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992b14a7 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 */
992b14a7 5
6//_________________________________________________________________________
7//
8// Split clusters with some criteria and calculate invariant mass
9// to identify them as pi0 or conversion
10//
11//
83351853 12//-- Author: Gustavo Conesa (LPSC-Grenoble)
992b14a7 13//_________________________________________________________________________
14
15
16// --- ROOT system ---
17class TList ;
18class TObjString;
19class TLorentzVector;
20
21// --- ANALYSIS system ---
5c46c992 22class AliAODCaloCluster;
23
745913ae 24#include "AliAnaCaloTrackCorrBaseClass.h"
992b14a7 25
745913ae 26class AliAnaInsideClusterInvariantMass : public AliAnaCaloTrackCorrBaseClass {
992b14a7 27
28 public:
3c1d9afb 29
992b14a7 30 AliAnaInsideClusterInvariantMass() ; // default ctor
31 virtual ~AliAnaInsideClusterInvariantMass() { ; } //virtual dtor
992b14a7 32
b94e038e 33 void CheckLocalMaximaMCOrigin(AliVCluster* cluster, Int_t mcindex, Int_t noverlaps,
34 Float_t e1, Float_t e2, Float_t mass);
b583134f 35 //, Float_t m02, TLorentzVector l1, TLorentzVector l2);
b2e375c7 36
992b14a7 37 TObjString * GetAnalysisCuts();
38
39 TList * GetCreateOutputObjects();
dbe09c26 40
4914e781 41 void GetMCIndex(AliVCluster * cluster, Int_t & mcindex, Int_t & mcTag);
b2e375c7 42
b94e038e 43 void GetMCPrimaryKine(AliVCluster* cluster, Int_t mcindex, Int_t mcTag, Bool_t matched,
0186b6a2 44 Float_t & eprim, Float_t & asymGen, Float_t & angleGen, Int_t & noverlaps );
b2e375c7 45
b94e038e 46 void FillAngleHistograms(Int_t nMax, Bool_t matched, Int_t mcindex,
47 Float_t en, Float_t e1 , Float_t e2,
48 Float_t angle, Float_t mass, Float_t anglePrim,
49 Float_t m02, Float_t asym, Int_t pid, Int_t noverlaps);
b2e375c7 50
b94e038e 51 void FillArmenterosHistograms(Int_t nMax, Int_t ebin, Int_t mcindex,
1a8c88c1 52 Float_t pi0E, Float_t m02, Int_t pid);
cb99fa55 53
b94e038e 54 void FillThetaStarHistograms(Int_t nMax, Bool_t matched, Int_t mcindex,
1a8c88c1 55 Float_t pi0E, Float_t m02, Int_t pid);
29555e96 56
b94e038e 57 void FillEBinHistograms(Int_t ebin, Int_t nMax, Int_t mcindex, Float_t splitFrac,
58 Float_t mass, Float_t asym, Float_t l0);
59
60 void FillMCHistograms(Float_t en, Float_t e1 , Float_t e2,
61 Int_t ebin, Int_t mcindex,Int_t noverlaps,
62 Float_t l0, Float_t mass,
63 Int_t nMax, Bool_t matched,
64 Float_t splitFrac, Float_t asym,
65 Float_t eprim, Float_t asymGen);
66
67 void FillMCOverlapHistograms(Float_t en, Float_t enprim,
68 Int_t nc, Float_t mass, Float_t l0,
69 Float_t asym, Float_t splitFrac,
70 Int_t nlm, Int_t ebin, Bool_t matched,
71 Int_t mcindex, Int_t noverlaps);
72
73 void FillSSWeightHistograms(AliVCluster *cluster, Int_t nlm, Int_t absId1, Int_t absId2);
74
75 void FillSSExtraHistograms(AliVCluster *cluster, Int_t nMax,
76 Bool_t matched, Int_t mcindex,
77 Float_t mass , Int_t ebin);
4914e781 78
ff6aa4ce 79 void FillNLMDiffCutHistograms(AliVCluster *cluster, AliVCaloCells *cells, Bool_t matched);
80
b94e038e 81 void FillNCellHistograms(Int_t ncells, Float_t energy, Int_t nMax,
82 Bool_t matched, Int_t mcindex,
83 Float_t mass , Float_t l0);
b2e375c7 84
b94e038e 85 void FillTrackMatchingHistograms(AliVCluster * cluster,Int_t nMax, Int_t mcindex);
dbe09c26 86
b94e038e 87 void FillHistograms1(Float_t en, Float_t e1, Float_t e2,
88 Int_t nMax, Float_t mass, Float_t l0,
89 Float_t eta, Float_t phi,
90 Bool_t matched, Int_t mcindex);
1253480f 91
92
b94e038e 93 void FillHistograms2(Float_t en, Float_t eprim,
94 Float_t e1, Float_t e2, Int_t nMax,
95 Float_t mass, Float_t l0,
96 Bool_t matched, Int_t mcindex);
97
98 void FillIdPi0Histograms(Float_t en, Float_t e1, Float_t e2,
99 Int_t nc, Int_t nMax, Float_t t12diff,
100 Float_t mass, Float_t l0,
101 Float_t eta, Float_t phi,
102 Bool_t matched, Int_t mcindex);
103
104 void FillIdEtaHistograms(Float_t en, Float_t e1, Float_t e2,
105 Int_t nc, Int_t nMax, Float_t t12diff,
106 Float_t mass, Float_t l0,
107 Float_t eta, Float_t phi,
108 Bool_t matched, Int_t mcindex);
109
110 void FillIdConvHistograms(Float_t en, Int_t nMax, Float_t asym,
111 Float_t mass, Float_t l0,
112 Bool_t matched, Int_t mcindex);
1253480f 113
992b14a7 114 void Init();
115
116 void InitParameters();
1253480f 117
118 void MakeAnalysisFillHistograms() ;
119
71e3889f 120 void Print(const Option_t * opt) const;
1253480f 121
71e3889f 122 void SetMinNCells(Int_t cut) { fMinNCells = cut ; }
2cb134fb 123
124 void SetMinBadChannelDistance(Float_t cut) { fMinBadDist = cut ; }
992b14a7 125
09a5b22d 126 void SetWCorrectionParameter(Int_t i, Float_t p = 0.07) { if( i<2 ) fWSimu[i] = p; }
8edbd100 127
883411b2 128 void SwitchOnFillAngleHistograms() { fFillAngleHisto = kTRUE ; }
129 void SwitchOffFillAngleHistograms() { fFillAngleHisto = kFALSE ; }
cb99fa55 130
131 void SwitchOnFillArmenterosHistograms() { fFillArmenterosHisto = kTRUE ; }
132 void SwitchOffFillArmenterosHistograms() { fFillArmenterosHisto = kFALSE ; }
133
29555e96 134 void SwitchOnFillThetaStarHistograms() { fFillThetaStarHisto = kTRUE ; }
135 void SwitchOffFillThetaStarHistograms() { fFillThetaStarHisto = kFALSE ; }
136
883411b2 137 void SwitchOnFillExtraSSHistograms() { fFillSSExtraHisto = kTRUE ; }
138 void SwitchOffFillExtraSSHistograms() { fFillSSExtraHisto = kFALSE ; }
1253480f 139
140 void SwitchOnFillHighMultHistograms() { fFillHighMultHisto = kTRUE ; }
141 void SwitchOffFillHighMultHistograms() { fFillHighMultHisto = kFALSE ; }
142
143 void SwitchOnFillIdConvHistograms() { fFillIdConvHisto = kTRUE ; }
144 void SwitchOffFillIdConvHistograms() { fFillIdConvHisto = kFALSE ; }
8e81c2cf 145
1253480f 146 void SwitchOnFillIdEtaHistograms() { fFillIdEtaHisto = kTRUE ; }
147 void SwitchOffFillIdEtaHistograms() { fFillIdEtaHisto = kFALSE ; }
148
8edbd100 149 void SwitchOnFillTMHistograms() { fFillTMHisto = kTRUE ; }
150 void SwitchOffFillTMHistograms() { fFillTMHisto = kFALSE ; }
151
8e81c2cf 152 void SwitchOnFillTMResidualHistograms() { fFillTMResidualHisto = kTRUE ; }
153 void SwitchOffFillTMResidualHistograms() { fFillTMResidualHisto = kFALSE ; }
154
b2e375c7 155 void SwitchOnFillMCPrimaryHistograms() { fFillMCHisto = kTRUE ; }
156 void SwitchOffFillMCPrimaryHistograms() { fFillMCHisto = kFALSE ; }
2a77f6f4 157
19391b8c 158 void SwitchOnFillSSWeightHistograms() { fFillSSWeightHisto = kTRUE ; }
159 void SwitchOffFillSSWeightHistograms() { fFillSSWeightHisto = kFALSE ; }
160
ff6aa4ce 161 void SwitchOnFillNLMDiffCutsHistograms() { fFillNLMDiffCutHisto = kTRUE ; }
162 void SwitchOffFillNLMDiffCutsHistograms() { fFillNLMDiffCutHisto = kFALSE ; }
163
19391b8c 164 void SwitchOnFillEbinHistograms() { fFillEbinHisto = kTRUE ; }
165 void SwitchOffFillEbinHistograms() { fFillEbinHisto = kFALSE ; }
dbe09c26 166
b2e375c7 167 void SwitchOnFillMCOverlapHistograms() { fFillMCOverlapHisto = kTRUE ; }
168 void SwitchOffFillMCOverlapHistograms() { fFillMCOverlapHisto = kFALSE ; }
4914e781 169
170 void SwitchOnFillNCellHistograms() { fFillNCellHisto = kTRUE ; }
171 void SwitchOffFillNCellHistograms() { fFillNCellHisto = kFALSE ; }
