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\title{\boldmath{ $\bar{\Xi}_c^-(2645)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\bar{\Xi}_c^-(2645)$ is the charged $\Xi_c$ member of the lightest $4$-plet of $SU(4)$. The mass has been measured and is taken from \cite{Yao:2006px}. The width has not been measured and therefore we use the theoretical calculation of \cite{Ivanov:1999bk}  which is below the experimental limit. The mass is such that only the strong decays to the lightest $\Xi_c$ and a pion is possible and we assume these are the only modes with the relative rates given by isospin. The $\bar{\Xi}_c^-(2645)$ is allowed to be off-shell by ten times the width.
The $\bar{\Xi}_c^-(2645)$ has mass $2646.6$~MeV and is unstable. The $\bar{\Xi}_c^-(2645)$ has spin $3/2$, charge $-1$ and is colour neutral.
 The $\bar{\Xi}_c^-(2645)$ is a baryon and is from the $(56,0^+_0)$ $35$plet.The $\bar{\Xi}_c^-(2645)$ has width $3$~MeV. The lower limit on the mass of the particle is $30$~MeV and the upper limit is $30$~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 -4324.
\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 $\bar{\Xi}_c^-(2645)$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Xi}_c^-(2645)$.}
\endlastfoot
\label{tab:-4324decaymodes}
0.666667 & $*****$ & on & $ \bar{\Xi}_c^0, \pi^- $  & Only allowed strong decay of $\bar{\Xi}_c^-(2645)$. The relative rates for the two modes is given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.333333 & $*****$ & on & $ \bar{\Xi}_c^-, \pi^0 $  & Only allowed strong decay of $\bar{\Xi}_c^-(2645)$. The relative rates for the two modes is given by isospin.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
\end{longtable}The $\bar{\Xi}_c^-(2645)$ decay modes are given in Table~\ref{tab:-4324decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Xi*_c+Mass| for the $\bar{\Xi}_c^-(2645)$.
The width generator is \verb|Xi*_c+Width| for the $\bar{\Xi}_c^-(2645)$.

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 The particle was checked by Peter Richardson at 9:28:14 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 18:11:5 on the 3rd of July 2008.

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