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1 | #ifndef ALIANAPI0_H | |
2 | #define ALIANAPI0_H | |
3 | /* Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. * | |
4 | * See cxx source for full Copyright notice */ | |
5 | ||
6 | //_________________________________________________________________________ | |
7 | // Class to fill two-photon invariant mass histograms | |
8 | // to be used to extract pi0 raw yield. | |
9 | // Input is produced by AliAnaPhoton (or any other analysis producing output AliAODPWG4Particles), | |
10 | // it will do nothing if executed alone | |
11 | // | |
12 | //-- Author: Dmitri Peressounko (RRC "KI") | |
13 | //-- Adapted to CaloTrackCorr frame by Lamia Benhabib (SUBATECH) | |
14 | //-- and Gustavo Conesa (INFN-Frascati) | |
15 | ||
16 | //Root | |
17 | class TList; | |
18 | class TH3F ; | |
19 | class TH2F ; | |
20 | class TObjString; | |
21 | ||
22 | //Analysis | |
23 | #include "AliAnaCaloTrackCorrBaseClass.h" | |
24 | class AliAODEvent ; | |
25 | class AliESDEvent ; | |
26 | class AliAODPWG4Particle ; | |
27 | ||
28 | class AliAnaPi0 : public AliAnaCaloTrackCorrBaseClass { | |
29 | ||
30 | public: | |
31 | AliAnaPi0() ; // default ctor | |
32 | virtual ~AliAnaPi0() ;//virtual dtor | |
33 | ||
34 | //------------------------------- | |
35 | // General analysis frame methods | |
36 | //------------------------------- | |
37 | ||
38 | TObjString * GetAnalysisCuts(); | |
39 | ||
40 | TList * GetCreateOutputObjects(); | |
41 | ||
42 | void Print(const Option_t * opt) const; | |
43 | ||
44 | void MakeAnalysisFillHistograms(); | |
45 | ||
46 | void InitParameters(); | |
47 | ||
48 | //Calorimeter options | |
49 | TString GetCalorimeter() const { return fCalorimeter ; } | |
50 | void SetCalorimeter(TString & det) { fCalorimeter = det ; } | |
51 | ||
52 | //------------------------------- | |
53 | // EVENT Bin Methods | |
54 | //------------------------------- | |
55 | ||
56 | Int_t GetEventIndex(AliAODPWG4Particle * part, Double_t * vert) ; | |
57 | ||
58 | //------------------------------- | |
59 | //Opening angle pair selection | |
60 | //------------------------------- | |
61 | void SwitchOnAngleSelection() { fUseAngleCut = kTRUE ; } | |
62 | void SwitchOffAngleSelection() { fUseAngleCut = kFALSE ; } | |
63 | ||
64 | void SwitchOnAngleEDepSelection() { fUseAngleEDepCut = kTRUE ; } | |
65 | void SwitchOffAngleEDepSelection() { fUseAngleEDepCut = kFALSE ; } | |
66 | ||
67 | void SetAngleCut(Float_t a) { fAngleCut = a ; } | |
68 | void SetAngleMaxCut(Float_t a) { fAngleMaxCut = a ; } | |
69 | ||
70 | void SwitchOnFillAngleHisto() { fFillAngleHisto = kTRUE ; } | |
71 | void SwitchOffFillAngleHisto() { fFillAngleHisto = kFALSE ; } | |
72 | ||
73 | //------------------------------------------ | |
74 | //Do analysis only with clusters in same SM or different combinations of SM | |
75 | //------------------------------------------ | |
76 | void SwitchOnSameSM() { fSameSM = kTRUE ; } | |
77 | void SwitchOffSameSM() { fSameSM = kFALSE ; } | |
78 | ||
79 | void SwitchOnSMCombinations() { fFillSMCombinations = kTRUE ; } | |
80 | void SwitchOffSMCombinations() { fFillSMCombinations = kFALSE ; } | |
81 | ||
82 | //------------------------------- | |
83 | //Histogram filling options off by default | |
84 | //------------------------------- | |
85 | void SwitchOnInvPtWeight() { fMakeInvPtPlots = kTRUE ; } | |
86 | void SwitchOffInvPtWeight() { fMakeInvPtPlots = kFALSE ; } | |
