Variables
tuple	TtSemiLepHypWMassDeltaTopMass

Variable Documentation

tuple TtSemiLepHypWMassDeltaTopMass_cfi::TtSemiLepHypWMassDeltaTopMass

Initial value:

00001 cms.EDProducer("TtSemiLepHypWMassDeltaTopMass",
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
00009     match = cms.InputTag("findTtSemiLepJetCombWMassDeltaTopMass"),
00010     ## number of considered jets
00011     nJetsConsidered = cms.InputTag("findTtSemiLepJetCombWMassDeltaTopMass","NumberOfConsideredJets"),
00012     ## specify jet correction level as, Uncorrected, L1Offset, L2Relative, L3Absolute, L4Emf,
00013     ## L5Hadron, L6UE, L7Parton, a flavor specification will be added automatically, when chosen
00014     jetCorrectionLevel = cms.string("L3Absolute"),
00015     ## different ways to calculate a neutrino pz:
00016     ## -1 : take MET as neutrino directly, i.e. pz = 0
00017     ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz;
00018     ## if two real solutions...
00019     ##  0 : take the one closer to the lepton pz if neutrino pz < 300 GeV,
00020     ##      otherwise the more central one
00021     ##  1 : always take the one closer to the lepton pz
00022     ##  2 : always take the more central one, i.e. minimize neutrino pz
00023     ##  3 : maximize the cosine of the angle between lepton and reconstructed W
00024     ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex
00025     neutrinoSolutionType = cms.int32(-1)
00026 )

Definition at line 6 of file TtSemiLepHypWMassDeltaTopMass_cfi.py.

TtSemiLepHypWMassDeltaTopMass_cfi Namespace Reference

Variables

Variable Documentation