| 300 |
|
[EVERYTHING IS 7TEV HERE, UPDATE WITH NEW RESULTS \\ |
| 301 |
|
ADD TABLE WITH FRACTION OF EVENTS THAT HAVE A TRUE ISOLATED TRACK] |
| 302 |
|
|
| 303 |
+ |
\begin{table}[!h] |
| 304 |
+ |
\begin{center} |
| 305 |
+ |
{\footnotesize |
| 306 |
+ |
\begin{tabular}{l||c|c|c|c|c} |
| 307 |
+ |
\hline |
| 308 |
+ |
Sample & SRA & SRB & SRC & SRD & SRE\\ |
| 309 |
+ |
\hline |
| 310 |
+ |
\hline |
| 311 |
+ |
Muon Frac. \ttdl\ with true iso. trk. & $0.32 \pm 0.03$ & $0.30 \pm 0.03$ & $0.32 \pm 0.06$ & $0.34 \pm 0.10$ & $0.35 \pm 0.16$ \\ |
| 312 |
+ |
\hline |
| 313 |
+ |
\hline |
| 314 |
+ |
Electron Frac. \ttdl\ with true iso. trk. & $0.32 \pm 0.03$ & $0.31 \pm 0.04$ & $0.33 \pm 0.06$ & $0.38 \pm 0.11$ & $0.38 \pm 0.19$ \\ |
| 315 |
+ |
\hline |
| 316 |
+ |
\end{tabular}} |
| 317 |
+ |
\caption{ Fraction of \ttdl\ events with a true isolated track. |
| 318 |
+ |
\label{tab:trueisotrk}} |
| 319 |
+ |
\end{center} |
| 320 |
+ |
\end{table} |
| 321 |
+ |
|
| 322 |
+ |
|
| 323 |
|
In this section we compare the performance of the isolated track veto in data and MC using tag-and-probe studies |
| 324 |
|
with samples of Z$\to$ee and Z$\to\mu\mu$. The purpose of these studies is to demonstrate that the efficiency |
| 325 |
|
to satisfy the isolated track veto requirements is well-reproduced in the MC, since if this were not the case |
| 364 |
|
|
| 365 |
|
\begin{itemize} |
| 366 |
|
\item Electron passes full analysis ID/iso selection |
| 367 |
< |
\item \pt\ $>$ 30 GeV, $|\eta|<2.5$ |
| 368 |
< |
|
| 349 |
< |
\item Matched to 1 of the 2 electron tag-and-probe triggers |
| 350 |
< |
\begin{itemize} |
| 351 |
< |
\item \verb=HLT_Ele17_CaloIdVT_CaloIsoVT_TrkIdT_TrkIsoVT_SC8_Mass30_v*= |
| 352 |
< |
\item \verb=HLT_Ele17_CaloIdVT_CaloIsoVT_TrkIdT_TrkIsoVT_Ele8_Mass30_v*= |
| 353 |
< |
\end{itemize} |
| 367 |
> |
\item \pt\ $>$ 30 GeV, $|\eta|<2.1$ |
| 368 |
> |
\item Matched to the single electron trigger \verb=HLT_Ele27_WP80_v*= |
| 369 |
|
\end{itemize} |
| 370 |
|
|
| 371 |
|
\item{Probe criteria} |
| 380 |
|
\begin{itemize} |
| 381 |
|
\item Muon passes full analysis ID/iso selection |
| 382 |
|
\item \pt\ $>$ 30 GeV, $|\eta|<2.1$ |
| 383 |
< |
\item Matched to 1 of the 2 electron tag-and-probe triggers |
| 383 |
> |
\item Matched to 1 of the 2 single muon triggers |
| 384 |
|
\begin{itemize} |
| 385 |
|
\item \verb=HLT_IsoMu30_v*= |
| 386 |
|
\item \verb=HLT_IsoMu30_eta2p1_v*= |
| 398 |
|
