| 68 |
|
the final state. For example, in MC we find that the |
| 69 |
|
lepton isolation efficiency differs by $\approx 4\%$ |
| 70 |
|
{\bf per lepton} between $Z$ events and $t\bar{t}$ events\cite{ref:top}. |
| 71 |
+ |
{\bf \color{red} VERIFY THAT THESE VALUES ARE UNCHANGED IN 38X MC. } |
| 72 |
|
%\noindent {\bf This figure should be cut off at 100 GeV, and |
| 73 |
|
%the y-axis should be zero-suppressed} |
| 74 |
|
|
| 83 |
|
and two benchmark SUSY points. The uncertainties are calculated |
| 84 |
|
assuming a 5\% uncertainty to the hadronic energy scale in CMS. |
| 85 |
|
|
| 86 |
< |
For $t\bar{t}$ we find uncertainties of 8\% (baseline |
| 87 |
< |
selection) and 30\% (signal region D); for LM0 and LM1 we find |
| 88 |
< |
14\% and 6\% respectively for signal region D. |
| 86 |
> |
For $t\bar{t}$ we find uncertainties of 3\% (baseline |
| 87 |
> |
selection) and 21\% (signal region D); for LM0 and LM1 we find |
| 88 |
> |
15\% and 6\% respectively for signal region D |
| 89 |
> |
{\bf \color{red} THESE VALUES HAVE BEEN RECALCULATED FOR 38X MC, AWAITING VERIFICATION} |