87 | ||
88 | void SwitchOnFillBadDistHisto() { fFillBadDistHisto = kTRUE ; } | |
89 | void SwitchOffFillBadDistHisto() { fFillBadDistHisto = kFALSE ; } | |
90 | ||
91 | //------------------------------------------- | |
92 | //Cuts for multiple analysis, off by default | |
93 | //------------------------------------------- | |
94 | void SwitchOnMultipleCutAnalysis() { fMultiCutAna = kTRUE ; } | |
95 | void SwitchOffMultipleCutAnalysis() { fMultiCutAna = kFALSE ; } | |
96 | ||
97 | void SetNPtCuts (Int_t s) { if(s <= 10)fNPtCuts = s ; } | |
98 | void SetNAsymCuts (Int_t s) { if(s <= 10)fNAsymCuts = s ; } | |
99 | void SetNNCellCuts(Int_t s) { if(s <= 10)fNCellNCuts = s ; } | |
100 | void SetNPIDBits (Int_t s) { if(s <= 10)fNPIDBits = s ; } | |
101 | ||
102 | void SetPtCutsAt (Int_t p,Float_t v) { if(p < 10)fPtCuts[p] = v ; } | |
103 | void SetAsymCutsAt(Int_t p,Float_t v) { if(p < 10)fAsymCuts[p] = v ; } | |
104 | void SetNCellCutsAt(Int_t p,Int_t v) { if(p < 10)fCellNCuts[p]= v ; } | |
105 | void SetPIDBitsAt (Int_t p,Int_t v) { if(p < 10)fPIDBits[p] = v ; } | |
106 | ||
107 | void SwitchOnFillSSCombinations() { fFillSSCombinations = kTRUE ; } | |
108 | void SwitchOffFillSSCombinations() { fFillSSCombinations = kFALSE ; } | |
109 | ||
110 | void SwitchOnFillAsymmetryHisto() { fFillAsymmetryHisto = kTRUE ; } | |
111 | void SwitchOffFillAsymmetryHisto() { fFillAsymmetryHisto = kFALSE ; } | |
112 | ||
113 | void SwitchOnFillOriginHisto() { fFillOriginHisto = kTRUE ; } | |
114 | void SwitchOffFillOriginHisto() { fFillOriginHisto = kFALSE ; } | |
115 | ||
116 | void SwitchOnFillArmenterosThetaStarHisto() { fFillArmenterosThetaStar = kTRUE ; } | |
117 | void SwitchOffFillArmenterosThetaStarHisto() { fFillArmenterosThetaStar = kFALSE ; } | |
118 | ||
119 | //MC analysis related methods | |
120 | ||
121 | void SwitchOnConversionChecker() { fCheckConversion = kTRUE ; } | |
122 | void SwitchOffConversionChecker() { fCheckConversion = kFALSE ; } | |
123 | ||
124 | void SwitchOnMultipleCutAnalysisInSimulation() { fMultiCutAnaSim = kTRUE ; } | |
125 | void SwitchOffMultipleCutAnalysisInSimulation() { fMultiCutAnaSim = kFALSE ; } | |
126 | ||
127 | void SwitchOnCheckAcceptanceInSector() { fCheckAccInSector = kTRUE ; } | |
128 | void SwitchOffCheckAcceptanceInSector(){ fCheckAccInSector = kFALSE ; } | |
129 | ||
130 | void FillAcceptanceHistograms(); | |
131 | void FillMCVersusRecDataHistograms(Int_t index1, Int_t index2, | |
132 | Float_t pt1, Float_t pt2, | |
133 | Int_t ncells1, Int_t ncells2, | |
134 | Double_t mass, Double_t pt, Double_t asym, | |
135 | Double_t deta, Double_t dphi); | |
136 | ||
137 | void FillArmenterosThetaStar(Int_t pdg, TLorentzVector meson, | |
138 | TLorentzVector daugh1, TLorentzVector daugh2); | |
139 | ||
140 | ||
141 | private: | |
142 | ||
143 | TList ** fEventsList ; //![GetNCentrBin()*GetNZvertBin()*GetNRPBin()] Containers for photons in stored events | |
144 | ||
145 | TString fCalorimeter ; // Select Calorimeter for IM | |
146 | Int_t fNModules ; // Number of EMCAL/PHOS modules, set as many histogras as modules | |
147 | ||
148 | Bool_t fUseAngleCut ; // Select pairs depending on their opening angle | |
149 | Bool_t fUseAngleEDepCut ; // Select pairs depending on their opening angle | |
150 | Float_t fAngleCut ; // Select pairs with opening angle larger than a threshold | |
151 | Float_t fAngleMaxCut ; // Select pairs with opening angle smaller than a threshold | |
152 | ||
