% 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{ $K_2^{*0}(1430)$}\ \ \ \ \ \ \ $*****$}
\maketitle
The $K_2^{*0}(1430)$ is the neutral kaon member of the lightest tensor multiplet. The mass, width and decays are well measured and taken from \cite{Yao:2006px}. The limit on the off-shellness of the particle is set to two times the width. EvtGen models the $K^*\pi\pi$ modes as three body modes and does not include the $K\omega$ and $K\eta$ modes. 
The $K_2^{*0}(1430)$ has mass $1432.4$~MeV and is unstable. The $K_2^{*0}(1430)$ has spin $2$, charge $0$ and is colour neutral.
 The $K_2^{*0}(1430)$ is a meson and is from the $1^3P_2$ multiplet.The $K_2^{*0}(1430)$ has width $109$~MeV. The lower limit on the mass of the particle is $218$~MeV and the upper limit is $218$~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 315.
\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 $K_2^{*0}(1430)$ (continues).}
\endfoot
\caption{The decay modes of the $K_2^{*0}(1430)$.}
\endlastfoot
\label{tab:315decaymodes}
0.333500 & $*****$ & on & $ K^+, \pi^- $  & Decay of the $K_2^{*0}(1430)$ to a kaon and a pion with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMeson2PScalar::Tensor2PScalar \\ 
\hline
0.166750 & $*****$ & on & $ K^0, \pi^0 $  & Decay of the $K_2^{*0}(1430)$ to a kaon and a pion with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMeson2PScalar::Tensor2PScalar \\ 
\hline
0.165079 & $*****$ & on & $ K^{*+}, \pi^- $  & Decay of the $K_2^{*0}(1430)$ to a $K^*$ and a pion with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorPScalar::TensorVP \\ 
\hline
0.089557 & $****$ & on & $ K^{*+}, \rho^- $  & Decay of the $K_2^{*0}(1430)$ to a $K^*$ and two pions, modelled as the $\rho$, with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorVector::TVV \\ 
\hline
0.082540 & $*****$ & on & $ K^{*0}, \pi^0 $  & Decay of the $K_2^{*0}(1430)$ to a $K^*$ and a pion with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorPScalar::TensorVP \\ 
\hline
0.058145 & $*****$ & on & $ K^+, \rho^- $  & Decay of the $K_2^{*0}(1430)$ to a kaon and a rho meson with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorPScalar::TensorVP \\ 
\hline
0.044779 & $****$ & on & $ K^{*0}, \rho^0 $  & Decay of the $K_2^{*0}(1430)$ to a $K^*$ and two pions, modelled as the $\rho$, with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorVector::TVV \\ 
\hline
0.029073 & $*****$ & on & $ K^0, \rho^0 $  & Decay of the $K_2^{*0}(1430)$ to a kaon and a rho meson with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorPScalar::TensorVP \\ 
\hline
0.029073 & $****$ & on & $ K^0, \omega $  & Decay of the $K_2^{*0}(1430)$ to a kaon and an omega meson with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMesonVectorPScalar::TensorVP \\ 
\hline
0.001504 & $***$ & on & $ K^0, \eta $  & The decay of the $K_2^{*0}(1430)$ to a kaon and an $\eta$ with branching ratio from \cite{Yao:2006px} with minor changes to ensure the branching ratios sum to one.   & Herwig::TensorMeson2PScalar::Tensor2PScalar \\ 
\hline
\end{longtable}The $K_2^{*0}(1430)$ decay modes are given in Table~\ref{tab:315decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|K_20mass| for the $K_2^{*0}(1430)$.
The width generator is \verb|K_20width| for the $K_2^{*0}(1430)$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 16:0:45 on the 22nd of August 2007. The most recently changed decay mode was modified at 20:54:10 on the 14th of April 2007. The particle data was last modified at 13:50:28 on the 21st of August 2007.

\end{document}
