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

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compatible with a constant within the statistical uncertainty.<br />

acceptance [%]<br />

0.1<br />

0.09<br />

0.08<br />

0.<strong>07</strong><br />

0.06<br />

0.05<br />

0.04<br />

0.03<br />

0.02<br />

0.01<br />

ATLAS Internal<br />

2ID + TL<br />

w/o pileup reweighting<br />

w/ pileup reweighting<br />

0<br />

0 5 10 15 20<br />

Figure 5.14: Acceptance as a function of the mean number of interactions per bunch crossing (〈µ〉). The<br />

black dots are raw MC events and the magenta stars are MC events after pile-up reweighting (they show<br />

the region of 〈µ〉 relevant for the data used in this analysis).<br />

5.6.2 3ID Analysis<br />

The additional, orthogonal, channel used in the combined result to be presented in Chapter 8 corresponds<br />

to that where three fully reconstructed leptons (electron, muons) are selected. As mentioned above, this<br />

part of the analysis was performed by a different group in the collaboration. However it is explained here<br />

for completeness and clarity of the final result, which combines the two channels.<br />

The 3ID selection is very similar to that of the 2ID+TL. The main difference, which ensures orthogo-<br />

nality, is that instead of requiring exactly two ID leptons and one TL, three ID leptons are required, with<br />

the leading lepton having pT > 25 GeV. In the 2ID+TL selection this is automatically ensured by the<br />

pT > 25 GeV cut used in the TL selection. Also, no b-tagging requirement is used in this analysis.<br />

In the initial selection events are required to pass one of the single leptons triggers, and to include at<br />

least one good primary vertex. Events which contain any jet with pT > 20 GeV that fails the jet cleaning<br />

requirements [102] are rejected. Events with noise bursts in the LAr calorimeter or with cosmic rays are<br />

discarded. Events with exactly three ID leptons are selected, provided the three leptons are matched to<br />

the same primary vertex. At least one of the reconstructed leptons has to match a trigger lepton. The<br />

71<br />

< µ >

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