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File indexing completed on 2024-04-06 12:31:21
0001 import FWCore.ParameterSet.Config as cms 0002 0003 # 0004 # module to make the mvaDiscriminator hypothesis 0005 # 0006 ttSemiLepHypMVADisc = cms.EDProducer("TtSemiLepHypMVADisc", 0007 ## met input 0008 mets = cms.InputTag("patMETs"), 0009 ## jet input 0010 jets = cms.InputTag("selectedPatJets"), 0011 ##lepton input 0012 leps = cms.InputTag("selectedPatMuons"), 0013 ## jet combination chosen by MVA 0014 match = cms.InputTag("findTtSemiLepJetCombMVA"), 0015 ## number of considered jets 0016 nJetsConsidered = cms.InputTag("findTtSemiLepJetCombMVA","NumberOfConsideredJets"), 0017 ## specify jet correction level as, Uncorrected, L1Offset, L2Relative, L3Absolute, L4Emf, 0018 ## L5Hadron, L6UE, L7Parton, a flavor specification will be added automatically, when 0019 ## chosen 0020 jetCorrectionLevel = cms.string("L3Absolute"), 0021 ## different ways to calculate a neutrino pz: 0022 ## -1 : take MET as neutrino directly, i.e. pz = 0 0023 ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz; 0024 ## if two real solutions... 0025 ## 0 : take the one closer to the lepton pz if neutrino pz < 300 GeV, 0026 ## otherwise the more central one 0027 ## 1 : always take the one closer to the lepton pz 0028 ## 2 : always take the more central one, i.e. minimize neutrino pz 0029 ## 3 : maximize the cosine of the angle between lepton and reconstructed W 0030 ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex 0031 neutrinoSolutionType = cms.int32(-1) 0032 ) 0033 0034
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