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events is checked in a \ttll\ control sample, |
16 |
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selected by requiring |
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\begin{itemize} |
18 |
< |
\item exactly 2 selected electrons or muons with \pt $>$ 20 GeV |
18 |
> |
\item exactly 2 electrons or muons with \pt $>$ 20 GeV |
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\item \met\ $>$ 50 GeV |
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\item $\geq1$ b-tagged jet |
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\item Z-veto ($|m_{\ell\ell} - 91| > 15$ GeV) |
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It should be noted that in the case of \ttll\ events |
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with a single reconstructed lepton, the other lepton may be |
52 |
|
mis-reconstructed as a jet. For example, a hadronic tau may be |
53 |
< |
mis-identified as a jet (since no $\tau$ identification is used). |
53 |
> |
misidentified as a jet (since no $\tau$ identification is used). |
54 |
|
In this case only 1 additional jet from radiation may suffice for |
55 |
|
a \ttll\ event to enter the signal sample. As a result, both the |
56 |
|
samples with $\ttbar+1$ jet and $\ttbar+\ge2$ jets are relevant for |
147 |
|
used, the MadGraph $K_3$ and $K_4$ are used, etc. |
148 |
|
% |
149 |
|
In order to do so, it is first necessary to count the number of |
150 |
< |
additional jets from radiation and exclude leptons mis-identified as |
151 |
< |
jets. A jet is considered a mis-identified lepton if it is matched to a |
150 |
> |
additional jets from radiation and exclude leptons misidentified as |
151 |
> |
jets. A jet is considered a misidentified lepton if it is matched to a |
152 |
|
generator-level second lepton with sufficient energy to satisfy the jet |
153 |
|
\pt\ requirement ($\pt>30~\GeV$). Then \ttll\ events that need two |
154 |
|
radiation jets to enter our selection are scaled by $K_4$, |