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\title{\boldmath{ $\psi(2S)$}\ \ \ \ \ \ \ $*****$}
\maketitle
The $\psi(2S)$ is the second vector $c\bar{c}$ state. The mass and width are measured and are taken from \cite{Yao:2006px}. A number of decay modes have been measured although there are not enough to saturate the total width. The remainder is modelled as a partonic decay. The $\psi(2S)$ is allowed to be off-shell by ten times the width.
The $\psi(2S)$ has mass $3686.093$~MeV and is unstable. The $\psi(2S)$ has spin $1$, charge $0$ and is colour neutral.
 The $\psi(2S)$ is a meson and is from the $2^3S_1$ multiplet.The $\psi(2S)$ has width $0.337$~MeV. The lower limit on the mass of the particle is $3.37$~MeV and the upper limit is $3.37$~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 100443.
\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 $\psi(2S)$ (continues).}
\endfoot
\caption{The decay modes of the $\psi(2S)$.}
\endlastfoot
\label{tab:100443decaymodes}
0.318000 & $*****$ & on & $ J/\psi(1S), \pi^+, \pi^- $  & The decay of $\psi(2S)$ to the $J/\psi$ and two pions with branching ratio taken from \cite{Yao:2006px}.   & Herwig::OniumToOniumPiPi::OniumPiPi \\ 
\hline
0.183208 & $***$ & on & $ g, g, g $  & Partonic decay of $\psi(2S)$ which is included to ensure the branching ratios sum to unity.   & Herwig::Quarkonium::QDecayME130 \\ 
\hline
0.164600 & $*****$ & on & $ J/\psi(1S), \pi^0, \pi^0 $  & The decay of $\psi(2S)$ to the $J/\psi$ and two pions with branching ratio taken from \cite{Yao:2006px}.   & Herwig::OniumToOniumPiPi::OniumPiPi \\ 
\hline
0.092000 & $*****$ & on & $ \chi_{c0}(1P), \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.087000 & $*****$ & on & $ \chi_{c1}(1P), \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.081000 & $*****$ & on & $ \chi_{c2}(1P), \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.030900 & $*****$ & on & $ J/\psi(1S), \eta $  & The decay of $\psi(2S)$ to the $J/\psi$ and an eta with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.007350 & $*****$ & on & $ e^-, e^+ $  & The decay of the $\psi(2S)$ to an $l^+l^-$ pair. The branching ratio was obtained by averaging the branching ratios from \cite{Yao:2006px} using the decayer to give the correct phase-space effects.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.007340 & $*****$ & on & $ \mu^-, \mu^+ $  & The decay of the $\psi(2S)$ to an $l^+l^-$ pair. The branching ratio was obtained by averaging the branching ratios from \cite{Yao:2006px} using the decayer to give the correct phase-space effects.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.002850 & $*****$ & on & $ \tau^-, \tau^+ $  & The decay of the $\psi(2S)$ to an $l^+l^-$ pair. The branching ratio was obtained by averaging the branching ratios from \cite{Yao:2006px} using the decayer to give the correct phase-space effects.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.002600 & $****$ & on & $ \eta_c, \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.001260 & $****$ & on & $ J/\psi(1S), \pi^0 $  & The decay of $\psi(2S)$ to the $J/\psi$ and a pion with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.001000 & $***$ & on & $ h_c, \pi^0 $  & Decay of the $\psi(2S)$ to an with branching ratio calculated using the product $\mathcal{B}(\psi(2S)\to\pi^0h_c)\times\mathcal{B}(h_c\to\gamma\eta_c)$ from \cite{Rosner:2005ry}  and our value of $\mathcal{B}(h_c\to\gamma\eta_c)$.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001000 & $****$ & on & $ K_1^+(1270), K^- $  & Decay of the $\psi(2S)$ to $K_1K$. The branching ratio for the charged mode is taken from \cite{Yao:2006px} and the neutral mode inferred using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001000 & $****$ & on & $ K_1^-(1270), K^+ $  & Decay of the $\psi(2S)$ to $K_1K$. The branching ratio for the charged mode is taken from \cite{Yao:2006px} and the neutral mode inferred using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001000 & $****$ & on & $ \bar{K}_1(1270)^0, K^0 $  & Decay of the $\psi(2S)$ to $K_1K$. The branching ratio for the charged mode is taken from \cite{Yao:2006px} and the neutral mode inferred using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.001000 & $****$ & on & $ K_1^0(1270), \bar{K}^0 $  & Decay of the $\psi(2S)$ to $K_1K$. The branching ratio for the charged mode is taken from \cite{Yao:2006px} and the neutral mode inferred using isospin.