| 31 |
|
We use PF-based isolation with a cone size of $\Delta R<0.3$, using the effective area rho corrections documented at~\cite{ref:Egammaiso}, |
| 32 |
|
and we require a relative isolation $<$ 0.15. |
| 33 |
|
Electrons in the transition region defined by $1.4442 < |\eta_{SC}| < 1.566$ are rejected. |
| 34 |
+ |
Electrons with a selected muon with \pt $>$ 10 GeV within $\Delta R<0.1$ are rejected. |
| 35 |
|
The electron selection requirements are listed in Table~\ref{table:electrons} for completeness. |
| 36 |
|
|
| 37 |
|
\begin{table}[htb] |
| 83 |
|
\end{center} |
| 84 |
|
\end{table} |
| 85 |
|
|
| 85 |
– |
\subsubsection{PF Leptons} |
| 86 |
– |
|
| 87 |
– |
For consistency with pfmet, both electrons and muons are required to be reconstructed as PF electrons and PF muons, respectively, |
| 88 |
– |
with \pt $>$ 20 GeV. For defining the dilepton invariant mass, the 4-momenta of the PF leptons are used. |
| 89 |
– |
|
| 86 |
|
\subsection{Photons} |
| 87 |
|
\label{sec:phosel} |
| 88 |
|
|