b2e375c7 172
1253480f 173 void SwitchOnSplitClusterDistToBad() { fCheckSplitDistToBad = kTRUE ; }
174 void SwitchOffSplitClusterDistToBad() { fCheckSplitDistToBad = kFALSE ; }
175
ff6aa4ce 176 void SetNWeightForShowerShape(Int_t n) { fSSWeightN = n ; }
177 void SetWeightForShowerShape(Int_t i, Float_t v)
5cd814a9 178 { if (i < 20) fSSWeight[i] = v ; }
dbe09c26 179
ff6aa4ce 180 void SetNumberOfNLocMaxSettings(Int_t n) { fNLMSettingN = n ; }
181 void SetNLocMaxMinE (Int_t i, Float_t v) { if (i < 5) fNLMMinE [i] = v ; }
182 void SetNLocMaxMinDiff(Int_t i, Float_t v) { if (i < 5) fNLMMinDiff[i] = v ; }
183
184
185 void SetNECellCutForShowerShape(Int_t n) { fSSECellCutN = n ; }
186 void SetECellCutForShowerShape(Int_t i, Float_t v)
5cd814a9 187 { if (i < 20) fSSECellCut[i] = v ; }
19391b8c 188
1253480f 189
19391b8c 190 void RecalculateClusterShowerShapeParametersWithCellCut(const AliEMCALGeometry * geom, AliVCaloCells* cells, AliVCluster * cluster,
191 Float_t & l0, Float_t & l1,
192 Float_t & disp, Float_t & dEta, Float_t & dPhi,
193 Float_t & sEta, Float_t & sPhi, Float_t & sEtaPhi,Float_t eCellMin = 0.);
194
2a77f6f4 195
992b14a7 196 //For histograms
cb99fa55 197 enum mcTypes { kmcPhoton = 1, kmcConversion = 2, kmcPi0 = 3, kmcPi0Conv = 4,
198 kmcEta = 5, kmcHadron = 6 };
992b14a7 199
200 private:
201
3c1d9afb 202 Int_t fMinNCells ; // Study clusters with ncells larger than cut
203 Float_t fMinBadDist ; // Minimal distance to bad channel to accept cluster
b2e375c7 204 Float_t fHistoECut ; // Fixed E cut for some histograms
1253480f 205 Bool_t fCheckSplitDistToBad; // Check the distance to bad channel and to EMCal borders of split clusters
243c2909 206
883411b2 207 Bool_t fFillAngleHisto; // Fill splitted clusters angle histograms
8edbd100 208 Bool_t fFillTMHisto ; // Fill track matching histos,
8e81c2cf 209 Bool_t fFillTMResidualHisto ; // Fill track matching histos, residuals
210 Bool_t fFillSSExtraHisto ; // Fill shower shape extra histos
74e3eb22 211 Bool_t fFillMCHisto ; // Fill MC energy fraction histos
dbe09c26 212 Bool_t fFillSSWeightHisto ; // Fill weigth histograms
ff6aa4ce 213 Bool_t fFillNLMDiffCutHisto ; // Fill NLM histograms for different settings
19391b8c 214 Bool_t fFillEbinHisto ; // Fill E bin histograms
b2e375c7 215 Bool_t fFillMCOverlapHisto ; // Fill MC particles overlap histograms
4914e781 216 Bool_t fFillNCellHisto ; // Fill n cells in cluster dependent histograms
1253480f 217 Bool_t fFillIdConvHisto ; // Fill histograms for clusters identified as conversion
218 Bool_t fFillIdEtaHisto ; // Fill histograms for clusters identified as Eta
219 Bool_t fFillHighMultHisto; // Fill centrality/event plane histograms
cb99fa55 220 Bool_t fFillArmenterosHisto; // Fill armenteros type histo
29555e96 221 Bool_t fFillThetaStarHisto; // Fill cosThetaStar histos
1253480f 222
5cd814a9 223 Float_t fSSWeight[20]; // List of weights to test
19391b8c 224 Int_t fSSWeightN; // Total number of weights to test
225
5cd814a9 226 Float_t fSSECellCut[20]; // List of cell min energy cuts to test
19391b8c 227 Int_t fSSECellCutN; // Total number of cell min energy cuts to test
ff6aa4ce 228
229 Float_t fNLMMinE [5]; // List of local maxima min energy
230 Float_t fNLMMinDiff[5]; // List of local maxima min difference cell energy
231 Int_t fNLMSettingN; // Total number of NLM settings to test
dbe09c26 232
09a5b22d 233 Float_t fWSimu[2]; // Constant and slope of the linear correction factor for the shower
234 // shape weight in simulation, about 1-0.07*w
8edbd100 235
1a8c88c1 236 TLorentzVector fClusterMomentum; //! Cluster momentum
237 TLorentzVector fSubClusterMom1; //! Sub-Cluster momentum
238 TLorentzVector fSubClusterMom2; //! Sub-Cluster momentum
239 TLorentzVector fSubClusterMomSum; //! Sub-Cluster momentum sum, armenteros
240 TLorentzVector fSubClusterMomBoost; //! Sub-Cluster momentum boosted, armenteros
241
242 TLorentzVector fPrimaryMom; //! Primary momentum
243 TLorentzVector fGrandMotherMom; //! Primary momentum
244 TLorentzVector fMCDaughMom1; //! Primary momentum
245 TLorentzVector fMCDaughMom2; //! Primary momentum
246 TVector3 fProdVertex; //! primary production vertex
247
992b14a7 248 //Histograms
249
c7e9a4e9 250 TH2F * fhMassNLocMax1[7][2] ; //! Split Inv Mass vs cluster E, NLM=1, different MC particle types, track matching on/off
251 TH2F * fhMassNLocMax2[7][2] ; //! Split Inv Mass vs cluster E, NLM=2, different MC particle types, track matching on/off
252 TH2F * fhMassNLocMaxN[7][2] ; //! Split Inv Mass vs cluster E, NLM>2, different MC particle types, track matching on/off
5c46c992 253
c7e9a4e9 254 TH2F * fhMassSplitENLocMax1[7][2] ; //! Split Inv Mass vs E1+E2, NLM=1, different MC particle types, track matching on/off
255 TH2F * fhMassSplitENLocMax2[7][2] ; //! Split Inv Mass vs E1+E2, NLM=2, different MC particle types, track matching on/off
256 TH2F * fhMassSplitENLocMaxN[7][2] ; //! Split Inv Mass vs E1+E2, NLM>2, different MC particle types, track matching on/off
257
cb99fa55 258 TH2F * fhAsymNLocMax1[7][2] ; //! Asymmetry of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
259 TH2F * fhAsymNLocMax2[7][2] ; //! Asymmetry of 2 cells local maxima vs E, 1-6 for different MC particle types
260 TH2F * fhAsymNLocMaxN[7][2] ; //! Asymmetry of >2 cells local maxima vs E, 1-6 for different MC particle types
261
e671adc2 262 TH2F * fhSplitEFractionvsAsyNLocMax1[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1 vs |A|
263 TH2F * fhSplitEFractionvsAsyNLocMax2[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2 vs |A|
264 TH2F * fhSplitEFractionvsAsyNLocMaxN[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2 vs |A|
cb99fa55 265
2c36e041 266 TH2F * fhMassAsyCutNLocMax1 ; //! Mass(E) asym selection, not matched, Mass of split clusters, NLM = 1
267 TH2F * fhMassAsyCutNLocMax2 ; //! Mass(E) asym selection, not matched, Mass of split clusters, NLM = 1
268 TH2F * fhMassAsyCutNLocMaxN ; //! Mass(E) asym selection, not matched, Mass of split clusters, NLM > 2
cb99fa55 269
2c36e041 270 TH2F * fhM02AsyCutNLocMax1 ; //! M02(E) asym selection, not matched, M02, NLM = 1
271 TH2F * fhM02AsyCutNLocMax2 ; //! M02(E) asym selection, not matched, M02, NLM = 2
272 TH2F * fhM02AsyCutNLocMaxN ; //! M02(E) asym selection, not matched, M02, NLM > 2
e671adc2 273
2c36e041 274 TH2F * fhMassM02CutNLocMax1 ; //! Mass(E) M02 selection, not matched, Mass of split clusters, NLM = 1
275 TH2F * fhMassM02CutNLocMax2 ; //! Mass(E) M02 selection, not matched, Mass of split clusters, NLM = 1
276 TH2F * fhMassM02CutNLocMaxN ; //! Mass(E) M02 selection, not matched, Mass of split clusters, NLM > 2
2a77f6f4 277
2c36e041 278 TH2F * fhAsymM02CutNLocMax1 ; //! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM = 1
279 TH2F * fhAsymM02CutNLocMax2 ; //! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM = 2
280 TH2F * fhAsymM02CutNLocMaxN ; //! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM > 2
281
282 TH2F * fhMassEnCutNLocMax1 ; //! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
283 TH2F * fhMassEnCutNLocMax2 ; //! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
