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\title{Check List for Particle : \boldmath{ $f_0(1370)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &10221 & & & Mass & 1395& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 275& & & Gen  & \verb: f'_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  & $f_0(1370) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:f'_00mass: \ \ & Width Gen.  & \verb:f'_00width: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $0$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 275& Upper cut & 275& PDG link &m147 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $f_0(1370)$ is the lightest isospin neutral meson from the lightest scalar meson multiplet. The choice of which meson to assign to this role is complicated and the $f_0(1370)$ could be replaced by the $f_0(980)$. Although the $f_0(1370)$ has been observed the measurement of the mass and width is complicated and model dependent. The \cite{Yao:2006px} only gives a range for both the mass and width rather than a value. We have therefore choosen to use the values from \cite{Abele:2001js}  which is related to our choice from \cite{Abele:2001pv}  for the branching ratios. We use the information in Table~4 of \cite{Abele:2001pv}  to obtain the branching ratios. The limits on the off-shell mass are set to the width because if the decay becomes too off-shell the decayers become inefficient.
\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 $f_0(1370)$ (continues).}
\endfoot
\caption{The decay modes of the $f_0(1370)$.}
\endlastfoot
\label{tab:10221decaymodes}
0.438181 & $**$ & $\sigma$, $\sigma$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.150788 & $**$ & $\rho^+$, $\rho^-$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.075394 & $**$ & $\rho^0$, $\rho^0$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.052606 & $**$ & $\pi^+$, $\pi^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.050424 & $**$ & $\pi^0(1300)$, $\pi^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.050424 & $**$ & $\pi^-(1300)$, $\pi^+$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.050424 & $**$ & $\pi^+(1300)$, $\pi^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.026364 & $**$ & $K^0$, $\bar{K}^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.026364 & $**$ & $K^+$, $K^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.026303 & $**$ & $\pi^0$, $\pi^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.017091 & $**$ & $a_1^-(1260)$, $\pi^+$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.017091 & $**$ & $a_1^+(1260)$, $\pi^-$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.017091 & $**$ & $a_1^0(1260)$, $\pi^0$ & & Herwig::PScalarPScalarVector::PPVDecayer& \\ 
& & & & & \\ \hline
0.001455 & $**$ & $\eta$, $\eta$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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