153 | //Multiple cuts analysis | |
154 | Bool_t fMultiCutAna; // Do analysis with several or fixed cut | |
155 | Bool_t fMultiCutAnaSim; // Do analysis with several or fixed cut, in the simulation related part | |
156 | Int_t fNPtCuts; // Number of pt cuts | |
157 | Float_t fPtCuts[10]; // Array with different pt cuts | |
158 | Int_t fNAsymCuts; // Number of assymmetry cuts | |
159 | Float_t fAsymCuts[10]; // Array with different assymetry cuts | |
160 | Int_t fNCellNCuts; // Number of cuts with number of cells in cluster | |
161 | Int_t fCellNCuts[10]; // Array with different cell number cluster cuts | |
162 | Int_t fNPIDBits ; // Number of possible PID bit combinations | |
163 | Int_t fPIDBits[10]; // Array with different PID bits | |
164 | ||
165 | //Switchs of different analysis options | |
166 | Bool_t fMakeInvPtPlots; // D plots with inverse pt weight | |
167 | Bool_t fSameSM; // Select only pairs in same SM; | |
168 | Bool_t fFillSMCombinations; // Fill histograms with different cluster pairs in SM combinations | |
169 | Bool_t fCheckConversion; // Fill histograms with tagged photons as conversion | |
170 | Bool_t fFillBadDistHisto; // Do plots for different distances to bad channels | |
171 | Bool_t fFillSSCombinations; // Do invariant mass for different combination of shower shape clusters | |
172 | Bool_t fFillAngleHisto; // Fill histograms with pair opening angle | |
173 | Bool_t fFillAsymmetryHisto; // Fill histograms with asymmetry vs pt | |
174 | Bool_t fFillOriginHisto; // Fill histograms depending on their origin | |
175 | Bool_t fFillArmenterosThetaStar; // Fill armenteros histograms | |
176 | ||
177 | Bool_t fCheckAccInSector; // Check that the decay pi0 falls in the same SM or sector | |
178 | ||
179 | //Histograms | |
180 | ||
181 | //Event characterization | |
182 | TH1F * fhAverTotECluster; //! Average number of clusters in SM | |
183 | TH1F * fhAverTotECell; //! Average number of cells in SM | |
184 | TH2F * fhAverTotECellvsCluster; //! Average number of cells in SM | |
185 | TH1F * fhEDensityCluster; //! Deposited energy in event per cluster | |
186 | TH1F * fhEDensityCell; //! Deposited energy in event per cell vs cluster | |
187 | TH2F * fhEDensityCellvsCluster; //! Deposited energy in event per cell vs cluster | |
188 | ||
189 | TH2F ** fhReMod ; //![fNModules] REAL two-photon invariant mass distribution for different calorimeter modules. | |
190 | TH2F ** fhReSameSideEMCALMod ; //![fNModules-2] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
191 | TH2F ** fhReSameSectorEMCALMod ; //![fNModules/2] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
192 | TH2F ** fhReDiffPHOSMod ; //![fNModules] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
193 | TH2F ** fhMiMod ; //![fNModules] MIXED two-photon invariant mass distribution for different calorimeter modules. | |
194 | TH2F ** fhMiSameSideEMCALMod ; //![fNModules-2] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
195 | TH2F ** fhMiSameSectorEMCALMod ; //![fNModules/2] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
196 | TH2F ** fhMiDiffPHOSMod ; //![fNModules-1] REAL two-photon invariant mass distribution for different clusters in different calorimeter modules. | |
197 | ||
198 | // Pairs with at least one cluster tagged as conversion | |
199 | TH2F * fhReConv ; //! REAL two-photon invariant mass distribution one of the pair was 2 clusters with small mass | |