284 TH2F * fhMassEnCutNLocMaxN ; //! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2
285
286 TH2F * fhM02EnCutNLocMax1 ; //! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
287 TH2F * fhM02EnCutNLocMax2 ; //! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
288 TH2F * fhM02EnCutNLocMaxN ; //! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2
289
290 TH2F * fhAsymEnCutNLocMax1 ; //! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
291 TH2F * fhAsymEnCutNLocMax2 ; //! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
292 TH2F * fhAsymEnCutNLocMaxN ; //! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2
a6d3b0a8 293
294 TH2F * fhSplitEFracEnCutNLocMax1 ; //! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
295 TH2F * fhSplitEFracEnCutNLocMax2 ; //! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1
296 TH2F * fhSplitEFracEnCutNLocMaxN ; //! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2
e671adc2 297
77cadd95 298 TH2F * fhMassSplitECutNLocMax1 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
299 TH2F * fhMassSplitECutNLocMax2 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
300 TH2F * fhMassSplitECutNLocMaxN ; //! 85% of split energy, not matched, Mass of split clusters, NLM > 2
667432ef 301
cb99fa55 302 TH2F * fhMassM02NLocMax1[7][2] ; //! Mass of splitted clusters when 1 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
303 TH2F * fhMassM02NLocMax2[7][2] ; //! Mass of splitted clusters when 2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
304 TH2F * fhMassM02NLocMaxN[7][2] ; //! Mass of splitted clusters when >2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
0137016b 305
b8eb40fc 306 TH2F * fhMassM02NLocMax1Ebin[4] ; //! Mass of splitted clusters when 1 local max vs M02, 4 E bins, neutral clusters
307 TH2F * fhMassM02NLocMax2Ebin[4] ; //! Mass of splitted clusters when 2 local max vs M02, 4 E bins, neutral clusters
308 TH2F * fhMassM02NLocMaxNEbin[4] ; //! Mass of splitted clusters when >2 local max vs M02, 4 E bins, neutral clusters
309
310 TH2F * fhMassAsyNLocMax1Ebin[4] ; //! Mass of Mass of splitted clusters when 1 local max vs asymmetry, 4 E bins, neutral clusters
311 TH2F * fhMassAsyNLocMax2Ebin[4] ; //! Mass of Mass of splitted clusters when 2 local max vs asymmetry, 4 E bins, neutral clusters
312 TH2F * fhMassAsyNLocMaxNEbin[4] ; //! Mass of Mass of splitted clusters when >2 local max vs asymmetry, 4 E bins, neutral clusters
313
314 TH2F * fhAsyMCGenRecoNLocMax1EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 1 local max, 4 E bins, neutral clusters
315 TH2F * fhAsyMCGenRecoNLocMax2EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 2 local max, 4 E bins, neutral clusters
316 TH2F * fhAsyMCGenRecoNLocMaxNEbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when >2 local max, 4 E bins, neutral clusters
7b686344 317
b583134f 318 TH2F * fhAsyMCGenRecoDiffMCPi0[3]; //! reconstructed-generated asymmetry of splitted clusters vs E from pi0, for 3 NLM cases
319 TH2F * fhAsyMCGenRecoDiffMCPi0Conv[3]; //! reconstructed-generated asymmetry of splitted clusters vs E from converted pi0, for 3 NLM cases
320
cb99fa55 321 TH2F * fhMassDispEtaNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
322 TH2F * fhMassDispEtaNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
323 TH2F * fhMassDispEtaNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
d2655d46 324
e671adc2 325 TH2F * fhMassDispEtaNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
326 TH2F * fhMassDispEtaNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
327 TH2F * fhMassDispEtaNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
d2655d46 328
cb99fa55 329 TH2F * fhMassDispPhiNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
330 TH2F * fhMassDispPhiNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
331 TH2F * fhMassDispPhiNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
d2655d46 332
e671adc2 333 TH2F * fhMassDispPhiNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
334 TH2F * fhMassDispPhiNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
335 TH2F * fhMassDispPhiNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
d2655d46 336
cb99fa55 337 TH2F * fhMassDispAsyNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
338 TH2F * fhMassDispAsyNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
339 TH2F * fhMassDispAsyNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
d2655d46 340
e671adc2 341 TH2F * fhMassDispAsyNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
342 TH2F * fhMassDispAsyNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
343 TH2F * fhMassDispAsyNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
d2655d46 344
cb99fa55 345 TH2F * fhNLocMax [7][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types
346 TH2F * fhNLocMaxM02Cut[7][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
29555e96 347 TH2F * fhNLocMaxIdPi0 [7][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after pi0 selection
5c46c992 348
cb99fa55 349 TH2F * fhSplitClusterENLocMax[7][2] ; //! Number of maxima in cluster vs E of splitted clusters, 1-6 for different MC particle types
350 TH2F * fhSplitClusterEPi0NLocMax[7][2] ; //! Number of maxima in cluster vs E of splitted clusters when cluster id as pi0, 1-6 for different MC particle types
29555e96 351
352 TH2F * fhLM1NLocMax [7][2] ; //! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types
353 TH2F * fhLM1NLocMaxM02Cut[7][2] ; //! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
354 TH2F * fhLM1NLocMaxIdPi0 [7][2] ; //! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, pi0 selection
355
356 TH2F * fhLM2NLocMax [7][2] ; //! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types
357 TH2F * fhLM2NLocMaxM02Cut[7][2] ; //! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
358 TH2F * fhLM2NLocMaxIdPi0 [7][2] ; //! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, pi0 selection
cc909e6f 359
cb99fa55 360 TH2F * fhM02NLocMax1 [7][2] ; //! M02 vs E for N max in cluster = 1, 1-6 for different MC particle types
361 TH2F * fhM02NLocMax2 [7][2] ; //! M02 vs E for N max in cluster = 2, 1-6 for different MC particle types
362 TH2F * fhM02NLocMaxN [7][2] ; //! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types
8e81c2cf 363
e671adc2 364 TH2F * fhMCAsymM02NLocMax1MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 1, for 4 energy bins
365 TH2F * fhMCAsymM02NLocMax2MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 2, for 4 energy bins
366 TH2F * fhMCAsymM02NLocMaxNMCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster > 2, for 4 energy bins
8e81c2cf 367
cb99fa55 368 TH2F * fhMCGenFracNLocMax1[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
369 TH2F * fhMCGenFracNLocMax2[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
370 TH2F * fhMCGenFracNLocMaxN[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
4914e781 371
cb99fa55 372 TH2F * fhMCGenFracNLocMax1NoOverlap[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, no overlap found
373 TH2F * fhMCGenFracNLocMax2NoOverlap[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, no overlap found
