| 15 |
|
on \url{https://twiki.cern.ch/twiki/bin/viewauth/CMS/SUSYstop#SINGLE_LEPTON_CHANNEL} (revision r20) |
| 16 |
|
\begin{itemize} |
| 17 |
|
\item satisfy the trigger requirement (see |
| 18 |
< |
Table.~\ref{tab:TrigData}). |
| 18 |
> |
Table~\ref{tab:TrigData}). |
| 19 |
|
Note that the analysis triggers are inclusive single lepton triggers. |
| 20 |
|
Dilepton triggers are used only for the dilepton control region. |
| 21 |
|
\item select events with one high \pt\ electron or muon, requiring |
| 31 |
|
\item $E/p_{\rm{in}} < 4$ (electrons only) |
| 32 |
|
\item We remove electron events with $\met > 50$ GeV and $M_T > 100$ |
| 33 |
|
GeV with at least one crystal in the supercluster with laser |
| 34 |
< |
correction in $>$2.\footnote{This is an ad-hoc removal based on |
| 34 |
> |
correction $>$2.\footnote{This is an ad-hoc removal based on |
| 35 |
|
run-event numbers, since the |
| 36 |
|
problem was found very recently and the filter was not available |
| 37 |
|
when we processed the events.} |
| 127 |
|
Yield UL (optimistic) & 147 (10\%) & 94 (10\%) & 47 (15\%) & 25 (20\%) & 14 (25\%) & 8.6 (30\%) & 7.5 (50\%) \\ |
| 128 |
|
Yield UL (pessimistic) & 200 (15\%) & 152 (20\%) & 64 (25\%) & 30 (30\%) & 15 (35\%) & 9.7 (50\%) & 8.2 (100\%) \\ |
| 129 |
|
\hline |
| 130 |
< |
T2tt m(stop) = 250 m($\chi^0$) = 0 & $424 \pm 19$& $256 \pm 15$& $71 \pm 8$& $19 \pm 4$& $1 \pm 0$& $0 \pm 0$& $0 \pm 0$ \\ |
| 131 |
< |
T2tt m(stop) = 300 m($\chi^0$) = 50 & $396 \pm 11$& $316 \pm 10$& $113 \pm 6$& $37 \pm 3$& $14 \pm 2$& $2 \pm 1$& $0 \pm 0$ \\ |
| 132 |
< |
T2tt m(stop) = 300 m($\chi^0$) = 100 & $174 \pm 7$& $130 \pm 7$& $42 \pm 4$& $16 \pm 2$& $8 \pm 2$& $3 \pm 1$& $2 \pm 1$ \\ |
| 133 |
< |
T2tt m(stop) = 350 m($\chi^0$) = 0 & $305 \pm 6$& $282 \pm 6$& $162 \pm 5$& $69 \pm 3$& $26 \pm 2$& $11 \pm 1$& $4 \pm 1$ \\ |
| 134 |
< |
T2tt m(stop) = 450 m($\chi^0$) = 0 & $96 \pm 2$& $96 \pm 2$& $72 \pm 1$& $48 \pm 1$& $28 \pm 1$& $14 \pm 1$& $6 \pm 0$ \\ |
| 130 |
> |
T2tt m(stop) = 250 m($\chi^0$) = 0 & $315 \pm 18$& $193 \pm 14$& $53 \pm 8$& $13 \pm 4$& $2 \pm 2$& $0 \pm 0$& $0 \pm 0$ \\ \hline |
| 131 |
> |
T2tt m(stop) = 300 m($\chi^0$) = 50 & $296 \pm 11$& $236 \pm 10$& $88 \pm 6$& $28 \pm 3$& $10 \pm 2$& $2 \pm 1$& $0 \pm 0$ \\ \hline |
