% particle data information automatically produced from the herwig database
\documentclass[a4paper]{article}
\usepackage{cite,longtable}
\bibliographystyle{JHEP}
\topmargin -1.5cm
\textheight 26cm
\textwidth 20cm
\oddsidemargin -2cm
\evensidemargin 0cm
\begin{document}
\title{\boldmath{ ${\Xi}_c(2790)^0$}\ \ \ \ \ \ \ $***$}
\maketitle
The ${\Xi}_c(2790)^0$ is the neutral $\Xi_c$ member of the $SU(4)$ decuplet which includes the $\Lambda_c(2593)^+$. The mass is taken from \cite{Yao:2006px} but the width and branching ratios have not been measured. Only the $\Xi_c'\pi$ mode has been observed. We have calculated the branching ratios and width using heavy quark symmetry and the results of \cite{Ivanov:1999bk} , in practice the $\Xi_c^*\pi$ is strongly phase-space supressed and so we only include the $\Xi_c'\pi$ modes. The ${\Xi}_c(2790)^0$ is allowed to be off-shell by ten times the width.
The ${\Xi}_c(2790)^0$ has mass $2791.9$~MeV and is unstable. The ${\Xi}_c(2790)^0$ has spin $1/2$, charge $0$ and is colour neutral.
 The ${\Xi}_c(2790)^0$ is a baryon and is from the $(56,0^+_0)$ $40$plet.The ${\Xi}_c(2790)^0$ has width $1.13$~MeV. The lower limit on the mass of the particle is $11.3$~MeV and the upper limit is $11.3$~MeV. These are the deviations from the on-shell value. The branching ratios are fixed.
The properties of the particle and its antiparticle are taken to be charge-conjugate to each other.
 The PDG code is 14312.
\setlongtables
\begin{longtable}[t]{|c|c|c|p{1in}|p{2.5in}|c|}
\hline
Branching & Rating & On/ & Outgoing  & Description & Decayer  \\ 
Ratio     &                                 & Off & Particles &             &         \\ 
\hline
\endhead
\caption{The decay modes of the ${\Xi}_c(2790)^0$ (continues).}
\endfoot
\caption{The decay modes of the ${\Xi}_c(2790)^0$.}
\endlastfoot
\label{tab:14312decaymodes}
0.666667 & $***$ & on & $ {\Xi'}_c^+, \pi^- $  & The decay of the ${\Xi}_c(2790)^0$ to $\Xi'_c\pi$ with branching ratio given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.333333 & $***$ & on & $ {\Xi'}_c^0, \pi^0 $  & The decay of the ${\Xi}_c(2790)^0$ to $\Xi'_c\pi$ with branching ratio given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
\end{longtable}The ${\Xi}_c(2790)^0$ decay modes are given in Table~\ref{tab:14312decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Xi_c10Mass| for the ${\Xi}_c(2790)^0$.
The width generator is \verb|Xi_c10Width| for the ${\Xi}_c(2790)^0$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 9:20:48 on the 4th of February 2009. The most recently changed decay mode was modified at 23:10:55 on the 3rd of April 2005. The particle data was last modified at 18:31:19 on the 3rd of July 2008.

\end{document}
