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

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Appendix B<br />

Backgrounds to the 3ID analysis<br />

B.1 Monte Carlo Background<br />

Similarly to what is done for the 2ID+TL analysis, the background coming from diboson (WW and ZZ)<br />

plus jets and t¯t + W/Z are estimated from MC simulation.<br />

B.2 Fake Leptons Background<br />

Background to the 3ID candidate events in which at least one jet is reconstructed as a lepton is separated<br />

in two categories: background events with one fake lepton, and background events with two or three fake<br />

leptons. Background events with one fake lepton are evaluated using a combination of data and MC samples.<br />

The Z+jets background is estimated using a DD normalization to the MC estimate. Z+jets, along with<br />

other sources of one fake lepton background, are evaluated at the final selection level using a loose lepton<br />

reconstruction selection and a multiplicative factor to scale to the final selection. This loose selection is<br />

achieved by relaxing the leptons requirements. Loose muons are defined as in Section 5.3.1, but without<br />

the isolation requirement. Loose electrons are obtained with the selection described in Section 5.3.2, but<br />

relaxing the isolation requirement to < 6 GeV. Events with two fake leptons (such as W+jets and single lep-<br />

ton t¯t events) or three fake leptons (such as multijet and hadronic t¯t events) are estimated with DD methods.<br />

To enhance the statistical power of the MC samples, the background with one fake lepton is estimated<br />

with the loose lepton selection described above. A multiplicative factor of 0.063 ± 0.013, corresponding to<br />

the MC probability for events with loose leptons to pass the signal region (SR) lepton criteria, is applied to<br />

the final results in each of the background sources.<br />

The dominant contribution to events with one fake lepton comes from Z+jets events, with a leptonic<br />

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