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The FR are measured as a function of $P_T$ and $|\eta|$. |
| 114 |
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The FR projections on the $P_T$ and $|\eta|$ axes for the muon FR and for |
| 115 |
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the three (V1, V2, V3) electron FR in the different trigger samples |
| 116 |
< |
are displayed in Figures~\ref{fig:muFR} and~\ref{fig:eleFR}. |
| 116 |
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are displayed in |
| 117 |
> |
{\color{red} Figures~\ref{fig:muFR} and~\ref{fig:eleFR} (old)} and |
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{\color{blue}Figures~\ref{fig:muFR2} and~\ref{fig:eleFR2} (new)}. |
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> |
|
| 120 |
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|
| 121 |
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|
| 122 |
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\begin{figure}[htb] |
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\begin{center} |
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+ |
{\color{red} |
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\includegraphics[width=0.48\linewidth]{MuFakeRatesJune1.pdf} |
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\includegraphics[width=0.48\linewidth]{muFReta.pdf} |
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|
\caption{\label{fig:muFR}The muon fake rate as a function of $P_T$ |
| 128 |
< |
and $|\eta|$ in the different jet samples.} |
| 128 |
> |
and $|\eta|$ in the different jet samples. (Old plots updated below).} |
| 129 |
> |
} |
| 130 |
> |
\end{center} |
| 131 |
> |
\end{figure} |
| 132 |
> |
|
| 133 |
> |
|
| 134 |
> |
|
| 135 |
> |
\begin{figure}[htb] |
| 136 |
> |
\begin{center} |
| 137 |
> |
{\color{blue} |
| 138 |
> |
\includegraphics[width=0.31\linewidth, angle=90]{MuFakeRatesJuly7.pdf} |
| 139 |
> |
\includegraphics[width=0.31\linewidth, angle=90]{muFReta7July.pdf} |
| 140 |
> |
\caption{\label{fig:muFR2}The muon fake rate as a function of $P_T$ |
| 141 |
> |
and $|\eta|$ in the different jet samples. Note that these now start at |
| 142 |
> |
$P_T=$ 10 GeV instead of $P_T=$5 GeV as they did in the earlier analysis |
| 143 |
> |
because of a preselection aplied in our data handling. For this reason |
| 144 |
> |
the $\eta$-projections cannot be directly compared since the this is |
| 145 |
> |
dominated by muons of $P_T$ near threshold. Note also that the |
| 146 |
> |
muon identification requirements have changed a little bit, as |
| 147 |
> |
described in Section 3.1.5. (New updated plots).} |
| 148 |
> |
} |
| 149 |
|
\end{center} |
| 150 |
|
\end{figure} |
| 151 |
|
|
| 152 |
+ |
|
| 153 |
+ |
|
| 154 |
|
\begin{figure}[htb] |
| 155 |
|
\begin{center} |
| 156 |
+ |
{\color{red} |
| 157 |
|
\includegraphics[width=\linewidth]{ElFakeRatesJune1.pdf} |
| 158 |
|
\includegraphics[width=\linewidth]{eFReta.pdf} |
| 159 |
|
\caption{\label{fig:eleFR}The electron fake rates |
| 160 |
|
(V1,V2,V3) as a function of $P_T$ and $|\eta|$ |
| 161 |
< |
in the different jet samples.} |
| 161 |
> |
in the different jet samples. (Old plots updated below).} |
| 162 |
> |
} |
| 163 |
|
\end{center} |
| 164 |
|
\end{figure} |
| 165 |
|
|
| 166 |
+ |
|
| 167 |
+ |
|
| 168 |
+ |
\begin{figure}[htb] |
| 169 |
+ |
\begin{center} |
| 170 |
+ |
{\color{blue} |
| 171 |
+ |
\includegraphics[width=0.4\linewidth,angle=90 ]{ElFakeRatesJuly7.pdf} |
| 172 |
+ |
\includegraphics[width=0.4\linewidth,angle=90]{eFRetaJuly7.pdf} |
| 173 |
+ |
\caption{\label{fig:eleFR2}The electron fake rates |
| 174 |
+ |
(V1,V2,V3) as a function of $P_T$ and $|\eta|$ |
| 175 |
+ |
in the different jet samples. |
| 176 |
+ |
Note that the spike removal has been added to the electron |
| 177 |
+ |
selection since the earlier analysis. This is a very |
| 178 |
+ |
small effect. (New updated plots).} |
| 179 |
+ |
} |
| 180 |
+ |
\end{center} |
| 181 |
+ |
\end{figure} |
| 182 |
+ |
|
| 183 |
+ |
|
| 184 |
|
The fake rates are reasonably stable with respect to |
| 185 |
|
jet trigger variations, within the $\approx 50\%$ which |
| 186 |
|
we believe to be a realistic goal for the FR systematics. |
| 196 |
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FR does not appear to change very fast as a function of $P_T$. |
| 197 |
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|
| 198 |
|
|
| 199 |
+ |
\clearpage |
| 200 |
+ |
|
| 201 |
|
\subsection{Loosening the isolation requirement for the muon FO} |
| 202 |
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Loosening the isolation requirement for the muon FO would reduce the |
| 203 |
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muon FR. This is in general ``a good thing''\texttrademark. |
