% particle data information automatically produced from the herwig database
\documentclass[a4paper]{article}
\usepackage{cite,longtable}
\bibliographystyle{JHEP}
\topmargin -1.5cm
\textheight 26cm
\textwidth 20cm
\oddsidemargin -2cm
\evensidemargin 0cm
\begin{document}
\title{\boldmath{ $\chi_{b0}(3P)$}\ \ \ \ \ \ \ $*$}
\maketitle
The $\chi_{b0}(3P)$ has not been observed and is included because it is included in EvtGen and when interfacing with EvtGen it is produced. The properties are taken from \cite{Kwong:1988ae}  apart from the total width and $gg$ branching ratio which are calculated from the results in \cite{Kwong:1988ae}  using the same corrections as for the 2P level. The $\chi_{b0}(3P)$ is allowed to be off-shell by ten times the width.
The $\chi_{b0}(3P)$ has mass $10500.7$~MeV and is unstable. The $\chi_{b0}(3P)$ has spin $0$, charge $0$ and is colour neutral.
 The $\chi_{b0}(3P)$ is a meson and is from the $3^3P_0$ multiplet.The $\chi_{b0}(3P)$ has width $0.71$~MeV. The lower limit on the mass of the particle is $7.1$~MeV and the upper limit is $7.1$~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 210551.
\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 $\chi_{b0}(3P)$ (continues).}
\endfoot
\caption{The decay modes of the $\chi_{b0}(3P)$.}
\endlastfoot
\label{tab:210551decaymodes}
0.977300 & $**$ & on & $ g, g $  & Decay of $\chi_{b0}(3P)$ with branching ratio calculated using the partial width from \cite{Kwong:1988ae} .   & Herwig::Quarkonium::QDecayME0 \\ 
\hline
0.010500 & $*$ & on & $ \Upsilon(3S), \gamma $  & Decay of $\chi_{b0}(3P)$ with branching ratio calculated using the partial width from \cite{Kwong:1988ae} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005000 & $*$ & on & $ \Upsilon(1S), \gamma $  & Decay of $\chi_{b0}(3P)$ with branching ratio calculated using the partial width from \cite{Kwong:1988ae} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.004600 & $*$ & on & $ \Upsilon(2S), \gamma $  & Decay of $\chi_{b0}(3P)$ with branching ratio calculated using the partial width from \cite{Kwong:1988ae} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002600 & $*$ & on & $ \Upsilon_1(2D), \gamma $  & Decay of $\chi_{b0}(3P)$ with branching ratio calculated using the partial width from \cite{Kwong:1988ae} .   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\chi_{b0}(3P)$ decay modes are given in Table~\ref{tab:210551decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|chi_b03PMass| for the $\chi_{b0}(3P)$.
The width generator is \verb|chi_b03PWidth| for the $\chi_{b0}(3P)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 8:50:9 on the 24th of April 2007. The most recently changed decay mode was modified at 11:17:47 on the 30th of July 2005. The particle data was last modified at 16:24:39 on the 10th of October 2006.

\end{document}
