Variables
tuple	findTtSemiLepJetCombWMassDeltaTopMass

Variable Documentation

tuple TtSemiLepJetCombWMassDeltaTopMass_cfi::findTtSemiLepJetCombWMassDeltaTopMass

Initial value:

00001 cms.EDProducer("TtSemiLepJetCombWMassDeltaTopMass",
00002     ## jet input 
00003     jets  = cms.InputTag("selectedPatJets"),
00004     ## lepton input 
00005     leps  = cms.InputTag("selectedPatMuons"),
00006     ## met input
00007     mets  = cms.InputTag("patMETs"),
00008     maxNJets  = cms.int32(4),
00009     ## nominal WMass parameter (in GeV)
00010     wMass    = cms.double(80.4),
00011     ## use b-tagging two distinguish between light and b jets
00012     useBTagging = cms.bool(False),
00013     ## choose algorithm for b-tagging
00014     bTagAlgorithm = cms.string("trackCountingHighEffBJetTags"),
00015     ## minimum b discriminator value required for b jets and
00016     ## maximum b discriminator value allowed for non-b jets
00017     minBDiscBJets     = cms.double(1.0),
00018     maxBDiscLightJets = cms.double(3.0),
00019     ## different ways to calculate a neutrino pz:
00020     ## -1 : take MET as neutrino directly, i.e. pz = 0
00021     ## or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz;
00022     ## if two real solutions...
00023     ##  0 : take the one closer to the lepton pz if neutrino pz < 300 GeV,
00024     ##      otherwise the more central one
00025     ##  1 : always take the one closer to the lepton pz
00026     ##  2 : always take the more central one, i.e. minimize neutrino pz
00027     ##  3 : maximize the cosine of the angle between lepton and reconstructed W
00028     ## in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex
00029     neutrinoSolutionType = cms.int32(-1)
00030 )

Definition at line 6 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.

TtSemiLepJetCombWMassDeltaTopMass_cfi Namespace Reference

Variables

Variable Documentation