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\title{\boldmath{ $K^{*+}(1410)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $K^{*+}(1410)$ is the first excited vector kaon. The mass and width are measured although not with great accuracy. The branching ratio of only one mode, $K\pi$ has been measured. There is a lower limit on the $K^*\pi$ mode and an upper limit on the $K\rho$ mode. The limit on the off-shell mass is twice the particle's width. We have chosen to assume that the branching ratio is saturated by the $K^*\pi$ mode and not to include a $K\rho$ mode. This differs to the choice made in EvtGEN. This state was not included in FORTRAN HERWIG.
The $K^{*+}(1410)$ has mass $1414$~MeV and is unstable. The $K^{*+}(1410)$ has spin $1$, charge $1$ and is colour neutral.
 The $K^{*+}(1410)$ is a meson and is from the $2^3S_1$ multiplet.The $K^{*+}(1410)$ has width $232$~MeV. The lower limit on the mass of the particle is $464$~MeV and the upper limit is $464$~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 100323.
\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 $K^{*+}(1410)$ (continues).}
\endfoot
\caption{The decay modes of the $K^{*+}(1410)$.}
\endlastfoot
\label{tab:100323decaymodes}
0.622667 & $***$ & on & $ K^{*0}, \pi^+ $  & The decay of $K^{*+}(1410)$ to $K^*\pi$. This is assumed to be dominant with branching ratio given by one minus the sub-dominant $K\pi$ mode. The relative rates for the two $K^*\pi$ modes is determined by isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.311333 & $***$ & on & $ K^{*+}, \pi^0 $  & The decay of $K^{*+}(1410)$ to $K^*\pi$. This is assumed to be dominant with branching ratio given by one minus the sub-dominant $K\pi$ mode. The relative rates for the two $K^*\pi$ modes is determined by isospin.   & Herwig::VectorMesonVectorPScalar::VectorVP \\ 
\hline
0.044000 & $***$ & on & $ K^0, \pi^+ $  & The decay of $K^{*+}(1410)$ to $K\pi$. The branching ratio is taken from \cite{Yao:2006px}. The relative rates for the two $K\pi$ modes is determined by isospin.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.022000 & $***$ & on & $ K^+, \pi^0 $  & The decay of $K^{*+}(1410)$ to $K\pi$. The branching ratio is taken from \cite{Yao:2006px}. The relative rates for the two $K\pi$ modes is determined by isospin.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
\end{longtable}The $K^{*+}(1410)$ decay modes are given in Table~\ref{tab:100323decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|K'*+mass| for the $K^{*+}(1410)$.
The width generator is \verb|K'*+width| for the $K^{*+}(1410)$.

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 The particle was checked by Peter Richardson at 21:37:52 on the 20th of October 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 16:43:35 on the 7th of September 2007.

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