good agreement between data and MC. To be more quantitative, we compare the data vs. MC efficiencies to satisfy |
| 399 |
|
absolute track isolation requirements varying from $>$ 1 GeV to $>$ 5 GeV, as summarized in Table~\ref{tab:isotrk}. |
| 400 |
|
In the $\geq$0 and $\geq$1 jet bins where the efficiencies can be tested with statistical precision, the data and MC |
| 401 |
< |
efficiencies agree within 7\%, and we apply this as a systematic uncertainty on the isolated track veto efficiency. |
| 401 |
> |
efficiencies agree within 6\%, and we apply this as a systematic uncertainty on the isolated track veto efficiency. |
| 402 |
|
For the higher jet multiplicity bins the statistical precision decreases, but we do not observe any evidence for |
| 403 |
|
a data vs. MC discrepancy in the isolated track veto efficiency. |
| 404 |
|
|
| 409 |
|
|
| 410 |
|
\begin{figure}[hbt] |
| 411 |
|
\begin{center} |
| 412 |
< |
%\includegraphics[width=0.3\linewidth]{plots/el_tkiso_0j.pdf}% |
| 413 |
< |
%\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_0j.pdf} |
| 414 |
< |
%\includegraphics[width=0.3\linewidth]{plots/el_tkiso_1j.pdf}% |
| 415 |
< |
%\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_1j.pdf} |
| 416 |
< |
%\includegraphics[width=0.3\linewidth]{plots/el_tkiso_2j.pdf}% |
| 417 |
< |
%\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_2j.pdf} |
| 418 |
< |
%\includegraphics[width=0.3\linewidth]{plots/el_tkiso_3j.pdf}% |
| 419 |
< |
%\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_3j.pdf} |
| 420 |
< |
%\includegraphics[width=0.3\linewidth]{plots/el_tkiso_4j.pdf}% |
| 421 |
< |
%\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_4j.pdf} |
| 412 |
> |
\includegraphics[width=0.3\linewidth]{plots/el_tkiso_0j.pdf}% |
| 413 |
> |
\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_0j.pdf} |
| 414 |
> |
\includegraphics[width=0.3\linewidth]{plots/el_tkiso_1j.pdf}% |
| 415 |
> |
\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_1j.pdf} |
| 416 |
> |
\includegraphics[width=0.3\linewidth]{plots/el_tkiso_2j.pdf}% |
| 417 |
> |
\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_2j.pdf} |
| 418 |
> |
\includegraphics[width=0.3\linewidth]{plots/el_tkiso_3j.pdf}% |
| 419 |
> |
\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_3j.pdf} |
| 420 |
> |
\includegraphics[width=0.3\linewidth]{plots/el_tkiso_4j.pdf}% |
| 421 |
> |
\includegraphics[width=0.3\linewidth]{plots/mu_tkiso_4j.pdf} |
