| 12 |
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of the individual leptons, and, in the case of muons, the $|\eta|$ |
| 13 |
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of the muons. We believe that this model is adequate for |
| 14 |
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the trigger efficiency precision needed for this analysis. |
| 15 |
< |
Details are given in App.~\ref{sec:appendix_trigger}. |
| 15 |
> |
Details are given in Appendix~\ref{sec:appendix_trigger}. |
| 16 |
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|
| 17 |
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We take the trigger efficiency for $ee$ as 100\%. The trigger efficiency |
| 18 |
< |
for the $e\mu$ and $\mu\mu$ final states is summarized in Figures xx. |
| 18 |
> |
for the $e\mu$ and $\mu\mu$ final states is summarized in |
| 19 |
> |
Figures~\ref{fig:emuModel} and~\ref{fig:mumuModel}. |
| 20 |
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We estimate the systematic uncertainties on the trigger modeling |
| 21 |
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to be at the few percent level. |
| 22 |
|
|
| 23 |
< |
\noindent {\color{red}Figure xx will be a two dimensional table of the |
| 24 |
< |
trigger efficiency as a function of the pt of the two leptons. |
| 24 |
< |
We need to wait for the xx in the previous section to be completes before we can |
| 25 |
< |
fill out this table.} |
| 23 |
> |
{\bf The trigger efficiency model will be applied when |
| 24 |
> |
we move to 38x Monte Carlo. For now, we take the efficiency as 100\%.} |
