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Comparing UserCode/Vuko/Notes/WZCSA07/selection.tex (file contents):
Revision 1.9 by vuko, Sat Jun 21 09:48:32 2008 UTC vs.
Revision 1.10 by vuko, Sat Jun 21 15:32:35 2008 UTC

#	Line 46 | Line 46 | $3\mu$     &   HLTSingleMuonIso
46		\label{tab:hlteff}
47		\end{table}
48
49	+
50	+	\begin{figure}[tbp]
51	+	\begin{center}
52	+	\scalebox{0.7}{\includegraphics{figs/mu_isol.eps}}
53	+	\caption{Muon isolation variables for the muon associated
54	+	to the \W-boson decay in $2e1\mu$ events: the left plot
55	+	shows the sum of calorimetric energy in a $\Delta R=0.3$ cone
56	+	around the muon candidate; the right plot shows the sum of
57	+	transverse momenta of tracks within a $\Delta R = 0.25$ cone around
58	+	the muon candidate. The normalization of signal and background
59	+	distributions is arbitrary.
60	+	}
61	+	\label{fig:mu_isol}
62	+	\end{center}
63	+	\end{figure}
64	+
65	+	\begin{figure}[tb]
66	+	\begin{center}
67	+	\scalebox{0.6}{\includegraphics{figs/mu_SIP.eps}}
68	+	\caption{
69	+	Muon impact parameter significance distribution
70	+	in $2e1\mu$ events. The normalization of signal and background
71	+	distributions is arbitrary.
72	+	}
73	+	\label{fig:mu_SIP}
74	+	\end{center}
75	+	\end{figure}
76	+
77	+
78		\subsection{Lepton identification}
79		\label{sec:leptonId}
80
#	Line 76 | Line 105 | satisfy $S_{IP}<3$. This requirement is
105		and not for electrons. For electrons, a significant fraction of the
106		background comes from fake electrons and not from heavy quark decays,
107		and a cut on the impact parameter significance shows no improvement
108	<	in significance there.
108	>	in significance there, as can be seen in Figure~\ref{fig:wl_IP_SvsCut}.
109
110	+	\begin{figure}[p]
111	+	\begin{center}
112	+	\scalebox{0.6}{\includegraphics{figs/wl_IP_eff.eps}}
113	+	\caption{Efficiency for signal and background as a function
114	+	of the cut value on the \W-boson lepton impact parameter
115	+	significance. All other cuts but the cut on this variable
116	+	are applied.
117	+	%    Only events with 81.1 GeV $< M_Z < $ 101.1 \gev
118	+	%    are considered.
119	+	}
120	+	\label{fig:wl_IP_eff}
121	+	\end{center}
122	+	%\end{figure}
123	+
124	+	%\begin{figure}[bt]
125	+	\begin{center}
126	+	\scalebox{0.6}{\includegraphics{figs/wl_IP_SvsCut.eps}}
127	+	\caption{Signal significance as a function of the cut value on
128	+	the \W-boson lepton impact parameter significance. All other cuts but
129	+	the cut on this variable are applied.
130	+	%    Only events with 81.1 GeV $< M_Z < $ 101.1 \gev are considered.
131	+	}
132	+	\label{fig:wl_IP_SvsCut}
133	+	\end{center}
134	+	\end{figure}
135
136
137		\begin{table}[tbp]

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