| 422 |
|
\caption{ |
| 423 |
|
\label{fig:tnp} Comparison of the absolute track isolation in data vs. MC for electrons (left) and muons (right) |
| 424 |
|
for events with the \njets\ requirement varied from \njets\ $\geq$ 0 to \njets\ $\geq$ 4. |
| 436 |
|
\begin{tabular}{l|c|c|c|c|c} |
| 437 |
|
|
| 438 |
|
%Electrons: |
| 439 |
< |
%Total MC yields : 323790 |
| 440 |
< |
%Total DATA yields : 2772586 |
| 439 |
> |
%Selection : ((((((((((abs(tagAndProbeMass-91)<15)&&(qProbe*qTag<0))&&((eventSelection&1)==1))&&(abs(tag->eta())<2.1))&&(tag->pt()>30.0))&&(HLT_Ele27_WP80_tag > 0))&&(met<30))&&(nbl==0))&&((leptonSelection&8)==8))&&(probe->pt()>30))&&(drprobe<0.05) |
| 440 |
> |
%Total MC yields : 2497277 |
| 441 |
> |
%Total DATA yields : 2649453 |
| 442 |
|
%Muons: |
| 443 |
< |
%Total MC yields : 456138 |
| 443 |
> |
%Selection : ((((((((((abs(tagAndProbeMass-91)<15)&&(qProbe*qTag<0))&&((eventSelection&2)==2))&&(abs(tag->eta())<2.1))&&(tag->pt()>30.0))&&(HLT_IsoMu24_tag > 0))&&(met<30))&&(nbl==0))&&((leptonSelection&65536)==65536))&&(probe->pt()>30))&&(drprobe<0.05) |
| 444 |
> |
%Total MC yields : 3749863 |
| 445 |
|
%Total DATA yields : 4210022 |
| 446 |
+ |
%Info in <TCanvas::MakeDefCanvas>: created default TCanvas with name c1 |
| 447 |
+ |
%Info in <TCanvas::Print>: pdf file plots/nvtx.pdf has been created |
| 448 |
|
|
| 449 |
|
\hline |
| 450 |
|
\hline |
| 451 |
|
e + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 452 |
|
\hline |
| 453 |
< |
data & 0.097 $\pm$ 0.0002 & 0.035 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0001 & 0.005 $\pm$ 0.0000 \\ |
| 454 |
< |
mc & 0.096 $\pm$ 0.0005 & 0.034 $\pm$ 0.0003 & 0.015 $\pm$ 0.0002 & 0.008 $\pm$ 0.0002 & 0.005 $\pm$ 0.0001 \\ |
| 455 |
< |
data/mc & 1.01 $\pm$ 0.01 & 1.04 $\pm$ 0.01 & 1.06 $\pm$ 0.02 & 1.04 $\pm$ 0.02 & 1.01 $\pm$ 0.02 \\ |
| 453 |
> |
data & 0.098 $\pm$ 0.0002 & 0.036 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0001 & 0.006 $\pm$ 0.0000 \\ |
| 454 |
> |
mc & 0.097 $\pm$ 0.0002 & 0.034 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0001 & 0.005 $\pm$ 0.0000 \\ |
| 455 |
> |
data/mc & 1.00 $\pm$ 0.00 & 1.04 $\pm$ 0.00 & 1.04 $\pm$ 0.01 & 1.03 $\pm$ 0.01 & 1.02 $\pm$ 0.01 \\ |
| 456 |
|
|
| 457 |
|
\hline |
| 458 |
|
\hline |
| 459 |
|
$\mu$ + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 460 |
|
\hline |
| 461 |
|
data & 0.094 $\pm$ 0.0001 & 0.034 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0000 & 0.006 $\pm$ 0.0000 \\ |
