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\title{\boldmath{ $J/\psi(1S)$}\ \ \ \ \ \ \ $*****$}
\maketitle
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 $\gamma gg$.
The $J/\psi(1S)$ has mass $3096.916$~MeV and is unstable. The $J/\psi(1S)$ has spin $1$, charge $0$ and is colour neutral.
 The $J/\psi(1S)$ is a meson and is from the $1^3S_1$ multiplet.The $J/\psi(1S)$ has width $0.0934$~MeV. The lower limit on the mass of the particle is $0.934$~MeV and the upper limit is $0.934$~MeV. These are the deviations from the on-shell value. The branching ratios are fixed.
The properties of the particle and its antiparticle are taken to be charge-conjugate to each other.
 The PDG code is 443.
\setlongtables
\begin{longtable}[t]{|c|c|c|p{1in}|p{2.5in}|c|}
\hline
Branching & Rating & On/ & Outgoing  & Description & Decayer  \\ 
Ratio     &                                 & Off & 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 & $***$ & on & $ g, g, g $  & Partonic decay of $J/\psi(1S)$ which is added to ensure the branching ratios sum to one.   & Herwig::Quarkonium::QDecayME130 \\ 
\hline
0.079100 & $***$ & on & $ u, \bar{u} $  & Partonic decay of $J/\psi(1S)$ with branching ratio calculated from the leptonic decays, with appropriate charge and colour factors.   & Herwig::Quarkonium::QDecayME0 \\ 
\hline
0.059350 & $*****$ & on & $ e^-, e^+ $  & The decay of the $J/\psi(1S)$ to $l^+l^-$ with branching ratio obtained by averaging the electron and muon decay from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.059350 & $*****$ & on & $ \mu^-, \mu^+ $  & The decay of the $J/\psi(1S)$ to $l^+l^-$ with branching ratio obtained by averaging the electron and muon decay from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.050000 & $***$ & on & $ g, g, \gamma $  & Partonic decay of $J/\psi(1S)$ which is added to ensure the branching ratios sum to one.   & Herwig::Quarkonium::QDecayME130 \\ 
\hline
0.019800 & $***$ & on & $ d, \bar{d} $  & Partonic decay of $J/\psi(1S)$ with branching ratio calculated from the leptonic decays, with appropriate charge and colour factors.   & Herwig::Quarkonium::QDecayME0 \\ 
\hline
0.019800 & $***$ & on & $ s, \bar{s} $  & Partonic decay of $J/\psi(1S)$ with branching ratio calculated from the leptonic decays, with appropriate charge and colour factors.   & Herwig::Quarkonium::QDecayME0 \\ 
\hline
0.013000 & $****$ & on & $ \gamma, \eta_c $  & The radiative decay of the $J/\psi(1S)$ to the $\eta_c$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.008500 & $***$ & on & $ \omega, \pi^+, \pi^-, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.005630 & $****$ & on & $ \rho^+, \pi^- $  & The decay of the $J/\psi(1S)$ to a rho meson and a pion. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.005630 & $****$ & on & $ \rho^-, \pi^+ $  & The decay of the $J/\psi(1S)$ to a rho meson and a pion. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.005630 & $****$ & on & $ \rho^0, \pi^0 $  & The decay of the $J/\psi(1S)$ to a rho meson and a pion. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.005000 & $***$ & on & $ \gamma, \pi^+, \pi^-, \pi^0, \pi^0 $  & Radiative decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\rho\rho$ mode has been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.004750 & $***$ & on & $ \omega, \pi^+, \pi^- $  & The decay of the $J/\psi(1S)$ to the omega and two pions, the branching ratio is obtained from the \cite{Yao:2006px} after subtracting the contribution of the $f_2\omega$.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.004710 & $****$ & on & $ \gamma, \eta' $  & The radiative decay of the $J/\psi(1S)$ to the $\eta'$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.004500 & $***$ & on & $ p^+, \bar{p}^-, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\Delta\Delta$ modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.004500 & $***$ & on & $ n^0, \bar{n}^0, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\Delta\Delta$ modes have been subtracted, the value for the $p\bar{p}$ mode is used which is in agreement with the measurement of the neutron mode given the large error.   & Herwig::Mambo::Mambo \\ 
\hline
