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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 | // | |
12 | //-- Author: Gustavo Conesa (LPSC-Grenoble) | |
13 | //_________________________________________________________________________ | |
14 | ||
15 | ||
16 | // --- ROOT system --- | |
17 | class TList ; | |
18 | class TObjString; | |
19 | class TLorentzVector; | |
20 | ||
21 | // --- ANALYSIS system --- | |
745913ae | 22 | #include "AliAnaCaloTrackCorrBaseClass.h" |
992b14a7 | 23 | |
745913ae | 24 | class AliAnaInsideClusterInvariantMass : public AliAnaCaloTrackCorrBaseClass { |
992b14a7 | 25 | |
26 | public: | |
27 | AliAnaInsideClusterInvariantMass() ; // default ctor | |
28 | virtual ~AliAnaInsideClusterInvariantMass() { ; } //virtual dtor | |
992b14a7 | 29 | |
992b14a7 | 30 | |
31 | TObjString * GetAnalysisCuts(); | |
32 | ||
33 | TList * GetCreateOutputObjects(); | |
34 | ||
243c2909 | 35 | TLorentzVector GetCellMomentum(const Int_t absId, Float_t energy, AliVCaloCells* cells) ; |
992b14a7 | 36 | |
992b14a7 | 37 | void Init(); |
38 | ||
39 | void InitParameters(); | |
40 | ||
41 | void MakeAnalysisFillHistograms() ; | |
992b14a7 | 42 | |
29ca9cad | 43 | void SetCalorimeter(TString & det) { fCalorimeter = det ; } |
dbba06ca | 44 | |
29ca9cad | 45 | void SetM02Cut(Float_t cut) { fM02Cut = cut ; } |
992b14a7 | 46 | |
5287b56e | 47 | void SetMinNCells(Int_t cut) { fMinNCells = cut ; } |
992b14a7 | 48 | |
243c2909 | 49 | void SetPi0MassRange(Float_t min, Float_t max) { fMassPi0Min = min ; fMassPi0Max = max ; } |
50 | void SetEtaMassRange(Float_t min, Float_t max) { fMassEtaMin = min ; fMassEtaMax = max ; } | |
51 | void SetConMassRange(Float_t min, Float_t max) { fMassConMin = min ; fMassConMax = max ; } | |
52 | ||
53 | void SplitEnergy(const Int_t absId1, const Int_t absId2, | |
54 | AliVCluster *cluster, | |
55 | AliVCaloCells* cells, | |
29ca9cad | 56 | Float_t & e1, Float_t & e2, |
57 | const Int_t nMax//, Int_t *absIdList, Float_t *maxEList, | |
58 | ); | |
992b14a7 | 59 | |
60 | void Print(const Option_t * opt) const; | |
61 | ||
62 | //For histograms | |
c5693f62 | 63 | enum mcTypes { kmcPhoton = 1, kmcConversion = 2, kmcPi0 = 3, |
64 | kmcEta = 4, kmcElectron = 5, kmcHadron = 6 }; | |
992b14a7 | 65 | |
66 | private: | |
67 | ||
68 | TString fCalorimeter ; // Calorimeter where the gamma is searched | |
29ca9cad | 69 | Float_t fM02Cut ; // Study clusters with l0 larger than cut |
e23a0471 | 70 | Int_t fMinNCells ; // Study clusters with ncells larger than cut |
243c2909 | 71 | Float_t fMassEtaMin; // Min Eta mass |
72 | Float_t fMassEtaMax; // Max Eta mass | |
73 | Float_t fMassPi0Min; // Min Pi0 mass | |
74 | Float_t fMassPi0Max; // Min Pi0 mass | |
75 | Float_t fMassConMin; // Min Conversions mass | |
76 | Float_t fMassConMax; // Min Conversions mass | |
77 | ||
992b14a7 | 78 | //Histograms |
79 | ||
80 | TH2F * fhMassNLocMax1[7] ; //! Mass of 2 highest energy cells when 1 local max, 1-6 for different MC particle types | |
81 | TH2F * fhMassNLocMax2[7] ; //! Mass of 2 cells local maxima vs E, 1-6 for different MC particle types | |
82 | TH2F * fhMassNLocMaxN[7] ; //! Mass of >2 cells local maxima vs E, 1-6 for different MC particle types | |
83 | ||
84 | TH2F * fhNLocMax[7] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types | |
29ca9cad | 85 | TH2F * fhNLocMaxEMax[7] ; //! Number of maxima in cluster vs E of each maxima, 1-6 for different MC particle types |
86 | TH2F * fhNLocMaxEFrac[7] ; //! Number of maxima in cluster vs fraction of cluster E of each maxima, 1-6 for different MC particle types | |
992b14a7 | 87 | TH2F * fhNLocMaxM02Cut[7]; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut |
88 | ||
89 | TH2F * fhM02NLocMax1[7] ; //! M02 vs E for N max in cluster = 1, 1-6 for different MC particle types | |
90 | TH2F * fhM02NLocMax2[7] ; //! M02 vs E for N max in cluster = 2, 1-6 for different MC particle types | |
91 | TH2F * fhM02NLocMaxN[7] ; //! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types | |
92 | ||
93 | TH2F * fhNCellNLocMax1[7] ; //! n cells in cluster vs E for N max in cluster = 1, 1-6 for different MC particle types | |
94 | TH2F * fhNCellNLocMax2[7] ; //! n cells in cluster vs E for N max in cluster = 2, 1-6 for different MC particle types | |
95 | TH2F * fhNCellNLocMaxN[7] ; //! n cells in cluster vs E for N max in cluster > 2, 1-6 for different MC particle types | |
96 | ||
243c2909 | 97 | TH2F * fhM02Pi0LocMax1[7] ; //! M02 for Mass around pi0, N Local Maxima = 1 |
98 | TH2F * fhM02EtaLocMax1[7] ; //! M02 for Mass around eta, N Local Maxima = 1 | |
99 | TH2F * fhM02ConLocMax1[7] ; //! M02 for Mass around close to 0, N Local Maxima = 1 | |
992b14a7 | 100 | |
243c2909 | 101 | TH2F * fhM02Pi0LocMax2[7] ; //! M02 for Mass around pi0, N Local Maxima = 2 |
102 | TH2F * fhM02EtaLocMax2[7] ; //! M02 for Mass around eta, N Local Maxima = 2 | |
103 | TH2F * fhM02ConLocMax2[7] ; //! M02 for Mass around close to 0, N Local Maxima = 2 | |
104 | ||
105 | TH2F * fhM02Pi0LocMaxN[7] ; //! M02 for Mass around pi0, N Local Maxima > 2 | |
106 | TH2F * fhM02EtaLocMaxN[7] ; //! M02 for Mass around eta, N Local Maxima > 2 | |
107 | TH2F * fhM02ConLocMaxN[7] ; //! M02 for Mass around close to 0, N Local Maxima > 2 | |
108 | ||
109 | AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & g) ; // cpy ctor | |
29ca9cad | 110 | AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & g) ; // cpy assignment |
992b14a7 | 111 | |
dbba06ca | 112 | ClassDef(AliAnaInsideClusterInvariantMass,5) |
992b14a7 | 113 | |
114 | } ; | |
115 | ||
116 | #endif //ALIANAINSIDECLUSTERINVARIANTMASS_H | |
117 | ||
118 | ||
119 |