200 | TH2F * fhMiConv ; //! MIXED two-photon invariant mass distribution one of the pair was 2 clusters with small mass | |
201 | TH2F * fhReConv2 ; //! REAL two-photon invariant mass distribution both pair photons recombined from 2 clusters with small mass | |
202 | TH2F * fhMiConv2 ; //! MIXED two-photon invariant mass distribution both pair photons recombined from 2 clusters with small mass | |
203 | ||
204 | TH2F ** fhRe1 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry | |
205 | TH2F ** fhMi1 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry | |
206 | TH2F ** fhRe2 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry | |
207 | TH2F ** fhMi2 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry | |
208 | TH2F ** fhRe3 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry | |
209 | TH2F ** fhMi3 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry | |
210 | ||
211 | //Histograms weighted by inverse pT | |
212 | TH2F ** fhReInvPt1 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
213 | TH2F ** fhMiInvPt1 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
214 | TH2F ** fhReInvPt2 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
215 | TH2F ** fhMiInvPt2 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
216 | TH2F ** fhReInvPt3 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] REAL two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
217 | TH2F ** fhMiInvPt3 ; //![GetNCentrBin()*fNPIDBits*fNAsymCuts] MIXED two-photon invariant mass distribution for different centralities and Asymmetry, inverse pT | |
218 | ||
219 | //Multiple cuts: Assymmetry, pt, n cells, PID | |
220 | TH2F ** fhRePtNCellAsymCuts ; //![fNPtCuts*fNAsymCuts*fNCellNCuts*] REAL two-photon invariant mass distribution for different pt cut, n cell cuts and assymetry | |
221 | TH2F ** fhMiPtNCellAsymCuts ; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Mixed two-photon invariant mass distribution for different pt cut, n cell cuts and assymetry | |
222 | TH2F ** fhRePtNCellAsymCutsSM[12] ; //![fNPtCuts*fNAsymCuts*fNCellNCutsfNModules] REAL two-photon invariant mass distribution for different pt cut, n cell cuts and assymetry for each module | |
223 | ||
224 | TH2F ** fhRePIDBits ; //![fNPIDBits] REAL two-photon invariant mass distribution for different PID bits | |
225 | TH3F ** fhRePtMult ; //![fNAsymCuts] REAL two-photon invariant mass distribution for different track multiplicity and assymetry cuts | |
226 | TH2F * fhReSS[3] ; //! Combine clusters with 3 different cuts on shower shape | |
227 | ||
228 | // Asymmetry vs pt, in pi0/eta regions | |
229 | TH2F * fhRePtAsym ; //! REAL two-photon pt vs asymmetry | |
230 | TH2F * fhRePtAsymPi0 ; //! REAL two-photon pt vs asymmetry, close to pi0 mass | |
231 | TH2F * fhRePtAsymEta ; //! REAL two-photon pt vs asymmetry, close to eta mass | |
232 | ||
233 | //Centrality, Event plane bins | |
234 | TH1I * fhEventBin; //! Number of real pairs in a particular bin (cen,vz,rp) | |
235 | TH1I * fhEventMixBin; //! Number of mixed pairs in a particular bin (cen,vz,rp) | |
236 | TH1F * fhCentrality; //! Histogram with centrality bins with at least one pare | |
237 | TH1F * fhCentralityNoPair; //! Histogram with centrality bins with no pair | |
238 | ||
239 | TH2F * fhEventPlaneResolution; //! Histogram with Event plane resolution vs centrality | |
240 | ||
241 | // Pair opening angle | |
242 | TH2F * fhRealOpeningAngle ; //! Opening angle of pair versus pair energy | |