0.004300 & $****$ & on & $ f_2(1270), \omega $  & The decay of the $J/\psi(1S)$ to a $f_2$ meson and a omega. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003634 & $***$ & on & $ a_2^0(1320), \rho^0 $  & The decay of the $J/\psi(1S)$ to a $a_2$ meson and a rho. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003633 & $***$ & on & $ a_2^+(1320), \rho^- $  & The decay of the $J/\psi(1S)$ to a $a_2$ meson and a rho. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003633 & $***$ & on & $ a_2^-(1320), \rho^+ $  & The decay of the $J/\psi(1S)$ to a $a_2$ meson and a rho. The branching ratio is taken from \cite{Yao:2006px} with the contributions of the different modes given by isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003600 & $***$ & on & $ \omega, \pi^+, \pi^-, \pi^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after subtracting the $\omega\eta$ mode.   & Herwig::Mambo::Mambo \\ 
\hline
0.003350 & $****$ & on & $ K^{*+}, K_2^{*-}(1430) $  & The decay of the $J/\psi(1S)$ to a $K^*_2$ and a $K^*$ with branching ratio for the neutral mode extrapolated for the charged modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003350 & $****$ & on & $ K^{*-}, K_2^{*+}(1430) $  & The decay of the $J/\psi(1S)$ to a $K^*_2$ and a $K^*$ with branching ratio for the neutral mode extrapolated for the charged modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003350 & $****$ & on & $ \bar{K}^{*0}, K_2^{*0}(1430) $  & The decay of the $J/\psi(1S)$ to a $K^*_2$ and a $K^*$ with branching ratio for the neutral mode extrapolated for the charged modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003350 & $****$ & on & $ K^{*0}, \bar{K}_2^{*0}(1430) $  & The decay of the $J/\psi(1S)$ to a $K^*_2$ and a $K^*$ with branching ratio for the neutral mode extrapolated for the charged modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003300 & $***$ & on & $ \pi^+, \pi^-, \pi^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\rho\pi$ modes have been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003100 & $***$ & on & $ \gamma, \eta, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\eta'$ and $\eta(1405)$ sub-modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.003000 & $***$ & on & $ \gamma, \rho^+, \rho^- $  & Radiative decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002800 & $***$ & on & $ \gamma, \eta(1475) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $KK\pi$ mode.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002300 & $****$ & on & $ K^+, K^{*-} $  & The decay of the $J/\psi(1S)$ to $KK^*$ the branching ratio is obtained by averaging the charged and neutral modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.002300 & $****$ & on & $ K^-, K^{*+} $  & The decay of the $J/\psi(1S)$ to $KK^*$ the branching ratio is obtained by averaging the charged and neutral modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.002300 & $****$ & on & $ \bar{K}^0, K^{*0} $  & The decay of the $J/\psi(1S)$ to $KK^*$ the branching ratio is obtained by averaging the charged and neutral modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.002300 & $****$ & on & $ K^0, \bar{K}^{*0} $  & The decay of the $J/\psi(1S)$ to $KK^*$ the branching ratio is obtained by averaging the charged and neutral modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.002300 & $***$ & on & $ p^+, \bar{p}^-, \pi^+, \pi^-, \pi^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.002170 & $****$ & on & $ p^+, \bar{p}^- $  & The decay of the $J/\psi(1S)$ to two protons. The branching ratio is obtained by averaging the \cite{Yao:2006px} proton and neutron modes assuming isospin conservation.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.002170 & $*****$ & on & $ n^0, \bar{n}^0 $  & The decay of the $J/\psi(1S)$ to two neutrons. The branching ratio is obtained by averaging the \cite{Yao:2006px} proton and neutron modes assuming isospin conservation.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.002170 & $***$ & on & $ \omega, \pi^0, \pi^0 $  & The decay of the $J/\psi(1S)$ to the omega and two pions, the branching ratio is obtained from the \cite{Yao:2006px} after subtracting the contribution of the $f_2\omega$.