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.000950 & $***$ & on & $ \eta, \pi^+, \pi^-, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000730 & $***$ & on & $ p^+, \bar{p}^-, \pi^+, \pi^-, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000450 & $***$ & on & $ \eta', \pi^+, \pi^-, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000400 & $***$ & on & $ \pi^+, \pi^-, p^+, \bar{p}^- $  & Decay of $\psi(2S)$ to two pions and a proton-antiproton pair. The branching ratio is from \cite{Yao:2006px} after the $\Delta$ and $\rho^0p\bar{p}$ modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.000350 & $***$ & on & $ K^{*+}, \bar{K}^0, \rho^- $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000350 & $***$ & on & $ \bar{K}^{*0}, K^+, \rho^- $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000350 & $***$ & on & $ K^{*-}, K^0, \rho^+ $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000350 & $***$ & on & $ K^{*0}, K^-, \rho^+ $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000335 & $***$ & on & $ \bar{K}^{*0}, K^+, \pi^- $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000335 & $***$ & on & $ K^{*0}, K^-, \pi^+ $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000335 & $***$ & on & $ K^{*+}, \bar{K}^0, \pi^- $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000335 & $***$ & on & $ K^{*-}, K^0, \pi^+ $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000300 & $****$ & on & $ b_1^+, \pi^- $  & Decay of the $\psi(2S)$ to a $b_1$ and a pion. The rate is taken from \cite{Yao:2006px} is the average of the modes from \cite{Yao:2006px}.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.000300 & $****$ & on & $ b_1^-, \pi^+ $  & Decay of the $\psi(2S)$ to a $b_1$ and a pion. The rate is taken from \cite{Yao:2006px} is the average of the modes from \cite{Yao:2006px}.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.000300 & $****$ & on & $ b_1^0, \pi^0 $  & Decay of the $\psi(2S)$ to a $b_1$ and a pion. The rate is taken from \cite{Yao:2006px} is the average of the modes from \cite{Yao:2006px}.   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.000280 & $***$ & on & $ \Lambda^0, \bar{\Lambda}^0, \pi^+, \pi^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000266 & $***$ & on & $ n^0, \bar{p}^-, \pi^+ $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the $p\bar{p}\pi^0$ mode and the others are infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000266 & $***$ & on & $ p^+, \bar{n}^0, \pi^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the $p\bar{p}\pi^0$ mode and the others are infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000265 & $****$ & on & $ p^+, \bar{p}^- $  & Decay of the $\psi(2S)$ to a proton-antiproton pair with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000265 & $****$ & on & $ n^0, \bar{n}^0 $  & Decay of the $\psi(2S)$ to a neutron-antineutron pair with inferred from the proton-antiproton rate in \cite{Yao:2006px} using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000250 & $****$ & on & $ \Lambda^0, \bar{\Lambda}^0 $  & Decay of the $\psi(2S)$ to $\Lambda\bar{\Lambda}$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000230 & $****$ & on & $ \Sigma^+, \bar{\Sigma}^- $  & Decay of $\psi(2S)$ to $\Sigma\bar{\Sigma}$. The neutrak mode has been observed and the remaining modes are inferred using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000230 & $****$ & on & $ \Sigma^0, \bar{\Sigma}^0 $  & Decay of $\psi(2S)$ to $\Sigma\bar{\Sigma}$. The neutrak mode has been observed and the remaining modes are inferred using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000230 & $****$ & on & $ \Sigma^-, \bar{\Sigma}^+ $  & Decay of $\psi(2S)$ to $\Sigma\bar{\Sigma}$. The neutrak mode has been observed and the remaining modes are inferred using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000220 & $****$ & on & $ \rho^0, \pi^+, \pi^- $  & Decay of $\psi(2S)$ to a rho and two pions. The neutral rho mode has been observed and the branching ratio is taken from \cite{Yao:2006px}. The remaining modes are inferrred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000220 & $***$ & on & $ \rho^-, \pi^+, \pi^0 $  & Decay of $\psi(2S)$ to a rho and two pions. The neutral rho mode has been observed and the branching ratio is taken from \cite{Yao:2006px}. The remaining modes are inferrred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000220 & $***$ & on & $ \rho^+, \pi^-, \pi^0 $  & Decay of $\psi(2S)$ to a rho and two pions. The neutral rho mode has been observed and the branching ratio is taken from \cite{Yao:2006px}. The remaining modes are inferrred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000210 & $***$ & on & $ f_2(1270), \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000200 & $***$ & on & $ \omega, f_2(1270) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000200 & $****$ & on & $ \Xi^0, \bar{\Xi}^0 $  & Decay of $\psi(2S)$ to $\Xi\bar{\Xi}$. The branching ratio is calculated by averaging the modes in \cite{Yao:2006px} using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000200 & $****$ & on & $ \Xi^-, \bar{\Xi}^+ $  & Decay of $\psi(2S)$ to $\Xi\bar{\Xi}$. The branching ratio is calculated by averaging the modes in \cite{Yao:2006px} using isospin.   & Herwig::VectorMeson2Fermion::Vector2Leptons \\ 
\hline
0.000190 & $***$ & on & $ \bar{K}^{*0}, K_2^{*0}(1430) $  & Decay of $\psi(2S)$. The branching ratio for the neutral mode is from \cite{Yao:2006px} and the rest are infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000190 & $***$ & on & $ K^{*+}, K_2^{*-}(1430) $  & Decay of $\psi(2S)$. The branching ratio for the neutral mode is from \cite{Yao:2006px} and the rest are infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000190 & $***$ & on & $ K^{*-}, K_2^{*+}(1430) $  & Decay of $\psi(2S)$. The branching ratio for the neutral mode is from \cite{Yao:2006px} and the rest are infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000190 & $***$ & on & $ K^{*0}, \bar{K}_2^{*0}(1430) $  & Decay of $\psi(2S)$. The branching ratio for the neutral mode is from \cite{Yao:2006px} and the rest are infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000190 & $***$ & on & $ \omega, f_0(1710) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} including the $KK$ decay of $f_0(1710)$   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000185 & $***$ & on & $ \omega, K^+, K^- $  & Decay of $\psi(2S)$ to omega and two kaons. The charged mode has been obsereved and the neutral mode is inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000185 & $***$ & on & $ \omega, K^0, \bar{K}^0 $  & Decay of $\psi(2S)$ to omega and two kaons. The charged mode has been obsereved and the neutral mode is inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000180 & $***$ & on & $ \bar{\Lambda}^0, p^+, K^-, \pi^+, \pi^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000180 & $***$ & on & $ \Lambda^0, \bar{p}^-, K^+, \pi^+, \pi^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000175 & $***$ & on & $ K^{*+}, K^-, \rho^0 $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000175 & $***$ & on & $ K^{*-}, K^+, \rho^0 $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000175 & $***$ & on & $ \bar{K}^{*0}, K^0, \rho^0 $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000175 & $***$ & on & $ K^{*0}, \bar{K}^0, \rho^0 $  & Decay of $\psi(2S)$ with branching ratio calculated by isospin averaging the observed $K^*K\rho$ modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000168 & $***$ & on & $ K^{*-}, K^+, \pi^0 $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000168 & $***$ & on & $ K^{*+}, K^-, \pi^0 $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000168 & $***$ & on & $ K^{*0}, \bar{K}^0, \pi^0 $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000168 & $***$ & on & $ \bar{K}^{*0}, K^0, \pi^0 $  & Decay of $\psi(2S)$ to $K^*Kpi$. The branching ratio is taken from the $K^{*0}K^+pi^-$ mode from \cite{Yao:2006px} and assuming the $Kpi$ system is in an $I=1/2$ state.