1 |
|
\section{Acceptance and efficiency systematics} |
2 |
|
\label{sec:systematics} |
3 |
|
|
4 |
+ |
{\bf \color{red} MANY OF THESE STUDIES NEED TO BE UPDATED WITH 38X MC} |
5 |
|
This is a search for new physics contributions to |
6 |
|
events with high \met and lots of jet activity. |
7 |
|
As seen in Section~\ref{sec:results}, there is no |
17 |
|
|
18 |
|
The systematic uncertainty on the lepton acceptance consists |
19 |
|
of two parts: the trigger efficiency uncertainty and the |
20 |
< |
ID and isolation of uncertainty. We discuss these in turn. |
20 |
> |
ID and isolation uncertainty. We discuss these in turn. |
21 |
|
|
22 |
|
The trigger efficiency |
23 |
|
for two leptons of $P_T>10$ GeV, with one lepton of |
24 |
|
$P_T>20$ GeV is very high, except in some corners |
25 |
< |
of phase space, see Section~\ref{sec:trgEff}. |
25 |
> |
of phase space, see Section~\ref{sec:trgeffsum}. |
26 |
|
We estimate the efficiency uncertainty to be a few percent, |
27 |
|
mostly in the low $P_T$ region. |
28 |
|
|
66 |
|
the final state. For example, in MC we find that the |
67 |
|
lepton isolation efficiency differs by $\approx 4\%$ |
68 |
|
{\bf per lepton} between $Z$ events and $t\bar{t}$ events\cite{ref:top}. |
69 |
< |
\noindent {\bf This figure should be cut off at 100 GeV, and |
70 |
< |
the y-axis should be zero-suppressed} |
69 |
> |
%\noindent {\bf This figure should be cut off at 100 GeV, and |
70 |
> |
%the y-axis should be zero-suppressed} |
71 |
|
|
72 |
|
Another significant source of systematic uncertainty is |
73 |
|
associated with the jet and $\met$ energy scale. The impact |