Variables | |
tuple | TtSemiLepHypMVADisc |
00001 cms.EDProducer("TtSemiLepHypMVADisc", 00002 ## met input 00003 mets = cms.InputTag("patMETs"), 00004 ## jet input 00005 jets = cms.InputTag("selectedPatJets"), 00006 ##lepton input 00007 leps = cms.InputTag("selectedPatMuons"), 00008 ## jet combination chosen by MVA 00009 match = cms.InputTag("findTtSemiLepJetCombMVA"), 00010 ## number of considered jets 00011 nJetsConsidered = cms.InputTag("findTtSemiLepJetCombMVA","NumberOfConsideredJets"), 00012 ## specify jet correction level as, Uncorrected, L1Offset, L2Relative, L3Absolute, L4Emf, 00013 ## L5Hadron, L6UE, L7Parton, a flavor specification will be added automatically, when 00014 ## chosen 00015 jetCorrectionLevel = cms.string("L3Absolute"), 00016 ## different ways to calculate a neutrino pz: 00017 ## -1 : take MET as neutrino directly, i.e. pz = 0 00018 ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz; 00019 ## if two real solutions... 00020 ## 0 : take the one closer to the lepton pz if neutrino pz < 300 GeV, 00021 ## otherwise the more central one 00022 ## 1 : always take the one closer to the lepton pz 00023 ## 2 : always take the more central one, i.e. minimize neutrino pz 00024 ## 3 : maximize the cosine of the angle between lepton and reconstructed W 00025 ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex 00026 neutrinoSolutionType = cms.int32(-1) 00027 )
Definition at line 6 of file TtSemiLepHypMVADisc_cfi.py.