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\title{Check List for Particle : \boldmath{ $\bar{n}^0(1440)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &-12112 & & & Mass & 1440& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 300& & & Gen  & \verb: nbar(1440): & &\\ 
       & & & & 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  & $\bar{n}^0(1440) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:n(1440)0Mass: \ \ & Width Gen.  & \verb:n(1440)0Width: \ \ & Type        & baryon \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$****$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & variable \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1/2$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 300& Upper cut & 600& PDG link &b061 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The neutral mebmer of first excited multiplet of nucleon-like baryons. The mass and width are taken from \cite{Yao:2006px}. The branching ratios use the central values from \cite{Yao:2006px} with minor adjustments to ensure the branching ratios sum to one.
The lower limit on the mass is set so that the $N\pi$ mode is allowed and the upper limit to twice the width. Given the small mass differences for the $N\pi\pi$ and $\Delta\pi$ modes the option of varying the branching ratios with the off-shell mass is used to pervent the unaccessible decay modes being selected.
\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 $\bar{n}^0(1440)$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{n}^0(1440)$.}
\endlastfoot
\label{tab:-12112decaymodes}
0.433245 & $****$ & $\bar{p}^-$, $\pi^+$ & & Herwig::SU3BaryonOctetOctetScalar::SU3StrongRoper& \\ 
& & & & & \\ \hline
0.216622 & $****$ & $\bar{n}^0$, $\pi^0$ & & Herwig::SU3BaryonOctetOctetScalar::SU3StrongRoper& \\ 
& & & & & \\ \hline
0.131223 & $****$ & $\bar{\Delta}^+$, $\pi^-$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3RoperDecuplet& \\ 
& & & & & \\ \hline
0.087482 & $****$ & $\bar{\Delta}^0$, $\pi^0$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3RoperDecuplet& \\ 
& & & & & \\ \hline
0.058321 & $***$ & $\bar{n}^0$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.043741 & $****$ & $\bar{\Delta}^-$, $\pi^+$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3RoperDecuplet& \\ 
& & & & & \\ \hline
0.029161 & $***$ & $\bar{n}^0$, $\pi^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000205 & $***$ & $\bar{n}^0$, $\gamma$ & & Herwig::SU3BaryonOctetOctetPhoton::SU3RoperGamma& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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