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Variables
TtSemiLepHypWMassDeltaTopMass_cfi Namespace Reference

Variables

tuple ttSemiLepHypWMassDeltaTopMass
 

Variable Documentation

tuple TtSemiLepHypWMassDeltaTopMass_cfi.ttSemiLepHypWMassDeltaTopMass
Initial value:
1 = cms.EDProducer("TtSemiLepHypWMassDeltaTopMass",
2  ## met input
3  mets = cms.InputTag("patMETs"),
4  ## jet input
5  jets = cms.InputTag("selectedPatJets"),
6  ## lepton input
7  leps = cms.InputTag("selectedPatMuons"),
8  ## jet combination
9  match = cms.InputTag("findTtSemiLepJetCombWMassDeltaTopMass"),
10  ## number of considered jets
11  nJetsConsidered = cms.InputTag("findTtSemiLepJetCombWMassDeltaTopMass","NumberOfConsideredJets"),
12  ## specify jet correction level as, Uncorrected, L1Offset, L2Relative, L3Absolute, L4Emf,
13  ## L5Hadron, L6UE, L7Parton, a flavor specification will be added automatically, when chosen
14  jetCorrectionLevel = cms.string("L3Absolute"),
15  ## different ways to calculate a neutrino pz:
16  ## -1 : take MET as neutrino directly, i.e. pz = 0
17  ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz;
18  ## if two real solutions...
19  ## 0 : take the one closer to the lepton pz if neutrino pz < 300 GeV,
20  ## otherwise the more central one
21  ## 1 : always take the one closer to the lepton pz
22  ## 2 : always take the more central one, i.e. minimize neutrino pz
23  ## 3 : maximize the cosine of the angle between lepton and reconstructed W
24  ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex
25  neutrinoSolutionType = cms.int32(-1)
26 )

Definition at line 6 of file TtSemiLepHypWMassDeltaTopMass_cfi.py.