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\title{\boldmath{ $\bar{\Lambda}_c^-(2593)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\bar{\Lambda}_c^-(2593)$ is the first excited $\Lambda_c$ resonance. This particle was not previously included however there is strong evidence for its existance. The mass and width are taken from \cite{Yao:2006px} although the width has not been accurately measured. The branching ratios are also taken from \cite{Yao:2006px}. The $\bar{\Lambda}_c^-(2593)$ is allowed to be off-shell by five times the width.
The $\bar{\Lambda}_c^-(2593)$ has mass $2595.4$~MeV and is unstable. The $\bar{\Lambda}_c^-(2593)$ has spin $1/2$, charge $-1$ and is colour neutral.
 The $\bar{\Lambda}_c^-(2593)$ is a baryon and is from the $(56,0^+_0)$ $\bar{10}$plet.The $\bar{\Lambda}_c^-(2593)$ has width $3.6$~MeV. The lower limit on the mass of the particle is $18$~MeV and the upper limit is $18$~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 -14122.
\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 $\bar{\Lambda}_c^-(2593)$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Lambda}_c^-(2593)$.}
\endlastfoot
\label{tab:-14122decaymodes}
0.240000 & $****$ & on & $ \bar{\Sigma}_c^{- -}, \pi^+ $  & Decay of $\bar{\Lambda}_c^-(2593)$  to $\Sigma_c\pi$. The branching ratios of the two measured modes are the same in \cite{Yao:2006px} and therefore we assume isospin conservation and add all there modes with the same branching ratio.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.240000 & $****$ & on & $ \bar{\Sigma}_c^{-}, \pi^0 $  & Decay of $\bar{\Lambda}_c^-(2593)$  to $\Sigma_c\pi$. The branching ratios of the two measured modes are the same in \cite{Yao:2006px} and therefore we assume isospin conservation and add all there modes with the same branching ratio.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.240000 & $****$ & on & $ \bar{\Sigma}_c^0, \pi^- $  & Decay of $\bar{\Lambda}_c^-(2593)$  to $\Sigma_c\pi$. The branching ratios of the two measured modes are the same in \cite{Yao:2006px} and therefore we assume isospin conservation and add all there modes with the same branching ratio.   & Herwig::StrongHeavyBaryon::HeavyStrong \\ 
\hline
0.186667 & $***$ & on & $ \bar{\Lambda}_c^-, \pi^+, \pi^- $  & Decay of $\bar{\Lambda}_c^-(2593)$  to $\Lambda_c\pi\pi$. Branching ratio calculated after subtracting the $\Sigma_c\pi$ sub-modes and assuming isospin conservation.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.093333 & $***$ & on & $ \bar{\Lambda}_c^-, \pi^0, \pi^0 $  & Decay of $\bar{\Lambda}_c^-(2593)$  to $\Lambda_c\pi\pi$. Branching ratio calculated after subtracting the $\Sigma_c\pi$ sub-modes and assuming isospin conservation.   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\bar{\Lambda}_c^-(2593)$ decay modes are given in Table~\ref{tab:-14122decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Lambda'_cMass| for the $\bar{\Lambda}_c^-(2593)$.
The width generator is \verb|Lambda'_cWidth| for the $\bar{\Lambda}_c^-(2593)$.

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 The particle was checked by Peter Richardson at 9:19:35 on the 4th of February 2009. The most recently changed decay mode was modified at 11:15:29 on the 26th of July 2005. The particle data was last modified at 18:21:39 on the 3rd of July 2008.

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