1 #ifndef ALIANAINSIDECLUSTERINVARIANTMASS_H
2 #define ALIANAINSIDECLUSTERINVARIANTMASS_H
3 /* Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. *
4 * See cxx source for full Copyright notice */
6 //_________________________________________________________________________
8 // Split clusters with some criteria and calculate invariant mass
9 // to identify them as pi0 or conversion
12 //-- Author: Gustavo Conesa (LPSC-Grenoble)
13 //_________________________________________________________________________
16 // --- ROOT system ---
21 // --- ANALYSIS system ---
22 class AliAODCaloCluster;
24 #include "AliAnaCaloTrackCorrBaseClass.h"
26 class AliAnaInsideClusterInvariantMass : public AliAnaCaloTrackCorrBaseClass {
30 AliAnaInsideClusterInvariantMass() ; // default ctor
31 virtual ~AliAnaInsideClusterInvariantMass() { ; } //virtual dtor
33 TObjString * GetAnalysisCuts();
35 TList * GetCreateOutputObjects();
39 void InitParameters();
41 void MakeAnalysisFillHistograms() ;
43 void Print(const Option_t * opt) const;
45 void SetCalorimeter(TString & det) { fCalorimeter = det ; }
47 void SetM02Cut(Float_t min=0, Float_t max=10) { fM02MinCut = min ; fM02MaxCut = max ; }
49 void SetMinNCells(Int_t cut) { fMinNCells = cut ; }
51 void SetMinBadChannelDistance(Float_t cut) { fMinBadDist = cut ; }
53 void SwitchOnFillAngleHistograms() { fFillAngleHisto = kTRUE ; }
54 void SwitchOffFillAngleHistograms() { fFillAngleHisto = kFALSE ; }
56 void SwitchOnFillExtraSSHistograms() { fFillSSExtraHisto = kTRUE ; }
57 void SwitchOffFillExtraSSHistograms() { fFillSSExtraHisto = kFALSE ; }
59 void SwitchOnFillTMResidualHistograms() { fFillTMResidualHisto = kTRUE ; }
60 void SwitchOffFillTMResidualHistograms() { fFillTMResidualHisto = kFALSE ; }
62 void SwitchOnMCFractionHistograms() { fFillMCFractionHisto = kTRUE ; }
63 void SwitchOffMCFractionHistograms() { fFillMCFractionHisto = kFALSE ; }
67 enum mcTypes { kmcPhoton = 1, kmcConversion = 2, kmcPi0 = 3,
68 kmcEta = 4, kmcElectron = 5, kmcHadron = 6, kmcPi0Conv = 7 };
72 TString fCalorimeter ; // Calorimeter where the gamma is searched
73 Float_t fM02MaxCut ; // Study clusters with l0 smaller than cut
74 Float_t fM02MinCut ; // Study clusters with l0 larger than cut
75 Int_t fMinNCells ; // Study clusters with ncells larger than cut
76 Float_t fMinBadDist ; // Minimal distance to bad channel to accept cluster
78 Bool_t fFillAngleHisto; // Fill splitted clusters angle histograms
79 Bool_t fFillTMResidualHisto ; // Fill track matching histos, residuals
80 Bool_t fFillSSExtraHisto ; // Fill shower shape extra histos
81 Bool_t fFillMCFractionHisto ; // Fill MC energy fraction histos
85 TH2F * fhMassNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
86 TH2F * fhMassNLocMax2[8][2] ; //! Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
87 TH2F * fhMassNLocMaxN[8][2] ; //! Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
89 TH2F * fhAsymNLocMax1[8][2] ; //! Asymmetry of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
90 TH2F * fhAsymNLocMax2[8][2] ; //! Asymmetry of 2 cells local maxima vs E, 1-6 for different MC particle types
91 TH2F * fhAsymNLocMaxN[8][2] ; //! Asymmetry of >2 cells local maxima vs E, 1-6 for different MC particle types
93 TH2F * fhSplitEFractionvsAsyNLocMax1[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1 vs |A|
94 TH2F * fhSplitEFractionvsAsyNLocMax2[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2 vs |A|
95 TH2F * fhSplitEFractionvsAsyNLocMaxN[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2 vs |A|
97 TH2F * fhMassM02CutNLocMax1 ; //! M02(E) selection, not matched, Mass of split clusters, NLM = 1
98 TH2F * fhMassM02CutNLocMax2 ; //! M02(E) selection, not matched, Mass of split clusters, NLM = 1
99 TH2F * fhMassM02CutNLocMaxN ; //! M02(E) selection, not matched, Mass of split clusters, NLM > 2
101 TH2F * fhAsymM02CutNLocMax1 ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM = 1
102 TH2F * fhAsymM02CutNLocMax2 ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM = 2
103 TH2F * fhAsymM02CutNLocMaxN ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM > 2
