% 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{ ${\Xi'}_c^0$}\ \ \ \ \ \ \ $****$}
\maketitle
The ${\Xi'}_c^0$ is the neutral $\Xi_c$ member of the $SU(3)$ sextet which includes the $\Sigma_c$ and $\Omega_c^0$. The mass is taken from \cite{Yao:2006px} but the width has not been measured. Due to the mass difference with the $\Xi_c$ there are no allowed strong decays and therefore we assume that the radiative mode is the only one. We use the theoretical value of the width from \cite{Ivanov:1999bk}  and allow the ${\Xi'}_c^0$ to be off-shell by ten times this width.
The ${\Xi'}_c^0$ has mass $2578$~MeV and is unstable. The ${\Xi'}_c^0$ has spin $1/2$, charge $0$ and is colour neutral.
 The ${\Xi'}_c^0$ is a baryon and is from the $(56,0^+_0)$ $40$plet.The ${\Xi'}_c^0$ has width $0.00017$~MeV. The lower limit on the mass of the particle is $0.0017$~MeV and the upper limit is $0.0017$~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 4312.
\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 ${\Xi'}_c^0$ (continues).}
\endfoot
\caption{The decay modes of the ${\Xi'}_c^0$.}
\endlastfoot
\label{tab:4312decaymodes}
1.000000 & $****$ & on & $ \Xi_c^0, \gamma $  & Radiative decay of ${\Xi'}_c^0$ with is assumed to be the only mode as strong modes are not possible   & Herwig::RadiativeHeavyBaryon::HeavyGamma \\ 
\hline
\end{longtable}The ${\Xi'}_c^0$ decay modes are given in Table~\ref{tab:4312decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Xi'_c0Mass| for the ${\Xi'}_c^0$.
The width generator is \verb|Xi'_c0Width| for the ${\Xi'}_c^0$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 9:43:5 on the 4th of February 2009. The most recently changed decay mode was modified at 10:44:42 on the 26th of July 2005. The particle data was last modified at 19:5:36 on the 3rd of July 2008.

\end{document}
