\documentclass[a4paper]{article}
\usepackage{cite,longtable}
\bibliographystyle{JHEP}
\topmargin -1.5cm
\textheight 26cm
\textwidth 20cm
\oddsidemargin -2cm
\evensidemargin 0cm
\pagestyle{empty}
\begin{document}
\title{Check List for Particle : \boldmath{ $p^+(1535)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &22212 & & & Mass & 1535& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 150& & & Gen  & \verb: p(1535)+: & &\\ 
       & & & & 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  & $p^+(1535) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:p(1535)+Mass: \ \ & Width Gen.  & \verb:p(1535)+Width: \ \ & Type        & baryon \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$****$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & variable \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1/2$& Charge & $1$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 450& Upper cut & 600& PDG link &b063 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $p^+(1535)$ is the charged member of the isospin doublet of excited nucleons from the third multiplet. The mass and width are taken from \cite{Yao:2006px}. The branching ratios are not given in \cite{Yao:2006px} and therefore we have taken the average value from \cite{Yao:2006px} for the $N\eta$ rate and the only measurements of the $\Delta\pi$, $N\rho$ and $N(\pi\pi)^{I=0}$ rates. The $N(1440)\pi$ rate was placed at just below the limit as there is evidence for this state. The radiative modes we placed at the central value of the range from \cite{Yao:2006px}. Finally the $N\pi$ rate was adjusted to ensure the branching ratios sum to unity, this gives a rate consistent with the range from \cite{Yao:2006px}. The off-shell mass is limited below to ensure the $N\pi$ mode is kinematically possible and above by four times the width. Given the small mass differences for the $N\rho$ 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 $p^+(1535)$ (continues).}
\endfoot
\caption{The decay modes of the $p^+(1535)$.}
\endlastfoot
\label{tab:22212decaymodes}
0.529000 & $*****$ & $p^+$, $\eta$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.239000 & $****$ & $n^0$, $\pi^+$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.119500 & $****$ & $p^+$, $\pi^0$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong2& \\ 
& & & & & \\ \hline
0.040000 & $***$ & $n^0(1440)$, $\pi^+$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong4& \\ 
& & & & & \\ \hline
0.020000 & $***$ & $p^+(1440)$, $\pi^0$ & & Herwig::SU3BaryonOctetOctetScalar::SU3Strong4& \\ 
& & & & & \\ \hline
0.013333 & $***$ & $n^0$, $\rho^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.013333 & $***$ & $p^+$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.006667 & $***$ & $p^+$, $\rho^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.006667 & $***$ & $p^+$, $\pi^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005000 & $***$ & $\Delta^{+\,+}$, $\pi^-$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3OctetDecuplet2& \\ 
& & & & & \\ \hline
0.003333 & $***$ & $\Delta^+$, $\pi^0$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3OctetDecuplet2& \\ 
& & & & & \\ \hline
0.002500 & $***$ & $p^+$, $\gamma$ & & Herwig::SU3BaryonOctetOctetPhoton::SU3Gamma2& \\ 
& & & & & \\ \hline
0.001667 & $***$ & $\Delta^0$, $\pi^+$ & & Herwig::SU3BaryonOctetDecupletScalar::SU3OctetDecuplet2& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