374 TH2F * fhMCGenFracNLocMaxNNoOverlap[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, no overlap found
4914e781 375
b8eb40fc 376 TH2F * fhMCGenFracAfterCutsNLocMax1MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, MCPi0 after M02 and asymmetry cut
377 TH2F * fhMCGenFracAfterCutsNLocMax2MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, MCPi0, after M02 and asymmetry cut
378 TH2F * fhMCGenFracAfterCutsNLocMaxNMCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, MCPi0, after M02 and asymmetry cut
667432ef 379
cb99fa55 380 TH2F * fhMCGenSplitEFracNLocMax1[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
381 TH2F * fhMCGenSplitEFracNLocMax2[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
382 TH2F * fhMCGenSplitEFracNLocMaxN[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
667432ef 383
cb99fa55 384 TH2F * fhMCGenSplitEFracNLocMax1NoOverlap[7][2];//! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, no overlap
385 TH2F * fhMCGenSplitEFracNLocMax2NoOverlap[7][2];//! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, no overlap
386 TH2F * fhMCGenSplitEFracNLocMaxNNoOverlap[7][2];//! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, no overlap
4914e781 387
667432ef 388 TH2F * fhMCGenSplitEFracAfterCutsNLocMax1MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
389 TH2F * fhMCGenSplitEFracAfterCutsNLocMax2MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
390 TH2F * fhMCGenSplitEFracAfterCutsNLocMaxNMCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
bb2d339b 391
cb99fa55 392 TH2F * fhMCGenEFracvsSplitEFracNLocMax1[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 1, MC pi0
393 TH2F * fhMCGenEFracvsSplitEFracNLocMax2[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 2, MC pi0
394 TH2F * fhMCGenEFracvsSplitEFracNLocMaxN[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster > 2, MC pi0
bb2d339b 395
cb99fa55 396 TH2F * fhMCGenEvsSplitENLocMax1[7][2] ; //! E generated particle vs E1+E2 for N max in cluster = 1, 1-6 for different MC particle types
397 TH2F * fhMCGenEvsSplitENLocMax2[7][2] ; //! E generated particle vs E1+E2 for N max in cluster = 2, 1-6 for different MC particle types
398 TH2F * fhMCGenEvsSplitENLocMaxN[7][2] ; //! E generated particle vs E1+E2 for N max in cluster > 2, 1-6 for different MC particle types
bb2d339b 399
cb99fa55 400 TH2F * fhMCGenFracNLocMaxEbin[7][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, not matched to track
401 TH2F * fhMCGenFracNLocMaxEbinMatched[7][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, matched to track
53f2c382 402
cb99fa55 403 TH2F * fhM02MCGenFracNLocMax1Ebin[7][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
404 TH2F * fhM02MCGenFracNLocMax2Ebin[7][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
405 TH2F * fhM02MCGenFracNLocMaxNEbin[7][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
8e81c2cf 406
cb99fa55 407 TH2F * fhMassMCGenFracNLocMax1Ebin[7][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
408 TH2F * fhMassMCGenFracNLocMax2Ebin[7][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
409 TH2F * fhMassMCGenFracNLocMaxNEbin[7][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
8e81c2cf 410
cb99fa55 411 TH2F * fhNCellNLocMax1[7][2] ; //! n cells in cluster vs E for N max in cluster = 1, 1-6 for different MC particle types
412 TH2F * fhNCellNLocMax2[7][2] ; //! n cells in cluster vs E for N max in cluster = 2, 1-6 for different MC particle types
413 TH2F * fhNCellNLocMaxN[7][2] ; //! n cells in cluster vs E for N max in cluster > 2, 1-6 for different MC particle types
992b14a7 414
4914e781 415 TH2F * fhNCellMassEHighNLocMax1MCPi0 ; //! n cells in cluster vs mass for high energy clusters, for N max in cluster = 1, for MC pi0
416 TH2F * fhNCellM02EHighNLocMax1MCPi0 ; //! n cells in cluster vs m02 for high energy clusters, for N max in cluster = 1, for MC pi0
417 TH2F * fhNCellMassELowNLocMax1MCPi0 ; //! n cells in cluster vs mass for low energy clusters, for N max in cluster = 1, for MC pi0
418 TH2F * fhNCellM02ELowNLocMax1MCPi0 ; //! n cells in cluster vs m02 for low energy clusters, for N max in cluster = 1, for MC pi0
419
420 TH2F * fhNCellMassEHighNLocMax2MCPi0 ; //! n cells in cluster vs mass for high energy clusters, for N max in cluster = 2, for MC pi0
421 TH2F * fhNCellM02EHighNLocMax2MCPi0 ; //! n cells in cluster vs m02 for high energy clusters, for N max in cluster = 2, for MC pi0
422 TH2F * fhNCellMassELowNLocMax2MCPi0 ; //! n cells in cluster vs mass for low energy clusters, for N max in cluster = 2, for MC pi0
423 TH2F * fhNCellM02ELowNLocMax2MCPi0 ; //! n cells in cluster vs m02 for low energy clusters, for N max in cluster = 2, for MC pi0
424
425 TH2F * fhNCellMassEHighNLocMaxNMCPi0 ; //! n cells in cluster vs mass for high energy clusters, for N max in cluster > 2, for MC pi0
426 TH2F * fhNCellM02EHighNLocMaxNMCPi0 ; //! n cells in cluster vs m02 for high energy clusters, for N max in cluster > 2, for MC pi0
427 TH2F * fhNCellMassELowNLocMaxNMCPi0 ; //! n cells in cluster vs mass for low energy clusters, for N max in cluster > 2, for MC pi0
428 TH2F * fhNCellM02ELowNLocMaxNMCPi0 ; //! n cells in cluster vs m02 for low energy clusters, for N max in cluster > 2, for MC pi0
429
cb99fa55 430 TH2F * fhM02Pi0NLocMax1[7][2] ; //! M02 for Mass around pi0, N Local Maxima = 1
431 TH2F * fhM02EtaNLocMax1[7][2] ; //! M02 for Mass around eta, N Local Maxima = 1
432 TH2F * fhM02ConNLocMax1[7][2] ; //! M02 for Mass around close to 0, N Local Maxima = 1
c8710850 433
cb99fa55 434 TH2F * fhM02Pi0NLocMax2[7][2] ; //! M02 for Mass around pi0, N Local Maxima = 2
435 TH2F * fhM02EtaNLocMax2[7][2] ; //! M02 for Mass around eta, N Local Maxima = 2
436 TH2F * fhM02ConNLocMax2[7][2] ; //! M02 for Mass around close to 0, N Local Maxima = 2
5c46c992 437
cb99fa55 438 TH2F * fhM02Pi0NLocMaxN[7][2] ; //! M02 for Mass around pi0, N Local Maxima > 2
439 TH2F * fhM02EtaNLocMaxN[7][2] ; //! M02 for Mass around eta, N Local Maxima > 2
440 TH2F * fhM02ConNLocMaxN[7][2] ; //! M02 for Mass around close to 0, N Local Maxima > 2
fc01318e 441
cb99fa55 442 TH2F * fhMassPi0NLocMax1[7][2] ; //! Mass for selected pi0, N Local Maxima = 1
443 TH2F * fhMassEtaNLocMax1[7][2] ; //! Mass for selected around eta, N Local Maxima = 1
444 TH2F * fhMassConNLocMax1[7][2] ; //! Mass for selected around close to 0, N Local Maxima = 1
e671adc2 445
cb99fa55 446 TH2F * fhMassPi0NLocMax2[7][2] ; //! Mass for selected around pi0, N Local Maxima = 2
447 TH2F * fhMassEtaNLocMax2[7][2] ; //! Mass for selected around eta, N Local Maxima = 2
448 TH2F * fhMassConNLocMax2[7][2] ; //! Mass for selected around close to 0, N Local Maxima = 2
bb2d339b 449
cb99fa55 450 TH2F * fhMassPi0NLocMaxN[7][2] ; //! Mass for selected around pi0, N Local Maxima > 2
451 TH2F * fhMassEtaNLocMaxN[7][2] ; //! Mass for selected around eta, N Local Maxima > 2
452 TH2F * fhMassConNLocMaxN[7][2] ; //! Mass for selected around close to 0, N Local Maxima > 2
bb2d339b 453
cb99fa55 454 TH2F * fhNCellPi0NLocMax1[7][2] ; //! n cells for selected around pi0, N Local Maxima = 1