243 | TH2F * fhRealCosOpeningAngle ; //! Cosinus of opening angle of pair version pair energy | |
244 | TH2F * fhMixedOpeningAngle ; //! Opening angle of pair versus pair energy | |
245 | TH2F * fhMixedCosOpeningAngle ; //! Cosinus of opening angle of pair version pair energy | |
246 | ||
247 | //MC analysis histograms | |
248 | //Pi0 Acceptance | |
249 | TH1F * fhPrimPi0E ; //! Spectrum of Primary | |
250 | TH1F * fhPrimPi0Pt ; //! Spectrum of Primary | |
251 | TH1F * fhPrimPi0PtRejected ; //! Spectrum of Primary,rejected | |
252 | TH1F * fhPrimPi0AccE ; //! Spectrum of primary with accepted daughters | |
253 | TH1F * fhPrimPi0AccPt ; //! Spectrum of primary with accepted daughters | |
254 | TH2F * fhPrimPi0Y ; //! Rapidity distribution of primary particles vs pT | |
255 | TH2F * fhPrimPi0AccY ; //! Rapidity distribution of primary with accepted daughters vs pT | |
256 | TH2F * fhPrimPi0Yeta ; //! PseudoRapidity distribution of primary particles vs pT | |
257 | TH2F * fhPrimPi0YetaYcut ; //! PseudoRapidity distribution of primary particles vs pT, Y<1 | |
258 | TH2F * fhPrimPi0AccYeta ; //! PseudoRapidity distribution of primary with accepted daughters vs pT | |
259 | TH2F * fhPrimPi0Phi ; //! Azimutal distribution of primary particles vs pT | |
260 | TH2F * fhPrimPi0AccPhi; //! Azimutal distribution of primary with accepted daughters vs pT | |
261 | TH2F * fhPrimPi0OpeningAngle ; //! Opening angle of pair versus pair energy, primaries | |
262 | TH2F * fhPrimPi0OpeningAngleAsym ; //! Opening angle of pair versus pair E asymmetry, pi0 primaries | |
263 | TH2F * fhPrimPi0CosOpeningAngle ; //! Cosinus of opening angle of pair version pair energy, pi0 primaries | |
264 | TH2F * fhPrimPi0PtCentrality ; //! primary pi0 reconstructed centrality vs pT | |
265 | TH2F * fhPrimPi0PtEventPlane ; //! primary pi0 reconstructed event plane vs pT | |
266 | TH2F * fhPrimPi0AccPtCentrality ; //! primary pi0 with accepted daughters reconstructed centrality vs pT | |
267 | TH2F * fhPrimPi0AccPtEventPlane ; //! primary pi0 with accepted daughters reconstructed event plane vs pT | |
268 | ||
269 | //Eta acceptance | |
270 | TH1F * fhPrimEtaE ; //! Spectrum of Primary | |
271 | TH1F * fhPrimEtaPt ; //! Spectrum of Primary | |
272 | TH1F * fhPrimEtaPtRejected ; //! Spectrum of Primary, rejected | |
273 | TH1F * fhPrimEtaAccE ; //! Spectrum of primary with accepted daughters | |
274 | TH1F * fhPrimEtaAccPt ; //! Spectrum of primary with accepted daughters | |
275 | TH2F * fhPrimEtaY ; //! Rapidity distribution of primary particles vs pT | |
276 | TH2F * fhPrimEtaAccY ; //! Rapidity distribution of primary with accepted daughters vs pT | |
277 | TH2F * fhPrimEtaYeta ; //! PseudoRapidity distribution of primary particles vs pT | |
278 | TH2F * fhPrimEtaYetaYcut ; //! PseudoRapidity distribution of primary particles vs pT, Y<1 | |
279 | TH2F * fhPrimEtaAccYeta ; //! PseudoRapidity distribution of primary with accepted daughters vs pT | |
280 | TH2F * fhPrimEtaPhi ; //! Azimutal distribution of primary particles vs pT | |
281 | TH2F * fhPrimEtaAccPhi; //! Azimutal distribution of primary with accepted daughters vs pT | |
282 | TH2F * fhPrimEtaOpeningAngle ; //! Opening angle of pair versus pair energy, eta primaries | |
283 | TH2F * fhPrimEtaOpeningAngleAsym ; //! Opening angle of pair versus pair E asymmetry, eta primaries | |
284 | TH2F * fhPrimEtaCosOpeningAngle ; //! Cosinus of opening angle of pair version pair energy, eta primaries | |
