% 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{ $\Xi_b^{*0}$}\ \ \ \ \ \ \ $**$}
\maketitle
The $\Xi_b^{*0}$ has not been observed and is only included to complete the lightest baryon multiplet with one bottom quark. The mass is obtained using the mass difference from the charm system and the mass of the $\Xi_b$, this gives a higher value than theoretical calculations. The mass difference is such that $\Xi_b\pi$ is the only allowed strong decay modes and therefore we assume that this is the only mode. The width is calculated using the same strong coupling as for the charm system and the decayer. The $\Xi_b^{*0}$ is allowed to be off-shell by ten times this width.
The $\Xi_b^{*0}$ has mass $5968.5$~MeV and is unstable. The $\Xi_b^{*0}$ has spin $3/2$, charge $0$ and is colour neutral.
 The $\Xi_b^{*0}$ is a baryon and is from the $(56,0^+_0)$ $35$plet.The $\Xi_b^{*0}$ has width $3.5$~MeV. The lower limit on the mass of the particle is $35$~MeV and the upper limit is $35$~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 5324.
\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 $\Xi_b^{*0}$ (continues).}
\endfoot
\caption{The decay modes of the $\Xi_b^{*0}$.}
\endlastfoot
\label{tab:5324decaymodes}
0.666667 & $**$ & on & $ \Xi_b^-, \pi^+ $  & Only allowed strong decay of $\Xi_b^{*0}$ which we assume is the only decay. The relative rates for the two modes is given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.333333 & $**$ & on & $ \Xi_b^0, \pi^0 $  & Only allowed strong decay of $\Xi_b^{*0}$ which we assume is the only decay. The relative rates for the two modes is given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
\end{longtable}The $\Xi_b^{*0}$ decay modes are given in Table~\ref{tab:5324decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Xi*_b0Mass| for the $\Xi_b^{*0}$.
The width generator is \verb|Xi*_b0Width| for the $\Xi_b^{*0}$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 9:24:39 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 13:54:35 on the 6th of July 2008.

\end{document}
