\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{ $\omega(1420)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &100223 & & & Mass & 1425& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 215& & & Gen  & \verb: omega': & &\\ 
       & & & & 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  & $\omega(1420) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:omega'mass: \ \ & Width Gen.  & \verb:omega'width: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 215& Upper cut & 430& PDG link &m125 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $\omega(1420)$ is the lightest isospin neutral member of the second vector multiplet. Its mass and width are not well measured, the values we use are the centre of the range given in \cite{Yao:2006px}. The determination of the branching ratios is uncertain. We have assumed that only $\omega\pi\pi$ and $\rho\pi$ modes exist and used the values for the branching ratios given in \cite{Henner:2002iv}  together with the only measurement of the ratio of $\Gamma(\omega\sigma)/\Gamma(b_1\pi)$ to determine the fraction of $b_1\pi$ in this mode to determine the branching ratios. The $\omega(1420)$ is allowed to be off-shell by twice the width above the central value and the width below it due to problems with off-shell decays.
\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 $\omega(1420)$ (continues).}
\endfoot
\caption{The decay modes of the $\omega(1420)$.}
\endlastfoot
\label{tab:100223decaymodes}
0.233000 & $***$ & $\rho^+$, $\pi^-$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.233000 & $***$ & $\rho^0$, $\pi^0$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.233000 & $***$ & $\rho^-$, $\pi^+$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.112876 & $***$ & $\omega$, $\sigma$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.062708 & $***$ & $b_1^+$, $\pi^-$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.062708 & $***$ & $b_1^-$, $\pi^+$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.062708 & $***$ & $b_1^0$, $\pi^0$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
