154 |
|
\hline |
155 |
|
\hline |
156 |
|
N jets $= 3$ (sensitive to $\ttbar+1$ extra jet from radiation) & |
157 |
< |
$K_3 = 0.97 \pm 0.03$\\ |
157 |
> |
$K_3 = 1.01 \pm 0.03$\\ |
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|
N jets $\ge4$ (sensitive to $\ttbar+\ge2$ extra jets from radiation) |
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< |
& $K_4 = 0.91 \pm 0.04$\\ |
159 |
> |
& $K_4 = 0.93 \pm 0.04$\\ |
160 |
|
\hline |
161 |
|
\end{tabular} |
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\caption{Data/MC scale factors used to account for differences in the |
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background by looking at the $M_T$ distribution of well identified |
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dilepton events. |
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We construct a transverse mass variable from the leading lepton and |
184 |
< |
the \met\. We distinguish between events with leading electrons and |
184 |
> |
the \met. We distinguish between events with leading electrons and |
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leading muons. |
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|
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The $t\bar{t}$ MC is corrected using the $K_3$ and $K_4$ factors |
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|
|
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|
\begin{table}[!h] |
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|
\begin{center} |
200 |
< |
\begin{tabular}{l||c|c|c|c} |
200 |
> |
{\footnotesize |
201 |
> |
\begin{tabular}{l||c||c|c|c|c|c|c} |
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|
\hline |
203 |
< |
Sample & CR4A & CR4B & CR4C & CR4D \\ |
203 |
> |
Sample & CR4PRESEL & CR4A & CR4B & CR4C & |
204 |
> |
CR4D & CR4E & CR4F\\ |
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|
\hline |
206 |
|
\hline |
207 |
< |
Muon Data/MC-SF & $0.91 \pm 0.04$ & $0.94 \pm 0.07$ & $1.06 \pm 0.13$ & $1.03 \pm 0.22$ \\ |
207 |
> |
$\mu$ Data/MC-SF & $1.01 \pm 0.03$ & $0.96 \pm 0.04$ & $0.99 \pm 0.07$ & $1.05 \pm 0.13$ & $0.91 \pm 0.20$ & $1.10 \pm 0.34$ & $1.50 \pm 0.67$ \\ |
208 |
|
\hline |
209 |
|
\hline |
210 |
< |
Electron Data/MC-SF & $0.95 \pm 0.04$ & $1.00 \pm 0.08$ & $0.85 \pm 0.12$ & $0.83 \pm 0.19$ \\ |
210 |
> |
e Data/MC-SF & $0.99 \pm 0.03$ & $0.99 \pm 0.05$ & $0.91 \pm 0.08$ & $0.84 \pm 0.13$ & $0.70 \pm 0.18$ & $0.73 \pm 0.29$ & $0.63 \pm 0.38$ \\ |
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|
\hline |
212 |
< |
\end{tabular} |
212 |
> |
\end{tabular}} |
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|
\caption{ Data/MC scale factors for total yields, applied to compare |
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the shapes of the distributions. |
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The uncertainties are statistical only. |
220 |
|
|
221 |
|
\begin{table}[!h] |
222 |
|
\begin{center} |
223 |
< |
\begin{tabular}{l||c|c|c|c} |
223 |
> |
{\footnotesize |
224 |
> |
\begin{tabular}{l||c||c|c|c|c|c|c} |
225 |
|
\hline |
226 |
< |
Sample & CR4A & CR4B & CR4C & CR4D \\ |
226 |
> |
Sample & CR4PRESEL & CR4A & CR4B & CR4C & |