| 132 |
> |
T2tt m(stop) = 300 m($\chi^0$) = 100 & $128 \pm 7$& $93 \pm 6$& $29 \pm 3$& $10 \pm 2$& $5 \pm 1$& $2 \pm 1$& $1 \pm 1$ \\ \hline |
| 133 |
> |
T2tt m(stop) = 350 m($\chi^0$) = 0 & $224 \pm 6$& $206 \pm 6$& $119 \pm 4$& $52 \pm 3$& $20 \pm 2$& $8 \pm 1$& $3 \pm 1$ \\ \hline |
| 134 |
> |
T2tt m(stop) = 450 m($\chi^0$) = 0 & $71 \pm 2$& $71 \pm 2$& $53 \pm 1$& $36 \pm 1$& $21 \pm 1$& $11 \pm 1$& $5 \pm 0$ \\ |
| 135 |
|
\hline |
| 136 |
|
\end{tabular} |
| 137 |
|
\caption{ Expected SM background contributions and signal yields for a few sample points, |
| 145 |
|
\end{table} |
| 146 |
|
|
| 147 |
|
\subsection{Control Region Selection} |
| 148 |
< |
\label{sec:CR} |
| 148 |
> |
\label{sec:CRsel} |
| 149 |
|
|
| 150 |
|
Control regions (CRs) are used to validate the background estimation |
| 151 |
|
procedure and derive systematic uncertainties for some |
| 301 |
|
The electron efficiencies are summarized in Table~\ref{tab:eltnpeff} for inclusive events (i.e. no jet requirements). These efficiencies are displayed in Fig.~\ref{fig:eltnpeff} |
| 302 |
|
for several different jet multiplicity requirements. In general we observe good agreement between the data and MC identification and isolation efficiencies. |
| 303 |
|
|
| 304 |
< |
Pending a better understanding of the very high \pt\ muon efficiency, we |
| 304 |
> |
% Pending a better understanding of the very high \pt\ muon efficiency, |
| 305 |
> |
We |
| 306 |
|
do not correct the MC for differences in lepton efficiency. In the |
| 307 |
|
background calculation, we do not take any systematics due to lepton |
| 308 |
|
selection |
| 332 |
|
MC ID & & & \\ |
| 333 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 334 |
|
\hline |
| 335 |
< |
20 - 30 & 0.9638 $\pm$ 0.0005 & 0.9590 $\pm$ 0.0006 & 0.9381 $\pm$ 0.0008 \\ |
| 336 |
< |
30 - 40 & 0.9649 $\pm$ 0.0002 & 0.9612 $\pm$ 0.0003 & 0.9372 $\pm$ 0.0005 \\ |
| 337 |
< |
40 - 50 & 0.9674 $\pm$ 0.0002 & 0.9651 $\pm$ 0.0002 & 0.9368 $\pm$ 0.0004 \\ |
| 338 |
< |
50 - 60 & 0.9644 $\pm$ 0.0005 & 0.9589 $\pm$ 0.0006 & 0.9325 $\pm$ 0.0009 \\ |
| 339 |
< |
60 - 80 & 0.9644 $\pm$ 0.0009 & 0.9586 $\pm$ 0.0011 & 0.9258 $\pm$ 0.0019 \\ |
