForceDecay == none Primary particle is tracked by GEANT | |
386 | // (In the latest, make sure that GEANT actually does all the decays you want) | |
387 | // | |
388 | ||
389 | if (fForceDecay != kNoDecay) { | |
390 | // Using lujet to decay particle | |
391 | Float_t energy=TMath::Sqrt(ptot*ptot+am*am); | |
392 | TLorentzVector pmom(p[0], p[1], p[2], energy); | |
393 | fDecayer->Decay(iPart,&pmom); | |
394 | // | |
395 | // select decay particles | |
396 | Int_t np=fDecayer->ImportParticles(particles); | |
397 | ||
398 | // Selecting GeometryAcceptance for particles fPdgCodeParticleforAcceptanceCut; | |
399 | if (fGeometryAcceptance) | |
400 | if (!CheckAcceptanceGeometry(np,particles)) continue; | |
401 | Int_t ncsel=0; | |
402 | Int_t* pFlag = new Int_t[np]; | |
403 | Int_t* pParent = new Int_t[np]; | |
404 | Int_t* pSelected = new Int_t[np]; | |
405 | Int_t* trackIt = new Int_t[np]; | |
406 | ||
407 | for (i=0; i<np; i++) { | |
408 | pFlag[i] = 0; | |
409 | pSelected[i] = 0; | |
410 | pParent[i] = -1; | |
411 | } | |
412 | ||
413 | if (np >1) { | |
414 | TParticle* iparticle = (TParticle *) particles->At(0); | |
415 | Int_t ipF, ipL; | |
416 | for (i = 1; i<np ; i++) { | |
417 | trackIt[i] = 1; | |
418 | iparticle = (TParticle *) particles->At(i); | |
419 | Int_t kf = iparticle->GetPdgCode(); | |
420 | Int_t ks = iparticle->GetStatusCode(); | |
421 | // flagged particle | |
422 | ||
423 | if (pFlag[i] == 1) { | |
424 | ipF = iparticle->GetFirstDaughter(); | |
425 | ipL = iparticle->GetLastDaughter(); | |
426 | if (ipF > 0) for (j=ipF-1; j<ipL; j++) pFlag[j]=1; | |
427 | continue; | |
428 | } | |
429 | ||
430 | // flag decay products of particles with long life-time (c tau > .3 mum) | |
431 | ||
432 | if (ks != 1) { | |
433 | //TParticlePDG *particle = pDataBase->GetParticle(kf); | |
434 | ||
435 | Double_t lifeTime = fDecayer->GetLifetime(kf); | |
436 | //Double_t mass = particle->Mass(); | |
437 | //Double_t width = particle->Width(); | |
438 | if (lifeTime > (Double_t) fMaxLifeTime) { | |
439 | ipF = iparticle->GetFirstDaughter(); | |
440 | ipL = iparticle->GetLastDaughter(); | |
441 | if (ipF > 0) for (j=ipF-1; j<ipL; j++) pFlag[j]=1; | |
442 | } else{ | |
443 | trackIt[i] = 0; | |
444 | pSelected[i] = 1; | |
2c890605 | 445 | } |
84555c93 | 446 | } // ks==1 ? |
447 | // | |
448 | // children | |
449 | ||
450 | if (ChildSelected(TMath::Abs(kf)) || fForceDecay == kAll && trackIt[i]) | |
451 | { | |
452 | if (fCutOnChild) { | |
453 | pc[0]=iparticle->Px(); | |
454 | pc[1]=iparticle->Py(); | |
455 | pc[2]=iparticle->Pz(); | |
456 | Bool_t childok = KinematicSelection(iparticle, 1); | |
457 | if(childok) { | |
458 | pSelected[i] = 1; | |
459 | ncsel++; | |
460 | } else { | |
461 | ncsel=-1; | |
462 | break; | |
463 | } // child kine cuts | |
464 | } else { | |
465 | pSelected[i] = 1; | |
466 | ncsel++; | |
467 | } // if child selection | |
468 | } // select muon | |
469 | } // decay particle loop | |
470 | } // if decay products | |
471 | ||
472 | Int_t iparent; | |
473 | if ((fCutOnChild && ncsel >0) || !fCutOnChild){ | |
474 | ipa++; | |
475 | // | |
476 | // Parent | |
477 | // quark | |
478 | PushTrack(0, -1, iquark[ihad], pq[ihad], origin0, polar, 0, kPPrimary, nt, wgtp); | |
479 | KeepTrack(nt); | |
480 | ntq[ihad] = nt; | |
481 | //printf("PushTrack: Q \t%5d trackit %1d part %8d name %10s \t from %3d \n",nt,0,iquark[ihad],pDataBase->GetParticle(iquark[ihad])->GetName(),-1); | |
