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10d100d4 | 1 | /************************************************************************** |
2 | * Copyright(c) 2005-2007, 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 | //----------------------------------------------------------------- | |
19 | // ITS PID method # 1 | |
20 | // Implementation of the ITS PID class | |
21 | // Very naive one... Should be made better by the detector experts... | |
22 | // Origin: Iouri Belikov, CERN, Jouri.Belikov@cern.ch | |
23 | //----------------------------------------------------------------- | |
24 | #include "TMath.h" | |
567624b5 | 25 | #include "AliVTrack.h" |
10d100d4 | 26 | #include "AliITSPIDResponse.h" |
27 | #include "AliITSPidParams.h" | |
28 | #include "AliExternalTrackParam.h" | |
29 | ||
10d100d4 | 30 | ClassImp(AliITSPIDResponse) |
31 | ||
15e979c9 | 32 | AliITSPIDResponse::AliITSPIDResponse(Bool_t isMC): |
10d100d4 | 33 | fRes(0.13), |
34 | fKp1(15.77), | |
35 | fKp2(4.95), | |
36 | fKp3(0.312), | |
37 | fKp4(2.14), | |
38 | fKp5(0.82) | |
39 | { | |
15e979c9 | 40 | if(!isMC){ |
41 | fBBtpcits[0]=0.73; | |
42 | fBBtpcits[1]=14.68; | |
43 | fBBtpcits[2]=0.905; | |
44 | fBBtpcits[3]=1.2; | |
45 | fBBtpcits[4]=6.6; | |
41cab740 | 46 | fBBdeu[0]=76.43; // parameters for the deuteron - tpcits - value from PbPb 2010 run (S.Trogolo - July 2014) |
47 | fBBdeu[1]=-34.21; | |
48 | fBBdeu[2]=113.2; | |
49 | fBBdeu[3]=-18.12; | |
50 | fBBdeu[4]=0.6019; | |
51 | fBBtri[0]=13.34; // parameters for the triton - tpcits - value from PbPb 2010 run (S.Trogolo - July 2014) | |
52 | fBBtri[1]=55.17; | |
53 | fBBtri[2]=66.41; | |
54 | fBBtri[3]=-6.601; | |
55 | fBBtri[4]=-0.4134; | |
62ccfebf | 56 | fBBsa[0]=2.73198E7; //pure PHOBOS parameterization |
88f46717 | 57 | fBBsa[1]=6.92389; |
58 | fBBsa[2]=1.90088E-6; | |
59 | fBBsa[3]=1.90088E-6; | |
60 | fBBsa[4]=3.40644E-7; | |
62ccfebf | 61 | fBBsaHybrid[0]=1.43505E7; //PHOBOS+Polinomial parameterization |
62 | fBBsaHybrid[1]=49.3402; | |
63 | fBBsaHybrid[2]=1.77741E-7; | |
64 | fBBsaHybrid[3]=1.77741E-7; | |
65 | fBBsaHybrid[4]=1.01311E-7; | |
66 | fBBsaHybrid[5]=77.2777; | |
67 | fBBsaHybrid[6]=33.4099; | |
68 | fBBsaHybrid[7]=46.0089; | |
69 | fBBsaHybrid[8]=-2.26583; | |
70 | fBBsaElectron[0]=4.05799E6; //electrons in the ITS | |
88f46717 | 71 | fBBsaElectron[1]=38.5713; |
72 | fBBsaElectron[2]=1.46462E-7; | |
73 | fBBsaElectron[3]=1.46462E-7; | |
74 | fBBsaElectron[4]=4.40284E-7; | |
8abeb05b | 75 | fResolSA[0]=1.; // 0 cluster tracks should not be used |
88f46717 | 76 | fResolSA[1]=0.25; // rough values for tracks with 1 |
77 | fResolSA[2]=0.131; // value from pp 2010 run (L. Milano, 16-Jun-11) | |
78 | fResolSA[3]=0.113; // value from pp 2010 run | |
8abeb05b | 79 | fResolSA[4]=0.104; // value from pp 2010 run |
15e979c9 | 80 | for(Int_t i=0; i<5;i++) fResolTPCITS[i]=0.13; |
41cab740 | 81 | fResolTPCITSDeu3[0]=0.06918; // deuteron resolution vs p |
82 | fResolTPCITSDeu3[1]=0.02498; // 3 ITS clusters for PId | |
83 | fResolTPCITSDeu3[2]=1.1; // value from PbPb 2010 run (July 2014) | |