| 462 |
< |
mc & 0.093 $\pm$ 0.0004 & 0.033 $\pm$ 0.0003 & 0.015 $\pm$ 0.0002 & 0.008 $\pm$ 0.0001 & 0.005 $\pm$ 0.0001 \\ |
| 463 |
< |
data/mc & 1.01 $\pm$ 0.00 & 1.04 $\pm$ 0.01 & 1.05 $\pm$ 0.01 & 1.06 $\pm$ 0.02 & 1.07 $\pm$ 0.02 \\ |
| 462 |
> |
mc & 0.093 $\pm$ 0.0001 & 0.033 $\pm$ 0.0001 & 0.015 $\pm$ 0.0001 & 0.009 $\pm$ 0.0000 & 0.006 $\pm$ 0.0000 \\ |
| 463 |
> |
data/mc & 1.01 $\pm$ 0.00 & 1.03 $\pm$ 0.00 & 1.03 $\pm$ 0.01 & 1.03 $\pm$ 0.01 & 1.02 $\pm$ 0.01 \\ |
| 464 |
|
|
| 465 |
|
\hline |
| 466 |
|
\hline |
| 467 |
|
e + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 468 |
|
\hline |
| 469 |
< |
data & 0.109 $\pm$ 0.0005 & 0.043 $\pm$ 0.0003 & 0.022 $\pm$ 0.0002 & 0.013 $\pm$ 0.0002 & 0.009 $\pm$ 0.0002 \\ |
| 470 |
< |
mc & 0.109 $\pm$ 0.0014 & 0.042 $\pm$ 0.0009 & 0.020 $\pm$ 0.0006 & 0.012 $\pm$ 0.0005 & 0.008 $\pm$ 0.0004 \\ |
| 471 |
< |
data/mc & 1.00 $\pm$ 0.01 & 1.04 $\pm$ 0.02 & 1.08 $\pm$ 0.04 & 1.13 $\pm$ 0.05 & 1.13 $\pm$ 0.06 \\ |
| 469 |
> |
data & 0.110 $\pm$ 0.0005 & 0.044 $\pm$ 0.0003 & 0.022 $\pm$ 0.0002 & 0.014 $\pm$ 0.0002 & 0.009 $\pm$ 0.0002 \\ |
| 470 |
> |
mc & 0.110 $\pm$ 0.0005 & 0.042 $\pm$ 0.0003 & 0.021 $\pm$ 0.0002 & 0.013 $\pm$ 0.0002 & 0.009 $\pm$ 0.0001 \\ |
| 471 |
> |
data/mc & 1.00 $\pm$ 0.01 & 1.04 $\pm$ 0.01 & 1.06 $\pm$ 0.02 & 1.08 $\pm$ 0.02 & 1.06 $\pm$ 0.03 \\ |
| 472 |
|
|
| 473 |
|
\hline |
| 474 |
|
\hline |
| 475 |
|
$\mu$ + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 476 |
|
\hline |
| 477 |
|
data & 0.106 $\pm$ 0.0004 & 0.043 $\pm$ 0.0003 & 0.023 $\pm$ 0.0002 & 0.014 $\pm$ 0.0002 & 0.010 $\pm$ 0.0001 \\ |
| 478 |
< |
mc & 0.107 $\pm$ 0.0012 & 0.042 $\pm$ 0.0008 & 0.021 $\pm$ 0.0005 & 0.013 $\pm$ 0.0004 & 0.009 $\pm$ 0.0004 \\ |
| 479 |
< |
data/mc & 1.00 $\pm$ 0.01 & 1.03 $\pm$ 0.02 & 1.07 $\pm$ 0.03 & 1.12 $\pm$ 0.04 & 1.17 $\pm$ 0.05 \\ |
| 478 |
> |
mc & 0.106 $\pm$ 0.0004 & 0.042 $\pm$ 0.0003 & 0.021 $\pm$ 0.0002 & 0.013 $\pm$ 0.0002 & 0.009 $\pm$ 0.0001 \\ |
| 479 |
> |
data/mc & 1.00 $\pm$ 0.01 & 1.04 $\pm$ 0.01 & 1.06 $\pm$ 0.01 & 1.08 $\pm$ 0.02 & 1.07 $\pm$ 0.02 \\ |
| 480 |
|
|
| 481 |
|
\hline |
| 482 |
|
\hline |
| 483 |
|
e + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 484 |
|
\hline |
| 485 |
< |
data & 0.115 $\pm$ 0.0012 & 0.049 $\pm$ 0.0008 & 0.026 $\pm$ 0.0006 & 0.017 $\pm$ 0.0005 & 0.012 $\pm$ 0.0004 \\ |
| 486 |
< |