482 | // hadron | |
483 | PushTrack(0, ntq[ihad], iPart, p, origin0, polar, 0, kPDecay, nt, wgtp); | |
484 | pParent[0] = nt; | |
485 | KeepTrack(nt); | |
486 | fNprimaries++; | |
487 | //printf("PushTrack: P \t%5d trackit %1d part %8d name %10s \t from %3d \n",nt,0,iPart,pDataBase->GetParticle(iPart)->GetName(),ntq[ihad]); | |
488 | ||
489 | // | |
490 | // Decay Products | |
491 | // | |
492 | for (i = 1; i < np; i++) { | |
493 | if (pSelected[i]) { | |
494 | TParticle* iparticle = (TParticle *) particles->At(i); | |
495 | Int_t kf = iparticle->GetPdgCode(); | |
496 | Int_t ipa = iparticle->GetFirstMother()-1; | |
2c890605 | 497 | |
84555c93 | 498 | och[0] = origin0[0]+iparticle->Vx()/10; |
499 | och[1] = origin0[1]+iparticle->Vy()/10; | |
500 | och[2] = origin0[2]+iparticle->Vz()/10; | |
501 | pc[0] = iparticle->Px(); | |
502 | pc[1] = iparticle->Py(); | |
503 | pc[2] = iparticle->Pz(); | |
2c890605 | 504 | |
84555c93 | 505 | if (ipa > -1) { |
506 | iparent = pParent[ipa]; | |
507 | } else { | |
508 | iparent = -1; | |
509 | } | |
510 | ||
511 | PushTrack(fTrackIt*trackIt[i], iparent, kf, | |
512 | pc, och, polar, | |
513 | 0, kPDecay, nt, wgtch); | |
514 | //printf("PushTrack: DD \t%5d trackit %1d part %8d name %10s \t from %3d \n",nt,fTrackIt*trackIt[i],kf,pDataBase->GetParticle(kf)->GetName(),iparent); | |
515 | pParent[i] = nt; | |
516 | KeepTrack(nt); | |
517 | fNprimaries++; | |
518 | } // Selected | |
519 | } // Particle loop | |
520 | } // Decays by Lujet | |
521 | particles->Clear(); | |
522 | if (pFlag) delete[] pFlag; | |
523 | if (pParent) delete[] pParent; | |
524 | if (pSelected) delete[] pSelected; | |
525 | if (trackIt) delete[] trackIt; | |
526 | } // kinematic selection | |
527 | else // nodecay option, so parent will be tracked by GEANT (pions, kaons, eta, omegas, baryons) | |
528 | { | |
529 | gAlice->GetMCApp()-> | |
530 | PushTrack(fTrackIt,-1,iPart,p,origin0,polar,0,kPPrimary,nt,wgtp); | |
531 | ipa++; | |
532 | fNprimaries++; | |
533 | } | |
2c890605 | 534 | break; |
535 | } // while(1) | |
84555c93 | 536 | } // hadron pair loop |
537 | } // event loop | |
538 | ||
2c890605 | 539 | SetHighWaterMark(nt); |
84555c93 | 540 | |
541 | AliGenEventHeader* header = new AliGenEventHeader("PARAM"); | |
542 | header->SetPrimaryVertex(fVertex); | |
543 | header->SetNProduced(fNprimaries); | |
544 | AddHeader(header); | |
2c890605 | 545 | |
84555c93 | 546 | } |
2c890605 | 547 | //____________________________________________________________________________________ |
548 | Int_t AliGenCorrHF::IpCharm(TRandom* ran) | |
549 | { | |
550 | // Composition of lower state charm hadrons, containing a c-quark | |
551 | Float_t random; | |
552 | Int_t ip; // +- 411,421,431,4122,4132,4232,4332 | |
553 | random = ran->Rndm(); | |
554 | // Rates from Pythia6.214 using 100Kevents with kPyCharmppMNRwmi at 14 TeV. | |
555 | ||
556 | if (random < 0.6027) { | |
557 | ip=421; | |
558 | } else if (random < 0.7962) { | |
559 | ip=411; | |
560 | } else if (random < 0.9127) { | |
561 | ip=431; | |
562 | } else if (random < 0.9899) { | |
563 | ip=4122; | |
564 | } else if (random < 0.9948) { | |
565 | ip=4132; | |
566 | } else if (random < 0.9999) { | |
567 | ip=4232; | |
568 | } else { | |
569 | ip=4332; | |
570 | } | |
571 | ||
572 | return ip; | |
573 | } | |
574 | ||
575 | Int_t AliGenCorrHF::IpBeauty(TRandom* ran) | |
576 | { | |
