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In Table~\ref{tab:cr1mtsf} we show the amount that we need to scale the Wjets MC |
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by in order to have agreement between data and Monte Carlo in the $M_T$ peak |
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region, defined as $60 < M_T < 100$ GeV. These scale factors are not terribly |
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important, but it is reassuring that they are not too different from 1. (ARE THESE |
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SCALED FOR TRIGGER EFFICIENCY???) |
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important, but it is reassuring that they are not too different from |
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1. [UPDATE WITH TRIGGER EFFICIENCIES] |
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|
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|
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\begin{table}[!h] |
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Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D & CR1E\\ |
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\hline |
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\hline |
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Muon \mt-SF & $0.75 \pm 0.01$ & $0.77 \pm 0.02$ & $0.78 \pm 0.03$ & $0.79 \pm 0.05$ & $0.88 \pm 0.08$ & $0.91 \pm 0.12$ \\ |
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Muon \mt-SF & $0.92 \pm 0.02$ & $0.97 \pm 0.03$ & $0.90 \pm 0.04$ & $0.91 \pm 0.06$ & $0.93 \pm 0.09$ & $0.98 \pm 0.13$ \\ |
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\hline |
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\hline |
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Electron \mt-SF & $0.84 \pm 0.02$ & $0.83 \pm 0.03$ & $0.80 \pm 0.04$ & $0.78 \pm 0.06$ & $0.76 \pm 0.09$ & $0.73 \pm 0.12$ \\ |
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Electron \mt-SF & $0.94 \pm 0.02$ & $0.90 \pm 0.04$ & $0.84 \pm 0.05$ & $0.80 \pm 0.07$ & $0.83 \pm 0.10$ & $0.77 \pm 0.13$ \\ |
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\hline |
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\end{tabular} |
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\caption{ \mt\ peak Data/MC scale factors applied to the single lepton |
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Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D & CR1E\\ |
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\hline |
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\hline |
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Muon MC & $481 \pm 20$ & $176 \pm 5$ & $121 \pm 4$ & $42 \pm 2$ & $18 \pm 2$ & $9 \pm 1$ \\ |
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Muon MC & $480 \pm 22$ & $173 \pm 5$ & $114 \pm 4$ & $40 \pm 2$ & $16 \pm 1$ & $8 \pm 1$ \\ |
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Muon Data & $629$ & $238$ & $139$ & $45$ & $12$ & $8$ \\ |
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\hline |
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Muon Data/MC SF: ($SFR^{\mu}_{wjet}$) & $1.31 \pm 0.08$ & $1.35 \pm 0.10$ & $1.15 \pm 0.11$ & $1.06 \pm 0.17$ & $0.68 \pm 0.21$ & $0.92 \pm 0.35$ \\ |
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Muon Data/MC SF: ($SFR^{\mu}_{wjet}$) & $1.31 \pm 0.08$ & $1.37 \pm 0.10$ & $1.22 \pm 0.11$ & $1.12 \pm 0.18$ & $0.75 \pm 0.23$ & $0.99 \pm 0.37$ \\ |
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\hline |
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\hline |
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Electron MC & $322 \pm 7$ & $119 \pm 4$ & $81 \pm 3$ & $30 \pm 2$ & $13 \pm 1$ & $5 \pm 1$ \\ |
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Electron Data & $487$ & $181$ & $103$ & $38$ & $16$ & $6$ \\ |
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Electron MC & $330 \pm 8$ & $118 \pm 4$ & $79 \pm 3$ & $29 \pm 2$ & $13 \pm 1$ & $5 \pm 1$ \\ |
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Electron Data & $473$ & $174$ & $100$ & $36$ & $16$ & $5$ \\ |
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\hline |
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Electron Data/MC SF: ($SFR^e_{wjet}$) & $1.51 \pm 0.08$ & $1.53 \pm 0.13$ & $1.28 \pm 0.14$ & $1.25 \pm 0.22$ & $1.25 \pm 0.34$ & $1.26 \pm 0.56$ \\ |
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Electron Data/MC SF: ($SFR^e_{wjet}$) & $1.43 \pm 0.07$ & $1.47 \pm 0.12$ & $1.27 \pm 0.14$ & $1.23 \pm 0.22$ & $1.26 \pm 0.34$ & $1.07 \pm 0.51$ \\ |
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\hline |
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\end{tabular}} |
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\caption{ Yields in \mt\ tail comparing the MC prediction (after |
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\end{center} |
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\end{table} |
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|
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|
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\begin{table}[!h] |
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\begin{center} |
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{\footnotesize |
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\begin{tabular}{l||c||c|c|c|c|c} |
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\hline |
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Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D & CR1E\\ |
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\hline |
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\hline |
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Muon W+jets MC & $300 \pm 23$ & $84 \pm 5$ & $52 \pm 4$ & $20 \pm 2$ & $9 \pm 2$ & $5 \pm 1$ \\ |
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Muon Data - non-W+jets MC & $449 \pm 26$ & $149 \pm 16$ & $78 \pm 12$ & $25 \pm 7$ & $5 \pm 4$ & $5 \pm 3$ \\ |
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\hline |
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Muon Data/MC SF: ($SFR^{\mu}_{wjet}$) & $1.50 \pm 0.14$ & $1.77 \pm 0.21$ & $1.49 \pm 0.26$ & $1.25 \pm 0.38$ & $0.56 \pm 0.39$ & $0.98 \pm 0.62$ \\ |
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\hline |
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\hline |
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Electron W+jets MC & $192 \pm 8$ & $55 \pm 4$ & $36 \pm 3$ & $14 \pm 2$ & $6 \pm 1$ & $3 \pm 1$ \\ |
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Electron Data - non-W+jets MC & $335 \pm 22$ & $111 \pm 13$ & $58 \pm 10$ & $20 \pm 6$ & $10 \pm 4$ & $3 \pm 2$ \\ |
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\hline |
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Electron Data/MC SF: ($SFR^e_{wjet}$) & $1.74 \pm 0.14$ & $2.02 \pm 0.29$ & $1.58 \pm 0.32$ & $1.49 \pm 0.50$ & $1.50 \pm 0.70$ & $1.10 \pm 0.80$ \\ |
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\hline |
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\end{tabular}} |
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\caption{ Yields in \mt\ tail comparing the \wjets\ MC prediction (after |
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applying SFs) to data after subtracting the non-\wjets\ component. CR1PRESEL refers to a sample with $\met>50$ |
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GeV and $\mt>150$ GeV. |
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The uncertainties are statistical only. |
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\label{tab:cr1wyields}} |
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\end{center} |
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\end{table} |
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|
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|
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\begin{figure}[hbt] |
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\begin{center} |