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\title{\boldmath{ $\rho^0(1450)$}\ \ \ \ \ \ \ $***$}
\maketitle
The $\rho^0(1450)$ is the charged member of the isospin triplet from the $2^3S_1$. It is mainly included to act as an intermediate particle in many of the hadronic matrix elements containing excited $\rho$ resonances. 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 numbers from \cite{Abele:2001pv}  assuming that there are only two and four pion modes. The $\rho^0(1450)$ is allowed to be off-shell by twice the width . It should be noted that the width is poorly measured and tends to change a lot between editions of the PDG.
The $\rho^0(1450)$ has mass $1459$~MeV and is unstable. The $\rho^0(1450)$ has spin $1$, charge $0$ and is colour neutral.
 The $\rho^0(1450)$ is a meson and is from the $2^3S_1$ multiplet.The $\rho^0(1450)$ has width $147$~MeV. The lower limit on the mass of the particle is $294$~MeV and the upper limit is $294$~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 100113.
\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 $\rho^0(1450)$ (continues).}
\endfoot
\caption{The decay modes of the $\rho^0(1450)$.}
\endlastfoot
\label{tab:100113decaymodes}
0.270072 & $***$ & on & $ \pi^+, \pi^- $  & The decay of the $\rho^0(1450)$ to two pions.   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.135037 & $***$ & on & $ \pi^-(1300), \pi^+ $  & The decay of the $\rho^0(1450)$ to the $\pi(1300)$ and a pion. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.135037 & $***$ & on & $ \pi^+(1300), \pi^- $  & The decay of the $\rho^0(1450)$ to the $\pi(1300)$ and a pion. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMeson2Meson::Vector2Meson \\ 
\hline
0.124088 & $***$ & on & $ \rho^0, \sigma $  & The decay of the $\rho^0(1450)$ to a rho and two pions in s-wave, this is a contribution to the four pion mode. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMesonVectorScalar::VVSDecayer \\ 
\hline
0.098540 & $***$ & on & $ a_1^+(1260), \pi^- $  & The decay of the $\rho^0(1450)$ to an $a_1(1260)$ and a pion, this is a contribution to the four pion mode. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.098540 & $***$ & on & $ a_1^-(1260), \pi^+ $  & The decay of the $\rho^0(1450)$ to an $a_1(1260)$ and a pion, this is a contribution to the four pion mode. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
0.080292 & $***$ & on & $ \rho^+, \rho^- $  & The decay of the $\rho^0(1450)$ to the two rho mesons. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMesonVectorVector::VectorVV \\ 
\hline
0.058394 & $***$ & on & $ h_1, \pi^0 $  & The decay of the $\rho^0(1450)$ to an $h_1$ and a pion, this is a contribution to the four pion mode. The branching ratio is taken from \cite{Abele:2001pv} .   & Herwig::VectorMesonPVectorPScalar::VAPDecayer \\ 
\hline
\end{longtable}The $\rho^0(1450)$ decay modes are given in Table~\ref{tab:100113decaymodes} and the total branching ratio is $1$.


The mass generator is \verb|rho'0mass| for the $\rho^0(1450)$.
The width generator is \verb|rho'0width| for the $\rho^0(1450)$.

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 The particle was checked by Peter Richardson at 21:37:37 on the 20th of October 2007. The most recently changed decay mode was modified at 22:2:37 on the 25th of July 2005. The particle data was last modified at 16:14:8 on the 7th of September 2007.

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