| 156 |
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|
| 157 |
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\begin{table}[!ht] |
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\begin{center} |
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+ |
{\footnotesize |
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|
\begin{tabular}{l|c|c|c} |
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\cline{2-4} |
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& \multicolumn{3}{c}{ \met\ cut for data/MC scale factors} \\ |
| 169 |
|
N jets $\ge4$ (sensitive to $\ttbar+\ge2$ extra jets from radiation) |
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& $K_4 = 0.94 \pm 0.02$ & $K_4 = 0.93 \pm 0.04$ & $K_4 = 1.00 \pm 0.08$ \\ |
| 171 |
|
\hline |
| 172 |
< |
\end{tabular} |
| 172 |
> |
\end{tabular}} |
| 173 |
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\caption{Data/MC scale factors used to account for differences in the |
| 174 |
|
fraction of events with additional hard jets from radiation in |
| 175 |
|
\ttll\ events. The values derived with the 100 GeV \met\ cut are applied |
| 196 |
|
|
| 197 |
|
The $t\bar{t}$ MC is corrected using the $K_3$ and $K_4$ factors |
| 198 |
|
from Section~\ref{sec:jetmultiplicity}. It is also normalized to the |
| 199 |
< |
total data yield separately for the \met\ requirements of signal |
| 200 |
< |
regions A, B, C, and D. These normalization factors are listed |
| 199 |
> |
total data yield separately for the \met\ requirements of the various signal |
| 200 |
> |
regions. These normalization factors are listed |
| 201 |
|
in Table~\ref{tab:cr4mtsf} and are close to unity. |
| 202 |
|
|
| 203 |
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The underlying \met\ and $M_T$ distributions are shown in |
