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\title{Check List for Particle : \boldmath{ $f_0(1500)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &9030221 & & & Mass & 1507& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 109& & & Gen  & \verb: f_0(1500): & &\\ 
       & & & & 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  & $f_0(1500) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:f0(1500)Mass: \ \ & Width Gen.  & \verb:f0(1500)Width: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & variable \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $0$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 327& Upper cut & 327& PDG link & & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The properties of the $f_0(1500)$ are not accurately measured, in common with other scalar mesons. The mass and width are taken from \cite{Yao:2006px} as are most of the branching ratios. We use the branching ratios from \cite{Yao:2006px} for the main modes but use the results from \cite{Abele:2001js}  to split the four pion mode up into submodes. The $f_0(1500)$ is allowed to be off-shell by three times the width. The branching ratios vary with the off-shell mass due to problems with the $\eta\eta'$ decay mode for masses below the central value.
\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 $f_0(1500)$ (continues).}
\endfoot
\caption{The decay modes of the $f_0(1500)$.}
\endlastfoot
\label{tab:9030221decaymodes}
0.232667 & $****$ & $\pi^+$, $\pi^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.127426 & $***$ & $\sigma$, $\sigma$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.116333 & $****$ & $\pi^0$, $\pi^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.081683 & $***$ & $\pi^-(1300)$, $\pi^+$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.081683 & $***$ & $\pi^+(1300)$, $\pi^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.081683 & $***$ & $\pi^0(1300)$, $\pi^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.051000 & $****$ & $\eta$, $\eta$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.043000 & $****$ & $K^+$, $K^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.043000 & $****$ & $K^0$, $\bar{K}^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.042475 & $***$ & $\rho^+$, $\rho^-$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.021238 & $***$ & $\rho^0$, $\rho^0$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.019604 & $***$ & $a_1^+(1260)$, $\pi^-$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.019604 & $***$ & $a_1^-(1260)$, $\pi^+$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.019604 & $***$ & $a_1^0(1260)$, $\pi^0$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.019000 & $****$ & $\eta$, $\eta'$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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