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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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 >