- 1) SUS-13-007: covers the single lepton + btag using the Lepton Spectrum (LS) and Delta Phi (DP) methods. Lepton studies are documented in AN-2013-035. Analysis notes: AN-12-390 and AN-12-416. Pre-approval date: Fri, Feb 1, 2013. Targeting Moriond.
- 2) AOD rereco is used for periods A, B, and part C; prompt reco is used for part C and D.
- 3) Efficiencies of leptonic and hadronic legs are shown to be not strongly correlated, thus they are measured separately. The lepton legs are mesured via Z T&P in events that are acquired by the analysis triggers (therefore with correctly biased kinematics).
- The triggers used for electrons:
-
HLT CleanPFHT350 Ele5 CaloIdT CaloIsoVL TrkIdT TrkIsoVL PFMET[45,50]
-
HLT CleanPFNoPUHT350 Ele5 CaloIdT CaloIsoVL TrkIdT TrkIsoVL PFMET[45,50]
-
HLT CleanPFHT300 Ele15 CaloIdT CaloIsoVL TrkIdT TrkIsoVL PFMET[45,50]
-
HLT CleanPFNoPUHT300 Ele15 CaloIdT CaloIsoVL TrkIdT TrkIsoVL PFMET[45,50]
-
HLT CleanPFHT300 Ele[40,60] CaloIdVT CaloIsoVL TrkIdT
(control trigger)
-
HLT CleanPFNoPUHT300 Ele[40,60] CaloIdVT CaloIsoVL TrkIdT
(control trigger)
- and for muons:
-
HLT PFHT350 Mu15 PFMET[45,50]
-
HLT PFNoPUHT350 Mu15 PFMET[45,50]
-
HLT PFHT400 Mu5 PFMET[45,50]
-
HLT PFNoPUHT400 Mu5 PFMET[45,50]
-
HLT Mu[40,60] PFHT350
(control trigger)
-
HLT Mu[40,60] PFNoPUHT350
(control trigger)
Summary tables:
Quantity |
PAT Object and Member Function |
barrel cut |
endcap cut |
comment* |
type |
pat::Electron |
|
|
|
p_T |
ele->pt() |
≥ 20 GeV |
|
|
abs(eta) |
(ele->isEB() || ele->isEE()) && fabs(ele->superCluster()->eta()) <= 2.5 |
|
|
|
Rel. Isolation |
charged + max (0., photon + neutral - (*eleRho)*Aeff) |
<0.15 |
same |
|
hadOverEM |
ele->hadronicOverEm() |
<0.12 |
<0.10 |
|
abs(deltaPhi) |
fabs(ele->deltaPhiSuperClusterTrackAtVtx()) |
<0.06 |
<0.03 |
|
abs(deltaEta) |
abs(ele->deltaEtaSuperClusterTrackAtVtx()) |
<0.004 |
<0.007 |
|
sigmaIetaIeta |
ele->scSigmaIEtaIEta() |
<0.01 |
<0.03 |
|
Conversion rejection |
!ConversionTools::hasMatchedConversion(*gsfel,hConversions,beamSpotPosition) |
True |
True |
Use the gsfel obtained with originalObjectRef; don't use the pat::Electron |
missingHits |
ele->gsfTrack()->trackerExpectedHitsInner().numberOfHits() |
<= 1 |
<= 1 |
|
dxy |
fabs(ele->gsfTrack()->dxy(vertexPosition)) |
< 0.02 |
same |
vertexPosition is the position of the first good vertex |
dz |
fabs(ele->gsfTrack()->dz(vertexPosition)) |
< 0.1 |
same |
|
abs(reco - PF) PT |
fabs(electron->pt() - (*ipfEl).pt()) |
< 10 GeV |
same |
(*ipfEl).particleId() == reco::PFCandidate::e && (*ipfEl) > 10. |
veto electron selection
Quantity |
PAT Object and Member Function |
barrel cut |
endcap cut |
comment* |
type |
pat::Electron |
|
|
|
p_T |
ele->pt() |
≥ 15 GeV |
|
|
abs(eta) |
ele->isEB() || ele->isEE() |
|
|
|
Rel. Isolation |
charged + max (0., photon + neutral - (*eleRho)*Aeff) |
<0.15 |
same |
|
