| 37 |
|
& \multicolumn{2}{c|}{Background with genuine \Z} & \multicolumn{4}{c|}{Background without |
| 38 |
|
genuine \Z boson} \\ |
| 39 |
|
Channel & $\Z+jets$ & $\Z b\bar{b}$ & $t\bar{t}$ & $\W+jets$ & $t\bar{t}$ + $\W+jets$ & Fit result \\ \hline |
| 40 |
< |
$3e$ Loose &2.8 & 2.9 & 0.8 & 0.1 & 0.9 & 1.0$ \pm $2.7 \\\hline |
| 41 |
< |
$3e$ Tight &0.8 & 1.2 & 0.4 & 0.1 & 0.5 & 0.7$ \pm $2.5 \\\hline |
| 42 |
< |
$2e1\mu$ Loose &1.3 & 4.7 & 4.5 & 0 & 4.5 & 4.2$ \pm $3.7 \\\hline |
| 43 |
< |
$2e1\mu$ Tight &0.0 & 0.1 & 0.5 & 0 & 0.5 & 0.6$ \pm $2.5 \\\hline |
| 44 |
< |
$2\mu1e$ Loose &4.1 & 2.9 & 0.5 & 0 & 0.5 & 0.9$ \pm $2.7 \\\hline |
| 45 |
< |
$2\mu1e$ Tight &0.8 & 1.3 & 0.4 & 0 & 0.4 & 0.6$ \pm $2.4 \\\hline |
| 46 |
< |
$3\mu$ Loose &1.9 & 4.2 & 4.1 & 0 & 4.1 & 2.3$ \pm $3.3 \\\hline |
| 47 |
< |
$3\mu$ Tight &0.1 & 0.3 & 0.2 & 0 & 0.2 & 0.4$ \pm $2.4 \\\hline |
| 40 |
> |
$3e$ Loose &7.08067 & 2.86817 & 1.12287 & 0.357018 & 1.47989 & 1.45557$ \pm $2.9589 \\\hline |
| 41 |
> |
$3e$ Tight &1.95631 & 1.20063 & 0.623349 & 0.357018 & 0.980367 & 1.11349$ \pm $2.83365 \\\hline |
| 42 |
> |
$2e1mu$ Loose &3.97174 & 4.73581 & 6.17639 & 0 & 6.17639 & 6.0224$ \pm $4.0679 \\\hline |
| 43 |
> |
$2e1mu$ Tight &0 & 0.0889355 & 0.734362 & 0 & 0.734362 & 0.97086$ \pm $2.80976 \\\hline |
| 44 |
> |
$2mu1e$ Loose &10.1004 & 2.93487 & 0.79839 & 0 & 0.79839 & 1.55994$ \pm $3.1279 \\\hline |
| 45 |
> |
$2mu1e$ Tight &1.81221 & 1.28956 & 0.648954 & 0 & 0.648954 & 0.979719$ \pm $2.67068 \\\hline |
| 46 |
> |
$3mu$ Loose &4.54662 & 4.17997 & 5.87059 & 0 & 5.87059 & 3.07779$ \pm $3.50566 \\\hline |
| 47 |
> |
$3mu$ Tight &0.144028 & 0.28904 & 0.324477 & 0 & 0.324477 & 0.470637$ \pm $2.46181 \\\hline |
| 48 |
|
\end{tabular} |
| 49 |
|
\end{center} |
| 50 |
|
\caption{Comparison between Monte Carlo truth information and the results of the fit for the background without genuine \Z boson. Number of events are obtained in the invariant mass range between 81 and 101 GeV. The ``Loose'' and ``Tight'' selection criteria applied for third lepton considered. |
| 62 |
|
\begin{center} |
| 63 |
|
\begin{tabular}{lcccc} \hline \hline |
| 64 |
|
& 3e &2e1$\mu$ &2$\mu$1e &3$\mu$\\ \hline |
| 65 |
< |
%$N_{Loose}$ - ZZ -Zgamma &19.7$\pm$1.1 &22.9$\pm$0.7 &22.9$\pm$1.1 &25.6$\pm$0.8 \\ |
