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Revision 1.33 by claudioc, Thu Jan 13 23:21:08 2011 UTC vs.
Revision 1.35 by claudioc, Fri Jan 14 00:21:24 2011 UTC

# Line 195 | Line 195 | boundaries of the excluded region are al
195   the boundaries using the method recommended by the SUSY
196   group\cite{ref:smooth}.  In addition, we show a limit
197   curve based on the LO cross-section, as well as the
198 < ``expected'' limit curve.  The expected limit curve is
198 > ``expected'' limit curve.  The expected limit curve was
199   calculated using the CLA function also available in cl95cms.
200 < Cross-section uncertainties due to variations of the factorization
200 > In general we found that the ``expected'' limit is very close
201 > to the observed limit, which is not surprising since the
202 > expected BG (1.4 $\pm$ 0.8 events) is fully consistent
203 > with the observation (1 event). Because of the quantization,
204 > we find that the expected and observed limits are either
205 > identical or differ by one or at most two grid points.
206 > We have approximated the expected limit as the observed limit
207 > minus 10 GeV\footnote{We show the expected limit only because
208 > this is what is recommended by SUSY management. We believe that
209 > quoting the agreement between the expected BG and the
210 > observation should be enough....}.
211 > Finally, we note that the sross-section uncertainties due to
212 > variations of the factorization
213   and renormalization scale are not included for the LO curve.
214   The results are shown in Figure~\ref{fig:msugra}
215  
# Line 227 | Line 239 | show the raw results, without smoothing)
239   mSUGRA parameter space,
240   assuming $\tan\beta=3$, sign of $\mu = +$ and $A_{0}=0$~GeVs
241   using different models for the nuisance parameters.
242 < PDF UNCERTAINTOES ARE NOT INCLUDED.}
242 > PDF UNCERTAINTIES ARE NOT INCLUDED.}
243   \end{center}
244   \end{figure}
245  
246 < We find that the set of excluded points is identical for the
247 < lognormal and gamma models.  There are small differences for the
248 < gaussian model. Following the recommendation of Reference~\cite{ref:cousins},
249 < we use the lognormal nuisance parameter model.
246 > We find that different assumptions on the PDFs for the nuisance
247 > parameters make very small differences to the set of excluded
248 > points.
249 > Following the recommendation of Reference~\cite{ref:cousins},
250 > we use the lognormal nuisance parameter model as the default.
251  
252  
253 < \clearpage
253 > % \clearpage
254  
255  
256   \subsubsection{Effect of signal contamination}
257   \label{sec:contlimit}
258 +
259   Signal contamination could affect the limit by inflating the
260   background expectation.  In our case we see no evidence of signal
261   contamination, within statistics.
# Line 260 | Line 274 | the data driven methods as confirmations
274  
275   Nevertheless, here we explore the possible effect of
276   signal contamination.  The procedure suggested to us
277 < is the following:
264 < \begin{itemize}
265 < \item At each point in mSUGRA space we modify the
277 > for the ABCD method is to modify the
278   ABCD background prediction from $A_D \cdot C_D/B_D$ to
279   $(A_D-A_S) \cdot (C_D-C_S) / (B_D - B_S)$, where the
280 < subscripts $D$ and $S$ referes to the number of observed data
280 > subscripts $D$ and $S$ refer to the number of observed data
281   events and expected SUSY events, respectively, in a given region.
282 < \item Similarly, at each point in mSugra space we modify the
283 < $P_T(\ell\ell)$ background prediction from
284 < $K \cdot K_C \cdot D'_D$ to $K \cdot K_C \cdot (D'_D - D'_S)$,
285 < where the subscript $D$ and $S$ are defined as above.
286 < \item At each point in mSUGRA space we recalculate $N_{UL}$
287 < using the weighted average of the modified $ABCD$ and
276 < $P_T(\ell\ell)$ method predictions.  
277 < \end{itemize}
278 <
279 < \noindent This procedure results in a reduced background prediction,
280 < and therefore a less stringent $N_{UL}$.  
282 > We then recalculate $N_{UL}$ at each point using this modified
283 > ABCD background estimation.  For simplicity we ignore
284 > information from the $P_T(\ell \ell)$
285 > background estimation.  This is conservative, since
286 > the $P_T(\ell\ell)$ background estimation happens to
287 > be numerically larger than the one from ABCD.
288  
289   Note, however, that in some cases this procedure is
290   nonsensical.  For example, take LM0 as a SUSY
# Line 291 | Line 298 | LM0 hypothesis.  Instead, we now get a n
298   BG prediction (which is nonsense, so we set it to zero),
299   and therefore a weaker limit.
300  
301 +
302 +
303 +
304   \begin{figure}[tbh]
305   \begin{center}
306   \includegraphics[width=0.5\linewidth]{sigcont.png}
# Line 302 | Line 312 | PDF UNCERTAINTIES ARE NOT INCLUDED.}
312   \end{center}
313   \end{figure}
314  
315 < Despite these reservations, we follow the procedure suggested
316 < to us.  A comparison of the exclusion region with and without
307 < the signal contamination is shown in Figure~\ref{fig:sigcont}
315 > A comparison of the exclusion region with and without
316 > signal contamination is shown in Figure~\ref{fig:sigcont}
317   (with no smoothing).  The effect of signal contamination is
318 < small.
318 > small, of the same order as the quantization of the scan.
319 >
320  
321   \subsubsection{mSUGRA scans with different values of tan$\beta$}
322   \label{sec:tanbetascan}

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