| 340 |
< |
80 - 100 & 0.9674 $\pm$ 0.0022 & 0.9602 $\pm$ 0.0029 & 0.9148 $\pm$ 0.0053 \\ |
| 341 |
< |
100 - 150 & 0.9632 $\pm$ 0.0031 & 0.9621 $\pm$ 0.0037 & 0.9270 $\pm$ 0.0068 \\ |
| 342 |
< |
150 - 200 & 0.9615 $\pm$ 0.0070 & 0.9519 $\pm$ 0.0092 & 0.8844 $\pm$ 0.0213 \\ |
| 343 |
< |
200 - 300 & 0.9615 $\pm$ 0.0119 & 0.9353 $\pm$ 0.0173 & 0.8923 $\pm$ 0.0384 \\ |
| 344 |
< |
300 - 10000 & 0.9667 $\pm$ 0.0232 & 0.9697 $\pm$ 0.0298 & 0.4000 $\pm$ 0.1549 \\ |
| 335 |
> |
20 - 30 & 0.9672 $\pm$ 0.0005 & 0.9640 $\pm$ 0.0006 & 0.9471 $\pm$ 0.0008 \\ |
| 336 |
> |
30 - 40 & 0.9684 $\pm$ 0.0002 & 0.9657 $\pm$ 0.0003 & 0.9446 $\pm$ 0.0004 \\ |
| 337 |
> |
40 - 50 & 0.9704 $\pm$ 0.0002 & 0.9687 $\pm$ 0.0002 & 0.9432 $\pm$ 0.0004 \\ |
| 338 |
> |
50 - 60 & 0.9684 $\pm$ 0.0005 & 0.9640 $\pm$ 0.0005 & 0.9414 $\pm$ 0.0009 \\ |
| 339 |
> |
60 - 80 & 0.9678 $\pm$ 0.0009 & 0.9640 $\pm$ 0.0010 & 0.9354 $\pm$ 0.0018 \\ |
| 340 |
> |
80 - 100 & 0.9709 $\pm$ 0.0021 & 0.9642 $\pm$ 0.0027 & 0.9234 $\pm$ 0.0051 \\ |
| 341 |
> |
100 - 150 & 0.9679 $\pm$ 0.0029 & 0.9654 $\pm$ 0.0035 & 0.9261 $\pm$ 0.0069 \\ |
| 342 |
> |
150 - 200 & 0.9643 $\pm$ 0.0069 & 0.9568 $\pm$ 0.0088 & 0.9045 $\pm$ 0.0198 \\ |
| 343 |
> |
200 - 300 & 0.9647 $\pm$ 0.0116 & 0.9388 $\pm$ 0.0171 & 0.8906 $\pm$ 0.0390 \\ |
| 344 |
> |
300 - 10000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 \\ |
| 345 |
|
\hline |
| 346 |
|
\hline |
| 347 |
|
MC ISO & & & \\ |
| 348 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 349 |
|
\hline |
| 350 |
< |
20 - 30 & 0.8968 $\pm$ 0.0007 & 0.9156 $\pm$ 0.0008 & 0.9301 $\pm$ 0.0009 \\ |
| 351 |
< |
30 - 40 & 0.9610 $\pm$ 0.0002 & 0.9633 $\pm$ 0.0003 & 0.9706 $\pm$ 0.0003 \\ |
| 352 |
< |
40 - 50 & 0.9877 $\pm$ 0.0001 & 0.9897 $\pm$ 0.0001 & 0.9912 $\pm$ 0.0002 \\ |
| 353 |
< |
50 - 60 & 0.9918 $\pm$ 0.0002 & 0.9928 $\pm$ 0.0002 & 0.9939 $\pm$ 0.0003 \\ |
| 354 |
< |
60 - 80 & 0.9926 $\pm$ 0.0004 & 0.9936 $\pm$ 0.0004 & 0.9948 $\pm$ 0.0005 \\ |
| 355 |
< |
80 - 100 & 0.9918 $\pm$ 0.0012 & 0.9923 $\pm$ 0.0013 & 0.9933 $\pm$ 0.0016 \\ |
| 356 |
< |
100 - 150 & 0.9900 $\pm$ 0.0016 & 0.9939 $\pm$ 0.0015 & 0.9927 $\pm$ 0.0023 \\ |
| 357 |
< |
