Variables
tuple	TtSemiLepHypWMassMaxSumPt

Variable Documentation

tuple TtSemiLepHypWMassMaxSumPt_cfi::TtSemiLepHypWMassMaxSumPt

Initial value:

00001 cms.EDProducer("TtSemiLepHypWMassMaxSumPt",
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("findTtSemiLepJetCombWMassMaxSumPt"),
00010     ## number of considered jets
00011     nJetsConsidered = cms.InputTag("findTtSemiLepJetCombWMassMaxSumPt","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 TtSemiLepHypWMassMaxSumPt_cfi.py.

TtSemiLepHypWMassMaxSumPt_cfi Namespace Reference

Variables

Variable Documentation