def computeMT2(visaVec, visbVec, metVec):
import array
import numpy
from ROOT.heppy import Davismt2
davismt2 = Davismt2()
metVector = array.array('d',[0.,metVec.px(), metVec.py()])
visaVector = array.array('d',[0.,visaVec.px(), visaVec.py()])
visbVector = array.array('d',[0.,visbVec.px(), visbVec.py()])
davismt2.set_momenta(visaVector,visbVector,metVector);
davismt2.set_mn(0);
return davismt2.get_mt2()
# This module is an adaptation and simplification of MT2Analyzer.py in heppy
import ROOT
from ROOT.heppy import Hemisphere
from ROOT.heppy import Davismt2
davismt2 = Davismt2()
def computeMT2(visApx, visApy, visBpx, visBpy, invispx, invispy):
# creates auxiliary arrays of transverse momenta
# calls DavisMt2 method
import array
import numpy
invisVector = array.array('d', [0., invispx, invispy])
visAVector = array.array('d', [0., visApx, visApy])
visBVector = array.array('d', [0., visBpx, visBpy])
davismt2.set_momenta(visAVector, visBVector, invisVector)
davismt2.set_mn(0)
return davismt2.get_mt2()
def getMT2(objects, met):
# objects - list of Objects
# met - ROOT.TLorentzVector()
# creates auxiliary arrays for objects and met
# calls Hemisphere method
if len(objects) >= 2:
def __call__(self,event):
# make python lists as Collection does not support indexing in slices
leps = [l for l in Collection(event,"lep","nlep",10)]
jets = [j for j in Collection(event,"jet","njet",100)]
(met, metphi) = event.met_pt, event.met_phi
metp4 = ROOT.reco.Particle.LorentzVector(met*cos(metphi),met*sin(metphi),0,met)
genLepsp4 = [l for l in Collection(event,"genLep","ngenLep",10)]
njet = len(jets); nlep = len(leps)
# prepare output
ret = dict([(name,0.0) for name in self.branches])
###### smear MET with Recoil Correction for V + Jets
# fill output
if len(genLepsp4)>=2:
genZp4 = ROOT.reco.Particle.LorentzVector( 0, 0, 0, 0 )
for l in genLepsp4:
genZp4 += ROOT.reco.Particle.LorentzVector( l.p4().Px(), l.p4().Py(), l.p4().Pz(), l.p4().Energy() )
# print 'genZ',genZp4.Pt()
# those need to be added to the tree
# ZGen_pt, ZGen_phi, ZGen_rap
# ZReco_pt, ZReco_phi
(met_corr, metphi_corr) = (met, metphi)
# recoilCorr.CorrectType2( met_corr, met_corr,
# genZp4.Pt(), genZp4.Phi(),
# ZReco_pt, ZReco_phi,
# u1_dummy, u2_dummy,
# RecoilCorrResolutionNSigmaU2, RecoilCorrResolutionNSigmaU1, RecoilCorrScaleNSigmaU1,
# rapBin,false);
# fill output
if njet >= 2:
###### for now clone of the code in ttHCoreEventAnalyzer.py
deltaPhiMin_had4 = 999.
for n,j in enumerate(jets):
if n>3: break
thisDeltaPhi = abs( deltaPhi( j.phi, metphi ) )
if thisDeltaPhi < deltaPhiMin_had4 : deltaPhiMin_had4 = thisDeltaPhi
ret["deltaPhiMin4"] = deltaPhiMin_had4
deltaPhiMin_had3 = 999.
for n,j in enumerate(jets):
if n>2: break
thisDeltaPhi = abs( deltaPhi( j.phi, metphi ) )
if thisDeltaPhi < deltaPhiMin_had3 : deltaPhiMin_had3 = thisDeltaPhi
ret["deltaPhiMin3"] = deltaPhiMin_had3
###### for now clone of the code in ttHTopoVarAnalyzer.py
objects40jc = [ j for j in jets if j.pt > 40 and abs(j.eta)<2.5]
if len(objects40jc)>=2:
from ROOT import Hemisphere
from ROOT import ReclusterJets
from ROOT import Davismt2
davismt2 = Davismt2()
pseudoViaKtJet1_had = ROOT.reco.Particle.LorentzVector( 0, 0, 0, 0 )
pseudoViaKtJet2_had = ROOT.reco.Particle.LorentzVector( 0, 0, 0, 0 )
objects = ROOT.std.vector(ROOT.reco.Particle.LorentzVector)()
for jet in objects40jc:
jetp4 = ROOT.reco.Particle.LorentzVector(jet.p4().Px(), jet.p4().Py(), jet.p4().Pz(), jet.p4().Energy())
objects.push_back(jetp4)
hemisphereViaKt = ReclusterJets(objects, 1.,50)
groupingViaKt=hemisphereViaKt.getGroupingExclusive(2)
if len(groupingViaKt)>=2:
pseudoViaKtJet1_had = groupingViaKt[0]
pseudoViaKtJet2_had = groupingViaKt[1]
ret["mt2_had_30"] = computeMT2(pseudoViaKtJet1_had, pseudoViaKtJet2_had, metp4)
print 'mt2(had-original)=',event.mt2,'--- mt2ViaKt_had(original)=',event.mt2ViaKt_had,'--- mt2(new)=',ret["mt2_had_30"]
return ret