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\begin{document}
\title{Check List for Particle : \boldmath{ $\chi_{c0}(1P)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &10441 & & & Mass & 3414.76& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 10.4& & & Gen  & \verb: chi_c0: & &\\ 
       & & & & 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  & $\chi_{c0}(1P) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:chi_c0mass: \ \ & Width Gen.  & \verb:chi_c01Pwidth: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $0$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 104& Upper cut & 104& PDG link &m056 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $\chi_{c0}(1P)$ is the lightest scalar $c\bar{c}$ state. The mass and width are measured and are taken from \cite{Yao:2006px}. The branching ratios for a number of modes are measured however the sum of the measured modes is insufficient to saturate the total width and therefore the remainder is modelled using parton modes. The $\chi_{c0}(1P)$ is allowed to be off-shell by ten times the width.
\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 $\chi_{c0}(1P)$ (continues).}
\endfoot
\caption{The decay modes of the $\chi_{c0}(1P)$.}
\endlastfoot
\label{tab:10441decaymodes}
0.788568 & $***$ & $g$, $g$ & & Herwig::Quarkonium::QDecayME0& \\ 
& & & & & \\ \hline
0.026000 & $***$ & $f_0(1370)$, $f_0(1710)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.016000 & $****$ & $\rho^-$, $\pi^+$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.016000 & $****$ & $\rho^+$, $\pi^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.016000 & $****$ & $\rho^0$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.013000 & $****$ & $J/\psi(1S)$, $\gamma$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.010000 & $****$ & $\bar{K}_1(1270)^0$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.010000 & $****$ & $K_1^0(1270)$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.010000 & $****$ & $K_1^-(1270)$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.010000 & $****$ & $K_1^+(1270)$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.007390 & $***$ & $\pi^-$, $\pi^+$, $\pi^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.005400 & $****$ & $K^0$, $\bar{K}^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.005400 & $****$ & $K^+$, $K^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.004800 & $****$ & $\pi^+$, $\pi^-$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.004400 & $***$ & $K^0$, $K^{*-}$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004400 & $***$ & $\bar{K}^0$, $K^{*+}$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004400 & $****$ & $K^-$, $K^{*0}$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004400 & $****$ & $K^+$, $\bar{K}^{*0}$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002770 & $***$ & $\pi^+$, $\pi^-$, $K^+$, $K^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002400 & $****$ & $\pi^0$, $\pi^0$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.002363 & $***$ & $K^{*0}_0(1430)$, $\bar{K}^{*0}_0(1430)$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.002363 & $***$ & $K^{*+}_0(1430)$, $K^{*-}_0(1430)$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.002300 & $***$ & $\omega$, $\omega$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.002200 & $***$ & $K^{*-}$, $K^+$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002200 & $***$ & $K^{*+}$, $K^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002200 & $***$ & $K^{*0}$, $\bar{K}^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002200 & $***$ & $\bar{K}^{*0}$, $K^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002150 & $***$ & $f_0(980)$, $f_0(980)$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.002100 & $***$ & $K^+$, $K^-$, $K^+$, $K^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001912 & $***$ & $K^{*+}_0(1430)$, $K_2^{*-}(1430)$ & & Herwig::ScalarMesonTensorScalar::STSDecayer& \\ 
& & & & & \\ \hline
0.001912 & $***$ & $K^{*-}_0(1430)$, $K_2^{*+}(1430)$ & & Herwig::ScalarMesonTensorScalar::STSDecayer& \\ 
& & & & & \\ \hline
0.001912 & $***$ & $K^{*0}_0(1430)$, $\bar{K}_2^{*0}(1430)$ & & Herwig::ScalarMesonTensorScalar::STSDecayer& \\ 
& & & & & \\ \hline
0.001912 & $***$ & $\bar{K}^{*0}_0(1430)$, $K_2^{*0}(1430)$ & & Herwig::ScalarMesonTensorScalar::STSDecayer& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $\pi^+$, $\pi^-$, $p^+$, $\bar{p}^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $\eta$, $\eta$ & & Herwig::ScalarScalarScalar::ScalarSS& \\ 
& & & & & \\ \hline
0.001800 & $****$ & $K^{*+}$, $K^{*-}$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.001800 & $****$ & $K^{*0}$, $\bar{K}^{*0}$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.001500 & $***$ & $K^+$, $K^-$, $K^0_S$, $K^0_S$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000900 & $****$ & $\phi$, $\phi$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.000440 & $***$ & $\Lambda^0$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000276 & $****$ & $\gamma$, $\gamma$ & & Herwig::ScalarVectorVector::SVV& \\ 
& & & & & \\ \hline
0.000216 & $***$ & $p^+$, $\bar{p}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000216 & $***$ & $n^0$, $\bar{n}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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