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000150 & $****$ & on & $ \eta', \gamma $  & Radiative decay of $\psi(2S)$ with branching ratio taken from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000136 & $***$ & on & $ \pi^+, \pi^-, \pi^0 $  & Decay of $\psi(2S)$ to three pions with branching ratio from \cite{Yao:2006px} after the subtraction of the $\rho\pi$ submodes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000133 & $***$ & on & $ p^+, \bar{p}^-, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the $p\bar{p}\pi^0$ mode and the others are infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000133 & $***$ & on & $ n^0, \bar{n}^0, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the $p\bar{p}\pi^0$ mode and the others are infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000128 & $***$ & on & $ \Delta^{+\,+}, \bar{\Delta}^{-\,-} $  & Decay of $\psi(2S)$ to $\Delta\bar{\Delta}$. The doubly charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000128 & $***$ & on & $ \Delta^+, \bar{\Delta}^- $  & Decay of $\psi(2S)$ to $\Delta\bar{\Delta}$. The doubly charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000128 & $***$ & on & $ \Delta^0, \bar{\Delta}^0 $  & Decay of $\psi(2S)$ to $\Delta\bar{\Delta}$. The doubly charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000128 & $***$ & on & $ \Delta^-, \bar{\Delta}^+ $  & Decay of $\psi(2S)$ to $\Delta\bar{\Delta}$. The doubly charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000110 & $****$ & on & $ \Sigma^{*-}, \bar{\Sigma}^{*+} $  & Decay of $\psi(2S)$ to $\Sigma^*\bar{\Sigma}^*$. The charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000110 & $****$ & on & $ \Sigma^{*0}, \bar{\Sigma}^{*0} $  & Decay of $\psi(2S)$ to $\Sigma^*\bar{\Sigma}^*$. The charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000110 & $****$ & on & $ \Sigma^{*+}, \bar{\Sigma}^{*-} $  & Decay of $\psi(2S)$ to $\Sigma^*\bar{\Sigma}^*$. The charged mode has been observed and the remaining modes are inferred using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000110 & $***$ & on & $ K^+, K^-, K^+, K^-, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000109 & $***$ & on & $ K^0, \bar{K}^{*0} $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000109 & $***$ & on & $ \bar{K}^0, K^{*0} $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000100 & $***$ & on & $ f_0(1710), \gamma $  & Radiative decay mode of $\psi(2S)$ with branching ratio calculated summing the two modes including the $f_0(1710)$ as a intermediate and using our branching ratios for the $f_0(1710)$.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000100 & $***$ & on & $ \phi, f_0(980) $  & Decay of $\psi(2S)$ to the $\phi$ and $f_0$. The branching ratio is calculated using our $f_0$ branching ratios and the branching ratio including the pionic decay of the $f_0$ from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.000100 & $***$ & on & $ \Lambda^0, \bar{n}^0, K^0 $  & Decay of $\psi(2S)$ with branching ratio infered fromj the observed mode using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ n^0, \bar{p}^-, \rho^+ $  & Decay of $\psi(2S)$ calculated by isospin averaging the observed modes from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ p^+, \bar{n}^0, \rho^- $  & Decay of $\psi(2S)$ calculated by isospin averaging the observed modes from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ \Lambda^0, \bar{p}^-, K^+ $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ \bar{\Lambda}^0, p^+, K^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ \bar{\Lambda}^0, n^0, \bar{K}^0 $  & Decay of $\psi(2S)$ with branching ratio infered fromj the observed mode using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000087 & $***$ & on & $ \rho^-, a_2^+(1320) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000087 & $***$ & on & $ \rho^+, a_2^-(1320) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000087 & $***$ & on & $ \rho^0, a_2^0(1320) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000080 & $***$ & on & $ \pi^+, \pi^- $  & Decay of $\psi(2S)$ to two pions with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.000070 & $***$ & on & $ \phi, K^+, K^- $  & Decay of $\psi(2S)$ to the phi and two kaons. The branching ratio for the charged mode is from \cite{Yao:2006px} a and the neutral mode is inferred using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000070 & $***$ & on & $ \phi, K^0, \bar{K}^0 $  & Decay of $\psi(2S)$ to the phi and two kaons. The branching ratio for the charged mode is from \cite{Yao:2006px} a and the neutral mode is inferred using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000069 & $****$ & on & $ \omega, p^+, \bar{p}^- $  & Decay of $\psi(2S)$ to two nucleons, the proton mode is observed and the neutron mode is infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000069 & $****$ & on & $ \omega, n^0, \bar{n}^0 $  & Decay of $\psi(2S)$ to two nucleons, the proton mode is observed and the neutron mode is infered using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000060 & $***$ & on & $ K^+, K^-, K^+, K^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000060 & $***$ & on & $ p^+, \bar{p}^-, \eta $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000060 & $***$ & on & $ n^0, \bar{n}^0, \eta $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px} for the proton mode and the neutron infered using isospin.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000053 & $****$ & on & $ K^+, K^- $  & Decay of $\psi(2S)$ to two kaons. The branching ratios for the neutral and charged modes from \cite{Yao:2006px} have been averaged assuming isospin conservation.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.000053 & $****$ & on & $ K^0_L, K^0_S $  & Decay of $\psi(2S)$ to two kaons. The branching ratios for the neutral and charged modes from \cite{Yao:2006px} have been averaged assuming isospin conservation.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.000053 & $****$ & on & $ \phi, \pi^+, \pi^- $  & Decay of $\psi(2S)$ to the phi and two pions. The branching ratio for the charged mode is from \cite{Yao:2006px} after the $f_0$ component has been subtracted. The neutral mode is inferred using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000050 & $***$ & on & $ p^+, \bar{p}^-, \rho^0 $  & Decay of $\psi(2S)$ calculated by isospin averaging the observed modes from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000050 & $***$ & on & $ n^0, \bar{n}^0, \rho^0 $  & Decay of $\psi(2S)$ calculated by isospin averaging the observed modes from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000044 & $***$ & on & $ \phi, f'_2(1525) $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000032 & $***$ & on & $ \omega, \eta' $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000031 & $***$ & on & $ \phi, \eta' $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000028 & $***$ & on & $ \phi, \eta $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000027 & $****$ & on & $ \phi, \pi^0, \pi^0 $  & Decay of $\psi(2S)$ to the phi and two pions. The branching ratio for the charged mode is from \cite{Yao:2006px} after the $f_0$ component has been subtracted. The neutral mode is inferred using isospin   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000027 & $***$ & on & $ p^+, \bar{p}^-, K^+, K^- $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000022 & $***$ & on & $ \rho^0, \eta $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000021 & $***$ & on & $ \omega, \pi^0 $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000020 & $***$ & on & $ \pi^+, \pi^-, \pi^+, \pi^- $  & Decay of $\psi(2S)$ to four pions with branching ratio from \cite{Yao:2006px} after the $\rho^0\pi^+\pi^-$ mode has been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.000019 & $***$ & on & $ \rho^0, \eta' $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000017 & $***$ & on & $ K^+, K^{*-} $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000017 & $***$ & on & $ K^-, K^{*+} $  & Decay of $\psi(2S)$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000011 & $***$ & on & $ \rho^0, \pi^0 $  & Decay of $\psi(2S)$ to $\rho\pi$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000011 & $***$ & on & $ \rho^+, \pi^- $  & Decay of $\psi(2S)$ to $\rho\pi$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.000011 & $***$ & on & $ \rho^-, \pi^+ $  & Decay of $\psi(2S)$ to $\rho\pi$ with branching ratio from \cite{Yao:2006px}.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
\end{longtable}The $\psi(2S)$ decay modes are given in Table~\ref{tab:100443decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|psi2smass| for the $\psi(2S)$.
The width generator is \verb|psi2Swidth| for the $\psi(2S)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 16:21:5 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 16:55:37 on the 3rd of August 2007.

\end{document}