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002100 & $***$ & on & $ \gamma, K^+, K^-, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.002090 & $***$ & on & $ p^+, \bar{p}^-, \eta $  & The decay of the  $J/\psi(1S)$ to a proton, antiproton pair and an eta meson with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002090 & $***$ & on & $ n^0, \bar{n}^0, \eta $  & Decay of $J/\psi(1S)$ added as required by isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002040 & $***$ & on & $ p^+, \bar{n}^0, \pi^- $  & The decay of the $J/\psi(1S)$ to a proton, antineutron and a pion with branching ratio from \cite{Yao:2006px} after averaging the isospin states.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002040 & $***$ & on & $ \bar{p}^-, n^0, \pi^+ $  & The decay of the  $J/\psi(1S)$ to a proton, antineutron and a pion with branching ratio from \cite{Yao:2006px}, after averaging the isospin states.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002000 & $***$ & on & $ \gamma, K^{*+}, K^{*-} $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002000 & $***$ & on & $ \gamma, K^{*0}, \bar{K}^{*0} $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001900 & $***$ & on & $ K^+_1(1400), K^- $  & The decay of the $J/\psi(1S)$ to a $K_1$ meson and a kaon. The branching ratio is from \cite{Yao:2006px}. The neutral modes have not been observed and are included as they are required by isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001900 & $***$ & on & $ K^-_1(1400), K^+ $  & The decay of the $J/\psi(1S)$ to a $K_1$ meson and a kaon. The branching ratio is from \cite{Yao:2006px}. The neutral modes have not been observed and are included as they are required by isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001900 & $***$ & on & $ \bar{K}_1(1400)^0, K^0 $  & The decay of the $J/\psi(1S)$ to a $K_1$ meson and a kaon. The branching ratio is from \cite{Yao:2006px}. The neutral modes have not been observed and are included as they are required by isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001900 & $***$ & on & $ K^0_1(1400), \bar{K}^0 $  & The decay of the $J/\psi(1S)$ to a $K_1$ meson and a kaon. The branching ratio is from \cite{Yao:2006px}. The neutral modes have not been observed and are included as they are required by isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001740 & $****$ & on & $ \omega, \eta $  & The decay of the $J/\psi(1S)$ to the omega and an eta with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.001660 & $***$ & on & $ \phi, \pi^+, \pi^-, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.001620 & $****$ & on & $ b_1^+, \pi^- $  & The decay of the $J/\psi(1S)$ to a $b_1$ meson and a pion. The branching ratio is obtained by averaging the branching ratios from the neutral and charged modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001620 & $****$ & on & $ b_1^-, \pi^+ $  & The decay of the $J/\psi(1S)$ to a $b_1$ meson and a pion. The branching ratio is obtained by averaging the branching ratios from the neutral and charged modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001620 & $****$ & on & $ b_1^0, \pi^0 $  & The decay of the $J/\psi(1S)$ to a $b_1$ meson and a pion. The branching ratio is obtained by averaging the branching ratios from the neutral and charged modes from \cite{Yao:2006px} using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001600 & $***$ & on & $ \gamma, \eta, \pi^0, \pi^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} after the $\eta'$ and $\eta(1405)$ sub-modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.001590 & $***$ & on & $ \gamma, \omega, \omega $  & Radiative decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001540 & $****$ & on & $ \Lambda^0, \bar{\Lambda}^0 $  & The decay of the $J/\psi(1S)$ to two $\Lambda$'s with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.001500 & $***$ & on & $ \gamma, \rho^0, \rho^0 $  & Radiative decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001470 & $****$ & on & $ \pi^+, \pi^- $  & The decay of the $J/\psi(1S)$ to two pions with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.001380 & $****$ & on & $ \gamma, f_2(1270) $  & The radiative decay of the $J/\psi(1S)$ to the $f_2$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001340 & $***$ & on & $ \gamma, f_0(1710) $  & Radiative decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} using our $f_0(1710)$ branching ratios as the \cite{Yao:2006px} number is only for the kaon decay mode of the $f_0(1710)$.