| 66 |
< |
%$N_{Loose} ^{non genuine Z}$ (Fit) &1.0$\pm$1.5 &11.2$\pm$5.5 &3.1$\pm$2.4 & 4.8$\pm$3.7\\ |
| 67 |
< |
$N$ - ZZ -Zgamma &12.2$\pm$1.1 &8.7$\pm$0.6 &12.8$\pm$1.0 &11.1$\pm$0.7\\ |
| 68 |
< |
$N^{non genuine Z}$ (Fit)&0.7$\pm$2.5 &0.6$\pm$2.5 &0.6$\pm$2.4 &0.4$\pm$2.4\\ |
| 69 |
< |
$N^{genuine Z}$ (matrix method)& 3.2$\pm$1.8 &0.7$\pm$0.9 &4.6$\pm$2.1 &0.9$\pm$1.1\\\hline |
| 70 |
< |
$N^{WZ}$ & 8.3$\pm$3.2 &7.4$\pm$2.8 &7.6$\pm$3.3 &9.8$\pm$2.7\\\hline |
| 71 |
< |
\WZ from MC &7.9&8.0& 8.9 &10.1\\ |
| 65 |
> |
$N$ - ZZ -Zgamma &12.4437$\pm$0.992046 &8.69811$\pm$0&13.1255$\pm$0.937399&10.5715$\pm$0\\ \hline |
| 66 |
> |
$N^{non genuine Z}$ (Fit)&1.11349$\pm$2.83365&0.97086$\pm$2.80976&0.979719$\pm$2.67068&0.470637$\pm$2.46181\\ \hline |
| 67 |
> |
$N^{genuine Z}$ (matrix method)&3.21939 $\pm$1.78953&0.948261 $\pm$1.05074&4.63515 $\pm$2.11436&0.945652 $\pm$1.13388\\ \hline |
| 68 |
> |
$N^{WZ}$ & 8.23222 $\pm$3.53155&7.74985 $\pm$3.15299 &7.55297 $\pm$3.54442&9.62584 $\pm$2.75094\\ \hline |
| 69 |
> |
\WZ from MC &7.9&8.1& 9.0 &10.1\\ |
| 70 |
|
|
| 71 |
|
\hline |
| 72 |
|
\end{tabular} |
| 77 |
|
\end{center} |
| 78 |
|
\end{table} |
| 79 |
|
|
| 80 |
+ |
|
| 81 |
+ |
\begin{table}[h] |
| 82 |
+ |
\begin{center} |
| 83 |
+ |
\begin{tabular}{lcccc} \hline \hline |
| 84 |
+ |
& 3e &2e1$\mu$ &2$\mu$1e &3$\mu$\\ \hline |
| 85 |
+ |
$N$ - ZZ -Zgamma &19.9098$\pm$1.00886&23.5941$\pm$0.00420358&23.3592$\pm$0.95001&25.5227$\pm$0.00420358\\ \hline |
| 86 |
+ |
$N^{non genuine Z}$ (Fit)&1.45557$\pm$2.9589&6.0224$\pm$4.0679&1.55994$\pm$3.1279&3.07779$\pm$3.50566\\ \hline |
| 87 |
+ |
$N^{genuine Z}$ (matrix method)&10.0606 $\pm$6.75575&15.8043 $\pm$8.41727)&14.4848 $\pm$6.80421&15.7609 $\pm$5.70923\\ \hline |
| 88 |
+ |
$N^{WZ}$ & 8.84029 $\pm$7.51757&7.78552 $\pm$11.1206&7.92435 $\pm$7.64947&9.75762 $\pm$7.37277\\ \hline |
| 89 |
+ |
\WZ from MC &8.1&9.0& 9.2 &11.3\\ |
| 90 |
+ |
|
| 91 |
+ |
\hline |
| 92 |
+ |
\end{tabular} |
| 93 |
+ |
|
| 94 |
+ |
\caption{Loose Sample: Expected number of selected events for an integrated luminosity of 300 |
| 95 |
+ |
pb$^{-1}$ for the signal and estimated background with 81 GeV $< M_Z < $ 101 GeV.} |
| 96 |
+ |
\label{tab:FinalXCLoose} |
| 97 |
+ |
\end{center} |
| 98 |
+ |