105 TH2F * fhMassSplitECutNLocMax1 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
106 TH2F * fhMassSplitECutNLocMax2 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
107 TH2F * fhMassSplitECutNLocMaxN ; //! 85% of split energy, not matched, Mass of split clusters, NLM > 2
109 TH2F * fhMassM02NLocMax1[8][2] ; //! Mass of splitted clusters when 1 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
110 TH2F * fhMassM02NLocMax2[8][2] ; //! Mass of splitted clusters when 2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
111 TH2F * fhMassM02NLocMaxN[8][2] ; //! Mass of splitted clusters when >2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
113 TH2F * fhMassM02NLocMax1Ebin[4] ; //! Mass of splitted clusters when 1 local max vs M02, 4 E bins, neutral clusters
114 TH2F * fhMassM02NLocMax2Ebin[4] ; //! Mass of splitted clusters when 2 local max vs M02, 4 E bins, neutral clusters
115 TH2F * fhMassM02NLocMaxNEbin[4] ; //! Mass of splitted clusters when >2 local max vs M02, 4 E bins, neutral clusters
117 TH2F * fhMassAsyNLocMax1Ebin[4] ; //! Mass of Mass of splitted clusters when 1 local max vs asymmetry, 4 E bins, neutral clusters
118 TH2F * fhMassAsyNLocMax2Ebin[4] ; //! Mass of Mass of splitted clusters when 2 local max vs asymmetry, 4 E bins, neutral clusters
119 TH2F * fhMassAsyNLocMaxNEbin[4] ; //! Mass of Mass of splitted clusters when >2 local max vs asymmetry, 4 E bins, neutral clusters
121 TH2F * fhAsyMCGenRecoNLocMax1EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 1 local max, 4 E bins, neutral clusters
122 TH2F * fhAsyMCGenRecoNLocMax2EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 2 local max, 4 E bins, neutral clusters
123 TH2F * fhAsyMCGenRecoNLocMaxNEbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when >2 local max, 4 E bins, neutral clusters
125 TH2F * fhMassDispEtaNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
126 TH2F * fhMassDispEtaNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
127 TH2F * fhMassDispEtaNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
129 TH2F * fhMassDispEtaNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
130 TH2F * fhMassDispEtaNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
131 TH2F * fhMassDispEtaNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
133 TH2F * fhMassDispPhiNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
134 TH2F * fhMassDispPhiNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
135 TH2F * fhMassDispPhiNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
137 TH2F * fhMassDispPhiNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
138 TH2F * fhMassDispPhiNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
139 TH2F * fhMassDispPhiNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
141 TH2F * fhMassDispAsyNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
142 TH2F * fhMassDispAsyNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
143 TH2F * fhMassDispAsyNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
145 TH2F * fhMassDispAsyNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
146 TH2F * fhMassDispAsyNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
147 TH2F * fhMassDispAsyNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
149 TH2F * fhNLocMax [8][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types
150 TH2F * fhNLocMaxM02Cut[8][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
152 TH2F * fhM02NLocMax1 [8][2] ; //! M02 vs E for N max in cluster = 1, 1-6 for different MC particle types
153 TH2F * fhM02NLocMax2 [8][2] ; //! M02 vs E for N max in cluster = 2, 1-6 for different MC particle types
154 TH2F * fhM02NLocMaxN [8][2] ; //! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types
156 TH2F * fhMCAsymM02NLocMax1MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 1, for 4 energy bins
157 TH2F * fhMCAsymM02NLocMax2MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 2, for 4 energy bins
158 TH2F * fhMCAsymM02NLocMaxNMCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster > 2, for 4 energy bins