577 | // Composition of lower state beauty hadrons, containing a b-quark | |
578 | Float_t random; | |
579 | Int_t ip; // +- 511,521,531,5122,5132,5232,5332 | |
580 | random = ran->Rndm(); | |
581 | // Rates from Pythia6.214 using 100Kevents with kPyBeautyppMNRwmi at 14 TeV. | |
582 | // B-Bbar mixing will be done by Pythia at the decay point | |
583 | if (random < 0.3965) { | |
584 | ip=-511; | |
585 | } else if (random < 0.7930) { | |
586 | ip=-521; | |
587 | } else if (random < 0.9112) { | |
588 | ip=-531; | |
589 | } else if (random < 0.9887) { | |
590 | ip=5122; | |
591 | } else if (random < 0.9943) { | |
592 | ip=5132; | |
593 | } else if (random < 0.9999) { | |
594 | ip=5232; | |
595 | } else { | |
596 | ip=5332; | |
597 | } | |
598 | ||
599 | return ip; | |
600 | } | |
601 | ||
602 | //____________________________________________________________________________________ | |
603 | Double_t AliGenCorrHF::ComputeIntegral(TFile* fG) // needed by GetQuarkPair | |
604 | { | |
605 | // Read QQbar kinematical 5D grid's cell occupancy weights | |
606 | Int_t* cell = new Int_t[6]; // cell[6]={wght,iy1,iy2,ipt1,ipt2,idph} | |
607 | TTree* tG = (TTree*) fG->Get("tGqq"); | |
608 | tG->GetBranch("cell")->SetAddress(cell); | |
609 | Int_t nbins = tG->GetEntries(); | |
610 | ||
611 | // delete previously computed integral (if any) | |
612 | if(fgIntegral) delete [] fgIntegral; | |
613 | ||
614 | fgIntegral = new Double_t[nbins+1]; | |
615 | fgIntegral[0] = 0; | |
616 | Int_t bin; | |
617 | for(bin=0;bin<nbins;bin++) { | |
618 | tG->GetEvent(bin); | |
619 | fgIntegral[bin+1] = fgIntegral[bin] + cell[0]; | |
620 | } | |
621 | // Normalize integral to 1 | |
622 | if (fgIntegral[nbins] == 0 ) { | |
623 | return 0; | |
624 | } | |
625 | for (bin=1;bin<=nbins;bin++) fgIntegral[bin] /= fgIntegral[nbins]; | |
626 | ||
627 | return fgIntegral[nbins]; | |
628 | } | |
629 | ||
630 | //____________________________________________________________________________________ | |
631 | void AliGenCorrHF::GetQuarkPair(TFile* fG, Double_t* fInt, Double_t &y1, Double_t &y2, Double_t &pt1, Double_t &pt2, Double_t &dphi) | |
632 | // modification of ROOT's TH3::GetRandom3 for 5D | |
633 | { | |
634 | // Read QQbar kinematical 5D grid's cell coordinates | |
635 | Int_t* cell = new Int_t[6]; // cell[6]={wght,iy1,iy2,ipt1,ipt2,idph} | |
636 | TTree* tG = (TTree*) fG->Get("tGqq"); | |
637 | tG->GetBranch("cell")->SetAddress(cell); | |
638 | Int_t nbins = tG->GetEntries(); | |
639 | Double_t rand[6]; | |
640 | gRandom->RndmArray(6,rand); | |
641 | Int_t ibin = TMath::BinarySearch(nbins,fInt,rand[0]); | |
642 | tG->GetEvent(ibin); | |
643 | y1 = fgy[cell[1]] + (fgy[cell[1]+1]-fgy[cell[1]])*rand[1]; | |
644 | y2 = fgy[cell[2]] + (fgy[cell[2]+1]-fgy[cell[2]])*rand[2]; | |
645 | pt1 = fgpt[cell[3]] + (fgpt[cell[3]+1]-fgpt[cell[3]])*rand[3]; | |
646 | pt2 = fgpt[cell[4]] + (fgpt[cell[4]+1]-fgpt[cell[4]])*rand[4]; | |
647 | dphi = fgdph[cell[5]]+ (fgdph[cell[5]+1]-fgdph[cell[5]])*rand[5]; | |
648 | } | |
649 | ||
650 | //____________________________________________________________________________________ | |
651 | void AliGenCorrHF::GetHadronPair(TFile* fG, Int_t idq, Double_t y1, Double_t y2, Double_t pt1, Double_t pt2, Int_t &id3, Int_t &id4, Double_t &pz3, Double_t &pz4, Double_t &pt3, Double_t &pt4) | |
652 | { | |
653 | // Generate a hadron pair | |
654 | Int_t (*fIpParaFunc )(TRandom*);//Pointer to particle type parametrisation function | |