84 | fResolTPCITSDeu4[0]=0.06756;// deuteron resolution vs p | |
85 | fResolTPCITSDeu4[1]=0.02078; // 4 ITS clusters for PId | |
86 | fResolTPCITSDeu4[2]=1.05; // value from PbPb 2010 run (July 2014) | |
87 | fResolTPCITSTri3[0]=0.07239; // triton resolution vs p | |
88 | fResolTPCITSTri3[1]=0.0192; // 3 ITS clusters for PId | |
89 | fResolTPCITSTri3[2]=1.1; // value from PbPb 2010 run (July 2014) | |
90 | fResolTPCITSTri4[0]=0.06083; // triton resolution | |
91 | fResolTPCITSTri4[1]=0.02579; // 4 ITS clusters for PId | |
92 | fResolTPCITSTri4[2]=1.15; // value from PbPb 2010 run (July 2014) | |
15e979c9 | 93 | }else{ |
99daa709 | 94 | fBBtpcits[0]=1.04; |
95 | fBBtpcits[1]=27.14; | |
96 | fBBtpcits[2]=1.00; | |
97 | fBBtpcits[3]=0.964; | |
98 | fBBtpcits[4]=2.59; | |
62ccfebf | 99 | fBBsa[0]=2.02078E7; //pure PHOBOS parameterization |
88f46717 | 100 | fBBsa[1]=14.0724; |
101 | fBBsa[2]=3.84454E-7; | |
102 | fBBsa[3]=3.84454E-7; | |
103 | fBBsa[4]=2.43913E-7; | |
62ccfebf | 104 | fBBsaHybrid[0]=1.05381E7; //PHOBOS+Polinomial parameterization |
105 | fBBsaHybrid[1]=89.3933; | |
106 | fBBsaHybrid[2]=2.4831E-7; | |
107 | fBBsaHybrid[3]=2.4831E-7; | |
108 | fBBsaHybrid[4]=7.80591E-8; | |
109 | fBBsaHybrid[5]=62.9214; | |
110 | fBBsaHybrid[6]=32.347; | |
111 | fBBsaHybrid[7]=58.7661; | |
112 | fBBsaHybrid[8]=-3.39869; | |
113 | fBBsaElectron[0]=2.26807E6; //electrons in the ITS | |
88f46717 | 114 | fBBsaElectron[1]=99.985; |
115 | fBBsaElectron[2]=0.000714841; | |
116 | fBBsaElectron[3]=0.000259585; | |
117 | fBBsaElectron[4]=1.39412E-7; | |
8abeb05b | 118 | fResolSA[0]=1.; // 0 cluster tracks should not be used |
88f46717 | 119 | fResolSA[1]=0.25; // rough values for tracks with 1 |
120 | fResolSA[2]=0.126; // value from pp 2010 simulations (L. Milano, 16-Jun-11) | |
121 | fResolSA[3]=0.109; // value from pp 2010 simulations | |
122 | fResolSA[4]=0.097; // value from pp 2010 simulations | |
15e979c9 | 123 | for(Int_t i=0; i<5;i++) fResolTPCITS[i]=0.13; |
124 | } | |
10d100d4 | 125 | } |
126 | ||
56576f1e | 127 | /* |
10d100d4 | 128 | //_________________________________________________________________________ |
129 | AliITSPIDResponse::AliITSPIDResponse(Double_t *param): | |
9ebbddd4 | 130 | fRes(param[0]), |
10d100d4 | 131 | fKp1(15.77), |
132 | fKp2(4.95), | |
133 | fKp3(0.312), | |
134 | fKp4(2.14), | |
135 | fKp5(0.82) | |
136 | { | |
137 | // | |
138 | // The main constructor | |
139 | // | |
6b4634a4 | 140 | for (Int_t i=0; i<5;i++) { |
141 | fBBsa[i]=0.; | |
142 | fBBtpcits[i]=0.; | |
143 | fResolSA[i]=0.; | |
144 | fResolTPCITS[i]=0.; | |
145 | } | |
10d100d4 | 146 | } |
56576f1e | 147 | */ |
10d100d4 | 148 | |
8abeb05b | 149 | //_________________________________________________________________________ |
15e979c9 | 150 | Double_t AliITSPIDResponse::BetheAleph(Double_t p, Double_t mass) const { |
10d100d4 | 151 | // |
152 | // returns AliExternalTrackParam::BetheBloch normalized to | |
153 | // fgMIP at the minimum | |
154 | // | |
15e979c9 | 155 | |
10d100d4 | 156 | Double_t bb= |
157 | AliExternalTrackParam::BetheBlochAleph(p/mass,fKp1,fKp2,fKp3,fKp4,fKp5); | |