\end{table} |
| 99 |
+ |
|
| 100 |
|
\begin{figure}[hbt] |
| 101 |
|
\begin{center} |
| 102 |
|
\scalebox{0.8}{\includegraphics{figs/MatrixMethod3eLooseTightZmassMWtCut.eps}} |
| 138 |
|
& \multicolumn{2}{c|}{Background with genuine \Z} & \multicolumn{4}{c|}{Background without |
| 139 |
|
genuine \Z boson} \\ |
| 140 |
|
Channel & $\Z+jets$ & $\Z b\bar{b}$ & $t\bar{t}$ & $\W+jets$ & $t\bar{t}$ + $\W+jets$ & Fit result \\ \hline |
| 141 |
< |
$3e$ Loose &16.4 & 12.7 & 1.1 & 0.1 & 1.2 & 2.8$ \pm $3.4 \\\hline |
| 142 |
< |
$3e$ Tight &4.9 & 5.0 & 0.5 & 0.1 & 0.7 & 1.7$ \pm $2.9 \\\hline |
| 143 |
< |
$2e1\mu$ Loose &15.8 & 78.9 & 9.0 & 0 & 9.0 & 11.6$ \pm $4.9 \\\hline |
| 144 |
< |
$2e1\mu$ Tight &0.3 & 2.0 & 0.7 & 0 & 0.7 & 1.0$ \pm $2.8 \\\hline |
| 145 |
< |
$2\mu1e$ Loose &20.4 & 15.4 & 1.3 & 0 & 1.3 & 2.9$ \pm $3.5 \\\hline |
| 146 |
< |
$2\mu1e$ Tight &5.8 & 5.6 & 0.5 & 0 & 0.5 & 1.7$ \pm $3.0 \\\hline |
| 147 |
< |
$3\mu$ Loose &16.8 & 84.9 & 8.5 & 0 & 8.5 & 7.1$ \pm $4.4 \\\hline |
| 148 |
< |
$3\mu$ Tight &0.3 & 2.3 & 0.2 & 0 & 0.2 & 0.7$ \pm $2.8 \\\hline |
| 141 |
> |
$3e$ Loose &44.5748 & 12.6511 & 1.62239 & 0.357018 & 1.9794 & 6.81271$ \pm $5.60783 \\\hline |
| 142 |
> |
$3e$ Tight &13.8877 & 5.04709 & 0.79839 & 0.357018 & 1.15541 & 3.76484$ \pm $7.74145 \\\hline |
| 143 |
> |
$2e1mu$ Loose &41.5198 & 78.9304 & 12.6155 & 0 & 12.6155 & 16.1879$ \pm $5.12531 \\\hline |
| 144 |
> |
$2e1mu$ Tight &0.993801 & 1.97881 & 0.883798 & 0 & 0.883798 & 1.63388$ \pm $2.94792 \\\hline |
| 145 |
> |
$2mu1e$ Loose &56.2794 & 15.3858 & 1.89565 & 0 & 1.89565 & 7.24906$ \pm $5.77249 \\\hline |
| 146 |
> |
$2mu1e$ Tight &17.2942 & 5.55847 & 0.79839 & 0 & 0.79839 & 4.53933$ \pm $7.00846 \\\hline |
| 147 |
> |
$3mu$ Loose &43.6972 & 84.8891 & 11.9976 & 0 & 11.9976 & 11.1603$ \pm $3.36046 \\\hline |
| 148 |
> |
$3mu$ Tight &0.806562 & 2.31232 & 0.324477 & 0 & 0.324477 & 0.836361$ \pm $2.47575 \\\hline |
| 149 |
|
\end{tabular} |
| 150 |
|
\end{center} |
| 151 |
|
\caption{Comparison between Monte Carlo truth information and the results of the fit for the background without genuine \Z boson. Number of events are obtained in the invariant mass range between 81 and 101 GeV. The ``Loose'' and ``Tight'' selection criteria applied for third lepton considered. |