455 TH2F * fhNCellEtaNLocMax1[7][2] ; //! n cells for selected around eta, N Local Maxima = 1
456 TH2F * fhNCellPi0NLocMax2[7][2] ; //! n cells for selected around pi0, N Local Maxima = 2
457 TH2F * fhNCellEtaNLocMax2[7][2] ; //! n cells for selected around eta, N Local Maxima = 2
458 TH2F * fhNCellPi0NLocMaxN[7][2] ; //! n cells for selected around pi0, N Local Maxima > 2
459 TH2F * fhNCellEtaNLocMaxN[7][2] ; //! n cells for selected around eta, N Local Maxima > 2
460
c7e9a4e9 461 TH2F * fhMassAfterCutsNLocMax1[7][2] ; //! Mass after M02, asymmetry cuts for MC part, N Local Maxima = 1
462 TH2F * fhMassAfterCutsNLocMax2[7][2] ; //! Mass after M02, asymmetry cuts for MC part, N Local Maxima = 2
463 TH2F * fhMassAfterCutsNLocMaxN[7][2] ; //! Mass after M02, asymmetry cuts for MC part, N Local Maxima > 2
464
465 TH2F * fhMassSplitEAfterCutsNLocMax1[7][2] ; //! Split Inv Mass vs E1+E2, NLM=1, after M02, asymmetry cuts, different MC particle types, track matching on/off
466 TH2F * fhMassSplitEAfterCutsNLocMax2[7][2] ; //! Split Inv Mass vs E1+E2, NLM=2, after M02, asymmetry cuts, different MC particle types, track matching on/off
467 TH2F * fhMassSplitEAfterCutsNLocMaxN[7][2] ; //! Split Inv Mass vs E1+E2, NLM>2, after M02, asymmetry cuts, different MC particle types, track matching on/off
468
469 TH2F * fhMassSplitEPi0NLocMax1[7][2] ; //! Split Inv Mass vs E1+E2, NLM=1, after pi0 selection, different MC particle types, track matching on/off
470 TH2F * fhMassSplitEPi0NLocMax2[7][2] ; //! Split Inv Mass vs E1+E2, NLM=2, after pi0 selection, different MC particle types, track matching on/off
471 TH2F * fhMassSplitEPi0NLocMaxN[7][2] ; //! Split Inv Mass vs E1+E2, NLM>2, after pi0 selection, different MC particle types, track matching on/off
167f2534 472
cb99fa55 473 TH2F * fhAsyPi0NLocMax1[7][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
474 TH2F * fhAsyEtaNLocMax1[7][2] ; //! Asy for Mass around eta, N Local Maxima = 1
475 TH2F * fhAsyConNLocMax1[7][2] ; //! Asy for Mass around close to 0, N Local Maxima = 1
bb2d339b 476
cb99fa55 477 TH2F * fhAsyPi0NLocMax2[7][2] ; //! Asy for Mass around pi0, N Local Maxima = 2
478 TH2F * fhAsyEtaNLocMax2[7][2] ; //! Asy for Mass around eta, N Local Maxima = 2
479 TH2F * fhAsyConNLocMax2[7][2] ; //! Asy for Mass around close to 0, N Local Maxima = 2
fc01318e 480
cb99fa55 481 TH2F * fhAsyPi0NLocMaxN[7][2] ; //! Asy for Mass around pi0, N Local Maxima > 2
482 TH2F * fhAsyEtaNLocMaxN[7][2] ; //! Asy for Mass around eta, N Local Maxima > 2
483 TH2F * fhAsyConNLocMaxN[7][2] ; //! Asy for Mass around close to 0, N Local Maxima > 2
e671adc2 484
cb99fa55 485 TH2F * fhSplitEFractionNLocMax1[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1
486 TH2F * fhSplitEFractionNLocMax2[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2
487 TH2F * fhSplitEFractionNLocMaxN[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2
667432ef 488
cb99fa55 489 TH2F * fhSplitEFractionAfterCutsNLocMax1[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1, after M02 and asymmetry cut
490 TH2F * fhSplitEFractionAfterCutsNLocMax2[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2, after M02 and asymmetry cut
491 TH2F * fhSplitEFractionAfterCutsNLocMaxN[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2, after M02 and asymmetry cut
667432ef 492
cb99fa55 493 TH2F * fhMassSplitEFractionNLocMax1Ebin[7][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
494 TH2F * fhMassSplitEFractionNLocMax2Ebin[7][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
495 TH2F * fhMassSplitEFractionNLocMaxNEbin[7][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
5094c724 496
0186b6a2 497 TH2F * fhAnglePairNLocMax1[7][2] ; //! pair opening angle vs E
498 TH2F * fhAnglePairNLocMax2[7][2] ; //! pair opening angle vs E
499 TH2F * fhAnglePairNLocMaxN[7][2] ; //! pair opening angle vs E
c8710850 500
29555e96 501 TH2F * fhAnglePairAfterCutsNLocMax1[7][2] ; //! pair opening angle vs E
502 TH2F * fhAnglePairAfterCutsNLocMax2[7][2] ; //! pair opening angle vs E
503 TH2F * fhAnglePairAfterCutsNLocMaxN[7][2] ; //! pair opening angle vs E
504
505 TH2F * fhAnglePairPi0NLocMax1[7][2] ; //! pair opening angle vs E
506 TH2F * fhAnglePairPi0NLocMax2[7][2] ; //! pair opening angle vs E
507 TH2F * fhAnglePairPi0NLocMaxN[7][2] ; //! pair opening angle vs E
508
0186b6a2 509 TH2F * fhAnglePairMassNLocMax1[7][2] ; //! pair opening angle vs Mass for E > 7 GeV
510 TH2F * fhAnglePairMassNLocMax2[7][2] ; //! pair opening angle vs Mass for E > 7 GeV
511 TH2F * fhAnglePairMassNLocMaxN[7][2] ; //! pair opening angle vs Mass for E > 7 GeV
d261ae67 512
513 TH2F * fhAnglePairM02NLocMax1[7][2] ; //! pair opening angle vs M02 for E > 7 GeV
514 TH2F * fhAnglePairM02NLocMax2[7][2] ; //! pair opening angle vs M02 for E > 7 GeV
515 TH2F * fhAnglePairM02NLocMaxN[7][2] ; //! pair opening angle vs M02 for E > 7 GeV
0186b6a2 516
517 TH2F * fhAnglePairPrimPi0RecoNLocMax1; //! pair opening angle pi0 generated/reconstructed vs E
518 TH2F * fhAnglePairPrimPi0RecoNLocMax2; //! pair opening angle pi0 generated/reconstructed vs E
519 TH2F * fhAnglePairPrimPi0RecoNLocMaxN; //! pair opening angle pi0 generated/reconstructed vs E
520
29555e96 521 TH2F * fhAnglePairPrimPi0vsRecoNLocMax1; //! pair opening angle pi0 generated vs reconstructed
522 TH2F * fhAnglePairPrimPi0vsRecoNLocMax2; //! pair opening angle pi0 generated vs reconstructed
523 TH2F * fhAnglePairPrimPi0vsRecoNLocMaxN; //! pair opening angle pi0 generated vs reconstructed
524
4e5a94c5 525 TH2F * fhAnglePairOverM02NLocMax1[7][2]; //! pair opening angle / m02 vs E, NLM=1
526 TH2F * fhAnglePairOverM02NLocMax2[7][2]; //! pair opening angle / m02 vs E, NLM=2
527 TH2F * fhAnglePairOverM02NLocMaxN[7][2]; //! pair opening angle / m02 vs E, NLM=N
528
529 TH2F * fhAnglePairOverM02NLocMax1Overlap0[7][2];//! pair opening angle / m02 vs E, NLM=1
530 TH2F * fhAnglePairOverM02NLocMax2Overlap0[7][2];//! pair opening angle / m02 vs E, NLM=2
531 TH2F * fhAnglePairOverM02NLocMaxNOverlap0[7][2];//! pair opening angle / m02 vs E, NLM=N
532
533 TH2F * fhAnglePairPrimPi0OverM02NLocMax1; //! pair opening angle / m02 vs E, NLM=1, prim pi0
534 TH2F * fhAnglePairPrimPi0OverM02NLocMax2; //! pair opening angle / m02 vs E, NLM=2, prim pi0
535 TH2F * fhAnglePairPrimPi0OverM02NLocMaxN; //! pair opening angle / m02 vs E, NLM=N, prim pi0
536
29555e96 537 TH2F * fhArmNLocMax1[7][4] ; //! Armenteros of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
538 TH2F * fhArmNLocMax2[7][4] ; //! Armenteros of 2 cells local maxima vs E, 1-6 for different MC particle types
539 TH2F * fhArmNLocMaxN[7][4] ; //! Armenteros of >2 cells local maxima vs E, 1-6 for different MC particle types
540
541 TH2F * fhArmAfterCutsNLocMax1[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 1
542 TH2F * fhArmAfterCutsNLocMax2[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 2
543 TH2F * fhArmAfterCutsNLocMaxN[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima > 2
544
545 TH2F * fhArmPi0NLocMax1[7][4] ; //! Armenteros for selected pi0, N Local Maxima = 1
546 TH2F * fhArmPi0NLocMax2[7][4] ; //! Armenteros for selected pi0, N Local Maxima = 2