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.001325 & $***$ & on & $ \omega, K^{*+}, K^- $  & The decay of the $J/\psi(1S)$ to an omega, a $K^*$ and a kaon. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001325 & $***$ & on & $ \omega, K^{*-}, K^+ $  & The decay of the $J/\psi(1S)$ to an omega, a $K^*$ and a kaon. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001325 & $***$ & on & $ \omega, \bar{K}^{*0}, K^0 $  & The decay of the $J/\psi(1S)$ to an omega, a $K^*$ and a kaon. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001325 & $***$ & on & $ \omega, K^{*0}, \bar{K}^0 $  & The decay of the $J/\psi(1S)$ to an omega, a $K^*$ and a kaon. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001310 & $****$ & on & $ \Sigma^+, \bar{\Sigma}^- $  & The decay of the $J/\psi(1S)$ to $\Sigma\bar{\Sigma}$. The branching ratio is measured for the neutral mode and extrapolated for hte charged modes using isospin   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.001310 & $****$ & on & $ \Sigma^0, \bar{\Sigma}^0 $  & The decay of the $J/\psi(1S)$ to $\Sigma\bar{\Sigma}$. The branching ratio is measured for the neutral mode and extrapolated for hte charged modes using isospin   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.001310 & $****$ & on & $ \Sigma^-, \bar{\Sigma}^+ $  & The decay of the $J/\psi(1S)$ to $\Sigma\bar{\Sigma}$. The branching ratio is measured for the neutral mode and extrapolated for hte charged modes using isospin   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.001300 & $***$ & on & $ p^+, \bar{p}^-, \omega $  & The decay of the $J/\psi(1S)$ to an pmega and a proton-antiproton pair. The branching ratio is taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001300 & $***$ & on & $ n^0, \bar{n}^0, \omega $  & Decay of $J/\psi(1S)$ added as required by isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001100 & $***$ & on & $ \Delta^{+\,+}, \bar{\Delta}^{-\,-} $  & The decay of the $J/\psi(1S)$ to the $\Delta\bar{\Delta}$ the branching ratio is obtained from the doubly charged mode and the neutral mode is infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001100 & $***$ & on & $ \Delta^+, \bar{\Delta}^- $  & The decay of the $J/\psi(1S)$ to the $\Delta\bar{\Delta}$ the branching ratio is obtained from the doubly charged mode and the neutral mode is infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001100 & $***$ & on & $ \Delta^0, \bar{\Delta}^0 $  & The decay of the $J/\psi(1S)$ to the $\Delta\bar{\Delta}$ the branching ratio is obtained from the doubly charged mode and the neutral mode is infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001100 & $***$ & on & $ \Delta^-, \bar{\Delta}^+ $  & The decay of the $J/\psi(1S)$ to the $\Delta\bar{\Delta}$ the branching ratio is obtained from the doubly charged mode and the neutral mode is infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ \bar{p}^-, p^+, \pi^0 $  & The decay of the  $J/\psi(1S)$ to a proton, antiproton and a pion with branching ratio from \cite{Yao:2006px} after averaging the isospin states.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ n^0, \bar{n}^0, \pi^0 $  & The decay of the  $J/\psi(1S)$ to a neutron, antineutron and a pion. This mode has not been observed but is required by isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ p^+, \bar{K}^0, \bar{\Sigma}^{*-} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ \bar{p}^-, K^0, \Sigma^{*+} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ \bar{n}^0, K^+, \Sigma^{*-} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001020 & $***$ & on & $ n^0, K^-, \bar{\Sigma}^{*+} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001000 & $***$ & on & $ \gamma, \pi^+, \pi^-, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$  with branching ratio from \cite{Yao:2006px} after the $\gamma\rho^0\rho^0$ contribution has benn subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.000980 & $****$ & on & $ \gamma, \eta $  & The