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\begin{document}
\title{Check List for Particle : \boldmath{ $J/\psi(1S)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &443 & & & Mass & 3096.916& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0.0934& & & Gen  & \verb: Jpsi: & &\\ 
       & & & & 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  & $J/\psi(1S) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:jpsimass: \ \ & Width Gen.  & \verb:jpsiwidth: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$*****$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 0.934& Upper cut & 0.934& PDG link &m070 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $J/\psi(1S)$ is the lightest vector $c\bar{c}$ state. The mass and width are accurately measured and our values are taken from \cite{Yao:2006px}. A large number of decay modes have been observed and the branching ratios measured, however these modes are not sufficient to account for all the $J/\psi(1S)$ decays and we are forced to rely on partonic decays for the rest. Most of the two body modes from \cite{Yao:2006px} have been included, apart from some modes to resonances we do not include or for which the properties are poorly known. Most of the higher multiplicity modes are also included apart from some modes with large numbers of pions and kaons which we expect to be produced by the hadronization of the partonic modes and decays of intermediate resonances.

The branching ratios for partonic modes are assumed to be $\Gamma(\gamma gg) = 0.11\Gamma(\gamma gg)$ which gives about 7\% branching ratio to $\gamma gg$.
\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 $J/\psi(1S)$ (continues).}
\endfoot
\caption{The decay modes of the $J/\psi(1S)$.}
\endlastfoot
\label{tab:443decaymodes}
0.486225 & $***$ & $g$, $g$, $g$ & & Herwig::Quarkonium::QDecayME130& \\ 
& & & & & \\ \hline
0.079100 & $***$ & $u$, $\bar{u}$ & & Herwig::Quarkonium::QDecayME0& \\ 
& & & & & \\ \hline
0.059350 & $*****$ & $e^-$, $e^+$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.059350 & $*****$ & $\mu^-$, $\mu^+$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.050000 & $***$ & $g$, $g$, $\gamma$ & & Herwig::Quarkonium::QDecayME130& \\ 
& & & & & \\ \hline
0.019800 & $***$ & $s$, $\bar{s}$ & & Herwig::Quarkonium::QDecayME0& \\ 
& & & & & \\ \hline
0.019800 & $***$ & $d$, $\bar{d}$ & & Herwig::Quarkonium::QDecayME0& \\ 
& & & & & \\ \hline
0.013000 & $****$ & $\gamma$, $\eta_c$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.008500 & $***$ & $\omega$, $\pi^+$, $\pi^-$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.005630 & $****$ & $\rho^0$, $\pi^0$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.005630 & $****$ & $\rho^+$, $\pi^-$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.005630 & $****$ & $\rho^-$, $\pi^+$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.005000 & $***$ & $\gamma$, $\pi^+$, $\pi^-$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.004750 & $***$ & $\omega$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004710 & $****$ & $\gamma$, $\eta'$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.004500 & $***$ & $n^0$, $\bar{n}^0$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.004500 & $***$ & $p^+$, $\bar{p}^-$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.004300 & $****$ & $f_2(1270)$, $\omega$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003634 & $***$ & $a_2^0(1320)$, $\rho^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003633 & $***$ & $a_2^-(1320)$, $\rho^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003633 & $***$ & $a_2^+(1320)$, $\rho^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003600 & $***$ & $\omega$, $\pi^+$, $\pi^-$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.003350 & $****$ & $K^{*0}$, $\bar{K}_2^{*0}(1430)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003350 & $****$ & $K^{*-}$, $K_2^{*+}(1430)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003350 & $****$ & $\bar{K}^{*0}$, $K_2^{*0}(1430)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003350 & $****$ & $K^{*+}$, $K_2^{*-}(1430)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003300 & $***$ & $\pi^+$, $\pi^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003100 & $***$ & $\gamma$, $\eta$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.003000 & $***$ & $\gamma$, $\rho^+$, $\rho^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002800 & $***$ & $\gamma$, $\eta(1475)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002300 & $***$ & $p^+$, $\bar{p}^-$, $\pi^+$, $\pi^-$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002300 & $****$ & $K^0$, $\bar{K}^{*0}$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.002300 & $****$ & $\bar{K}^0$, $K^{*0}$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.002300 & $****$ & $K^+$, $K^{*-}$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.002300 & $****$ & $K^-$, $K^{*+}$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.002170 & $****$ & $p^+$, $\bar{p}^-$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.002170 & $***$ & $\omega$, $\pi^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002170 & $*****$ & $n^0$, $\bar{n}^0$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.002100 & $***$ & $\gamma$, $K^+$, $K^-$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002090 & $***$ & $n^0$, $\bar{n}^0$, $\eta$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002090 & $***$ & $p^+$, $\bar{p}^-$, $\eta$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002040 & $***$ & $\bar{p}^-$, $n^0$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002040 & $***$ & $p^+$, $\bar{n}^0$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002000 & $***$ & $\gamma$, $K^{*0}$, $\bar{K}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002000 & $***$ & $\gamma$, $K^{*+}$, $K^{*-}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $K^+_1(1400)$, $K^-$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $K^-_1(1400)$, $K^+$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $\bar{K}_1(1400)^0$, $K^0$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001900 & $***$ & $K^0_1(1400)$, $\bar{K}^0$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001740 & $****$ & $\omega$, $\eta$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.001660 & $***$ & $\phi$, $\pi^+$, $\pi^-$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001620 & $****$ & $b_1^0$, $\pi^0$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001620 & $****$ & $b_1^+$, $\pi^-$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001620 & $****$ & $b_1^-$, $\pi^+$ & & Herwig::VectorMesonPVectorPScalar::VAPDecayer& \\ 
& & & & & \\ \hline
0.001600 & $***$ & $\gamma$, $\eta$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001590 & $***$ & $\gamma$, $\omega$, $\omega$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001540 & $****$ & $\Lambda^0$, $\bar{\Lambda}^0$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.001500 & $***$ & $\gamma$, $\rho^0$, $\rho^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001470 & $****$ & $\pi^+$, $\pi^-$ & & Herwig::VectorMeson2Meson::Vector2Meson& \\ 
& & & & & \\ \hline
0.001380 & $****$ & $\gamma$, $f_2(1270)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001340 & $***$ & $\gamma$, $f_0(1710)$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.001325 & $***$ & $\omega$, $K^{*0}$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001325 & $***$ & $\omega$, $\bar{K}^{*0}$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001325 & $***$ & $\omega$, $K^{*-}$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001325 & $***$ & $\omega$, $K^{*+}$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001310 & $****$ & $\Sigma^+$, $\bar{\Sigma}^-$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.001310 & $****$ & $\Sigma^0$, $\bar{\Sigma}^0$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.001310 & $****$ & $\Sigma^-$, $\bar{\Sigma}^+$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.001300 & $***$ & $n^0$, $\bar{n}^0$, $\omega$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001300 & $***$ & $p^+$, $\bar{p}^-$, $\omega$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001100 & $***$ & $\Delta^-$, $\bar{\Delta}^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001100 & $***$ & $\Delta^{+\,+}$, $\bar{\Delta}^{-\,-}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001100 & $***$ & $\Delta^0$, $\bar{\Delta}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001100 & $***$ & $\Delta^+$, $\bar{\Delta}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $\bar{p}^-$, $K^0$, $\Sigma^{*+}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $\bar{n}^0$, $K^+$, $\Sigma^{*-}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $p^+$, $\bar{K}^0$, $\bar{\Sigma}^{*-}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $n^0$, $\bar{n}^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $n^0$, $K^-$, $\bar{\Sigma}^{*+}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001020 & $***$ & $\bar{p}^-$, $p^+$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001000 & $***$ & $\gamma$, $\pi^+$, $\pi^-$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000980 & $****$ & $\gamma$, $\eta$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000950 & $***$ & $\gamma$, $f_2(1270)$, $f_2(1270)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000900 & $***$ & $\eta'$, $n^0$, $\bar{n}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000900 & $***$ & $\eta'$, $p^+$, $\bar{p}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000900 & $****$ & $\Xi^0$, $\bar{\Xi}^0$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.000900 & $****$ & $\Xi^-$, $\bar{\Xi}^+$ & & Herwig::VectorMeson2Fermion::Vector2Leptons& \\ 
& & & & & \\ \hline
0.000890 & $***$ & $p^+$, $K^-$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000890 & $***$ & $\bar{p}^-$, $K^+$, $\Lambda^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000890 & $***$ & $n^0$, $\bar{K}^0$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000890 & $***$ & $\bar{n}^0$, $K^0$, $\Lambda^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000800 & $***$ & $\phi$, $f'_2(1525)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000790 & $***$ & $\gamma$, $f_1(1420)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000780 & $***$ & $\phi$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000760 & $****$ & $f_0(1710)$, $\omega$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.000740 & $****$ & $\phi$, $\eta$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000740 & $***$ & $\phi$, $K^0$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000740 & $***$ & $\phi$, $K^+$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000710 & $***$ & $\omega$, $K^0$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000710 & $***$ & $\omega$, $K^+$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000680 & $***$ & $\omega$, $f_1(1420)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000610 & $***$ & $\gamma$, $f_1(1285)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000580 & $***$ & $p^+$, $\bar{K}^0$, $\bar{\Sigma}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000580 & $***$ & $\bar{n}^0$, $K^+$, $\Sigma^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000580 & $***$ & $n^0$, $K^-$, $\bar{\Sigma}^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000580 & $***$ & $\bar{p}^-$, $K^0$, $\Sigma^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000570 & $***$ & $\gamma$, $f_0(1500)$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.000570 & $****$ & $f_0(1710)$, $\phi$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\bar{\Sigma}^0$, $\pi^0$, $\Lambda^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\bar{\Sigma}^+$, $\pi^-$, $\Lambda^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\bar{\Sigma}^-$, $\pi^+$, $\Lambda^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\Sigma^+$, $\pi^-$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\Sigma^0$, $\pi^0$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000530 & $***$ & $\Sigma^-$, $\pi^+$, $\bar{\Lambda}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000515 & $****$ & $\Sigma^{*0}$, $\bar{\Sigma}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000515 & $****$ & $\Sigma^{*+}$, $\bar{\Sigma}^{*-}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000515 & $****$ & $\Sigma^{*-}$, $\bar{\Sigma}^{*+}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $\bar{p}^-$, $K^+$, $\Sigma^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $\bar{K}^0$, $K^{*0}$, $\phi$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $n^0$, $\bar{K}^0$, $\bar{\Sigma}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $K^-$, $K^{*+}$, $\phi$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $K^+$, $K^{*-}$, $\phi$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $p^+$, $K^-$, $\bar{\Sigma}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $\bar{n}^0$, $K^0$, $\Sigma^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000510 & $***$ & $K^0$, $\bar{K}^{*0}$, $\phi$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000450 & $***$ & $\gamma$, $\eta(1405)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000450 & $***$ & $\gamma$, $f'_2(1525)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000450 & $****$ & $\omega$, $\pi^0$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000446 & $****$ & $\Xi^{*0}$, $\bar{\Xi}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000446 & $****$ & $\bar{\Xi}^{*+}$, $\Xi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000446 & $****$ & $\bar{\Xi}^{*0}$, $\Xi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000446 & $****$ & $\Xi^{*-}$, $\bar{\Xi}^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000400 & $****$ & $\phi$, $\eta'$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000400 & $***$ & $\gamma$, $\phi$, $\phi$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000380 & $***$ & $\gamma$, $p^+$, $\bar{p}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000380 & $***$ & $\gamma$, $n^0$, $\bar{n}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000320 & $****$ & $\phi$, $f_0(980)$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.000290 & $***$ & $\bar{n}^0$, $K^0$, $\Sigma^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000290 & $***$ & $n^0$, $\bar{K}^0$, $\bar{\Sigma}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000290 & $***$ & $\bar{p}^-$, $K^+$, $\Sigma^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000290 & $***$ & $p^+$, $K^-$, $\bar{\Sigma}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000260 & $***$ & $\phi$, $f_1(1285)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000237 & $****$ & $K^-$, $K^+$ & & Herwig::VectorMeson2Meson::Vector2Meson& \\ 
& & & & & \\ \hline
0.000220 & $***$ & $\Lambda^0$, $\bar{\Lambda}^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000193 & $****$ & $\rho^0$, $\eta$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000182 & $****$ & $\omega$, $\eta'$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\bar{\Sigma}^{*+}$, $\Sigma^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\Sigma^{*+}$, $\bar{\Sigma}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\Sigma^{*0}$, $\bar{\Sigma}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\Sigma^{*-}$, $\bar{\Sigma}^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\bar{\Sigma}^{*-}$, $\Sigma^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000155 & $***$ & $\bar{\Sigma}^{*0}$, $\Sigma^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000146 & $****$ & $K^0_L$, $K^0_S$ & & Herwig::VectorMeson2Meson::Vector2Meson& \\ 
& & & & & \\ \hline
0.000140 & $****$ & $\omega$, $f_0(980)$ & & Herwig::VectorMesonVectorScalar::VVSDecayer& \\ 
& & & & & \\ \hline
0.000105 & $****$ & $\rho^0$, $\eta'$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
0.000045 & $***$ & $\phi$, $p^+$, $\bar{p}^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000045 & $***$ & $\phi$, $n^0$, $\bar{n}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000033 & $****$ & $\gamma$, $\pi^0$ & & Herwig::VectorMesonVectorPScalar::VectorVP& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
