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Revision 1.31 by benhoob, Thu Dec 2 16:42:37 2010 UTC vs.
Revision 1.32 by benhoob, Thu Dec 2 17:48:33 2010 UTC

# Line 197 | Line 197 | The results are summarized in Table~\ref
197   \begin{table}[htb]
198   \begin{center}
199   \caption{\label{tab:victorybad}
200 < {\bf \color{red} Need to either update this with 38X MC  or remove it }
200 > {\bf \color{red} Should we either update this with 38X MC  or remove it?? }
201   Test of the data driven method in Monte Carlo
202   under different assumptions.  See text for details.}
203   \begin{tabular}{|l|c|c|c|c|c|c|c|c|}
# Line 290 | Line 290 | obtained using only $t\bar{t} \to$~dilep
290   giving an uncertainty of $0.04$.
291  
292   The uncertainty in $K_C$ due to the MET scale uncertainty is assessed by varying the hadronic energy scale using
293 < the same method as in~\ref{ref:top}, giving an uncertainty of 0.3. We also assess the impact of the MET resolution
293 > the same method as in~\cite{ref:top}, giving an uncertainty of 0.3. We also assess the impact of the MET resolution
294   uncertainty on $K_C$ by applying a random smearing to the MET. For each event, we determine the expected MET resolution
295   based on the sumJetPt, and smear the MET to simulate an increase in the resolution of 10\%, 20\%, 30\%, 40\% and 50\%.
296   The results show that $K_C$ does not depend strongly on the MET resolution and we therefore do not assess any uncertainty.

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