655 | fIpParaFunc = IpCharm; | |
656 | Double_t mq = 1.2; // c & b quark masses (used in AliPythia) | |
657 | if (idq == 5) { | |
658 | fIpParaFunc = IpBeauty; | |
659 | mq = 4.75; | |
660 | } | |
661 | Double_t z11, z12, z21, z22, pz1, pz2, e1, e2, mh, ptemp, rand[2]; | |
662 | char tag[100]; | |
663 | TH2F *h2h[12], *h2s[12]; // hard & soft Fragmentation Functions | |
664 | for (Int_t ipt = 0; ipt<fgnptbins; ipt++) { | |
665 | sprintf(tag,"h2h_pt%d",ipt); | |
666 | h2h[ipt] = (TH2F*) fG->Get(tag); | |
667 | sprintf(tag,"h2s_pt%d",ipt); | |
668 | h2s[ipt] = (TH2F*) fG->Get(tag); | |
669 | } | |
670 | ||
671 | if (y1*y2 < 0) { | |
672 | for (Int_t ipt = 0; ipt<fgnptbins; ipt++) { | |
673 | if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt]) | |
674 | h2h[ipt]->GetRandom2(z11, z21); | |
675 | if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt]) | |
676 | h2h[ipt]->GetRandom2(z12, z22); | |
677 | } | |
678 | } | |
679 | else { | |
680 | if (TMath::Abs(y1) > TMath::Abs(y2)) { | |
681 | for (Int_t ipt = 0; ipt<fgnptbins; ipt++) { | |
682 | if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt]) | |
683 | h2h[ipt]->GetRandom2(z11, z21); | |
684 | if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt]) | |
685 | h2s[ipt]->GetRandom2(z12, z22); | |
686 | } | |
687 | } | |
688 | else { | |
689 | for (Int_t ipt = 0; ipt<fgnptbins; ipt++) { | |
690 | if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt]) | |
691 | h2s[ipt]->GetRandom2(z11, z21); | |
692 | if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt]) | |
693 | h2h[ipt]->GetRandom2(z12, z22); | |
694 | } | |
695 | } | |
696 | } | |
697 | gRandom->RndmArray(2,rand); | |
698 | ptemp = TMath::Sqrt(pt1*pt1 + mq*mq); | |
699 | pz1 = ptemp*TMath::SinH(y1); | |
700 | e1 = ptemp*TMath::CosH(y1); | |
701 | ptemp = TMath::Sqrt(pt2*pt2 + mq*mq); | |
702 | pz2 = ptemp*TMath::SinH(y2); | |
703 | e2 = ptemp*TMath::CosH(y2); | |
704 | ||
705 | id3 = fIpParaFunc(gRandom); | |
706 | mh = TDatabasePDG::Instance()->GetParticle(id3)->Mass(); | |
707 | ptemp = z11*z21*(e1*e1-pz1*pz1) - mh*mh; | |
708 | pt3 = (idq-3)*rand[0]; // some smearing at low pt, try better | |
709 | if (ptemp > 0) pt3 = TMath::Sqrt(ptemp); | |
710 | if (pz1 > 0) pz3 = (z11*(e1 + pz1) - z21*(e1 - pz1)) / 2; | |
711 | else pz3 = (z21*(e1 + pz1) - z11*(e1 - pz1)) / 2; | |
712 | e1 = TMath::Sqrt(pz3*pz3 + pt3*pt3 + mh*mh); | |
713 | ||
714 | id4 = - fIpParaFunc(gRandom); | |
715 | mh = TDatabasePDG::Instance()->GetParticle(id4)->Mass(); | |
716 | ptemp = z12*z22*(e2*e2-pz2*pz2) - mh*mh; | |
717 | pt4 = (idq-3)*rand[1]; // some smearing at low pt, try better | |
718 | if (ptemp > 0) pt4 = TMath::Sqrt(ptemp); | |
719 | if (pz2 > 0) pz4 = (z12*(e2 + pz2) - z22*(e2 - pz2)) / 2; | |
720 | else pz4 = (z22*(e2 + pz2) - z12*(e2 - pz2)) / 2; | |
721 | e2 = TMath::Sqrt(pz4*pz4 + pt4*pt4 + mh*mh); | |
722 | ||
723 | // small corr. instead of using Frag. Func. depending on yQ (in addition to ptQ) | |
724 | Float_t ycorr = 0.2, y3, y4; | |
725 | gRandom->RndmArray(2,rand); | |
726 | y3 = 0.5 * TMath::Log((e1 + pz3 + 1.e-13)/(e1 - pz3 + 1.e-13)); | |
727 | y4 = 0.5 * TMath::Log((e2 + pz4 + 1.e-13)/(e2 - pz4 + 1.e-13)); | |
728 | if(TMath::Abs(y3)<ycorr && TMath::Abs(y4)<ycorr && rand[0]>0.5) { | |
729 | ptemp = TMath::Sqrt(e1*e1 - pz3*pz3); | |
730 | y3 = 4*(1 - 2*rand[1]); | |
731 | pz3 = ptemp*TMath::SinH(y3); | |
732 | pz4 = pz3; | |
733 | } | |
734 | } |