9ebbddd4 | 158 | return bb; |
10d100d4 | 159 | } |
160 | ||
4bd62e52 | 161 | //_________________________________________________________________________ |
162 | Double_t AliITSPIDResponse::Bethe(Double_t bg, const Double_t * const par, Bool_t isNuclei) const | |
163 | { | |
164 | ||
165 | const Double_t beta = bg/TMath::Sqrt(1.+ bg*bg); | |
166 | const Double_t gamma=bg/beta; | |
167 | Double_t bb=1.; | |
168 | ||
169 | Double_t eff=1.0; | |
170 | if(bg<par[2]) | |
171 | eff=(bg-par[3])*(bg-par[3])+par[4]; | |
172 | else | |
173 | eff=(par[2]-par[3])*(par[2]-par[3])+par[4]; | |
174 | ||
175 | if(gamma>=0. && beta>0.){ | |
176 | if(isNuclei){ | |
177 | //Parameterization for deuteron between 0.4 - 1.5 GeV/c; triton between 0.58 - 1.65 GeV/c | |
178 | bb=par[0] + par[1]/bg + par[2]/(bg*bg) + par[3]/(bg*bg*bg) + par[4]/(bg*bg*bg*bg); | |
179 | }else{ //Parameterization for pion, kaon, proton, electron | |
180 | bb=(par[1]+2.0*TMath::Log(gamma)-beta*beta)*(par[0]/(beta*beta))*eff; | |
181 | } | |
182 | } | |
183 | ||
184 | return bb; | |
185 | } | |
186 | ||
8abeb05b | 187 | //_________________________________________________________________________ |
bb40433d | 188 | Double_t AliITSPIDResponse::Bethe(Double_t p, Double_t mass, Bool_t isSA) const { |
189 | ||
190 | //OLD - Mantained for backward compatibility | |
191 | //from the mass check --> Set the Particle Type | |
192 | //at the end use the method Bethe(Double_t p, AliPID::EParticleType species, Bool_t isSA) const to set the right parameter | |
41cab740 | 193 | |
15e979c9 | 194 | // |
195 | // returns AliExternalTrackParam::BetheBloch normalized to | |
196 | // fgMIP at the minimum | |
197 | // | |
198 | ||
41cab740 | 199 | // NEW: Parameterization for Deuteron and Triton energy loss, reproduced with a polynomial in fixed p range |
200 | // fBBdeu --> parameters for deuteron | |
201 | // fBBtri --> parameters for triton | |
202 | ||
4bd62e52 | 203 | //NOTE |
204 | //NOTE: if changes are made here, please also check the alternative function below | |
205 | //NOTE | |
bb40433d | 206 | |
207 | AliPID::EParticleType species = AliPID::kPion; | |
208 | ||
41cab740 | 209 | if(TMath::AreEqualAbs(mass,AliPID::ParticleMass(0),0.00001)){ |
88f46717 | 210 | //if is an electron use a specific BB parameterization |
211 | //To be used only between 100 and 160 MeV/c | |
bb40433d | 212 | species=AliPID::kElectron; |
88f46717 | 213 | } |
41cab740 | 214 | |
bb40433d | 215 | if(TMath::AreEqualAbs(mass,AliPID::ParticleMass(5),0.002)) species=AliPID::kDeuteron; |
216 | if(TMath::AreEqualAbs(mass,AliPID::ParticleMass(6),0.001)) species=AliPID::kTriton; | |
217 | ||
218 | return Bethe(p,species,isSA); | |
4bd62e52 | 219 | } |
220 | ||
221 | //_________________________________________________________________________ | |
222 | Double_t AliITSPIDResponse::Bethe(Double_t p, AliPID::EParticleType species, Bool_t isSA) const | |
223 | { | |
bb40433d | 224 | // NEW - to be used |
225 | // Alternative bethe function assuming a particle type not a mass | |
4bd62e52 | 226 | // should be slightly faster |
227 | // | |
228 | ||
