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File indexing completed on 2023-03-17 11:26:12
0001 import FWCore.ParameterSet.Config as cms 0002 0003 # 0004 # module to make the WMassDeltaTopMass jet combination 0005 # 0006 findTtSemiLepJetCombWMassDeltaTopMass = cms.EDProducer("TtSemiLepJetCombWMassDeltaTopMass", 0007 ## jet input 0008 jets = cms.InputTag("selectedPatJets"), 0009 ## lepton input 0010 leps = cms.InputTag("selectedPatMuons"), 0011 ## met input 0012 mets = cms.InputTag("patMETs"), 0013 maxNJets = cms.int32(4), 0014 ## nominal WMass parameter (in GeV) 0015 wMass = cms.double(80.4), 0016 ## use b-tagging two distinguish between light and b jets 0017 useBTagging = cms.bool(False), 0018 ## choose algorithm for b-tagging 0019 bTagAlgorithm = cms.string("trackCountingHighEffBJetTags"), 0020 ## minimum b discriminator value required for b jets and 0021 ## maximum b discriminator value allowed for non-b jets 0022 minBDiscBJets = cms.double(1.0), 0023 maxBDiscLightJets = cms.double(3.0), 0024 ## different ways to calculate a neutrino pz: 0025 ## -1 : take MET as neutrino directly, i.e. pz = 0 0026 ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz; 0027 ## if two real solutions... 0028 ## 0 : take the one closer to the lepton pz if neutrino pz < 300 GeV, 0029 ## otherwise the more central one 0030 ## 1 : always take the one closer to the lepton pz 0031 ## 2 : always take the more central one, i.e. minimize neutrino pz 0032 ## 3 : maximize the cosine of the angle between lepton and reconstructed W 0033 ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex 0034 neutrinoSolutionType = cms.int32(-1) 0035 )
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