3 |
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|
4 |
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|
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The estimate of the uncertainty on this background is based on CR1, |
6 |
< |
defined by applying the full signal selection, but requiring 0 b-tags. |
7 |
< |
SPECIFY THE EXACT REQUIREMENT FOR THE BVETO AND SAY WHETHER THERE IS |
8 |
< |
AN ISOLATED TRACK VETO. |
6 |
> |
defined by applying the full signal selection, including the isolated track veto, but requiring 0 b-tags |
7 |
> |
(CSV medium working point as described in Sec.~\ref{sec:selection}). |
8 |
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The sample is dominanted by \wjets\ and is thus used to validate the MC modelling of this background. |
9 |
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|
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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 |
12 |
< |
region, defined as $XX < M_T < YY$ GeV. These scale factors are not terribly |
12 |
> |
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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|
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|
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\begin{table}[!h] |
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\begin{center} |
19 |
< |
\begin{tabular}{l||c||c|c|c|c} |
19 |
> |
\begin{tabular}{l||c||c|c|c|c|c} |
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|
\hline |
21 |
< |
Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D \\ |
21 |
> |
Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D & CR1E\\ |
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|
\hline |
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|
\hline |
24 |
< |
Muon \mt-SF & $0.91 \pm 0.03$ & $0.96 \pm 0.07$ & $0.88 \pm 0.11$ & $1.05 \pm 0.21$ & $1.27 \pm 0.41$ \\ |
24 |
> |
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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|
\hline |
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|
\hline |
27 |
< |
Electron \mt-SF & $0.82 \pm 0.03$ & $0.86 \pm 0.06$ & $1.09 \pm 0.15$ & $1.24 \pm 0.30$ & $1.11 \pm 0.40$ \\ |
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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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|
\hline |
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\end{tabular} |
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\caption{ \mt\ peak Data/MC scale factors applied to the single lepton |
43 |
|
|
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|
\begin{table}[!h] |
45 |
|
\begin{center} |
46 |
< |
\begin{tabular}{l||c||c|c|c|c} |
46 |
> |
{\footnotesize |
47 |
> |
\begin{tabular}{l||c||c|c|c|c|c} |
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|
\hline |
49 |
< |
Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D \\ |
49 |
> |
Sample & CR1PRESEL & CR1A & CR1B & CR1C & CR1D & CR1E\\ |
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|
\hline |
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|
\hline |
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< |
Muon MC & $456 \pm 73$ & $174 \pm 44$ & $51 \pm 7$ & $18 \pm 2$ & $10 \pm 2$ \\ |
53 |
< |
Muon Data & $657$ & $246$ & $142$ & $43$ & $12$ \\ |
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> |
Muon MC & $481 \pm 20$ & $176 \pm 5$ & $121 \pm 4$ & $42 \pm 2$ & $18 \pm 2$ & $9 \pm 1$ \\ |
53 |
> |
Muon Data & $629$ & $238$ & $139$ & $45$ & $12$ & $8$ \\ |
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|
\hline |
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< |
Muon Data/MC SF: ($SFR^{\mu}_{wjet}$) & $1.44 \pm 0.24$ & $1.41 \pm 0.37$ & $2.80 \pm 0.47$ & $2.37 \pm 0.46$ & $1.23 \pm 0.42$ \\ |
55 |
> |
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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|
\hline |
57 |
|
\hline |
58 |
< |
Electron MC & $396 \pm 64$ & $147 \pm 36$ & $54 \pm 4$ & $19 \pm 2$ & $8 \pm 2$ \\ |
59 |
< |
Electron Data & $702$ & $223$ & $144$ & $50$ & $23$ \\ |
58 |
> |
Electron MC & $322 \pm 7$ & $119 \pm 4$ & $81 \pm 3$ & $30 \pm 2$ & $13 \pm 1$ & $5 \pm 1$ \\ |
59 |
> |
Electron Data & $487$ & $181$ & $103$ & $38$ & $16$ & $6$ \\ |
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|
\hline |
61 |
< |
Electron Data/MC SF: ($SFR^e_{wjet}$) & $1.77 \pm 0.29$ & $1.52 \pm 0.39$ & $2.68 \pm 0.30$ & $2.57 \pm 0.49$ & $2.73 \pm 0.76$ \\ |
61 |
> |
Electron Data/MC SF: ($SFR^e_{wjet}$) & $1.51 \pm 0.08$ & $1.53 \pm 0.13$ & $1.28 \pm 0.14$ & $1.25 \pm 0.22$ & $1.25 \pm 0.34$ & $1.26 \pm 0.56$ \\ |
62 |
|
\hline |
63 |
< |
\end{tabular} |
63 |
> |
\end{tabular}} |
64 |
|
\caption{ Yields in \mt\ tail comparing the MC prediction (after |
65 |
|
applying SFs) to data. CR1PRESEL refers to a sample with $\met>50$ |
66 |
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GeV and $\mt>150$ GeV. |
67 |
< |
The uncertainties are statistical only. VERENA MAKE SURE YOU ADD SCALE FACTOR SYMBOLS TO THIS TABLE. |
67 |
> |
The uncertainties are statistical only. |
68 |
|
\label{tab:cr1yields}} |
69 |
|
\end{center} |
70 |
|
\end{table} |