34 |
|
LM0 and LM1 events from Table~\ref{tab:sigcont}: $8.6 \pm 1.6$ |
35 |
|
events and $3.6 \pm 0.5$ events respectively, where the uncertainties |
36 |
|
are from energy scale (Section~\ref{sec:systematics}), luminosity, |
37 |
< |
and lepton efficiency. Note that these expected SUSY yields |
38 |
< |
are computed using LO cross-sections, and are therefore underestimated. |
37 |
> |
and lepton efficiency. |
38 |
> |
|
39 |
> |
We also performed a scan of the mSUGRA parameter space. We set $\tan\beta=10$, |
40 |
> |
sign of $\mu = +$, $A_{0}=0$~GeV, and scan the $m_{0}$ and $m_{1/2}$ parameters |
41 |
> |
in steps of 10~GeV. For each scan point, we exclude the point if the expected |
42 |
> |
yield in the signal region exceeds 4.7, which is the 95\% CL upper limit |
43 |
> |
based on an expected background of $N_{BG}=1.4 \pm 0.8$ and a 20\% acceptance |
44 |
> |
uncertainty. The results are shown in Fig.~\ref{fig:msugra}. |
45 |
> |
|
46 |
> |
\begin{figure}[tbh] |
47 |
> |
\begin{center} |
48 |
> |
\includegraphics[width=0.6\linewidth]{msugra.png} |
49 |
> |
\caption{\label{fig:msugra}\protect Exclusion curve in the mSUGRA parameter space, |
50 |
> |
assuming $\tan\beta=10$, sign of $\mu = +$ and $A_{0}=0$~GeVs.} |
51 |
> |
\end{center} |
52 |
> |
\end{figure} |
53 |
> |
|
54 |
|
|
55 |
|
Conveying additional useful information about the results of |
56 |
|
a generic ``signature-based'' search such as the one described |
60 |
|
Other models of new physics in the dilepton final state |
61 |
|
can be confronted in an approximate way by simple |
62 |
|
generator-level studies that |
63 |
< |
compare the expected number of events in 35 pb$^{-1}$ |
63 |
> |
compare the expected number of events in 34.0~pb$^{-1}$ |
64 |
|
with our upper limit of 4.1 events. The key ingredients |
65 |
|
of such studies are the kinematical cuts described |
66 |
|
in this note, the lepton efficiencies, and the detector |
71 |
|
$P_T = 10$ GeV to 91\% for $P_T > 30$ GeV. The isolation |
72 |
|
efficiency in top events varies from $\approx 83\%$ (muons) |
73 |
|
and $\approx 89\%$ (electrons) at $P_T=10$ GeV to |
74 |
< |
$\approx 95\%$ for $P_T>60$ GeV. |
75 |
< |
{\bf \color{red} The following quantities were calculated |
61 |
< |
with Spring10 samples. } |
62 |
< |
The average detector |
74 |
> |
$\approx 95\%$ for $P_T>60$ GeV. {\bf \color{red} The following quantities were calculated |
75 |
> |
with Spring10 samples. } The average detector |
76 |
|
responses for SumJetPt and $\met/\sqrt{\rm SumJetPt}$ are |
77 |
|
$1.00 \pm 0.05$ and $0.94 \pm 0.05$ respectively, where |
78 |
|
the uncertainties are from the jet energy scale uncertainty. |
87 |
|
signal region. |
88 |
|
% (SumJetPt $>$ 300 GeV and \met/$\sqrt{\rm SumJetPt} > 8.5$ |
89 |
|
% Gev$^{\frac{1}{2}}$). |
90 |
< |
{\bf \color{red} The following numbers were derived from Spring10 samples.} |
90 |
> |
{\bf \color{red} The following numbers were derived from Spring10 samples, They should be the same for the Fall10 samples; this needs to be verified .} |
91 |
|
We find that the average SumJetPt response |
92 |
|
in the Monte Carlo is very close to one, with an RMS of order 10\% while |
93 |
|
the response of \met/$\sqrt{\rm SumJetPt}$ is approximately 0.94 with an |
102 |
|
|
103 |
|
\begin{figure}[tbh] |
104 |
|
\begin{center} |
105 |
< |
\includegraphics[width=\linewidth]{selectionEff.png} |
105 |
> |
\includegraphics[width=\linewidth]{selectionEffDec10.png} |
106 |
|
\caption{\label{fig:response} Left plots: the efficiencies |
107 |
|
as a function of the true quantities for the SumJetPt (top) and |
108 |
|
tcMET/$\sqrt{\rm SumJetPt}$ (bottom) requirements for the signal |
114 |
|
to the true quantity in MC. These plots are done using the LM0 |
115 |
|
Monte Carlo, but they are not expected to depend strongly on |
116 |
|
the underlying physics. |
117 |
< |
{\bf \color{red} These plots were made with Spring10 samples. } } |
117 |
> |
{\bf \color{red} These plots were made with Fall10 samples. } } |
118 |
|
\end{center} |
119 |
|
\end{figure} |
120 |
|
|
150 |
|
% Are the above correct? y |
151 |
|
% 1 29.995 0.50457E-06 |
152 |
|
% |
153 |
< |
% limit: less than 4.689 signal events |
153 |
> |
% limit: less than 4.689 signal events |