285 | TH2F * fhPrimEtaPtCentrality ; //! primary eta reconstructed centrality vs pT | |
286 | TH2F * fhPrimEtaPtEventPlane ; //! primary eta reconstructed event plane vs pT | |
287 | TH2F * fhPrimEtaAccPtCentrality ; //! primary eta with accepted daughters reconstructed centrality vs pT | |
288 | TH2F * fhPrimEtaAccPtEventPlane ; //! primary eta with accepted daughters reconstructed event plane vs pT | |
289 | ||
290 | // Primaries origin | |
291 | TH2F * fhPrimPi0PtOrigin ; //! Spectrum of generated pi0 vs mother | |
292 | TH2F * fhPrimEtaPtOrigin ; //! Spectrum of generated eta vs mother | |
293 | ||
294 | //Pair origin | |
295 | //Array of histograms ordered as follows: 0-Photon, 1-electron, 2-pi0, 3-eta, 4-a-proton, 5-a-neutron, 6-stable particles, | |
296 | // 7-other decays, 8-string, 9-final parton, 10-initial parton, intermediate, 11-colliding proton, 12-unrelated | |
297 | TH2F * fhMCOrgMass[13]; //! Mass vs pt of real pairs, check common origin of pair | |
298 | TH2F * fhMCOrgAsym[13]; //! Asymmetry vs pt of real pairs, check common origin of pair | |
299 | TH2F * fhMCOrgDeltaEta[13]; //! Delta Eta vs pt of real pairs, check common origin of pair | |
300 | TH2F * fhMCOrgDeltaPhi[13]; //! Delta Phi vs pt of real pairs, check common origin of pair | |
301 | ||
302 | //Multiple cuts in simulation, origin pi0 or eta | |
303 | TH2F ** fhMCPi0MassPtRec; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real pi0 pairs, reconstructed mass vs reconstructed pt of original pair | |
304 | TH2F ** fhMCPi0MassPtTrue; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real pi0 pairs, reconstructed mass vs generated pt of original pair | |
305 | TH2F ** fhMCPi0PtTruePtRec; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real pi0 pairs, reconstructed pt vs generated pt of pair | |
306 | TH2F ** fhMCEtaMassPtRec; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real eta pairs, reconstructed mass vs reconstructed pt of original pair | |
307 | TH2F ** fhMCEtaMassPtTrue; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real eta pairs, reconstructed mass vs generated pt of original pair | |
308 | TH2F ** fhMCEtaPtTruePtRec; //![fNPtCuts*fNAsymCuts*fNCellNCuts] Real eta pairs, reconstructed pt vs generated pt of pair | |
309 | ||
310 | TH2F * fhMCPi0PtOrigin ; //! Mass of reoconstructed pi0 pairs in calorimeter vs mother | |
311 | TH2F * fhMCEtaPtOrigin ; //! Mass of reoconstructed pi0 pairs in calorimeter vs mother | |
312 | ||
313 | TH2F * fhReMCFromConversion ; //! Invariant mass of 2 clusters originated in conversions | |
314 | TH2F * fhReMCFromNotConversion ; //! Invariant mass of 2 clusters not originated in conversions | |
315 | TH2F * fhReMCFromMixConversion ; //! Invariant mass of 2 clusters one from conversion and the other not | |
316 | ||
317 | TH2F * fhArmPrimPi0[4]; //! Armenteros plots for primary pi0 in 6 energy bins | |
318 | TH2F * fhArmPrimEta[4]; //! Armenteros plots for primary eta in 6 energy bins | |
319 | TH2F * fhCosThStarPrimPi0; //! cos(theta*) plots vs E for primary pi0, same as asymmetry ... | |
320 | TH2F * fhCosThStarPrimEta; //! cos(theta*) plots vs E for primary eta, same as asymmetry ... | |
321 | ||
322 | AliAnaPi0( const AliAnaPi0 & api0) ; // cpy ctor | |
323 | AliAnaPi0 & operator = (const AliAnaPi0 & api0) ; // cpy assignment | |
324 | ||
325 | ClassDef(AliAnaPi0,27) | |
326 | } ; | |
327 | ||
328 | ||
329 | #endif //ALIANAPI0_H | |
330 | ||
331 | ||
332 |