160 TH2F * fhMCGenFracNLocMax1[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
161 TH2F * fhMCGenFracNLocMax2[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
162 TH2F * fhMCGenFracNLocMaxN[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
164 TH2F * fhMCGenFracAfterCutsNLocMax1MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, MCPi0 after M02 and asymmetry cut
165 TH2F * fhMCGenFracAfterCutsNLocMax2MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, MCPi0, after M02 and asymmetry cut
166 TH2F * fhMCGenFracAfterCutsNLocMaxNMCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, MCPi0, after M02 and asymmetry cut
168 TH2F * fhMCGenSplitEFracNLocMax1[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
169 TH2F * fhMCGenSplitEFracNLocMax2[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
170 TH2F * fhMCGenSplitEFracNLocMaxN[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
172 TH2F * fhMCGenSplitEFracAfterCutsNLocMax1MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
173 TH2F * fhMCGenSplitEFracAfterCutsNLocMax2MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
174 TH2F * fhMCGenSplitEFracAfterCutsNLocMaxNMCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
176 TH2F * fhMCGenEFracvsSplitEFracNLocMax1[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 1, MC pi0
177 TH2F * fhMCGenEFracvsSplitEFracNLocMax2[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 2, MC pi0
178 TH2F * fhMCGenEFracvsSplitEFracNLocMaxN[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster > 2, MC pi0
180 TH2F * fhMCGenEvsSplitENLocMax1[8][2] ; //! E generated particle vs E1+E2 for N max in cluster = 1, 1-6 for different MC particle types
181 TH2F * fhMCGenEvsSplitENLocMax2[8][2] ; //! E generated particle vs E1+E2 for N max in cluster = 2, 1-6 for different MC particle types
182 TH2F * fhMCGenEvsSplitENLocMaxN[8][2] ; //! E generated particle vs E1+E2 for N max in cluster > 2, 1-6 for different MC particle types
184 TH2F * fhMCGenFracNLocMaxEbin[8][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, not matched to track
185 TH2F * fhMCGenFracNLocMaxEbinMatched[8][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, matched to track
187 TH2F * fhM02MCGenFracNLocMax1Ebin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
188 TH2F * fhM02MCGenFracNLocMax2Ebin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
189 TH2F * fhM02MCGenFracNLocMaxNEbin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
191 TH2F * fhMassMCGenFracNLocMax1Ebin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
192 TH2F * fhMassMCGenFracNLocMax2Ebin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
193 TH2F * fhMassMCGenFracNLocMaxNEbin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
195 TH2F * fhNCellNLocMax1[8][2] ; //! n cells in cluster vs E for N max in cluster = 1, 1-6 for different MC particle types
196 TH2F * fhNCellNLocMax2[8][2] ; //! n cells in cluster vs E for N max in cluster = 2, 1-6 for different MC particle types
197 TH2F * fhNCellNLocMaxN[8][2] ; //! n cells in cluster vs E for N max in cluster > 2, 1-6 for different MC particle types
199 TH2F * fhM02Pi0LocMax1[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 1
200 TH2F * fhM02EtaLocMax1[8][2] ; //! M02 for Mass around eta, N Local Maxima = 1
201 TH2F * fhM02ConLocMax1[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 1
203 TH2F * fhM02Pi0LocMax2[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 2
204 TH2F * fhM02EtaLocMax2[8][2] ; //! M02 for Mass around eta, N Local Maxima = 2
205 TH2F * fhM02ConLocMax2[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 2
207 TH2F * fhM02Pi0LocMaxN[8][2] ; //! M02 for Mass around pi0, N Local Maxima > 2
208 TH2F * fhM02EtaLocMaxN[8][2] ; //! M02 for Mass around eta, N Local Maxima > 2
209 TH2F * fhM02ConLocMaxN[8][2] ; //! M02 for Mass around close to 0, N Local Maxima > 2
211 TH2F * fhMassPi0LocMax1[8][2] ; //! Mass for selected pi0, N Local Maxima = 1
212 TH2F * fhMassEtaLocMax1[8][2] ; //! Mass for selected around eta, N Local Maxima = 1
