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Revision 1.7 by claudioc, Thu Nov 11 12:34:18 2010 UTC vs.
Revision 1.8 by claudioc, Thu Nov 11 16:22:13 2010 UTC

# Line 1 | Line 1
1 < \section{Acceptance systematics}
1 > \section{Acceptance and efficiency systematics}
2   \label{sec:systematics}
3  
4   This is a search for new physics contributions to
# Line 7 | Line 7 | As seen in Section~\ref{sec:results}, th
7   evidence for a contribution beyond SM expectations.
8  
9   Strictly speaking it is impossible to talk about
10 < ``acceptance systematics'' because these kinds of
10 > ``acceptance and efficiency systematics'' because these kinds of
11   systematics only apply to a well defined final state.
12 < Nevertheless, we can at least make some qualitative
13 < statements.
12 > Nevertheless, we can make general statements about the
13 > systematic uncertainties, including quantitative
14 > estimates of the systematic uncertainties associated with
15 > a few specific processes.
16  
17   The systematic uncertainty on the lepton acceptance consists
18   of two parts: the trigger efficiency uncertainty and the
# Line 62 | Line 64 | Note that the isolation efficiency depen
64   the final state.  For example, in MC we find that the
65   lepton isolation efficiency differs by $\approx 4\%$
66   {\bf per lepton} between $Z$ events and $t\bar{t}$ events\cite{ref:top}.
67 + \noindent {\bf This figure should be cut off at 100 GeV, and
68 + the y-axis should be zero-suppressed}
69  
70   Another significant source of systematic uncertainty is
71   associated with the jet and $\met$ energy scale.  The impact
72 < of this uncertainty is very final-state dependent.  Final
73 < states characterized by lots of hadronic activity and \met are much
72 > of this uncertainty is final-state dependent.  Final
73 > states characterized by lots of hadronic activity and \met are
74   less sensitive than final states where the \met and SumJetPt
75   are typically close to the requirement.  To be more quantitative,
76   we have used the method of Reference~\cite{ref:top} to evaluate

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