Changeset 502 in svn for trunk

Timestamp:

Jul 21, 2009, 10:47:30 AM (15 years ago)

Author:

Xavier Rouby

Message:

update new tau-jet figure + caption

Location:

trunk/paper

Files:

• CommPhysComp/notes.pdf (modified) ( previous)
• CommPhysComp/notes.tex (modified) (1 diff)
• notes.pdf (modified) ( previous)
• notes.tex (modified) (2 diffs)

trunk/paper/CommPhysComp/notes.tex

@@ -506 +506 @@
 %\includegraphics[width=0.6\columnwidth]{Tau}
 \includegraphics[width=0.80\columnwidth]{fig5}
-\caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone shown as the red one is used for the \textit{electromagnetic collimation}, while the green cone is the cone radius used to reconstruct the jet originating from the $\tau$-decay.}
+\caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone serves to apply the \textit{electromagnetic collimation}, while the broader cone is used to reconstruct the jet originating from the $\tau$-decay.}
 \label{h_WW_ss_cut1}
 \end{center}

trunk/paper/notes.tex

@@ -459 +459 @@
 \begin{figure}[!h]
 \begin{center}
-\includegraphics[width=0.6\columnwidth]{Tau}
-\caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone shown as the red one is used for the \textit{electromagnetic collimation}, while the green cone is the cone radius used to reconstruct the jet originating from the $\tau$-decay.}
+\includegraphics[width=0.96\columnwidth]{Tau}
+\caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone serves to apply the \textit{electromagnetic collimation}, while the broader cone is used to reconstruct the jet originating from the $\tau$-decay.}
 \label{h_WW_ss_cut1}
 \end{center}
@@ -624 +624 @@
 Similarly, the jet resolution is evaluated for an \textsc{atlas}-like detector. The $pp \rightarrow gg$ events are here arranged in $8$ adjacent bins in $p_T$. A $k_T$ reconstruction algorithm with $R=0.6$ is chosen and the maximal matching distance between the \textsc{mc}-jets and the reconstructed jets is set to $\Delta R=0.2$. The relative energy resolution is evaluated in each bin by:
 \begin{equation}
-\frac{\sigma(E)}{E} = \sqrt{~~ \Bigg \langle ~\Bigg( \frac{E^\textrm{rec} - E^\textrm{MC}}{E^\textrm{rec}} \Bigg)^2 ~ \Bigg \rangle ~ - ~ \Bigg \langle \frac{E^\textrm{rec} - E^\textrm{MC}}{ E^\textrm{rec} } \Bigg \rangle^2}.
+\frac{\sigma(E)}{E} = \sqrt{ \Bigg \langle \Bigg( \frac{E^\textrm{rec} - E^\textrm{MC}}{E^\textrm{rec}} \Bigg)^2  \Bigg \rangle  -  \Bigg \langle \frac{E^\textrm{rec} - E^\textrm{MC}}{ E^\textrm{rec} } \Bigg \rangle^2}.
 \end{equation}