Variables | |
bTagAlgorithm | |
choose algorithm for b-tagging More... | |
findTtSemiLepJetCombWMassDeltaTopMass | |
jets | |
jet input More... | |
leps | |
lepton input More... | |
maxBDiscLightJets | |
maxNJets | |
mets | |
met input More... | |
minBDiscBJets | |
minimum b discriminator value required for b jets and maximum b discriminator value allowed for non-b jets More... | |
neutrinoSolutionType | |
different ways to calculate a neutrino pz: -1 : take MET as neutrino directly, i.e. More... | |
useBTagging | |
use b-tagging two distinguish between light and b jets More... | |
wMass | |
nominal WMass parameter (in GeV) More... | |
TtSemiLepJetCombWMassDeltaTopMass_cfi.bTagAlgorithm |
choose algorithm for b-tagging
Definition at line 19 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.findTtSemiLepJetCombWMassDeltaTopMass |
Definition at line 6 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.jets |
jet input
Definition at line 8 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.leps |
lepton input
Definition at line 10 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.maxBDiscLightJets |
Definition at line 23 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.maxNJets |
Definition at line 13 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.mets |
met input
Definition at line 12 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.minBDiscBJets |
minimum b discriminator value required for b jets and maximum b discriminator value allowed for non-b jets
Definition at line 22 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.neutrinoSolutionType |
different ways to calculate a neutrino pz: -1 : take MET as neutrino directly, i.e.
pz = 0 or use mW = 80.4 GeV to solve the quadratic equation for the neutrino pz; if two real solutions... 0 : take the one closer to the lepton pz if neutrino pz < 300 GeV, otherwise the more central one 1 : always take the one closer to the lepton pz 2 : always take the more central one, i.e. minimize neutrino pz 3 : maximize the cosine of the angle between lepton and reconstructed W in all these cases (0, 1, 2, 3), only the real part is used if solutions are complex
Definition at line 34 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.useBTagging |
use b-tagging two distinguish between light and b jets
Definition at line 17 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.
TtSemiLepJetCombWMassDeltaTopMass_cfi.wMass |
nominal WMass parameter (in GeV)
Definition at line 15 of file TtSemiLepJetCombWMassDeltaTopMass_cfi.py.