547 TH2F * fhArmPi0NLocMaxN[7][4] ; //! Armenteros for selected pi0, N Local Maxima > 2
548
549 TH2F * fhCosThStarNLocMax1[7][2] ; //! cos(theta^star) vs E, NLM=1
550 TH2F * fhCosThStarNLocMax2[7][2] ; //! cos(theta^star) vs E, NLM=2
551 TH2F * fhCosThStarNLocMaxN[7][2] ; //! cos(theta^star) vs E, NLM>2
552
553 TH2F * fhCosThStarAfterCutsNLocMax1[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry cuts, NLM=1
554 TH2F * fhCosThStarAfterCutsNLocMax2[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry cuts, NLM=2
555 TH2F * fhCosThStarAfterCutsNLocMaxN[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry cuts, NLM>2
556
557 TH2F * fhCosThStarPi0NLocMax1[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM=1
558 TH2F * fhCosThStarPi0NLocMax2[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM=2
559 TH2F * fhCosThStarPi0NLocMaxN[7][2] ; //! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM>2
c8710850 560
cb99fa55 561 TH2F * fhTrackMatchedDEtaNLocMax1[7] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
562 TH2F * fhTrackMatchedDPhiNLocMax1[7] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
563 TH2F * fhTrackMatchedDEtaNLocMax2[7] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
564 TH2F * fhTrackMatchedDPhiNLocMax2[7] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
565 TH2F * fhTrackMatchedDEtaNLocMaxN[7] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
566 TH2F * fhTrackMatchedDPhiNLocMaxN[7] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
567
568 TH2F * fhTrackMatchedDEtaNLocMax1Pos[7] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
569 TH2F * fhTrackMatchedDPhiNLocMax1Pos[7] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
570 TH2F * fhTrackMatchedDEtaNLocMax2Pos[7] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
571 TH2F * fhTrackMatchedDPhiNLocMax2Pos[7] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
572 TH2F * fhTrackMatchedDEtaNLocMaxNPos[7] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
573 TH2F * fhTrackMatchedDPhiNLocMaxNPos[7] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
574
575 TH2F * fhTrackMatchedDEtaNLocMax1Neg[7] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
576 TH2F * fhTrackMatchedDPhiNLocMax1Neg[7] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
577 TH2F * fhTrackMatchedDEtaNLocMax2Neg[7] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
578 TH2F * fhTrackMatchedDPhiNLocMax2Neg[7] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
579 TH2F * fhTrackMatchedDEtaNLocMaxNNeg[7] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
580 TH2F * fhTrackMatchedDPhiNLocMaxNNeg[7] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
b2e375c7 581
1253480f 582 TH2F * fhCentralityPi0NLocMax1 ; //! Centrality for selected pi0, N Local Maxima = 1
583 TH2F * fhCentralityEtaNLocMax1 ; //! Centrality for selected eta, N Local Maxima = 1
584 TH2F * fhCentralityPi0NLocMax2 ; //! Centrality for selected pi0, N Local Maxima = 2
585 TH2F * fhCentralityEtaNLocMax2 ; //! Centrality for selected eta, N Local Maxima = 2
586 TH2F * fhCentralityPi0NLocMaxN ; //! Centrality for selected pi0, N Local Maxima > 2
587 TH2F * fhCentralityEtaNLocMaxN ; //! Centrality for selected eta, N Local Maxima > 2
c8710850 588
589 TH2F * fhEventPlanePi0NLocMax1 ; //! Event plane for selected pi0, N Local Maxima = 1
590 TH2F * fhEventPlaneEtaNLocMax1 ; //! Event plane for selected eta, N Local Maxima = 1
591 TH2F * fhEventPlanePi0NLocMax2 ; //! Event plane for selected pi0, N Local Maxima = 2
592 TH2F * fhEventPlaneEtaNLocMax2 ; //! Event plane for selected eta, N Local Maxima = 2
593 TH2F * fhEventPlanePi0NLocMaxN ; //! Event plane for selected pi0, N Local Maxima > 2
594 TH2F * fhEventPlaneEtaNLocMaxN ; //! Event plane for selected eta, N Local Maxima > 2
595
9554fc65 596 TH2F * fhClusterEtaPhiNLocMax1 ; //! Eta vs Phi of clusters with N Local Maxima = 1, E > 8 GeV
597 TH2F * fhClusterEtaPhiNLocMax2 ; //! Eta vs Phi of clusters with N Local Maxima = 2, E > 8 GeV
598 TH2F * fhClusterEtaPhiNLocMaxN ; //! Eta vs Phi of clusters with N Local Maxima > 2, E > 8 GeV
599 TH2F * fhPi0EtaPhiNLocMax1 ; //! Eta vs Phi of pi0's with N Local Maxima = 1, E > 8 GeV
600 TH2F * fhPi0EtaPhiNLocMax2 ; //! Eta vs Phi of pi0's with N Local Maxima = 2, E > 8 GeV
601 TH2F * fhPi0EtaPhiNLocMaxN ; //! Eta vs Phi of pi0's with N Local Maxima > N, E > 8 GeV
602 TH2F * fhEtaEtaPhiNLocMax1 ; //! Eta vs Phi of eta's with N Local Maxima = 1, E > 8 GeV
603 TH2F * fhEtaEtaPhiNLocMax2 ; //! Eta vs Phi of eta's with N Local Maxima = 2, E > 8 GeV
604 TH2F * fhEtaEtaPhiNLocMaxN ; //! Eta vs Phi of eta's with N Local Maxima > N, E > 8 GeV
605
dbe09c26 606 TH2F * fhPi0CellE[3] ; //! pi0's energy vs cluster cell energy with NLM = 1, = 2, > 2
607 TH2F * fhPi0CellEFrac[3] ; //! pi0's energy vs cluster cell energy fraction with NLM = 1, = 2, > 2
608 TH2F * fhPi0CellLogEFrac[3] ; //! pi0's energy vs cluster log cell energy fraction with NLM = 1, = 2, > 2
19391b8c 609 TH2F * fhPi0CellEMaxEMax2Frac [3]; //! pi0's energy vs fraction of 2 main maxima energy with NLM = 1, = 2, > 2
610 TH2F * fhPi0CellEMaxClusterFrac [3]; //! pi0's energy vs energy fraction of main LM and cluster energy with NLM = 1, = 2, > 2
611 TH2F * fhPi0CellEMax2ClusterFrac[3]; //! pi0's energy vs energy fraction of second LM and cluster energy with NLM = 1, = 2, > 2
612 TH2F * fhPi0CellEMaxFrac [3]; //! pi0's energy vs energy fraction of main LM and cluster cell energy with NLM = 1, = 2, > 2
613 TH2F * fhPi0CellEMax2Frac [3]; //! pi0's energy vs energy fraction of second LM and cluster cell energy with NLM = 1, = 2, > 2
614
5cd814a9 615 TH2F * fhM02WeightPi0[3][20] ; //! M02 for selected pi0 with different weight, with NLM = 1, = 2, > 2
616 TH2F * fhM02ECellCutPi0[3][20] ; //! M02 for selected pi0 with different cut on cell energy, with NLM = 1, = 2, > 2
dbe09c26 617
a1fd1b69 618 TH2F * fhPi0EPairDiffTimeNLM1; //! E vs Pair of clusters time difference vs E, for selected pi0, NLM=1
619 TH2F * fhPi0EPairDiffTimeNLM2; //! E vs Pair of clusters time difference vs E, for selected pi0, NLM=2
620 TH2F * fhPi0EPairDiffTimeNLMN; //! E vs Pair of clusters time difference vs E, for selected pi0, NLM>2
621 TH2F * fhEtaEPairDiffTimeNLM1; //! E vs Pair of clusters time difference vs E, for selected eta, NLM=1
622 TH2F * fhEtaEPairDiffTimeNLM2; //! E vs Pair of clusters time difference vs E, for selected eta, NLM=2
623 TH2F * fhEtaEPairDiffTimeNLMN; //! E vs Pair of clusters time difference vs E, for selected eta, NLM>2
624
cb99fa55 625 TH2F * fhMCEM02Overlap0[3][7]; //! E vs M02 for different MC origin, no other MC particles contributes, neutral cluster
626 TH2F * fhMCEM02Overlap1[3][7]; //! E vs M02 for different MC origin, 1 other MC particles contributes, neutral cluster
627 TH2F * fhMCEM02OverlapN[3][7]; //! E vs M02 for different MC origin, N other MC particles contributes, neutral cluster
628 TH2F * fhMCEM02Overlap0Match[3][7]; //! E vs M02 for different MC origin, no other MC particles contributes, charged cluster
629 TH2F * fhMCEM02Overlap1Match[3][7]; //! E vs M02 for different MC origin, 1 other MC particles contributes, charged cluster
