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CERN-THESIS-2012-153 26/07/2012 - CERN Document Server

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fake rate [%]<br />

0.5<br />

0.45<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

40 60 80 100 120 140 160 180 200<br />

(a)<br />

ATLAS<br />

∫<br />

Internal<br />

­1<br />

L dt ~ 100 pb<br />

jet p [GeV]<br />

T<br />

fake rate [%]<br />

0.5<br />

0.45<br />

0.4<br />

0.35<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

1 2 3 4 5 6 7 8 9 10<br />

(b)<br />

ATLAS<br />

∫<br />

Internal<br />

­1<br />

L dt ~ 100 pb<br />

PV (#tracks ≥ 5)<br />

Figure 6.1: TL fake rate measured from γ+jets events vs. (a) jet pT and (b) number of primary vertices.<br />

The quoted integrated luminosity is a result of the photon trigger prescale.<br />

the matrix of each of the jets. Note that this technique gives the number of fake leptons, not the number of<br />

events with at least one fake lepton.<br />

Figure 6.2: Illustration showing a dilepton + 3 jet event being reconstructed as a trilepton + 2 jet event<br />

with a fake lepton.<br />

Because of the b-tag requirement in the event selection, only events with at least a b-tagged jet contribute<br />

to the fake prediction, and a b-tagged jet only contributes to that prediction if there is another jet in the<br />

event that is b-tagged. This accounts for the fact that if a fake TL emerges from a b-tagged jet, the jet itself<br />

will be removed by the overlap removal and can no longer provide a tag. The 2ID+TL selection requires a<br />

Z-boson candidate, i.e. an opposite-charge, same-flavor, lepton pair. Therefore the parent sample with two<br />

77

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