| 60 |
|
$\met/\sqrt{\rm SumJetPt}$ requirement |
| 61 |
|
replaced by a $P_T(\ell\ell)/\sqrt{\rm SumJetPt}$ requirement |
| 62 |
|
is $N_{D'}=1$. Thus the BG prediction is |
| 63 |
< |
$N_D = K \cdot N_{D'} = 1.5$ |
| 64 |
< |
where $K=1.5 \pm xx$ as derived in Sec.~\ref{sec:victory}. |
| 63 |
> |
$N_D = K \cdot K_C \cdot N_{D'} = 1.5$ |
| 64 |
> |
where $K=1.5 \pm xx$ as derived in Sec.~\ref{sec:victory} and |
| 65 |
> |
$K_C = 1$. |
| 66 |
|
Note that if we were to subtract off from region $D'$ |
| 67 |
|
the {\color{red} 0.4 $\pm$ 0.4} DY events estimated from |
| 68 |
|
Section~\ref{sec:othBG}, the background |
| 115 |
|
rate of opposite sign isolated dilepton events |
| 116 |
|
at high \met and high SumJetPt. The extraction of |
| 117 |
|
quantitative limits on new physics models is discussed |
| 118 |
< |
in Section~\ref{sec:limits}. |
| 118 |
> |
in Section~\ref{sec:limit}. |
