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