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\title{\boldmath{ $\bar{\Xi}_{b1}^{*0}$}\ \ \ \ \ \ \ $*$}
\maketitle
The $\bar{\Xi}_{b1}^{*0}$ has not been observed and is only included to complete the multiplet. The mass is obtained using the mass difference from the charm system and the mass of the $\Xi_b$. The decay modes and width are calculated using the results of \cite{Ivanov:1999bk}  assuming the couplings are the same in the bottom and charm systems. The $\bar{\Xi}_{b1}^{*0}$ is allowed  to be off-shell by ten times the width.
The $\bar{\Xi}_{b1}^{*0}$ has mass $6138.4$~MeV and is unstable. The $\bar{\Xi}_{b1}^{*0}$ has spin $3/2$, charge $0$ and is colour neutral.
 The $\bar{\Xi}_{b1}^{*0}$ is a baryon and is from the $(56,0^+_0)$ $40$plet.The $\bar{\Xi}_{b1}^{*0}$ has width $1.2$~MeV. The lower limit on the mass of the particle is $12$~MeV and the upper limit is $12$~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 -15324.
\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 $\bar{\Xi}_{b1}^{*0}$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Xi}_{b1}^{*0}$.}
\endlastfoot
\label{tab:-15324decaymodes}
0.333000 & $**$ & on & $ \bar{\Xi'}_b^+, \pi^- $  & Decay of $\bar{\Xi}_{b1}^{*0}$ to $\Xi_b'\pi$ with branching ratio calculated as described above.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.333000 & $**$ & on & $ \bar{\Xi}_b^{*+}, \pi^- $  & Decay of $\bar{\Xi}_{b1}^{*0}$ to $\Xi_b^*\pi$ with branching ratio calculated as described above.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.167000 & $**$ & on & $ \bar{\Xi'}_b^0, \pi^0 $  & Decay of $\bar{\Xi}_{b1}^{*0}$ to $\Xi_b'\pi$ with branching ratio calculated as described above.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.167000 & $**$ & on & $ \bar{\Xi}_b^{*0}, \pi^0 $  & Decay of $\bar{\Xi}_{b1}^{*0}$ to $\Xi_b^*\pi$ with branching ratio calculated as described above.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
\end{longtable}The $\bar{\Xi}_{b1}^{*0}$ decay modes are given in Table~\ref{tab:-15324decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Xi_b1*0Mass| for the $\bar{\Xi}_{b1}^{*0}$.
The width generator is \verb|Xi_b1*0Width| for the $\bar{\Xi}_{b1}^{*0}$.

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 The particle was checked by Peter Richardson at 9:22:15 on the 4th of February 2009. The most recently changed decay mode was modified at 21:49:35 on the 9th of August 2005. The particle data was last modified at 13:58:55 on the 6th of July 2008.

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