mc & 0.114 $\pm$ 0.0032 & 0.046 $\pm$ 0.0021 & 0.023 $\pm$ 0.0015 & 0.015 $\pm$ 0.0012 & 0.010 $\pm$ 0.0010 \\ |
| 487 |
< |
data/mc & 1.01 $\pm$ 0.03 & 1.09 $\pm$ 0.05 & 1.13 $\pm$ 0.08 & 1.09 $\pm$ 0.09 & 1.14 $\pm$ 0.12 \\ |
| 485 |
> |
data & 0.117 $\pm$ 0.0012 & 0.050 $\pm$ 0.0008 & 0.026 $\pm$ 0.0006 & 0.017 $\pm$ 0.0005 & 0.012 $\pm$ 0.0004 \\ |
| 486 |
> |
mc & 0.120 $\pm$ 0.0012 & 0.048 $\pm$ 0.0008 & 0.025 $\pm$ 0.0006 & 0.016 $\pm$ 0.0005 & 0.011 $\pm$ 0.0004 \\ |
| 487 |
> |
data/mc & 0.97 $\pm$ 0.01 & 1.05 $\pm$ 0.02 & 1.05 $\pm$ 0.03 & 1.07 $\pm$ 0.04 & 1.07 $\pm$ 0.05 \\ |
| 488 |
|
|
| 489 |
|
\hline |
| 490 |
|
\hline |
| 491 |
|
$\mu$ + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 492 |
|
\hline |
| 493 |
|
data & 0.111 $\pm$ 0.0010 & 0.048 $\pm$ 0.0007 & 0.026 $\pm$ 0.0005 & 0.018 $\pm$ 0.0004 & 0.013 $\pm$ 0.0004 \\ |
| 494 |
< |
mc & 0.114 $\pm$ 0.0027 & 0.046 $\pm$ 0.0018 & 0.024 $\pm$ 0.0013 & 0.014 $\pm$ 0.0010 & 0.010 $\pm$ 0.0009 \\ |
| 495 |
< |
data/mc & 0.98 $\pm$ 0.03 & 1.04 $\pm$ 0.04 & 1.12 $\pm$ 0.07 & 1.26 $\pm$ 0.10 & 1.30 $\pm$ 0.12 \\ |
| 494 |
> |
mc & 0.115 $\pm$ 0.0010 & 0.048 $\pm$ 0.0006 & 0.025 $\pm$ 0.0005 & 0.016 $\pm$ 0.0004 & 0.012 $\pm$ 0.0003 \\ |
| 495 |
> |
data/mc & 0.97 $\pm$ 0.01 & 1.01 $\pm$ 0.02 & 1.04 $\pm$ 0.03 & 1.09 $\pm$ 0.04 & 1.09 $\pm$ 0.04 \\ |
| 496 |
|
|
| 497 |
|
\hline |
| 498 |
|
\hline |
| 499 |
|
e + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 500 |
|
\hline |
| 501 |
< |
data & 0.122 $\pm$ 0.0030 & 0.058 $\pm$ 0.0022 & 0.034 $\pm$ 0.0017 & 0.023 $\pm$ 0.0014 & 0.017 $\pm$ 0.0012 \\ |
| 502 |
< |
mc & 0.125 $\pm$ 0.0080 & 0.060 $\pm$ 0.0057 & 0.032 $\pm$ 0.0043 & 0.023 $\pm$ 0.0036 & 0.017 $\pm$ 0.0031 \\ |
| 503 |
< |
data/mc & 0.98 $\pm$ 0.07 & 0.97 $\pm$ 0.10 & 1.06 $\pm$ 0.15 & 1.01 $\pm$ 0.17 & 1.01 $\pm$ 0.20 \\ |
| 501 |
> |
data & 0.123 $\pm$ 0.0031 & 0.058 $\pm$ 0.0022 & 0.034 $\pm$ 0.0017 & 0.023 $\pm$ 0.0014 & 0.017 $\pm$ 0.0012 \\ |
| 502 |
> |
mc & 0.131 $\pm$ 0.0030 & 0.055 $\pm$ 0.0020 & 0.030 $\pm$ 0.0015 & 0.020 $\pm$ 0.0013 & 0.015 $\pm$ 0.0011 \\ |
| 503 |
> |
data/mc & 0.94 $\pm$ 0.03 & 1.06 $\pm$ 0.06 & 1.14 $\pm$ 0.08 & 1.16 $\pm$ 0.10 & 1.17 $\pm$ 0.12 \\ |
| 504 |
|
|
| 505 |
|
\hline |
| 506 |
|
\hline |
| 507 |
|
$\mu$ + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 508 |
|
\hline |
| 509 |
|
data & 0.121 $\pm$ 0.0025 & 0.055 $\pm$ 0.0018 & 0.033 $\pm$ 0.0014 & 0.022 $\pm$ 0.0011 & 0.017 $\pm$ 0.0010 \\ |
| 510 |