150 - 200 & 0.9904 $\pm$ 0.0036 & 0.9904 $\pm$ 0.0043 & 0.9950 $\pm$ 0.0050 \\ |
| 358 |
< |
200 - 300 & 0.9921 $\pm$ 0.0056 & 1.0000 $\pm$ 0.0000 & 0.9831 $\pm$ 0.0168 \\ |
| 350 |
> |
20 - 30 & 0.8966 $\pm$ 0.0007 & 0.9153 $\pm$ 0.0008 & 0.9298 $\pm$ 0.0009 \\ |
| 351 |
> |
30 - 40 & 0.9610 $\pm$ 0.0002 & 0.9632 $\pm$ 0.0003 & 0.9707 $\pm$ 0.0003 \\ |
| 352 |
> |
40 - 50 & 0.9876 $\pm$ 0.0001 & 0.9897 $\pm$ 0.0001 & 0.9912 $\pm$ 0.0002 \\ |
| 353 |
> |
50 - 60 & 0.9921 $\pm$ 0.0002 & 0.9927 $\pm$ 0.0003 & 0.9939 $\pm$ 0.0003 \\ |
| 354 |
> |
60 - 80 & 0.9927 $\pm$ 0.0004 & 0.9937 $\pm$ 0.0004 & 0.9947 $\pm$ 0.0005 \\ |
| 355 |
> |
80 - 100 & 0.9920 $\pm$ 0.0012 & 0.9921 $\pm$ 0.0013 & 0.9932 $\pm$ 0.0016 \\ |
| 356 |
> |
100 - 150 & 0.9898 $\pm$ 0.0017 & 0.9923 $\pm$ 0.0017 & 0.9933 $\pm$ 0.0022 \\ |
| 357 |
> |
150 - 200 & 0.9901 $\pm$ 0.0037 & 0.9922 $\pm$ 0.0039 & 0.9950 $\pm$ 0.0050 \\ |
| 358 |
> |
200 - 300 & 0.9919 $\pm$ 0.0057 & 1.0000 $\pm$ 0.0000 & 0.9828 $\pm$ 0.0171 \\ |
| 359 |
|
300 - 10000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 \\ |
| 360 |
|
\hline |
| 361 |
|
\hline |
| 362 |
|
DATA ID & & & \\ |
| 363 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 364 |
|
\hline |
| 365 |
< |
20 - 30 & 0.9446 $\pm$ 0.0005 & 0.9430 $\pm$ 0.0006 & 0.9203 $\pm$ 0.0008 \\ |
| 366 |
< |
30 - 40 & 0.9474 $\pm$ 0.0003 & 0.9448 $\pm$ 0.0003 & 0.9237 $\pm$ 0.0005 \\ |
| 367 |
< |
40 - 50 & 0.9515 $\pm$ 0.0002 & 0.9502 $\pm$ 0.0003 & 0.9252 $\pm$ 0.0004 \\ |
| 368 |
< |
50 - 60 & 0.9458 $\pm$ 0.0005 & 0.9405 $\pm$ 0.0006 & 0.9163 $\pm$ 0.0010 \\ |
| 369 |
< |
60 - 80 & 0.9457 $\pm$ 0.0010 & 0.9386 $\pm$ 0.0013 & 0.9115 $\pm$ 0.0020 \\ |
| 370 |
< |
80 - 100 & 0.9393 $\pm$ 0.0029 & 0.9346 $\pm$ 0.0035 & 0.9091 $\pm$ 0.0055 \\ |
| 371 |
< |
100 - 150 & 0.9355 $\pm$ 0.0040 & 0.9392 $\pm$ 0.0045 & 0.8843 $\pm$ 0.0085 \\ |
| 372 |
< |
150 - 200 & 0.9526 $\pm$ 0.0078 & 0.9534 $\pm$ 0.0099 & 0.8772 $\pm$ 0.0217 \\ |
| 373 |
< |
200 - 300 & 0.9017 $\pm$ 0.0195 & 0.9302 $\pm$ 0.0194 & 0.8448 $\pm$ 0.0475 \\ |
| 374 |
< |
300 - 10000 & 0.7083 $\pm$ 0.0656 & 0.7333 $\pm$ 0.1142 & 0.2000 $\pm$ 0.1033 \\ |
| 365 |
> |
20 - 30 & 0.9530 $\pm$ 0.0005 & 0.9517 $\pm$ 0.0006 & 0.9369 $\pm$ 0.0008 \\ |
