| 71 |
|
$P_T = 10$ GeV to 91\% for $P_T > 30$ GeV. The isolation |
| 72 |
|
efficiency in top events varies from $\approx 83\%$ (muons) |
| 73 |
|
and $\approx 89\%$ (electrons) at $P_T=10$ GeV to |
| 74 |
< |
$\approx 95\%$ for $P_T>60$ GeV. {\bf \color{red} The} |
| 75 |
< |
{\bf \color{red} following numbers were derived from Fall 10 samples. } |
| 74 |
> |
$\approx 95\%$ for $P_T>60$ GeV. |
| 75 |
> |
%{\bf \color{red} The following numbers were derived from Fall 10 samples. } |
| 76 |
|
The average detector |
| 77 |
|
responses for SumJetPt and $\met/\sqrt{\rm SumJetPt}$ are |
| 78 |
|
$1.00 \pm 0.05$ and $0.96 \pm 0.05$ respectively, where |
| 88 |
|
signal region. |
| 89 |
|
% (SumJetPt $>$ 300 GeV and \met/$\sqrt{\rm SumJetPt} > 8.5$ |
| 90 |
|
% Gev$^{\frac{1}{2}}$). |
| 91 |
< |
{\bf \color{red} The following numbers were derived from Fall10 samples } |
| 91 |
> |
%{\bf \color{red} The following numbers were derived from Fall10 samples } |
| 92 |
|
We find that the average SumJetPt response |
| 93 |
|
in the Monte Carlo is very close to one, with an RMS of order 11\% while |
| 94 |
|
the response of \met/$\sqrt{\rm SumJetPt}$ is approximately 0.96 with an |
| 115 |
|
to the true quantity in MC. These plots are done using the LM0 |
| 116 |
|
Monte Carlo, but they are not expected to depend strongly on |
| 117 |
|
the underlying physics. |
| 118 |
< |
{\bf \color{red} These plots were made with Fall10 samples. } } |
| 118 |
> |
%{\bf \color{red} These plots were made with Fall10 samples. } |
| 119 |
> |
} |
| 120 |
|
\end{center} |
| 121 |
|
\end{figure} |
| 122 |
|
|