hadOverEM |
ele->hadronicOverEm() |
<0.15 |
no cut |
|
abs(deltaPhi) |
fabs(ele->deltaPhiSuperClusterTrackAtVtx()) |
<0.8 |
<0.7 |
|
abs(deltaEta) |
abs(ele->deltaEtaSuperClusterTrackAtVtx()) |
<0.007 |
<0.01 |
|
sigmaIetaIeta |
ele->scSigmaIEtaIEta() |
<0.01 |
<0.03 |
|
dxy |
fabs(ele->gsfTrack()->dxy(vertexPosition)) |
< 0.04 |
same |
vertexPosition is the position of the first good vertex |
dz |
fabs(ele->gsfTrack()->dz(vertexPosition)) |
< 0.2 |
same |
|
Muons are selected using the POG tight muon recommended selection at
https://twiki.cern.ch/twiki/bin/view/CMSPublic/SWGuideMuonId
Quantity |
PAT Object and Member Function |
Cut |
Comment |
muon type |
pat::Muon |
|
|
ID |
muon -> isGlobalMuon() |
True |
|
ID |
muon -> isPFMuon() |
True |
|
pT |
muon -> pt() |
≥ 20 GeV |
|
abs(eta) |
muon-> eta() |
≤ 2.4 |
|
pf Rel. Isolation |
pfRelIso = (muon->pfIsolationR03().sumChargedHadronPt
+ max(0., muon->pfIsolationR03().sumNeutralHadronEt
+ muon->pfIsolationR03().sumPhotonEt - 0.5*muon->pfIsolationR03().sumPUPt ) )
/ muon->pt() |
< 0.12 |
Don't use pat::Muon->isoDeposit()->depositWithin(0.3) |
normChi2 |
muon->globalTrack()->chi2() / muon->globalTrack()->ndof() |
≤ 10 |
|
nValMuonHits |
muon->globalTrack()->hitPattern().numberOfValidMuonHits() |
> 0 |
|
numMatchedStations |
muon->numberOfMatchedStations() |
> 1 |
|
pixelHits |
muon->innerTrack()->hitPattern().numberOfValidPixelHits() |
> 0 |
|
numTrackerLayersWithMeasurement |
muon->track()->hitPattern().trackerLayersWithMeasurement() |
> 5 |
|
dxy |
fabs(muon->innerTrack()->dxy(vertexPosition)) |
< 0.02 |
vertexPosition is the position of the first good vertex |
dz |
fabs(muon->innerTrack()->dz(vertexPosition)) |
< 0.5 |
|
abs(reco - PF) |
fabs(muon->pt() - (*ipfMu).pt()) |
< 5 GeV |
(*ipfMu).particleId() == reco::PFCandidate::mu && (*ipfMu) > 10. |
Muon Veto Selection
Quantity |
PAT Object and Member Function |
Cut |
Comment |
Mu type |
pat::Muon |
|
|
ID |
muon->isGlobalMuon() || muon->isTrackerMuon() |
True |
|
ID |
muon -> isPFMuon() |
True |
|
pT |
muon -> pt() |
≥ 15 GeV |
|
abs(eta) |
fabs(muon -> eta()) |
≤ 2.5 |
|
pf Rel. Isolation |
pfRelIso = (muon->pfIsolationR03().sumChargedHadronPt
+ max(0., muon->pfIsolationR03().sumNeutralHadronEt
+ muon->pfIsolationR03().sumPhotonEt - 0.5*muon->pfIsolationR03().sumPUPt ) )
/ muon->pt() |
< 0.2 |
|
dxy |
fabs(muon->innerTrack()->dxy(vertexPosition)) |
< 0.2 |
vertexPosition is the position of the first good vertex |
dz |
fabs(muon->innerTrack()->dz(vertexPosition)) |
< 0.5 |
vertexPosition is the position of the first good vertex |
- 5) Lepton reconstruction and ID efficiency scale factors between data and MC were determined with the T&P method. Backrgound subtraction (and simulation) was applied in the fit. The scale factors are computed as the ratio of constant fits on the efficiencies over the threshold value.
