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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]<br />
1<br />
Total Integrated Luminosity [fb<br />
3.5<br />
3<br />
2.5<br />
2<br />
1.5<br />
1<br />
0.5<br />
ATLAS Online Luminosity<br />
LHC Delivered<br />
ATLAS Recorded<br />
1<br />
Total Delivered: 2.68 fb 1<br />
Total Recorded: 2.55 fb<br />
s = 7 TeV<br />
0<br />
02/03 31/03 29/04 28/05 <strong>26</strong>/06 25/<strong>07</strong> 24/08<br />
Day in 2011<br />
Figure 5.8: Cumulative luminosity versus day delivered to (green), and recorded by ATLAS (yellow) during<br />
stable beams and for pp collisions at 7 TeV center-of-mass energy in 2011.<br />
5.6 t¯t Signal<br />
As mentioned above, in order to reduce contribution from multijet background, only leptonic decays of the<br />
W- and the Z-boson are considered signal. Therefore, for the event selection, three high pT leptons, at<br />
least two jets and relatively high E miss<br />
T<br />
are required. The event selection is finalized with the reconstruction<br />
of the two top quarks, and corresponding constrainst on their masses. There are two base-line analyses<br />
for this search. The first one, ‘2ID +TL’ selects two isolated, fully reconstructed ID leptons, and one TL,<br />
whereas the second one, ‘3ID’, selects three ID leptons. Given that the selected TL in the 2ID+TL analysis<br />
is required to be exclusive of any electron or muon selected by the 3ID analysis, these two channels are<br />
orthogonal. The 2ID+TL channel increases the acceptance with respect to the 3ID channel alone by 22%.<br />
This thesis fully describes the 2ID+TL analysis, however, a brief description of the 3ID analysis is presented<br />
in Section 5.6.2 for completeness, given that the final result arises from a combination of both channels.<br />
5.6.1 2ID + TL Analysis<br />
Event Preselection<br />
At the preselection level, events are required to pass one of the single-lepton triggers, as described in Sec-<br />
tion 5.2, with the corresponding matching lepton candidate. To reject events from non-collision background,<br />
events are also required to have at least one good primary vertex. Events are discarded if any jet with<br />
pT > 20 GeV fails quality cuts designed to reject jets arising from calorimeter noise or activity inconsistent<br />
with the bunch-crossing time [100,102]. If an electron candidate and a muon candidate share a track, the<br />
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