| 366 |
> |
30 - 40 & 0.9556 $\pm$ 0.0003 & 0.9519 $\pm$ 0.0003 & 0.9362 $\pm$ 0.0005 \\ |
| 367 |
> |
40 - 50 & 0.9584 $\pm$ 0.0002 & 0.9558 $\pm$ 0.0003 & 0.9355 $\pm$ 0.0004 \\ |
| 368 |
> |
50 - 60 & 0.9540 $\pm$ 0.0005 & 0.9487 $\pm$ 0.0006 & 0.9314 $\pm$ 0.0010 \\ |
| 369 |
> |
60 - 80 & 0.9536 $\pm$ 0.0010 & 0.9466 $\pm$ 0.0012 & 0.9307 $\pm$ 0.0019 \\ |
| 370 |
> |
80 - 100 & 0.9505 $\pm$ 0.0028 & 0.9414 $\pm$ 0.0035 & 0.9289 $\pm$ 0.0053 \\ |
| 371 |
> |
100 - 150 & 0.9472 $\pm$ 0.0038 & 0.9454 $\pm$ 0.0045 & 0.9149 $\pm$ 0.0079 \\ |
| 372 |
> |
150 - 200 & 0.9628 $\pm$ 0.0073 & 0.9675 $\pm$ 0.0089 & 0.8950 $\pm$ 0.0217 \\ |
| 373 |
> |
200 - 300 & 0.9463 $\pm$ 0.0157 & 0.9290 $\pm$ 0.0206 & 0.8889 $\pm$ 0.0468 \\ |
| 374 |
> |
300 - 10000 & 0.9412 $\pm$ 0.0404 & 1.0000 $\pm$ 0.0000 & 0.4000 $\pm$ 0.2191 \\ |
| 375 |
|
\hline |
| 376 |
|
\hline |
| 377 |
|
DATA ISO & & & \\ |
| 378 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 379 |
|
\hline |
| 380 |
< |
20 - 30 & 0.8943 $\pm$ 0.0007 & 0.9144 $\pm$ 0.0008 & 0.9359 $\pm$ 0.0008 \\ |
| 381 |
< |
30 - 40 & 0.9598 $\pm$ 0.0002 & 0.9646 $\pm$ 0.0003 & 0.9746 $\pm$ 0.0003 \\ |
| 382 |
< |
40 - 50 & 0.9870 $\pm$ 0.0001 & 0.9903 $\pm$ 0.0001 & 0.9920 $\pm$ 0.0001 \\ |
| 383 |
< |
50 - 60 & 0.9913 $\pm$ 0.0002 & 0.9935 $\pm$ 0.0002 & 0.9952 $\pm$ 0.0003 \\ |
| 384 |
< |
60 - 80 & 0.9921 $\pm$ 0.0004 & 0.9931 $\pm$ 0.0004 & 0.9952 $\pm$ 0.0005 \\ |
| 385 |
< |
80 - 100 & 0.9920 $\pm$ 0.0011 & 0.9938 $\pm$ 0.0011 & 0.9943 $\pm$ 0.0015 \\ |
| 386 |
< |
100 - 150 & 0.9900 $\pm$ 0.0017 & 0.9943 $\pm$ 0.0015 & 0.9968 $\pm$ 0.0016 \\ |
| 387 |
< |
150 - 200 & 0.9972 $\pm$ 0.0020 & 0.9977 $\pm$ 0.0023 & 0.9950 $\pm$ 0.0050 \\ |
| 380 |
> |
20 - 30 & 0.8939 $\pm$ 0.0007 & 0.9144 $\pm$ 0.0008 & 0.9361 $\pm$ 0.0008 \\ |
| 381 |
> |
30 - 40 & 0.9598 $\pm$ 0.0002 & 0.9646 $\pm$ 0.0003 & 0.9744 $\pm$ 0.0003 \\ |
| 382 |
> |
40 - 50 & 0.9870 $\pm$ 0.0001 & 0.9901 $\pm$ 0.0001 & 0.9920 $\pm$ 0.0002 \\ |
| 383 |
> |
50 - 60 & 0.9912 $\pm$ 0.0002 & 0.9933 $\pm$ 0.0002 & 0.9953 $\pm$ 0.0003 \\ |
| 384 |
> |
60 - 80 & 0.9920 $\pm$ 0.0004 & 0.9934 $\pm$ 0.0005 & 0.9956 $\pm$ 0.0005 \\ |
| 385 |
> |
80 - 100 & 0.9926 $\pm$ 0.0011 & 0.9933 $\pm$ 0.0013 & 0.9955 $\pm$ 0.0014 \\ |
