fhMassNLocMax1[i][j] = 0;
fhMassNLocMax2[i][j] = 0;
fhMassNLocMaxN[i][j] = 0;
- fhArmNLocMax1[i][j] = 0;
- fhArmNLocMax2[i][j] = 0;
- fhArmNLocMaxN[i][j] = 0;
fhNLocMax[i][j] = 0;
fhNLocMaxM02Cut[i][j] = 0;
fhSplitClusterENLocMax [i][j] = 0;
fhMassPi0NLocMaxN[i][j] = 0;
fhMassEtaNLocMaxN[i][j] = 0;
fhMassConNLocMaxN[i][j] = 0;
-
- fhArmPi0NLocMax1[i][j] = 0;
- fhArmPi0NLocMax2[i][j] = 0;
- fhArmPi0NLocMaxN[i][j] = 0;
fhNCellPi0NLocMax1[i][j] = 0;
fhNCellEtaNLocMax1[i][j] = 0;
fhMassAfterCutsNLocMax2[i][j] = 0;
fhMassAfterCutsNLocMaxN[i][j] = 0;
- fhArmAfterCutsNLocMax1[i][j] = 0;
- fhArmAfterCutsNLocMax2[i][j] = 0;
- fhArmAfterCutsNLocMaxN[i][j] = 0;
fhSplitEFractionAfterCutsNLocMax1[i][j] = 0 ;
fhSplitEFractionAfterCutsNLocMax2[i][j] = 0 ;
}
+ for(Int_t i = 0; i < 7; i++)
+ {
+ for(Int_t j = 0; j < 4; j++)
+ {
+
+ fhArmNLocMax1[i][j] = 0;
+ fhArmNLocMax2[i][j] = 0;
+ fhArmNLocMaxN[i][j] = 0;
+
+ fhArmPi0NLocMax1[i][j] = 0;
+ fhArmPi0NLocMax2[i][j] = 0;
+ fhArmPi0NLocMaxN[i][j] = 0;
+
+ fhArmAfterCutsNLocMax1[i][j] = 0;
+ fhArmAfterCutsNLocMax2[i][j] = 0;
+ fhArmAfterCutsNLocMaxN[i][j] = 0;
+
+ }
+ }
+
InitParameters();
}
fhArmPi0NLocMaxN[0][ebin]->Fill(epsilon,alpha);
}
- if(IsDataMC() && mcIndex > 0 && mcIndex < 5)
+ if(IsDataMC() && mcIndex > 0 && mcIndex < 7)
{
if (nMax==1)
{
if(fFillArmenterosHisto)
{
- for(Int_t i = 0; i < 5; i++) // MC bin
+ for(Int_t i = 0; i < 7; i++) // MC bin
{
for(Int_t j = 0; j < 4; j++) // E bin
{
TH2F * fhAsymNLocMax2[7][2] ; //! Asymmetry of 2 cells local maxima vs E, 1-6 for different MC particle types
TH2F * fhAsymNLocMaxN[7][2] ; //! Asymmetry of >2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhArmNLocMax1[5][4] ; //! Armenteros of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhArmNLocMax2[5][4] ; //! Armenteros of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhArmNLocMaxN[5][4] ; //! Armenteros of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhArmNLocMax1[7][4] ; //! Armenteros of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
+ TH2F * fhArmNLocMax2[7][4] ; //! Armenteros of 2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhArmNLocMaxN[7][4] ; //! Armenteros of >2 cells local maxima vs E, 1-6 for different MC particle types
TH2F * fhSplitEFractionvsAsyNLocMax1[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1 vs |A|
TH2F * fhSplitEFractionvsAsyNLocMax2[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2 vs |A|
TH2F * fhMassEtaNLocMaxN[7][2] ; //! Mass for selected around eta, N Local Maxima > 2
TH2F * fhMassConNLocMaxN[7][2] ; //! Mass for selected around close to 0, N Local Maxima > 2
- TH2F * fhArmPi0NLocMax1[5][4] ; //! Armenteros for selected pi0, N Local Maxima = 1
- TH2F * fhArmPi0NLocMax2[5][4] ; //! Armenteros for selected pi0, N Local Maxima = 2
- TH2F * fhArmPi0NLocMaxN[5][4] ; //! Armenteros for selected pi0, N Local Maxima > 2
+ TH2F * fhArmPi0NLocMax1[7][4] ; //! Armenteros for selected pi0, N Local Maxima = 1
+ TH2F * fhArmPi0NLocMax2[7][4] ; //! Armenteros for selected pi0, N Local Maxima = 2
+ TH2F * fhArmPi0NLocMaxN[7][4] ; //! Armenteros for selected pi0, N Local Maxima > 2
TH2F * fhNCellPi0NLocMax1[7][2] ; //! n cells for selected around pi0, N Local Maxima = 1
TH2F * fhNCellEtaNLocMax1[7][2] ; //! n cells for selected around eta, N Local Maxima = 1
TH2F * fhMassAfterCutsNLocMax2[7][2] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 2
TH2F * fhMassAfterCutsNLocMaxN[7][2] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima > 2
- TH2F * fhArmAfterCutsNLocMax1[5][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 1
- TH2F * fhArmAfterCutsNLocMax2[5][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 2
- TH2F * fhArmAfterCutsNLocMaxN[5][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima > 2
+ TH2F * fhArmAfterCutsNLocMax1[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 1
+ TH2F * fhArmAfterCutsNLocMax2[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 2
+ TH2F * fhArmAfterCutsNLocMaxN[7][4] ; //! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima > 2
TH2F * fhAsyPi0NLocMax1[7][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
TH2F * fhAsyEtaNLocMax1[7][2] ; //! Asy for Mass around eta, N Local Maxima = 1