radiative decay of the $J/\psi(1S)$ to the $\eta$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000950 & $***$ & on & $ \gamma, f_2(1270), f_2(1270) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000900 & $****$ & on & $ \Xi^0, \bar{\Xi}^0 $  & The decay of the  $J/\psi(1S)$ to $\Xi\bar{\Xi}$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000900 & $****$ & on & $ \Xi^-, \bar{\Xi}^+ $  & The decay of the  $J/\psi(1S)$ to $\Xi\bar{\Xi}$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000900 & $***$ & on & $ \eta', p^+, \bar{p}^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron mode infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000900 & $***$ & on & $ \eta', n^0, \bar{n}^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron mode infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000890 & $***$ & on & $ p^+, K^-, \bar{\Lambda}^0 $  & Decay of $J/\psi(1S)$ to a nucleon, a kaon and a lambda. The proton antilambda mode has been observed and the rest are inferred.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000890 & $***$ & on & $ \bar{p}^-, K^+, \Lambda^0 $  & Decay of $J/\psi(1S)$ to a nucleon, a kaon and a lambda. The proton antilambda mode has been observed and the rest are inferred.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000890 & $***$ & on & $ \bar{n}^0, K^0, \Lambda^0 $  & Decay of $J/\psi(1S)$ to a nucleon, a kaon and a lambda. The proton antilambda mode has been observed and the rest are inferred.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000890 & $***$ & on & $ n^0, \bar{K}^0, \bar{\Lambda}^0 $  & Decay of $J/\psi(1S)$ to a nucleon, a kaon and a lambda. The proton antilambda mode has been observed and the rest are inferred.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000800 & $***$ & on & $ \phi, f'_2(1525) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000790 & $***$ & on & $ \gamma, f_1(1420) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $KK\pi$ mode which virtually saturates the $f_1(1420)$ width.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000780 & $***$ & on & $ \phi, \pi^+, \pi^- $  & Decay of $J/\psi(1S)$ with branching ratio ifrom \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000760 & $****$ & on & $ f_0(1710), \omega $  & The decay of the $J/\psi(1S)$ to the $f_1(1710)$ and the omega. The branching ratio is obtained from the rate in \cite{Yao:2006px} for the mode where the $f_1(1710)$ decays to kaons and our branching ratios for the $f_1(1710)$.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000740 & $****$ & on & $ \phi, \eta $  & The decay of the $J/\psi(1S)$ to the phi and an $\eta$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000740 & $***$ & on & $ \phi, K^0, \bar{K}^0 $  & The decay of the $J/\psi(1S)$ to the phi and two kaons. The branching ratio is from \cite{Yao:2006px} after the $f_1(1710)$ component has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000740 & $***$ & on & $ \phi, K^+, K^- $  & The decay of the $J/\psi(1S)$ to the phi and two kaons. The branching ratio is from \cite{Yao:2006px} after the $f_1(1710)$ component has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000710 & $***$ & on & $ \omega, K^+, K^- $  & The decay of the $J/\psi(1S)$ to the omega and two kaons. The branching ratio is from \cite{Yao:2006px} after the $f_1(1710)$ component has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000710 & $***$ & on & $ \omega, K^0, \bar{K}^0 $  & The decay of the $J/\psi(1S)$ to the omega and two kaons. The branching ratio is from \cite{Yao:2006px} after the $f_1(1710)$ component has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000680 & $***$ & on & $ \omega, f_1(1420) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000610 & $***$ & on & $ \gamma, f_1(1285) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000580 & $***$ & on & $ p^+, \bar{K}^0, \bar{\Sigma}^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000580 & $***$ & on & $ \bar{p}^-, K^0, \Sigma^+ $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000580 & $***$ & on & $ \bar{n}^0, K^+, \Sigma^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000580 & $***$ & on & $ n^0, K^-, \bar{\Sigma}^+ $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000570 & $****$ & on & $ f_0(1710), \phi $  & The decay of the $J/\psi(1S)$ to the $f_1(1710)$ and the phi. The branching ratio is obtained from the rate in \cite{Yao:2006px} for the mode where the $f_1(1710)$ decays to kaons and our branching ratios for the $f_1(1710)$.