229 | const Double_t m=AliPID::ParticleMassZ(species); | |
230 | const Double_t bg=p/m; | |
231 | Bool_t isNuclei=kFALSE; | |
88f46717 | 232 | |
4bd62e52 | 233 | //NOTE |
234 | //NOTE: if changes are made here, please also check the alternative function above | |
235 | //NOTE | |
236 | const Double_t *par=fBBtpcits; | |
237 | if(isSA){ | |
238 | if(species == AliPID::kElectron){ | |
239 | //if is an electron use a specific BB parameterization | |
240 | //To be used only between 100 and 160 MeV/c | |
241 | par=fBBsaElectron; | |
242 | }else{ | |
243 | par=fBBsa; | |
244 | } | |
245 | }else{ | |
246 | if(species == AliPID::kDeuteron) { | |
247 | par=fBBdeu; | |
248 | isNuclei=kTRUE; | |
249 | } | |
250 | if(species == AliPID::kTriton ) { | |
251 | par=fBBtri; | |
252 | isNuclei=kTRUE; | |
41cab740 | 253 | } |
15e979c9 | 254 | } |
41cab740 | 255 | |
4bd62e52 | 256 | return Bethe(bg, par, isNuclei); |
15e979c9 | 257 | } |
258 | ||
62ccfebf | 259 | //_________________________________________________________________________ |
260 | Double_t AliITSPIDResponse::BetheITSsaHybrid(Double_t p, Double_t mass) const { | |
261 | // | |
262 | // returns AliExternalTrackParam::BetheBloch normalized to | |
263 | // fgMIP at the minimum. The PHOBOS parameterization is used for beta*gamma>0.76. | |
264 | // For beta*gamma<0.76 a polinomial function is used | |
265 | ||
266 | Double_t bg=p/mass; | |
267 | Double_t beta = bg/TMath::Sqrt(1.+ bg*bg); | |
268 | Double_t gamma=bg/beta; | |
269 | Double_t bb=1.; | |
270 | ||
271 | Double_t par[9]; | |
272 | //parameters for pi, K, p | |
273 | for(Int_t ip=0; ip<9;ip++) par[ip]=fBBsaHybrid[ip]; | |
274 | //if it is an electron the PHOBOS part of the parameterization is tuned for e | |
275 | //in the range used for identification beta*gamma is >0.76 for electrons | |
276 | //To be used only between 100 and 160 MeV/c | |
277 | if(mass>0.0005 && mass<0.00052)for(Int_t ip=0; ip<5;ip++) par[ip]=fBBsaElectron[ip]; | |
278 | ||
279 | if(gamma>=0. && beta>0. && bg>0.1){ | |
280 | if(bg>0.76){//PHOBOS | |
281 | Double_t eff=1.0; | |
282 | if(bg<par[2]) | |
283 | eff=(bg-par[3])*(bg-par[3])+par[4]; | |
284 | else | |
285 | eff=(par[2]-par[3])*(par[2]-par[3])+par[4]; | |
286 | ||
287 | bb=(par[1]+2.0*TMath::Log(gamma)-beta*beta)*(par[0]/(beta*beta))*eff; | |
288 | }else{//Polinomial | |
289 | bb=par[5] + par[6]/bg + par[7]/(bg*bg) + par[8]/(bg*bg*bg); | |
290 | } | |
291 | } | |
292 | return bb; | |
293 | } | |
294 | ||
8abeb05b | 295 | //_________________________________________________________________________ |
41cab740 | 296 | Double_t AliITSPIDResponse::GetResolution(Double_t bethe, |
15e979c9 | 297 | Int_t nPtsForPid, |
41cab740 | 298 | Bool_t isSA, |
299 | Double_t p, | |
300 | AliPID::EParticleType type) const { | |
301 | // | |
10d100d4 | 302 | // Calculate expected resolution for truncated mean |
303 | // | |
41cab740 | 304 | // NEW: Added new variables which are Double_t p and AliPID::EParticleType type |
305 | // AliPID::EParticleType type is used to set the correct resolution for the different particles | |
