14 |
|
\usepackage{lscape} |
15 |
|
\usepackage{graphicx} |
16 |
|
\usepackage{pst-node} |
17 |
+ |
\usepackage{epstopdf} |
18 |
+ |
%\usepackage[croatian]{babel} |
19 |
+ |
|
20 |
+ |
\renewcommand{\dj}{d\kern-0.4em\char"16\kern-0.1em} |
21 |
+ |
\renewcommand{\DJ}{\raise0.3ex\hbox{-}\kern-0.36em D} |
22 |
+ |
|
23 |
+ |
|
24 |
|
\RequirePackage{xspace} |
25 |
|
\input noteWZsymbols |
26 |
|
|
31 |
|
|
32 |
|
\begin{titlepage} |
33 |
|
|
34 |
< |
% \analysisnote{2008/xxx} |
35 |
< |
\date{20 June 2008} |
34 |
> |
\analysisnote{EWK 2008/003} |
35 |
> |
\date{23 June 2008} |
36 |
|
|
37 |
|
\title{Study of the process\\ |
38 |
< |
$ \proton\proton\to \W\Z \to \ell^{\pm} \ellell (\ell=e,\mu)$\\ |
38 |
> |
$ \proton\proton\to \W\Z \to \ell^{\pm}\nu \ellell (\ell=e,\mu)$\\ |
39 |
|
at CMS} |
40 |
|
|
41 |
|
\begin{Authlist} |
42 |
< |
V.~Brigljevi\'c, S.~Morovi\'c, S.~Djuri\'c |
43 |
< |
\Instfoot{IRB}{Rudjer Bo\v skovi\'c Institute, 10002 Zagreb, Croatia} |
42 |
> |
V.~Brigljevi\'c, S.~Morovi\'c, S.~ \DJ uri\'c |
43 |
> |
\Instfoot{IRB}{Ru\dj er Bo\v skovi\'c Institute, 10002 Zagreb, Croatia} |
44 |
|
S.~Beauceron |
45 |
|
\Instfoot{CERN}{CERN, Geneva, Switzerland} |
46 |
|
K.~Kaadze, Y.~Maravin |
50 |
|
\begin{abstract} |
51 |
|
|
52 |
|
In this note, we investigate the discovery potential |
53 |
< |
for the $\proton\proton \to \W\Z \to \ell^{\pm} \ellell (\ell=e,\mu)$ process at CMS, |
54 |
< |
with full detector simulation of the signal and of the various backgrounds. |
53 |
> |
for the $\proton\proton \to \W\Z \to \ell^{\pm}\nu\ellell (\ell=e,\mu)$ process at CMS, |
54 |
> |
using full detector simulation of the signal and of the various physics and |
55 |
> |
instrumental backgrounds. |
56 |
> |
|
57 |
|
% We determine the signal significance as a function of |
58 |
|
% integrated luminosity at the LHC based on Standard Model |
59 |
|
% cross sections computed at the next to leading order in $\alpha_s$. |
60 |
< |
% We expect $\sim 97 $ signal $\W\Z \to \ell^{\pm} \ellell (\ell=e,\mu)$ events for $\sim 22$ background |
61 |
< |
% events per inverse femtobarn. The background is found |
62 |
< |
% to be dominated by the $\Zbbbar$, $\t\tbar$ and \ZZ processes with three true electrons or muons in the |
63 |
< |
% final state. The sensitivity of the analysis allows for a potential 5-sigma discovery |
64 |
< |
% of the $\proton\proton \to\W\Z$ channel with about 150 inverse picobarn. |
60 |
> |
% We expect $\sim 97 $ signal $\W\Z \to \ell^{\pm}\nu \ellell (\ell=e,\mu)$ events |
61 |
> |
% and $\sim 22$ background events per inverse femtobarn. The background is found |
62 |
> |
% to be dominated by the $\Zbbbar$, $\t\tbar$, and \ZZ processes. |
63 |
> |
% The sensitivity of the method allows for a potential 5-sigma discovery |
64 |
> |
% of the $\proton\proton \to\W\Z$ process with about 150 inverse picobarn. |
65 |
|
\end{abstract} |
66 |
|
|
67 |
|
\end{titlepage} |