227 |
> |
CR4D & CR4E & CR4F\\ |
228 |
|
\hline |
229 |
|
\hline |
230 |
< |
Muon MC & $199 \pm 7$ & $102 \pm 6$ & $29 \pm 3$ & $8 \pm 1$ \\ |
231 |
< |
Muon Data & $187$ & $108$ & $34$ & $9$ \\ |
230 |
> |
$\mu$ MC & $256 \pm 14$ & $152 \pm 11$ & $91 \pm 9$ & $26 \pm 5$ & $6 \pm 2$ & $4 \pm 2$ & $2 \pm 1$ \\ |
231 |
> |
$\mu$ Data & $251$ & $156$ & $98$ & $27$ & $8$ & $6$ & $4$ \\ |
232 |
|
\hline |
233 |
< |
Muon Data/MC SF & $0.94 \pm 0.08$ & $1.06 \pm 0.12$ & $1.17 \pm 0.23$ & $1.09 \pm 0.40$ \\ |
233 |
> |
$\mu$ Data/MC SF & $0.98 \pm 0.08$ & $1.02 \pm 0.11$ & $1.08 \pm 0.16$ & $1.04 \pm 0.28$ & $1.29 \pm 0.65$ & $1.35 \pm 0.80$ & $2.10 \pm 1.72$ \\ |
234 |
|
\hline |
235 |
|
\hline |
236 |
< |
Electron MC & $203 \pm 8$ & $97 \pm 5$ & $26 \pm 2$ & $8 \pm 1$ \\ |
237 |
< |
Electron Data & $201$ & $102$ & $25$ & $5$ \\ |
236 |
> |
e MC & $227 \pm 13$ & $139 \pm 11$ & $73 \pm 8$ & $21 \pm 4$ & $5 \pm 2$ & $2 \pm 1$ & $1 \pm 1$ \\ |
237 |
> |
e Data & $219$ & $136$ & $72$ & $19$ & $2$ & $1$ & $1$ \\ |
238 |
|
\hline |
239 |
< |
Electron Data/MC SF & $0.99 \pm 0.08$ & $1.06 \pm 0.12$ & $0.97 \pm 0.21$ & $0.60 \pm 0.29$ \\ |
239 |
> |
e Data/MC SF & $0.96 \pm 0.09$ & $0.98 \pm 0.11$ & $0.99 \pm 0.16$ & $0.92 \pm 0.29$ & $0.41 \pm 0.33$ & $0.53 \pm 0.62$ & $0.76 \pm 0.96$ \\ |
240 |
|
\hline |
241 |
< |
\end{tabular} |
241 |
> |
\hline |
242 |
> |
$\mu$+e MC & $483 \pm 19$ & $291 \pm 16$ & $164 \pm 13$ & $47 \pm 7$ & $11 \pm 3$ & $6 \pm 2$ & $3 \pm 2$ \\ |
243 |
> |
$\mu$+e Data & $470$ & $292$ & $170$ & $46$ & $10$ & $7$ & $5$ \\ |
244 |
> |
\hline |
245 |
> |
$\mu$+e Data/MC SF & $0.97 \pm 0.06$ & $1.00 \pm 0.08$ & $1.04 \pm 0.11$ & $0.99 \pm 0.20$ & $0.90 \pm 0.37$ & $1.11 \pm 0.57$ & $1.55 \pm 1.04$ \\ |
246 |
> |
\hline |
247 |
> |
\end{tabular}} |
248 |
|
\caption{ Yields in \mt\ tail comparing the MC prediction (after |
249 |
|
applying SFs) to data. The uncertainties are statistical only. |
250 |
|
\label{tab:cr4yields}} |
268 |
|
|
269 |
|
\begin{figure}[hbt] |
270 |
|
\begin{center} |
271 |
+ |
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met50_leadmuo_nj4.pdf}% |
272 |
+ |
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met50_leadele_nj4.pdf} |
273 |
|
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met150_leadmuo_nj4.pdf}% |
274 |
|
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met150_leadele_nj4.pdf} |
275 |
|
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met200_leadmuo_nj4.pdf}% |
276 |
|
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met200_leadele_nj4.pdf} |
265 |
– |
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met250_leadmuo_nj4.pdf}% |
266 |
– |
\includegraphics[width=0.5\linewidth]{plots/CR4plots/mt_met250_leadele_nj4.pdf} |
277 |
|
\caption{ |
278 |
|
Comparison of the \mt\ distribution in data vs. MC for events |
279 |
|
with a leading muon (left) and leading electron (right) |
280 |
|
satisfying the requirements of CR4. The \met\ requirements used are |
281 |
< |
150 GeV (top), 200 GeV (middle) and 250 GeV (bottom). |
281 |
> |
50 GeV (top), 200 GeV (middle) and 250 GeV (bottom). |
282 |
|
\label{fig:cr4mtrest} |
283 |
|
} |
284 |
|
\end{center} |