| 386 |
> |
100 - 150 & 0.9913 $\pm$ 0.0016 & 0.9949 $\pm$ 0.0015 & 0.9965 $\pm$ 0.0017 \\ |
| 387 |
> |
150 - 200 & 0.9969 $\pm$ 0.0022 & 0.9974 $\pm$ 0.0026 & 0.9944 $\pm$ 0.0055 \\ |
| 388 |
|
200 - 300 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 \\ |
| 389 |
|
300 - 10000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 \\ |
| 390 |
|
\hline |
| 392 |
|
Scale Factor ID & & & \\ |
| 393 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 394 |
|
\hline |
| 395 |
< |
20 - 30 & 0.9801 $\pm$ 0.0007 & 0.9833 $\pm$ 0.0009 & 0.9810 $\pm$ 0.0012 \\ |
| 396 |
< |
30 - 40 & 0.9819 $\pm$ 0.0004 & 0.9829 $\pm$ 0.0005 & 0.9856 $\pm$ 0.0007 \\ |
| 397 |
< |
40 - 50 & 0.9836 $\pm$ 0.0003 & 0.9845 $\pm$ 0.0004 & 0.9875 $\pm$ 0.0006 \\ |
| 398 |
< |
50 - 60 & 0.9808 $\pm$ 0.0007 & 0.9808 $\pm$ 0.0009 & 0.9826 $\pm$ 0.0014 \\ |
| 399 |
< |
60 - 80 & 0.9806 $\pm$ 0.0014 & 0.9791 $\pm$ 0.0017 & 0.9846 $\pm$ 0.0029 \\ |
| 400 |
< |
80 - 100 & 0.9709 $\pm$ 0.0037 & 0.9733 $\pm$ 0.0047 & 0.9937 $\pm$ 0.0084 \\ |
| 401 |
< |
100 - 150 & 0.9713 $\pm$ 0.0052 & 0.9762 $\pm$ 0.0060 & 0.9539 $\pm$ 0.0115 \\ |
| 402 |
< |
150 - 200 & 0.9907 $\pm$ 0.0109 & 1.0017 $\pm$ 0.0142 & 0.9918 $\pm$ 0.0343 \\ |
| 403 |
< |
200 - 300 & 0.9378 $\pm$ 0.0233 & 0.9946 $\pm$ 0.0278 & 0.9468 $\pm$ 0.0671 \\ |
| 404 |
< |
300 - 10000 & 0.7328 $\pm$ 0.0701 & 0.7562 $\pm$ 0.1200 & 0.5000 $\pm$ 0.3227 \\ |
| 395 |
> |
20 - 30 & 0.9853 $\pm$ 0.0007 & 0.9872 $\pm$ 0.0009 & 0.9893 $\pm$ 0.0012 \\ |
| 396 |
> |
30 - 40 & 0.9868 $\pm$ 0.0003 & 0.9857 $\pm$ 0.0005 & 0.9911 $\pm$ 0.0007 \\ |
| 397 |
> |
40 - 50 & 0.9877 $\pm$ 0.0003 & 0.9866 $\pm$ 0.0004 & 0.9918 $\pm$ 0.0006 \\ |
| 398 |
> |
50 - 60 & 0.9851 $\pm$ 0.0007 & 0.9841 $\pm$ 0.0009 & 0.9894 $\pm$ 0.0014 \\ |
| 399 |
> |
60 - 80 & 0.9853 $\pm$ 0.0014 & 0.9820 $\pm$ 0.0017 & 0.9949 $\pm$ 0.0028 \\ |
| 400 |
> |
80 - 100 & 0.9790 $\pm$ 0.0036 & 0.9763 $\pm$ 0.0046 & 1.0059 $\pm$ 0.0080 \\ |
| 401 |
> |
100 - 150 & 0.9786 $\pm$ 0.0049 & 0.9793 $\pm$ 0.0059 & 0.9879 $\pm$ 0.0113 \\ |
| 402 |
> |
150 - 200 & 0.9984 $\pm$ 0.0104 & 1.0112 $\pm$ 0.0131 & 0.9894 $\pm$ 0.0323 \\ |
| 403 |
> |
