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Revision 1.10 by claudioc, Sun Nov 14 11:18:28 2010 UTC vs.
Revision 1.14 by benhoob, Thu Dec 2 15:04:08 2010 UTC

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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
# Line 16 | Line 17 | a few specific processes.
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  
# Line 65 | Line 66 | Note that the isolation efficiency depen
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

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