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000570 & $***$ & on & $ \gamma, f_0(1500) $  & Decay of $J/\psi(1S)$ with branching ratio set to the lower limit from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000530 & $***$ & on & $ \Sigma^-, \pi^+, \bar{\Lambda}^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000530 & $***$ & on & $ \Sigma^0, \pi^0, \bar{\Lambda}^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000530 & $***$ & on & $ \Sigma^+, \pi^-, \bar{\Lambda}^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000530 & $***$ & on & $ \bar{\Sigma}^-, \pi^+, \Lambda^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000530 & $***$ & on & $ \bar{\Sigma}^0, \pi^0, \Lambda^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000530 & $***$ & on & $ \bar{\Sigma}^+, \pi^-, \Lambda^0 $  & Decay of $J/\psi(1S)$ to $\Sigma\Lambda\pi$. The branching ratio for the $\bar{\Sigma}^\pm\pi^\mp\Lambda$ mode is from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000515 & $****$ & on & $ \Sigma^{*0}, \bar{\Sigma}^{*0} $  & The decay of the $J/\psi(1S)$ to the $\Sigma^*\bar{\Sigma}^*$ the branching ratio is obtained from the charged mode and the neutral mode is infered usign isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000515 & $****$ & on & $ \Sigma^{*+}, \bar{\Sigma}^{*-} $  & The decay of the $J/\psi(1S)$ to the $\Sigma^*\bar{\Sigma}^*$ the branching ratio is obtained from the charged mode and the neutral mode is infered usign isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000515 & $****$ & on & $ \Sigma^{*-}, \bar{\Sigma}^{*+} $  & The decay of the $J/\psi(1S)$ to the $\Sigma^*\bar{\Sigma}^*$ the branching ratio is obtained from the charged mode and the neutral mode is infered usign isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ K^0, \bar{K}^{*0}, \phi $  & The decay of the $J/\psi(1S)$ to $KK^*$ and a phi the branching ratio is from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ \bar{K}^0, K^{*0}, \phi $  & The decay of the $J/\psi(1S)$ to $KK^*$ and a phi the branching ratio is from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ K^-, K^{*+}, \phi $  & The decay of the $J/\psi(1S)$ to $KK^*$ and a phi the branching ratio is from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ K^+, K^{*-}, \phi $  & The decay of the $J/\psi(1S)$ to $KK^*$ and a phi the branching ratio is from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ p^+, K^-, \bar{\Sigma}^{*0} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ \bar{p}^-, K^+, \Sigma^{*0} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ \bar{n}^0, K^0, \Sigma^{*0} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000510 & $***$ & on & $ n^0, \bar{K}^0, \bar{\Sigma}^{*0} $  & Decay of $J/\psi(1S)$ to nucleon, kaon and $\Sigma^*$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^{*0}$ mode. The remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000450 & $****$ & on & $ \omega, \pi^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000450 & $***$ & on & $ \gamma, f'_2(1525) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000450 & $***$ & on & $ \gamma, \eta(1405) $  & Decay of $J/\psi(1S)$ with branching ratio calculated from the $\eta\pi^+\pi^-$ contribution in \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000446 & $****$ & on & $ \Xi^{*0}, \bar{\Xi}^0 $  & The decay of $J/\psi(1S)$ to $\Xi^*\Xi$. The branching ratio was obtained by averaging the two observed modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000446 & $****$ & on & $ \Xi^{*-}, \bar{\Xi}^+ $  & The decay of $J/\psi(1S)$ to $\Xi^*\Xi$. The branching ratio was obtained by averaging the two observed modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000446 & $****$ & on & $ \bar{\Xi}^{*+}, \Xi^- $  & The decay of $J/\psi(1S)$ to $\Xi^*\Xi$. The branching ratio was obtained by averaging the two observed modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000446 & $****$ & on & $ \bar{\Xi}^{*0}, \Xi^0 $  & The decay of $J/\psi(1S)$ to $\Xi^*\Xi$. The branching ratio was obtained by averaging the two observed modes using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000400 & $***$ & on & $ \gamma, \phi, \phi $  & Decay of $J/\psi(1S)$  with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000400 & $****$ & on & $ \phi, \eta' $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000380 & $***$ & on & $ \gamma, p^+, \bar{p}^- $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron mode infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000380 & $***$ & on & $ \gamma, n^0, \bar{n}^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron mode infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000320 & $****$ & on & $ \phi, f_0(980) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000290 & $***$ & on & $ p^+, K^-, \bar{\Sigma}^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000290 & $***$ & on & $ \bar{p}^-, K^+, \Sigma^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000290 & $***$ & on & $ n^0, \bar{K}^0, \bar{\Sigma}^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000290 & $***$ & on & $ \bar{n}^0, K^0, \Sigma^0 $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px} for the $pK^-\bar{\Sigma}^0$ mode and the others infered from isospin conservation   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000260 & $***$ & on & $ \phi, f_1(1285) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000237 & $****$ & on & $ K^-, K^+ $  & Decay of $J/\psi(1S)$ to two kaons with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.000220 & $***$ & on & $ \Lambda^0, \bar{\Lambda}^0, \pi^0 $  & Decay of $J/\psi(1S)$ to two lambdas with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000193 & $****$ & on & $ \rho^0, \eta $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000182 & $****$ & on & $ \omega, \eta' $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000155 & $***$ & on & $ \Sigma^{*+}, \bar{\Sigma}^- $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000155 & $***$ & on & $ \Sigma^{*0}, \bar{\Sigma}^0 $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000155 & $***$ & on & $ \Sigma^{*-}, \bar{\Sigma}^+ $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000155 & $***$ & on & $ \bar{\Sigma}^{*+}, \Sigma^- $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000155 & $***$ & on & $ \bar{\Sigma}^{*0}, \Sigma^0 $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000155 & $***$ & on & $ \bar{\Sigma}^{*-}, \Sigma^+ $  & The charged mode has been obsereved and has branching ratio from \cite{Yao:2006px}. The other modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000146 & $****$ & on & $ K^0_L, K^0_S $  & Decay of $J/\psi(1S)$ to two kaons with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.000140 & $****$ & on & $ \omega, f_0(980) $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000105 & $****$ & on & $ \rho^0, \eta' $  & Decay of $J/\psi(1S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000045 & $***$ & on & $ \phi, p^+, \bar{p}^- $  & Decay of $J/\psi(1S)$ to a $\phi$ and two nucelons. The proton mode has been observed with the branching ratio from \cite{Yao:2006px}. The neutron mode is inferred using isospin/   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000045 & $***$ & on & $ \phi, n^0, \bar{n}^0 $  & Decay of $J/\psi(1S)$ to a $\phi$ and two nucelons. The proton mode has been observed with the branching ratio from \cite{Yao:2006px}. The neutron mode is inferred using isospin/   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000033 & $****$ & on & $ \gamma, \pi^0 $  & Decay of $J/\psi(1S)$  with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
\end{longtable}The $J/\psi(1S)$ decay modes are given in Table~\ref{tab:443decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|jpsimass| for the $J/\psi(1S)$.
The width generator is \verb|jpsiwidth| for the $J/\psi(1S)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 16:18:15 on the 15th of May 2008. The most recently changed decay mode was modified at 19:14:56 on the 10th of May 2008. The particle data was last modified at 9:25:33 on the 16th of August 2007.

\end{document}
