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# Content
1 \section{Signal and Background Modeling}
2 \label{sec:gen}
3 \subsection{Monte Carlo generators}
4 The signal and background samples for the full detector simulation
5 were generated with the leading order event generator PYTHIA~\cite{Sjostrand:2003wg}. To
6 accomodate NLO effect constant k-factors were applied.
7 Additionally the cross section calculator MCFM~\cite{Campbell:2005} was used to determine
8 the next-to-leading order differential cross section for the WZ
9 production process. To estimate the PDF uncertainty for the signal
10 process at NLO the NLO event generator MC@NLO 3.1~\cite{Frixione:2002ik} together with PDF set
11 CTEQ6M was used.
12
13 \subsection{Signal Definition}
14
15 This analysis is studying the final state of on-shell $W$ and $Z$
16 boson, both of them decaying leptonically. The fully final leptonic
17 final state $l^+ l^- l^\pm \nu$ also receives a contribution from the
18 $W\gamma *$ process, where the $\gamma *$ stands for a virtual photon
19 through the $WW\gamma$ vertex. In this analysis, only events with $l^+
20 l^-$ invariant mass consistent with $Z$ mass will be considered.
21
22 %# for bbll:
23 %#CS NLO ((Z/gamma*->l+l-)bb) = 830pb = 345 pb * 2.4, where:
24 %#- 345 pb is LO CS calculated with precision of ~0.15%
25 %#- 2.4 is MCMF calculated k-factor with precision ~30% (!)
26 %# 830x0.173 (== XS x eff.) = 143.59pb
27
28
29 \begin{table}[tbh]
30 \begin{tabular}{llllll} \hline
31 Sample & Generator & Sample name & Events & $\sigma \cdot \epsilon \cdot k$ & k-factor \\ \hline
32 WZ & Pythia & /WZ/CMSSW\_1\_6\_7-CSA07-1195663763/RECO & 58897 & 0.585 pb & 1.92 \\
33 $Zb\bar{b}$ & COMPHEP & /comphep-bbll/CMSSW\_1\_6\_7-CSA07-1198677426/RECO & 143.59 pb & 2.4 \\
34 ``Chowder'' & ALPGEN & /CSA07AllEvents/CMSSW\_1\_6\_7-CSA07-Chowder-A1-PDAllEvents-ReReco-100pb/RECO & 25 M & event weights & - \\
35 \hline
36 \end{tabular}
37
38 \caption{Monte Carlo samples used in this analysis}
39 \end{table}
40
41 \subsection{Signal and Background Monte Carlo samples}
42
43
44