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The event yields in data and Monte Carlo for SS and |
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OS are given in Tables~\ref{tab:yieldSS} and~\ref{tab:yieldOS}. |
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OS are given in Tables~\ref{tab:yieldOS} and~\ref{tab:yieldSS}. |
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\begin{table}[htb] |
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\begin{center} |
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\caption{\label{tab:yieldSS} Observed and MC-predicted yields in the SS |
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selection. Quoted uncertainties are MC statistics only. In case that |
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\caption{\label{tab:yieldOS} Observed and MC-predicted yields in the OS |
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selection. Quoted uncertainties are MC statistics only. In case that |
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no MC event passes the selection, we quote the uncertainty as the weight |
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of one MC event.} |
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\begin{tabular}{|l|c|c|c|c|c|} \hline |
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Final State & QCD & $\gamma +$ jet & DY & Total MC & Data \\ |
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\hline |
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ee & & & & & \\ |
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e$\mu$ & & & & & \\ |
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$\mu\mu$ & & & & & \\ |
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ee & 0.00$\pm$0.17 & 0.01 $\pm$ 0.004 & 0.83$\pm$0.02 & 0.84$\pm$0.17 & 2 \\ |
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e$\mu$ & 0.17$\pm$0.17 & 0.000$\pm$0.004 & 0.08 $\pm$ 0.01& 0.25$\pm$0.17 & 0 \\ |
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$\mu\mu$& 0.00$\pm$0.17 & 0 & 1.36$\pm$0.03 &1.36$\pm$0.17&3 \\ |
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\hline |
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All & & & & & \\ |
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All &0.17$\pm$0.17 &0.01$\pm$0.004 & 2.27$\pm$0.03 & 2.44$\pm$0.17 & 5 \\ |
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\hline |
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\end{tabular} |
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\end{center} |
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\end{table} |
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|
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\begin{table}[htb] |
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\begin{center} |
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\caption{\label{tab:yieldOS} Observed and MC-predicted yields in the OS |
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selection. Quoted uncertainties are MC statistics only. In case that |
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\caption{\label{tab:yieldSS} Observed and MC-predicted yields in the SS |
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selection. Quoted uncertainties are MC statistics only. In case that |
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no MC event passes the selection, we quote the uncertainty as the weight |
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of one MC event.} |
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\begin{tabular}{|l|c|c|c|c|c|} \hline |
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Final State & QCD & $\gamma +$ jet & DY & Total MC & Data \\ |
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Final State & QCD & $\gamma +$ jet & DY & Total MC & Data \\ |
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\hline |
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ee & 0.00$\pm$0.17 & 0.01 $\pm$ 0.004 & 0.83$\pm$0.02 & 0.84$\pm$0.17 & 2 \\ |
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e$\mu$ & 0.17$\pm$0.17 & 0.000$\pm$0.004& 0.08 $\pm$ 0.01& 0.25$\pm$0.17 & 0 \\ |
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$\mu\mu$ & 0.00$\pm$0.17 & 0.000 $\pm$ 0.004 & 1.36$\pm$0.03&1.36$\pm$0.17&3 \\ |
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ee & $0.0 \pm 0.2$ & $0.002 \pm 0.002$ & $0.01 \pm 0.003$&$ 0.01\pm 0.2$ &0 \\ |
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e$\mu$ & $0.0 \pm 0.2$ & $0.004 \pm 0.003$ & $0.005 \pm 0.002$&$ 0.01 \pm 0.2 $ &0 \\ |
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$\mu\mu$ & $0.0 \pm 0.2$ & 0 & $0.001 \pm 0.001$&$ 0.001\pm 0.2 $ &0 \\ |
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\hline |
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All &0.17$\pm$0.17 &0.01$\pm$0.004 & 2.27$\pm$0.03 & 2.44$\pm$0.17 & 5 \\ |
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All & $0.0 \pm 0.2$ & $0.006 \pm 0.003$ & $0.016 \pm 0.003$&$0.02\pm 0.3$ &0 \\ |
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\hline |
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\end{tabular} |
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\end{center} |
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|
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We find the $\gamma +$ jet MC predictions to be negligible. |
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The QCD statistics are so poor that we cannot make any quantitative |
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statement. |
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The OS data is dominated by Drell Yan. The agreement between |
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MC and data yields is good. |
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|
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For now we use the MC to predict the rate of SS events from Drell-Yan evens |
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off the $Z$ peak. These events are from electron charge misidentification. |
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For now we use the MC to predict the rate of SS events from Drell-Yan |
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off the $Z$ peak. These events are mostly from electron charge misidentification. |
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We have developed techniques to measure this charge flip probability |
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from $Z \to ee$ data\cite{ref:SSSusy}. However, this cannot be done at the |
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present level of statistics. Interestingly enough, we did find one SS |