630 TH2F * fhMCEM02OverlapNMatch[3][7]; //! E vs M02 for different MC origin, N other MC particles contributes, charged cluster
631
632 TH2F * fhMCEMassOverlap0[3][7]; //! E vs Mass for different MC origin, no other MC particles contributes, neutral cluster
633 TH2F * fhMCEMassOverlap1[3][7]; //! E vs Mass for different MC origin, 1 other MC particles contributes, neutral cluster
634 TH2F * fhMCEMassOverlapN[3][7]; //! E vs Mass for different MC origin, N other MC particles contributes, neutral cluster
635 TH2F * fhMCEMassOverlap0Match[3][7]; //! E vs Mass for different MC origin, no other MC particles contributes, charged cluster
636 TH2F * fhMCEMassOverlap1Match[3][7]; //! E vs Mass for different MC origin, 1 other MC particles contributes, charged cluster
637 TH2F * fhMCEMassOverlapNMatch[3][7]; //! E vs Mass for different MC origin, N other MC particles contributes, charged cluster
638
639 TH2F * fhMCESplitEFracOverlap0[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, no other MC particles contributes, neutral cluster
640 TH2F * fhMCESplitEFracOverlap1[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, 1 other MC particles contributes, neutral cluster
641 TH2F * fhMCESplitEFracOverlapN[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, N other MC particles contributes, neutral cluster
642 TH2F * fhMCESplitEFracOverlap0Match[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, no other MC particles contributes, charged cluster
643 TH2F * fhMCESplitEFracOverlap1Match[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, 1 other MC particles contributes, charged cluster
644 TH2F * fhMCESplitEFracOverlapNMatch[3][7]; //! E vs sum of splitted cluster energy / cluster energy for different MC origin, N other MC particles contributes, charged cluster
645
646 TH2F * fhMCEAsymOverlap0[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, neutral cluster
647 TH2F * fhMCEAsymOverlap1[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, neutral cluster
648 TH2F * fhMCEAsymOverlapN[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, neutral cluster
649 TH2F * fhMCEAsymOverlap0Match[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, charged cluster
650 TH2F * fhMCEAsymOverlap1Match[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, charged cluster
651 TH2F * fhMCEAsymOverlapNMatch[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, charged cluster
652
653 TH2F * fhMCENCellOverlap0[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, neutral cluster
654 TH2F * fhMCENCellOverlap1[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, neutral cluster
655 TH2F * fhMCENCellOverlapN[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, neutral cluster
656 TH2F * fhMCENCellOverlap0Match[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, charged cluster
657 TH2F * fhMCENCellOverlap1Match[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, charged cluster
658 TH2F * fhMCENCellOverlapNMatch[3][7]; //! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, charged cluster
659
660 TH2F * fhMCEEpriOverlap0[3][7]; //! E reco vs primary for different MC origin, no other MC particles contributes, neutral cluster
661 TH2F * fhMCEEpriOverlap1[3][7]; //! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster
662 TH2F * fhMCEEpriOverlapN[3][7]; //! E reco vs primary for different MC origin, N other MC particles contributes, neutral cluster
663 TH2F * fhMCEEpriOverlap0Match[3][7]; //! E reco vs primary for different MC origin, no other MC particles contributes, charged cluster
664 TH2F * fhMCEEpriOverlap1Match[3][7]; //! E reco vs primary for different MC origin, 1 other MC particles contributes, charged cluster
665 TH2F * fhMCEEpriOverlapNMatch[3][7]; //! E reco vs primary for different MC origin, N other MC particles contributes, charged cluster
666
667 TH2F * fhMCEEpriOverlap0IdPi0[3][7]; //! E reco vs primary for different MC origin, no other MC particles contributes, neutral cluster, neutral clusters id as pi0
668 TH2F * fhMCEEpriOverlap1IdPi0[3][7]; //! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster, neutral clusters id as pi0
669 TH2F * fhMCEEpriOverlapNIdPi0[3][7]; //! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster, neutral clusters is as pi0
cc909e6f 670
b2e375c7 671 TH2F * fhMCPi0MassM02Overlap0[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, no other MC particles contributes, neutral cluster, 4 E bins
672 TH2F * fhMCPi0MassM02Overlap1[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, 1 other MC particles contributes, neutral cluster, 4 E bins
673 TH2F * fhMCPi0MassM02OverlapN[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, N other MC particles contributes, neutral cluster, 4 E bins
674 TH2F * fhMCPi0MassM02Overlap0Match[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, no other MC particles contributes, charged cluster, 4 E bins
675 TH2F * fhMCPi0MassM02Overlap1Match[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, 1 other MC particles contributes, charged cluster, 4 E bins
676 TH2F * fhMCPi0MassM02OverlapNMatch[3][4]; //! MC Pi0 M02 vs Mass for different MC origin, N other MC particles contributes, charged cluster, 4 E bins
677
cb99fa55 678 TH2F * fhMCENOverlaps[3][7]; //! E vs number of Overlaps in MC, neutral cluster
679 TH2F * fhMCENOverlapsMatch[3][7]; //! E vs number of Overlaps in MC, charged cluster
b2e375c7 680
681 TH2F * fhMCPi0HighNLMPair; //! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons
682 TH2F * fhMCPi0LowNLMPair; //! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons
683 TH2F * fhMCPi0AnyNLMPair; //! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons
684 TH2F * fhMCPi0NoneNLMPair; //! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons
b2e375c7 685 // No match between highest energy local maxima and highest energy MC particle
686 TH2F * fhMCPi0HighNLMPairNoMCMatch; //! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons
687 TH2F * fhMCPi0LowNLMPairNoMCMatch; //! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons
688 TH2F * fhMCPi0AnyNLMPairNoMCMatch; //! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons
689 TH2F * fhMCPi0NoneNLMPairNoMCMatch; //! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons
36769d30 690
691 TH2F * fhMCPi0HighNLMPairOverlap; //! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons, overlap
692 TH2F * fhMCPi0LowNLMPairOverlap; //! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons, overlap
693 TH2F * fhMCPi0AnyNLMPairOverlap; //! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons, overlap
694 TH2F * fhMCPi0NoneNLMPairOverlap; //! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons, overlap
695 // No match between highest energy local maxima and highest energy MC particle
696 TH2F * fhMCPi0HighNLMPairNoMCMatchOverlap; //! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons, overlap
697 TH2F * fhMCPi0LowNLMPairNoMCMatchOverlap; //! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons, overlap
698 TH2F * fhMCPi0AnyNLMPairNoMCMatchOverlap; //! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons, overlap
