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the boundaries using the method recommended by the SUSY |
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group\cite{ref:smooth}. In addition, we show a limit |
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curve based on the LO cross-section, as well as the |
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``expected'' limit curve. The expected limit curve is |
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``expected'' limit curve. The expected limit curve was |
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calculated using the CLA function also available in cl95cms. |
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Cross-section uncertainties due to variations of the factorization |
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In general we found that the ``expected'' limit is very close |
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to the observed limit, which is not surprising since the |
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expected BG (1.4 $\pm$ 0.8 events) is fully consistent |
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with the observation (1 event). Because of the quantization, |
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we find that the expected and observed limits are either |
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identical or differ by one or at most two grid points. |
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We have approximated the expected limit as the observed limit |
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minus 10 GeV\footnote{We show the expected limit only because |
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this is what is recommended by SUSY management. We believe that |
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quoting the agreement between the expected BG and the |
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observation should be enough....}. |
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Finally, we note that the sross-section uncertainties due to |
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variations of the factorization |
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and renormalization scale are not included for the LO curve. |
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The results are shown in Figure~\ref{fig:msugra} |
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|
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mSUGRA parameter space, |
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assuming $\tan\beta=3$, sign of $\mu = +$ and $A_{0}=0$~GeVs |
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using different models for the nuisance parameters. |
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< |
PDF UNCERTAINTOES ARE NOT INCLUDED.} |
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PDF UNCERTAINTIES ARE NOT INCLUDED.} |
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|
\end{center} |
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\end{figure} |
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|
|
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We find that the set of excluded points is identical for the |
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lognormal and gamma models. There are small differences for the |
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gaussian model. Following the recommendation of Reference~\cite{ref:cousins}, |
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we use the lognormal nuisance parameter model. |
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> |
We find that different assumptions on the PDFs for the nuisance |
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> |
parameters make very small differences to the set of excluded |
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> |
points. |
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> |
Following the recommendation of Reference~\cite{ref:cousins}, |
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> |
we use the lognormal nuisance parameter model as the default. |
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|
|
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|
|
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< |
\clearpage |
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> |
% \clearpage |
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|
|
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|
|
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|
\subsubsection{Effect of signal contamination} |
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\label{sec:contlimit} |
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+ |
|
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Signal contamination could affect the limit by inflating the |
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background expectation. In our case we see no evidence of signal |
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contamination, within statistics. |
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|
|
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Nevertheless, here we explore the possible effect of |
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|
signal contamination. The procedure suggested to us |
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< |
is the following: |
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\begin{itemize} |
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\item At each point in mSUGRA space we modify the |
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> |
for the ABCD method is to modify the |
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|
ABCD background prediction from $A_D \cdot C_D/B_D$ to |
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|
$(A_D-A_S) \cdot (C_D-C_S) / (B_D - B_S)$, where the |
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< |
subscripts $D$ and $S$ referes to the number of observed data |
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> |
subscripts $D$ and $S$ refer to the number of observed data |
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|
events and expected SUSY events, respectively, in a given region. |
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\item Similarly, at each point in mSugra space we modify the |
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< |
$P_T(\ell\ell)$ background prediction from |
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< |
$K \cdot K_C \cdot D'_D$ to $K \cdot K_C \cdot (D'_D - D'_S)$, |
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< |
where the subscript $D$ and $S$ are defined as above. |
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< |
\item At each point in mSUGRA space we recalculate $N_{UL}$ |
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< |
using the weighted average of the modified $ABCD$ and |
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$P_T(\ell\ell)$ method predictions. |
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< |
\end{itemize} |
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|
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\noindent This procedure results in a reduced background prediction, |
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and therefore a less stringent $N_{UL}$. |
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> |
We then recalculate $N_{UL}$ at each point using this modified |
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> |
ABCD background estimation. For simplicity we ignore |
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> |
information from the $P_T(\ell \ell)$ |
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> |
background estimation. This is conservative, since |
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> |
the $P_T(\ell\ell)$ background estimation happens to |
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> |
be numerically larger than the one from ABCD. |
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|
|
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|
Note, however, that in some cases this procedure is |
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|
nonsensical. For example, take LM0 as a SUSY |
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|
BG prediction (which is nonsense, so we set it to zero), |
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|
and therefore a weaker limit. |
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|
|
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+ |
|
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+ |
|
303 |
+ |
|
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|
\begin{figure}[tbh] |
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|
\begin{center} |
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|
\includegraphics[width=0.5\linewidth]{sigcont.png} |
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|
\end{center} |
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|
\end{figure} |
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|
|
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< |
Despite these reservations, we follow the procedure suggested |
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< |
to us. A comparison of the exclusion region with and without |
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< |
the signal contamination is shown in Figure~\ref{fig:sigcont} |
315 |
> |
A comparison of the exclusion region with and without |
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> |
signal contamination is shown in Figure~\ref{fig:sigcont} |
317 |
|
(with no smoothing). The effect of signal contamination is |
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< |
small. |
318 |
> |
small, of the same order as the quantization of the scan. |
319 |
> |
|
320 |
|
|
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|
\subsubsection{mSUGRA scans with different values of tan$\beta$} |
322 |
|
\label{sec:tanbetascan} |