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\title{Check List for Particle : \boldmath{ $\Lambda^0(1670)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &33122 & & & Mass & 1670& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 35& & & Gen  & \verb: Lambda(1670)0: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $\Lambda^0(1670) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:Lambda(1670)0Mass: \ \ & Width Gen.  & \verb:Lambda(1670)0Width: \ \ & Type        & baryon \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$****$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1/2$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 68& Upper cut & 350& PDG link &b040 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

  The $\Lambda^0(1670)$ is an excited $\Lambda$ resonance. The mass and width are taken from \cite{Yao:2006px}. The branching ratio for the $N\bar{K}$ mode is taken to be at the low end of the range given in \cite{Yao:2006px} which seems more consistent with the measurements. This forces the remaining modes to the upper end of the range. The lower limit on the mass is set to allow the $\Sigma\pi$ and $NK$ modes while the upper limit is set to ten times the width. EvtGen includes the $\Lambda^0(1670)$ but takes at higher value of the $\Lambda\eta$ branching ratio and correspondingly a lower value for the $\Sigma\pi$ branching ratio.
\item References?
\end{itemize}
\setlongtables
\begin{longtable}[t]{|c|c|c|p{1in}|c|p{2.5in}|}
\hline
Branching & Rating & Outgoing  & Description & Decayer &  EvtGen \\ 
Ratio     &        & Particles &             &         & \\ 
\hline
\endhead
\caption{The decay modes of the $\Lambda^0(1670)$ (continues).}
\endfoot
\caption{The decay modes of the $\Lambda^0(1670)$.}
\endlastfoot
\label{tab:33122decaymodes}
0.250001 & $****$ & $\Lambda^0$, $\eta$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.183333 & $****$ & $\Sigma^+$, $\pi^-$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.183333 & $****$ & $\Sigma^0$, $\pi^0$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.183333 & $****$ & $\Sigma^-$, $\pi^+$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.100000 & $****$ & $p^+$, $K^-$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.100000 & $****$ & $n^0$, $\bar{K}^0$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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