200 - 300 & 0.9810 $\pm$ 0.0201 & 0.9896 $\pm$ 0.0284 & 0.9981 $\pm$ 0.0684 \\ |
| 404 |
> |
300 - 10000 & 0.9412 $\pm$ 0.0404 & 1.0000 $\pm$ 0.0000 & 0.4000 $\pm$ 0.2191 \\ |
| 405 |
|
\hline |
| 406 |
|
\hline |
| 407 |
|
Scale Factor ISO & & & \\ |
| 408 |
|
\pt\ range [GeV] & $|\eta|<0.8$ & $0.8<|\eta|<1.5$ & $1.5<|\eta|<2.1$ \\ |
| 409 |
|
\hline |
| 410 |
< |
20 - 30 & 0.9971 $\pm$ 0.0011 & 0.9987 $\pm$ 0.0012 & 1.0062 $\pm$ 0.0012 \\ |
| 411 |
< |
30 - 40 & 0.9987 $\pm$ 0.0003 & 1.0014 $\pm$ 0.0004 & 1.0042 $\pm$ 0.0004 \\ |
| 412 |
< |
40 - 50 & 0.9994 $\pm$ 0.0002 & 1.0006 $\pm$ 0.0002 & 1.0008 $\pm$ 0.0002 \\ |
| 413 |
< |
50 - 60 & 0.9995 $\pm$ 0.0003 & 1.0007 $\pm$ 0.0003 & 1.0014 $\pm$ 0.0004 \\ |
| 414 |
< |
60 - 80 & 0.9995 $\pm$ 0.0006 & 0.9994 $\pm$ 0.0006 & 1.0005 $\pm$ 0.0007 \\ |
| 415 |
< |
80 - 100 & 1.0002 $\pm$ 0.0016 & 1.0015 $\pm$ 0.0017 & 1.0010 $\pm$ 0.0022 \\ |
| 416 |
< |
100 - 150 & 1.0000 $\pm$ 0.0024 & 1.0005 $\pm$ 0.0021 & 1.0041 $\pm$ 0.0028 \\ |
| 417 |
< |
150 - 200 & 1.0068 $\pm$ 0.0042 & 1.0074 $\pm$ 0.0049 & 1.0000 $\pm$ 0.0071 \\ |
| 418 |
< |
200 - 300 & 1.0080 $\pm$ 0.0057 & 1.0000 $\pm$ 0.0000 & 1.0172 $\pm$ 0.0174 \\ |
| 410 |
> |
20 - 30 & 0.9970 $\pm$ 0.0012 & 0.9989 $\pm$ 0.0012 & 1.0068 $\pm$ 0.0013 \\ |
| 411 |
> |
30 - 40 & 0.9987 $\pm$ 0.0004 & 1.0014 $\pm$ 0.0004 & 1.0038 $\pm$ 0.0005 \\ |
| 412 |
> |
40 - 50 & 0.9994 $\pm$ 0.0002 & 1.0004 $\pm$ 0.0002 & 1.0008 $\pm$ 0.0002 \\ |
| 413 |
> |
50 - 60 & 0.9991 $\pm$ 0.0003 & 1.0006 $\pm$ 0.0003 & 1.0013 $\pm$ 0.0004 \\ |
| 414 |
> |
60 - 80 & 0.9993 $\pm$ 0.0006 & 0.9997 $\pm$ 0.0006 & 1.0009 $\pm$ 0.0008 \\ |
| 415 |
> |
80 - 100 & 1.0006 $\pm$ 0.0016 & 1.0012 $\pm$ 0.0018 & 1.0023 $\pm$ 0.0022 \\ |
| 416 |
> |
100 - 150 & 1.0015 $\pm$ 0.0023 & 1.0027 $\pm$ 0.0023 & 1.0032 $\pm$ 0.0028 \\ |
| 417 |
> |
150 - 200 & 1.0068 $\pm$ 0.0044 & 1.0053 $\pm$ 0.0047 & 0.9994 $\pm$ 0.0075 \\ |
| 418 |
> |
200 - 300 & 1.0081 $\pm$ 0.0058 & 1.0000 $\pm$ 0.0000 & 1.0175 $\pm$ 0.0177 \\ |
| 419 |
|
300 - 10000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 & 1.0000 $\pm$ 0.0000 \\ |
| 420 |
|
\hline |
| 421 |
|
\hline |
| 422 |
|
|
| 422 |
– |
|
| 423 |
|
\end{tabular} |
| 424 |
|
\end{center} |
| 425 |
|
\end{table} |