699 TH2F * fhMCPi0NoneNLMPairNoMCMatchOverlap; //! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons, overlap
700
83351853 701 TH2F * fhMCPi0DecayPhotonHitHighLM; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
702 TH2F * fhMCPi0DecayPhotonAdjHighLM; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
703 TH2F * fhMCPi0DecayPhotonHitOtherLM; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
704 TH2F * fhMCPi0DecayPhotonAdjOtherLM; //! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
36769d30 705 TH2F * fhMCPi0DecayPhotonAdjacent; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM
83351853 706 TH2F * fhMCPi0DecayPhotonHitNoLM; //! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas
b2e375c7 707
36769d30 708 TH2F * fhMCPi0DecayPhotonHitHighLMOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maxima, overlap
709 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
710 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
711 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
712 TH2F * fhMCPi0DecayPhotonAdjacentOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM, overlap
713 TH2F * fhMCPi0DecayPhotonHitNoLMOverlap; //! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas, overlap
714
b583134f 715 TH2F * fhMCPi0DecayPhotonHitHighLMDiffELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
716 TH2F * fhMCPi0DecayPhotonAdjHighLMDiffELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
717 TH2F * fhMCPi0DecayPhotonHitOtherLMDiffELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
718 TH2F * fhMCPi0DecayPhotonAdjOtherLMDiffELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
719
720 TH2F * fhMCPi0DecayPhotonHitHighLMOverlapDiffELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
721 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
722 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
723 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
724
725 TH2F * fhMCPi0DecayPhotonHitHighLMDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
726 TH2F * fhMCPi0DecayPhotonAdjHighLMDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
727 TH2F * fhMCPi0DecayPhotonHitOtherLMDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
728 TH2F * fhMCPi0DecayPhotonAdjOtherLMDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
729
730 TH2F * fhMCPi0DecayPhotonHitHighLMOverlapDiffELM2[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
731 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
732 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
733 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
29555e96 734
735
736 TH2F * fhMCPi0DecayPhotonHitHighLMDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
737 TH2F * fhMCPi0DecayPhotonAdjHighLMDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
738 TH2F * fhMCPi0DecayPhotonHitOtherLMDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
739 TH2F * fhMCPi0DecayPhotonAdjOtherLMDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
740
741 TH2F * fhMCPi0DecayPhotonHitHighLMOverlapDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
742 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
743 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
744 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM1vsELM1[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
745
746 TH2F * fhMCPi0DecayPhotonHitHighLMDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
747 TH2F * fhMCPi0DecayPhotonAdjHighLMDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
748 TH2F * fhMCPi0DecayPhotonHitOtherLMDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
749 TH2F * fhMCPi0DecayPhotonAdjOtherLMDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
750
751 TH2F * fhMCPi0DecayPhotonHitHighLMOverlapDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
752 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
753 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
754 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM2vsELM2[3]; //! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
755
b583134f 756
757 TH2F * fhMCPi0DecayPhotonHitHighLMMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maxima
758 TH2F * fhMCPi0DecayPhotonAdjHighLMMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima
759 TH2F * fhMCPi0DecayPhotonHitOtherLMMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high
760 TH2F * fhMCPi0DecayPhotonAdjOtherLMMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high
761 TH2F * fhMCPi0DecayPhotonAdjacentMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM
762 TH2F * fhMCPi0DecayPhotonHitNoLMMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas
763
764 TH2F * fhMCPi0DecayPhotonHitHighLMOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maxima, overlap
765 TH2F * fhMCPi0DecayPhotonAdjHighLMOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap
766 TH2F * fhMCPi0DecayPhotonHitOtherLMOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap
767 TH2F * fhMCPi0DecayPhotonAdjOtherLMOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap
768 TH2F * fhMCPi0DecayPhotonAdjacentOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM, overlap
769 TH2F * fhMCPi0DecayPhotonHitNoLMOverlapMass[3]; //! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas, overlap
770
771
b2e375c7 772 TH2F * fhMCEOverlapType; //! what particles overlap with pi0, neutral clusters
773 TH2F * fhMCEOverlapTypeMatch; //! what particles overlap with pi0, charged clusters
dbe09c26 774
ce49dd72 775 TH2F * fhMassBadDistClose[3]; //! split mass of clusters with second LM close to bad channel
776 TH2F * fhM02BadDistClose[3]; //! m02 of clusters with second LM close to bad channel
777 TH2F * fhMassOnBorder[3]; //! split mass of clusters with second LM on EMCAL border
778 TH2F * fhM02OnBorder[3]; //! m02 of clusters with second LM close to EMCAL border
ce49dd72 779
ff6aa4ce 780
781 TH2F * fhNLocMaxDiffCut [5][5] [2] ; //! Number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks
782 TH2F * fhM02NLocMaxDiffCut[5][5][3][2] ; //! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks
58a18c5d 783 TH2F * fhMassNLocMaxDiffCut[5][5][3][2] ; //! Mass for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks
ff6aa4ce 784
58a18c5d 785 TH2F * fhNLocMaxDiffCutPi0 [5][5] [2] ; //! Number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks, cluster selected as pi0
786 TH2F * fhM02NLocMaxDiffCutPi0[5][5][3][2] ; //! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks, cluster selected as pi0
787 TH2F * fhMassNLocMaxDiffCutPi0[5][5][3][2] ; //! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks
ff6aa4ce 788
2a77f6f4 789 AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & split) ; // cpy ctor
790 AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & split) ; // cpy assignment
992b14a7 791
5cd814a9 792 ClassDef(AliAnaInsideClusterInvariantMass,30)
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794} ;
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796#endif //ALIANAINSIDECLUSTERINVARIANTMASS_H
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