% particle data information automatically produced from the herwig database
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\title{\boldmath{ $\bar{\Sigma}^0(1750)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\bar{\Sigma}^0(1750)$ is added to complete the multiplet. This is not the state assigned to this role in \cite{Yao:2006px} but the properties of this state are better determined. The mass and width are taken from \cite{Yao:2006px}. The widths are estimated based on the results in \cite{Yao:2006px}. The lower limit on the mass is set to avoid problems with inaccessible decay modes and the upper limit to five times the mass. As the dominant mode is only just allow for the central value of the mass we use the option of varying the branching ratios with the off-shell mass of the particle.
The $\bar{\Sigma}^0(1750)$ has mass $1750$~MeV and is unstable. The $\bar{\Sigma}^0(1750)$ has spin $1/2$, charge $0$ and is colour neutral.
 The $\bar{\Sigma}^0(1750)$ is a baryon$40$plet.The $\bar{\Sigma}^0(1750)$ has width $90$~MeV. The lower limit on the mass of the particle is $250$~MeV and the upper limit is $450$~MeV. These are the deviations from the on-shell value. The branching ratios are allowed to vary with the off-shell mass of the particle.
The properties of the particle and its antiparticle are taken to be charge-conjugate to each other.
 The PDG code is -23212.
\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 $\bar{\Sigma}^0(1750)$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Sigma}^0(1750)$.}
\endlastfoot
\label{tab:-23212decaymodes}
0.550000 & $***$ & on & $ \bar{\Sigma}^0, \eta $  & Deay of $\bar{\Sigma}^0(1750)$. The branching ratio is set to the upper limit of the range given in \cite{Yao:2006px} to ensure the total is one.   & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2 \\ 
\hline
0.200000 & $***$ & on & $ \bar{\Lambda}^0, \pi^0 $  & Deay of $\bar{\Sigma}^0(1750)$. This mode is added to ensure the branching ratios sum to one   & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2 \\ 
\hline
0.125000 & $***$ & on & $ \bar{n}^0, K^0 $  & Deay of $\bar{\Sigma}^0(1750)$. The branching ratio is placed at the centre of the range given in \cite{Yao:2006px}.   & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2 \\ 
\hline
0.125000 & $***$ & on & $ \bar{p}^-, K^+ $  & Deay of $\bar{\Sigma}^0(1750)$. The branching ratio is placed at the centre of the range given in \cite{Yao:2006px}.   & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2 \\ 
\hline
\end{longtable}The $\bar{\Sigma}^0(1750)$ decay modes are given in Table~\ref{tab:-23212decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|Sigma(1750)0Mass| for the $\bar{\Sigma}^0(1750)$.
The width generator is \verb|Sigma(1750)0Width| for the $\bar{\Sigma}^0(1750)$.

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 The particle was checked by Peter Richardson at 9:35:15 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 16:24:39 on the 10th of October 2006.

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