213 TH2F * fhMassConLocMax1[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 1
215 TH2F * fhMassPi0LocMax2[8][2] ; //! Mass for selected around pi0, N Local Maxima = 2
216 TH2F * fhMassEtaLocMax2[8][2] ; //! Mass for selected around eta, N Local Maxima = 2
217 TH2F * fhMassConLocMax2[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 2
219 TH2F * fhMassPi0LocMaxN[8][2] ; //! Mass for selected around pi0, N Local Maxima > 2
220 TH2F * fhMassEtaLocMaxN[8][2] ; //! Mass for selected around eta, N Local Maxima > 2
221 TH2F * fhMassConLocMaxN[8][2] ; //! Mass for selected around close to 0, N Local Maxima > 2
223 TH2F * fhMassAfterCutsNLocMax1[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 1, not matched
224 TH2F * fhMassAfterCutsNLocMax2[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 2, not matched
225 TH2F * fhMassAfterCutsNLocMaxN[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima > 2, not matched
227 TH2F * fhAsyPi0LocMax1[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
228 TH2F * fhAsyEtaLocMax1[8][2] ; //! Asy for Mass around eta, N Local Maxima = 1
229 TH2F * fhAsyConLocMax1[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 1
231 TH2F * fhAsyPi0LocMax2[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 2
232 TH2F * fhAsyEtaLocMax2[8][2] ; //! Asy for Mass around eta, N Local Maxima = 2
233 TH2F * fhAsyConLocMax2[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 2
235 TH2F * fhAsyPi0LocMaxN[8][2] ; //! Asy for Mass around pi0, N Local Maxima > 2
236 TH2F * fhAsyEtaLocMaxN[8][2] ; //! Asy for Mass around eta, N Local Maxima > 2
237 TH2F * fhAsyConLocMaxN[8][2] ; //! Asy for Mass around close to 0, N Local Maxima > 2
239 TH2F * fhSplitEFractionNLocMax1[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1
240 TH2F * fhSplitEFractionNLocMax2[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2
241 TH2F * fhSplitEFractionNLocMaxN[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2
243 TH2F * fhSplitEFractionAfterCutsNLocMax1 ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1, after M02 and asymmetry cut
244 TH2F * fhSplitEFractionAfterCutsNLocMax2 ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2, after M02 and asymmetry cut
245 TH2F * fhSplitEFractionAfterCutsNLocMaxN ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2, after M02 and asymmetry cut
247 TH2F * fhMassSplitEFractionNLocMax1Ebin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 1, 1-6 for different MC particle types, not track matched
248 TH2F * fhMassSplitEFractionNLocMax2Ebin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 2, 1-6 for different MC particle types, not track matched
249 TH2F * fhMassSplitEFractionNLocMaxNEbin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster > 2, 1-6 for different MC particle types, not track matched
251 TH2F * fhAnglePairLocMax1[2] ; //! pair opening angle vs E
252 TH2F * fhAnglePairLocMax2[2] ; //! pair opening angle vs E
253 TH2F * fhAnglePairLocMaxN[2] ; //! pair opening angle vs E
255 TH2F * fhAnglePairMassLocMax1[2] ; //! pair opening angle vs Mass for E > 7 GeV
256 TH2F * fhAnglePairMassLocMax2[2] ; //! pair opening angle vs Mass for E > 7 GeV
257 TH2F * fhAnglePairMassLocMaxN[2] ; //! pair opening angle vs Mass for E > 7 GeV
259 TH2F * fhTrackMatchedDEtaLocMax1[8] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
260 TH2F * fhTrackMatchedDPhiLocMax1[8] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
261 TH2F * fhTrackMatchedDEtaLocMax2[8] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
262 TH2F * fhTrackMatchedDPhiLocMax2[8] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
263 TH2F * fhTrackMatchedDEtaLocMaxN[8] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
264 TH2F * fhTrackMatchedDPhiLocMaxN[8] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
266 AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & split) ; // cpy ctor
267 AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & split) ; // cpy assignment
269 ClassDef(AliAnaInsideClusterInvariantMass,18)
273 #endif //ALIANAINSIDECLUSTERINVARIANTMASS_H