| 2 |
|
\label{sec:eventReconstruction} |
| 3 |
|
|
| 4 |
|
The four possible final states of \WZ |
| 5 |
< |
production with electrons and muons are studied, $\rm e^\pm \epem$, $\mu^\pm \epem$, $\rm e^\pm \mu^+\mu^-$ |
| 5 |
> |
production with electrons and muons in the final state are studied, $\rm e^\pm \epem$, $\mu^\pm \epem$, $\rm e^\pm \mu^+\mu^-$ |
| 6 |
|
and $\mu^\pm \mu^+\mu^-$. They are associated to four possible classes, |
| 7 |
|
denoted as follows: |
| 8 |
|
\begin{itemize} |
| 16 |
|
\subsection{Trigger selection and efficiencies} |
| 17 |
|
|
| 18 |
|
Events stemming from the three-lepton final states of $\WZ$ production |
| 19 |
< |
are collected by the electron and muon triggers. For each channel, |
| 19 |
> |
are collected by the electron and/or muon triggers. For each channel, |
| 20 |
|
a minimun number of HLT requirements is chosen while keeping |
| 21 |
|
the HLT efficiency for selected events close to 100\%. The same |
| 22 |
|
HLT requirements are used for channels with the same Z decay mode: |
| 209 |
|
|
| 210 |
|
\subsection{Signal extraction} |
| 211 |
|
|
| 212 |
+ |
%\input D0Matrix |
| 213 |
+ |
\input zjetbackground |
| 214 |
|
|
| 213 |
– |
\subsection{Systematic uncertainties} |
| 215 |
|
|
| 216 |
+ |
\subsection{Systematic uncertainties} |
| 217 |
+ |
\input Sys |
| 218 |
|
|
| 219 |
|
|
| 220 |
|
\begin{figure}[bt] |