Selection |
data/MC (full simulation) |
data/MC (fast simulation) |
Electron ID + Isolation (average) |
0.9987 ± 0.0015(stat.)±0.02(sys.) |
0.9613 ± 0.0014(stat.)±0.08(sys.) |
Barrel |
|
0.9900 ± 0.0007(stat.)±0.03(sys.) |
Endcap |
|
0.8725 ± 0.0014(stat.)±0.07(sys.) |
Electron GSF tracking |
0.9944 ± 0.0003(stat.)±0.02(sys.) |
0.9902 ± 0.0004(stat.)±0.01(sys.) |
Muon ID1 |
0.9981 ± 0.0007(stat.)±0.02(sys.) |
0.9531 ± 0.0007(stat.)±0.03(sys.) |
Muon ID2 |
1.0015 ± 0.0006(stat.)±0.01(sys.) |
0.9902 ± 0.0005(stat.)±0.01(sys.) |
Muon track |
0.9953 ± 0.0001(stat.)±0.005(sys.) |
0.9951 ± 0.0001(stat.)±0.005(sys.) |
Trigger efficiencies: scale factor is to be applied on Monte Carlo. Individual triggers are listed with scale factors and systematic errors. "Overall" is a value that is compatible with the result of every trigger in the table. In case of the muons, additionally, a correction is to be applied on the scale factor different for barrel and endcap to account for eta dependence.
Electron trigger path |
Scale factor |
CleanPFHT350_Ele5_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET45 |
0.96 ± 0.04 |
CleanPFHT350_Ele5_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET50 |
0.96 ± 0.04 |
CleanPFNoPUHT350_Ele5_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET45 |
0.94 ± 0.07 |
CleanPFNoPUHT350_Ele5_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET50 |
0.95 ± 0.08 |
CleanPFHT300_Ele15_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET45 |
0.97 ± 0.07 |
CleanPFHT300_Ele15_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET50 |
0.97 ± 0.07 |
CleanPFNoPUHT300_Ele15_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET45 |
0.98 ± 0.03 |
CleanPFNoPUHT300_Ele15_CaloIdT_CaloIsoVL_TrkIdT_TrkIsoVL_PFMET50 |
0.98 ± 0.04 |
CleanPFHT300_Ele40_CaloIdVT_TrkIdT |
0.96 ± 0.02 |
CleanPFNoPUHT300_Ele40_CaloIdVT_TrkIdT |
0.96 ± 0.02 |
CleanPFHT300_Ele60_CaloIdVT_TrkIdT |
0.96 ± 0.02 |
CleanPFNoPUHT300_Ele60_CaloIdVT_TrkIdT |
0.96 ± 0.02 |
Ele30_CaloIdVT_TrkIdT |
0.96 ± 0.02 |
Ele25_CaloIdVT_CaloIsoVL_TrkIdVL_TrkIsoT_TriCentralPFNoPUJet30 |
0.97 ± 0.02 |
Overall |
0.96 ± 0.05 |
Muon trigger path |
Scale factor |
IsoMu24 |
0.88 ± 0.02 |
IsoMu24_eta2p1 |
0.90 ± 0.01 |
Mu40_PFHT350 |
0.91 ± 0.02 |
Mu40_PFNoPUHT350 |
0.91 ± 0.02 |
Mu60_PFHT350 |
0.91 ± 0.02 |
Mu60_PFNoPUHT350 |
0.92 ± 0.01 |
PFHT400_Mu5_PFMET45 |
0.92 ± 0.05 |
PFHT400_Mu5_PFMET50 |
0.92 ± 0.05 |
PFNoPUHT400_Mu5_PFMET45 |
0.93 ± 0.04 |
PFNoPUHT400_Mu5_PFMET50 |
0.93 ± 0.04 |
PFHT350_Mu15_PFMET45 |
0.93 ± 0.05 |
PFHT350_Mu15_PFMET50 |
0.93 ± 0.05 |
PFNoPUHT350_Mu15_PFMET45 |
0.92 ± 0.04 |
PFNoPUHT350_Mu15_PFMET50 |
0.92 ± 0.05 |
Overall |
0.91 ± 0.04 |
Scale factor for abs(eta) < 0.9 |
1.076 |
Scale factor for abs(eta) > 0.9 |
0.928 |
- 6) Fakes are attributed to QCD and are derived from data. (eg Section 4.2 in AN-12-390)
- 7) Both answers are no.
- 8) Systematic errors on trigger and selection efficiencies are given in 5), more details are in AN-13-035.