% particle data information automatically produced from the herwig database
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\title{\boldmath{ $\omega_3(1670)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\omega_3(1670)$ is the lightest isospin singlet from the lightest spin-$3$ multiplet. The mass and width are taken from \cite{Yao:2006px}. The branching ratios are not given in \cite{Yao:2006px} and therefore we have used the value of the ratio 
\begin{equation}
\frac{\Gamma(\omega\pi\pi)}{\Gamma(\rho\pi)} = 0.71\pm0.27,
\end{equation}
  together with the assumption that the $\omega\pi\pi$ mode is entirely due to $b_1\pi$, which is supported by the measurement of this mode, and the assumption that these are the only modes to obtain the branching ratios. Given the large width of the $\omega_3(1670)$ we allow it to be off-shell by twice the the width.
The $\omega_3(1670)$ has mass $1667$~MeV and is unstable. The $\omega_3(1670)$ has spin $3$, charge $0$ and is colour neutral.
 The $\omega_3(1670)$ is a meson and is from the $1^3D_3$ multiplet.The $\omega_3(1670)$ has width $168$~MeV. The lower limit on the mass of the particle is $336$~MeV and the upper limit is $336$~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 227.
\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 $\omega_3(1670)$ (continues).}
\endfoot
\caption{The decay modes of the $\omega_3(1670)$.}
\endlastfoot
\label{tab:227decaymodes}
0.194933 & $***$ & on & $ \rho^0, \pi^0 $  & The decay of $\omega_3(1670)$ to $\rho\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.194932 & $***$ & on & $ \rho^+, \pi^- $  & The decay of $\omega_3(1670)$ to $\rho\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.194932 & $***$ & on & $ \rho^-, \pi^+ $  & The decay of $\omega_3(1670)$ to $\rho\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.138401 & $***$ & on & $ b_1^0, \pi^0 $  & The decay of $\omega_3(1670)$ to $b_1\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.138401 & $***$ & on & $ b_1^+, \pi^- $  & The decay of $\omega_3(1670)$ to $b_1\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.138401 & $***$ & on & $ b_1^-, \pi^+ $  & The decay of $\omega_3(1670)$ to $b_1\pi$ with branching ratio calculated as described above.   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\omega_3(1670)$ decay modes are given in Table~\ref{tab:227decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|omega_3Mass| for the $\omega_3(1670)$.
The width generator is \verb|omega_3Width| for the $\omega_3(1670)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 14:38:46 on the 22nd 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 15:29:41 on the 21st of August 2007.

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