% particle data information automatically produced from the herwig database
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\title{\boldmath{ $\phi_3(1850)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\phi_3(1850)$ is the heavier isospin singlet from the lightest spin-$3$ multiplet. The mass and width have been measured although the error for the width is large. Two decay modes have been observed but the branching ratios are not given in \cite{Yao:2006px}. There is however one measurement, although with large errors, of the ratio of the branching ratios for these two modes
\begin{equation}
\frac{\Gamma(KK^*)}{\Gamma(K\bar{K})} = {0.55^{+0.85}\!\!\!\!\!\!}_{-0.45}
\end{equation}
  which we use together with the assumption that these are the only modes to calculate the branching ratios. Given the large width of the $\phi_3(1850)$ we allow it to be off-shell by five times the width.
The $\phi_3(1850)$ has mass $1854$~MeV and is unstable. The $\phi_3(1850)$ has spin $3$, charge $0$ and is colour neutral.
 The $\phi_3(1850)$ is a meson and is from the $1^3D_3$ multiplet.The $\phi_3(1850)$ has width $87$~MeV. The lower limit on the mass of the particle is $435$~MeV and the upper limit is $435$~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 337.
\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 $\phi_3(1850)$ (continues).}
\endfoot
\caption{The decay modes of the $\phi_3(1850)$.}
\endlastfoot
\label{tab:337decaymodes}
0.322582 & $***$ & on & $ K^+, K^- $  & The decay of $\phi_3(1850)$ to $K\bar{K}$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.322582 & $***$ & on & $ K^0, \bar{K}^0 $  & The decay of $\phi_3(1850)$ to $K\bar{K}$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.088709 & $***$ & on & $ K^{*+}, K^- $  & Te decay of $\phi_3(1850)$ to $KK^*$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.088709 & $***$ & on & $ K^{*-}, K^+ $  & Te decay of $\phi_3(1850)$ to $KK^*$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.088709 & $***$ & on & $ K^{*0}, \bar{K}^0 $  & Te decay of $\phi_3(1850)$ to $KK^*$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.088709 & $***$ & on & $ \bar{K}^{*0}, K^0 $  & Te decay of $\phi_3(1850)$ to $KK^*$ where the branching ratio is calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\phi_3(1850)$ decay modes are given in Table~\ref{tab:337decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|phi_3Mass| for the $\phi_3(1850)$.
The width generator is \verb|phi_3Width| for the $\phi_3(1850)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 9:7:33 on the 10th of August 2007. The most recently changed decay mode was modified at 23:10:55 on the 3rd of April 2005. The particle data was last modified at 23:40:33 on the 24th of April 2007.

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