306 | // default -> AliPID::EParticleType type = AliPID::kPion | |
307 | // Double_t p is used for the resolution of deuteron and triton, because they are function of the momentum | |
308 | // default -> Double_t p=0. | |
309 | ||
4bd62e52 | 310 | Float_t r=0.f; |
311 | Double_t c=1.; //this is a correction factor used for the nuclei resolution, while for pion/kaon/proton/electron is 1. | |
41cab740 | 312 | |
15e979c9 | 313 | if(isSA) r=fResolSA[nPtsForPid]; |
41cab740 | 314 | else{ |
4bd62e52 | 315 | const Double_t *par=0x0; |
316 | if(type==AliPID::kDeuteron){ | |
317 | if(nPtsForPid==3) par = fResolTPCITSDeu3; | |
318 | if(nPtsForPid==4) par = fResolTPCITSDeu4; | |
319 | c=par[2]; | |
320 | r=par[0]+par[1]*p; | |
321 | } else if(type==AliPID::kTriton){ | |
322 | if(nPtsForPid==3) par = fResolTPCITSTri3; | |
323 | if(nPtsForPid==4) par = fResolTPCITSTri4; | |
324 | c=par[2]; | |
41cab740 | 325 | r=par[0]+par[1]*p; |
4bd62e52 | 326 | } else{ |
327 | r=fResolTPCITS[nPtsForPid]; | |
41cab740 | 328 | } |
41cab740 | 329 | } |
15e979c9 | 330 | |
41cab740 | 331 | return r*bethe*c; |
332 | } | |
15e979c9 | 333 | |
334 | ||
8abeb05b | 335 | //_________________________________________________________________________ |
b52bfc67 | 336 | void AliITSPIDResponse::GetITSProbabilities(Float_t mom, Double_t qclu[4], Double_t condprobfun[AliPID::kSPECIES], Bool_t isMC) const { |
10d100d4 | 337 | // |
338 | // Method to calculate PID probabilities for a single track | |
339 | // using the likelihood method | |
340 | // | |
341 | const Int_t nLay = 4; | |
2ca1f4ee | 342 | const Int_t nPart= 4; |
10d100d4 | 343 | |
b52bfc67 | 344 | static AliITSPidParams pars(isMC); // Pid parametrisation parameters |
10d100d4 | 345 | |
2ca1f4ee | 346 | Double_t itsProb[nPart] = {1,1,1,1}; // e, p, K, pi |
10d100d4 | 347 | |
348 | for (Int_t iLay = 0; iLay < nLay; iLay++) { | |
2ca1f4ee | 349 | if (qclu[iLay] <= 50.) |
10d100d4 | 350 | continue; |
351 | ||
352 | Float_t dedx = qclu[iLay]; | |
353 | Float_t layProb = pars.GetLandauGausNorm(dedx,AliPID::kProton,mom,iLay+3); | |
354 | itsProb[0] *= layProb; | |
355 | ||
356 | layProb = pars.GetLandauGausNorm(dedx,AliPID::kKaon,mom,iLay+3); | |
10d100d4 | 357 | itsProb[1] *= layProb; |
358 | ||
359 | layProb = pars.GetLandauGausNorm(dedx,AliPID::kPion,mom,iLay+3); | |
360 | itsProb[2] *= layProb; | |
2ca1f4ee | 361 | |
362 | layProb = pars.GetLandauGausNorm(dedx,AliPID::kElectron,mom,iLay+3); | |
363 | itsProb[3] *= layProb; | |
10d100d4 | 364 | } |
365 | ||
366 | // Normalise probabilities | |
367 | Double_t sumProb = 0; | |
368 | for (Int_t iPart = 0; iPart < nPart; iPart++) { | |
369 | sumProb += itsProb[iPart]; | |
370 | } | |
2ca1f4ee | 371 | sumProb += itsProb[2]; // muon cannot be distinguished from pions |
10d100d4 | 372 | |
373 | for (Int_t iPart = 0; iPart < nPart; iPart++) { | |
374 | itsProb[iPart]/=sumProb; | |
375 | } | |
2ca1f4ee | 376 | condprobfun[AliPID::kElectron] = itsProb[3]; |
897a0e31 | 377 | condprobfun[AliPID::kMuon] = itsProb[2]; |
378 | condprobfun[AliPID::kPion] = itsProb[2]; | |
10d100d4 | 379 | condprobfun[AliPID::kKaon] = itsProb[1]; |