< |
mc & 0.125 $\pm$ 0.0070 & 0.053 $\pm$ 0.0047 & 0.027 $\pm$ 0.0035 & 0.018 $\pm$ 0.0028 & 0.013 $\pm$ 0.0024 \\ |
| 511 |
< |
data/mc & 0.97 $\pm$ 0.06 & 1.05 $\pm$ 0.10 & 1.20 $\pm$ 0.16 & 1.19 $\pm$ 0.20 & 1.28 $\pm$ 0.25 \\ |
| 510 |
> |
mc & 0.120 $\pm$ 0.0024 & 0.052 $\pm$ 0.0016 & 0.029 $\pm$ 0.0012 & 0.019 $\pm$ 0.0010 & 0.014 $\pm$ 0.0009 \\ |
| 511 |
> |
data/mc & 1.01 $\pm$ 0.03 & 1.06 $\pm$ 0.05 & 1.14 $\pm$ 0.07 & 1.14 $\pm$ 0.08 & 1.16 $\pm$ 0.10 \\ |
| 512 |
|
|
| 513 |
|
\hline |
| 514 |
|
\hline |
| 515 |
|
e + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 516 |
|
\hline |
| 517 |
< |
data & 0.130 $\pm$ 0.0079 & 0.069 $\pm$ 0.0060 & 0.044 $\pm$ 0.0048 & 0.031 $\pm$ 0.0041 & 0.021 $\pm$ 0.0034 \\ |
| 518 |
< |
mc & 0.136 $\pm$ 0.0219 & 0.045 $\pm$ 0.0134 & 0.027 $\pm$ 0.0108 & 0.022 $\pm$ 0.0093 & 0.016 $\pm$ 0.0084 \\ |
| 519 |
< |
data/mc & 0.96 $\pm$ 0.17 & 1.55 $\pm$ 0.48 & 1.62 $\pm$ 0.67 & 1.41 $\pm$ 0.63 & 1.28 $\pm$ 0.68 \\ |
| 517 |
> |
data & 0.129 $\pm$ 0.0080 & 0.070 $\pm$ 0.0061 & 0.044 $\pm$ 0.0049 & 0.031 $\pm$ 0.0042 & 0.021 $\pm$ 0.0034 \\ |
| 518 |
> |
mc & 0.132 $\pm$ 0.0075 & 0.059 $\pm$ 0.0053 & 0.035 $\pm$ 0.0041 & 0.025 $\pm$ 0.0035 & 0.017 $\pm$ 0.0029 \\ |
| 519 |
> |
data/mc & 0.98 $\pm$ 0.08 & 1.18 $\pm$ 0.15 & 1.26 $\pm$ 0.20 & 1.24 $\pm$ 0.24 & 1.18 $\pm$ 0.28 \\ |
| 520 |
|
|
| 521 |
|
\hline |
| 522 |
|
\hline |
| 523 |
|
$\mu$ + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 524 |
|
\hline |
| 525 |
|
data & 0.136 $\pm$ 0.0067 & 0.064 $\pm$ 0.0048 & 0.041 $\pm$ 0.0039 & 0.029 $\pm$ 0.0033 & 0.024 $\pm$ 0.0030 \\ |
| 526 |
< |
mc & 0.127 $\pm$ 0.0187 & 0.062 $\pm$ 0.0134 & 0.042 $\pm$ 0.0113 & 0.034 $\pm$ 0.0104 & 0.028 $\pm$ 0.0095 \\ |
| 527 |
< |
data/mc & 1.07 $\pm$ 0.17 & 1.04 $\pm$ 0.24 & 0.98 $\pm$ 0.28 & 0.85 $\pm$ 0.28 & 0.87 $\pm$ 0.32 \\ |
| 526 |
> |
mc & 0.130 $\pm$ 0.0063 & 0.065 $\pm$ 0.0046 & 0.035 $\pm$ 0.0034 & 0.020 $\pm$ 0.0026 & 0.013 $\pm$ 0.0022 \\ |
| 527 |
> |
data/mc & 1.04 $\pm$ 0.07 & 0.99 $\pm$ 0.10 & 1.19 $\pm$ 0.16 & 1.47 $\pm$ 0.25 & 1.81 $\pm$ 0.37 \\ |
| 528 |
> |
|
| 529 |
|
\hline |
| 530 |
|
\hline |
| 531 |
|
|
| 534 |
|
\end{table} |
| 535 |
|
|
| 536 |
|
|
| 517 |
– |
|
| 537 |
|
%Figure.~\ref{fig:reliso} compares the relative track isolation |
| 538 |
|
%for events with a track with $\pt > 10~\GeV$ in addition to a selected |
| 539 |
|
%muon for $\Z+4$ jet events and various \ttll\ components. The |
