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\title{\boldmath{ $\bar{\Lambda}^0(1520)$}\ \ \ \ \ \ \ $****$}
\maketitle
The lightest singlet $\Lambda$ with spin $3/2$. The mass and width are taken from \cite{Yao:2006px}. The branching ratios are taken from \cite{Yao:2006px} with the addition of the $\Sigma^0\gamma$ mode to ensure the branching ratios sum to one. The $\Lambda\pi\pi$ mode has been split assuming the $75.9\%$ of it comes from $\Sigma^*\pi$, this is below the average of the results in \cite{Yao:2006px} but saturates the $\Sigma\pi\pi$ mode. The lower limit on the mass is set to ensure the decays are kinematically allowed and the upper limit to ten times the width. 
The $\bar{\Lambda}^0(1520)$ has mass $1519.5$~MeV and is unstable. The $\bar{\Lambda}^0(1520)$ has spin $3/2$, charge $0$ and is colour neutral.
 The $\bar{\Lambda}^0(1520)$ is a baryon$\bar{10}$plet.The $\bar{\Lambda}^0(1520)$ has width $15.6$~MeV. The lower limit on the mass of the particle is $80$~MeV and the upper limit is $156$~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 -3124.
\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 $\bar{\Lambda}^0(1520)$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Lambda}^0(1520)$.}
\endlastfoot
\label{tab:-3124decaymodes}
0.223547 & $*****$ & on & $ \bar{p}^-, K^+ $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetScalar::SU3SingletOctet2 \\ 
\hline
0.223547 & $*****$ & on & $ \bar{n}^0, K^0 $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetScalar::SU3SingletOctet2 \\ 
\hline
0.139096 & $*****$ & on & $ \bar{\Sigma}^-, \pi^+ $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetScalar::SU3SingletOctet2 \\ 
\hline
0.139096 & $*****$ & on & $ \bar{\Sigma}^0, \pi^0 $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetScalar::SU3SingletOctet2 \\ 
\hline
0.139096 & $*****$ & on & $ \bar{\Sigma}^+, \pi^- $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetScalar::SU3SingletOctet2 \\ 
\hline
0.028780 & $****$ & on & $ \bar{\Sigma}^{*-}, \pi^+ $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.028780 & $****$ & on & $ \bar{\Sigma}^{*0}, \pi^0 $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.028780 & $****$ & on & $ \bar{\Sigma}^{*+}, \pi^- $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.019373 & $***$ & on & $ \bar{\Sigma}^0, \gamma $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetPhoton::SU3Gamma5 \\ 
\hline
0.014638 & $***$ & on & $ \bar{\Lambda}^0, \pi^+, \pi^- $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.007948 & $***$ & on & $ \bar{\Lambda}^0, \gamma $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SU3BaryonSingletOctetPhoton::SU3Gamma5 \\ 
\hline
0.007319 & $***$ & on & $ \bar{\Lambda}^0, \pi^0, \pi^0 $  & Decay of the $\bar{\Lambda}^0(1520)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\bar{\Lambda}^0(1520)$ decay modes are given in Table~\ref{tab:-3124decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Lambda(1520)0Mass| for the $\bar{\Lambda}^0(1520)$.
The width generator is \verb|Lambda(1520)0Width| for the $\bar{\Lambda}^0(1520)$.

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 The particle was checked by Peter Richardson at 9:19:18 on the 4th of February 2009. The most recently changed decay mode was modified at 21:43:54 on the 25th of July 2005. The particle data was last modified at 16:24:39 on the 10th of October 2006.

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