380 | condprobfun[AliPID::kProton] = itsProb[0]; | |
381 | return; | |
382 | } | |
15e979c9 | 383 | |
567624b5 | 384 | //_________________________________________________________________________ |
385 | Double_t AliITSPIDResponse::GetNumberOfSigmas( const AliVTrack* track, AliPID::EParticleType type) const | |
386 | { | |
387 | // | |
388 | // number of sigmas | |
389 | // | |
390 | UChar_t clumap=track->GetITSClusterMap(); | |
391 | Int_t nPointsForPid=0; | |
392 | for(Int_t i=2; i<6; i++){ | |
393 | if(clumap&(1<<i)) ++nPointsForPid; | |
394 | } | |
395 | Float_t mom=track->P(); | |
bb40433d | 396 | |
567624b5 | 397 | //check for ITS standalone tracks |
398 | Bool_t isSA=kTRUE; | |
399 | if( track->GetStatus() & AliVTrack::kTPCin ) isSA=kFALSE; | |
400 | ||
401 | const Float_t dEdx=track->GetITSsignal(); | |
402 | ||
403 | //TODO: in case of the electron, use the SA parametrisation, | |
404 | // this needs to be changed if ITS provides a parametrisation | |
405 | // for electrons also for ITS+TPC tracks | |
406 | return GetNumberOfSigmas(mom,dEdx,type,nPointsForPid,isSA || (type==AliPID::kElectron)); | |
407 | } | |
408 | ||
409 | //_________________________________________________________________________ | |
1d59271b | 410 | Double_t AliITSPIDResponse::GetSignalDelta( const AliVTrack* track, AliPID::EParticleType type, Bool_t ratio/*=kFALSE*/) const |
567624b5 | 411 | { |
412 | // | |
413 | // Signal - expected | |
414 | // | |
415 | const Float_t mom=track->P(); | |
416 | const Double_t chargeFactor = TMath::Power(AliPID::ParticleCharge(type),2.); | |
417 | Bool_t isSA=kTRUE; | |
418 | if( track->GetStatus() & AliVTrack::kTPCin ) isSA=kFALSE; | |
419 | ||
420 | const Float_t dEdx=track->GetITSsignal(); | |
421 | ||
422 | //TODO: in case of the electron, use the SA parametrisation, | |
423 | // this needs to be changed if ITS provides a parametrisation | |
424 | // for electrons also for ITS+TPC tracks | |
425 | ||
1d59271b | 426 | const Float_t bethe = Bethe(mom,AliPID::ParticleMassZ(type), isSA || (type==AliPID::kElectron))*chargeFactor; |
427 | ||
428 | Double_t delta=-9999.; | |
429 | if (!ratio) delta=dEdx-bethe; | |
430 | else if (bethe>1.e-20) delta=dEdx/bethe; | |
431 | ||
432 | return delta; | |
567624b5 | 433 | } |
434 | ||
8abeb05b | 435 | //_________________________________________________________________________ |
436 | Int_t AliITSPIDResponse::GetParticleIdFromdEdxVsP(Float_t mom, Float_t signal, Bool_t isSA) const{ | |
437 | // method to get particle identity with simple cuts on dE/dx vs. momentum | |
438 | ||
439 | Double_t massp=AliPID::ParticleMass(AliPID::kProton); | |
440 | Double_t massk=AliPID::ParticleMass(AliPID::kKaon); | |
441 | Double_t bethep=Bethe(mom,massp,isSA); | |
442 | Double_t bethek=Bethe(mom,massk,isSA); | |
443 | if(signal>(0.5*(bethep+bethek))) return AliPID::kProton; | |
444 | Double_t masspi=AliPID::ParticleMass(AliPID::kPion); | |
445 | Double_t bethepi=Bethe(mom,masspi,isSA); | |
446 | if(signal>(0.5*(bethepi+bethek))) return AliPID::kKaon; | |
447 | return AliPID::kPion; | |
448 | ||
449 | } |