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\title{Check List for Particle : \boldmath{ $\rho_3^-(1690)$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &-217 & & & Mass & 1688.8& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 161& & & Gen  & \verb: rho_3-: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $\rho_3^-(1690) $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:rho_3+Mass: \ \ & Width Gen.  & \verb:rho_3+Width: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $3$& Charge & $-1$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 540& Upper cut & 644& PDG link &m015 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $\rho_3^-(1690)$ is the charged member of the isospin triplet from the lightest spin-$3$ multiplet. The mass and width are measured with reasonable precision and the branching ratios of a number of modes are known. We have used the branching ratios from \cite{Yao:2006px} together with some assumptions to obtain the branching ratios. We have used the \cite{Yao:2006px} rates for the $\pi\pi\pi\pi$, $\pi\pi$, $K\bar{K}\pi$, and $K\bar{K}$ modes with a minor renormalisation to ensure the sum is unity. We have assumed that the $K\bar{K}\pi$ mode is solely due to $KK^*$. We have also split the four pion mode into various two-body channels. This was done using measured $\omega\pi$ rate, the most recent measurement of ratio of $a_2\pi$ to the four pion rate and assigning the remainder of the mode to $\rho\rho$. Given the large width of the $\rho_3^-(1690)$ we allow it to be off-shell by four times the width above the central value of the mass and chose the lower limit so that the $a_2\pi$ decay mode is kinematically allowed.
\item References?
\end{itemize}
\setlongtables
\begin{longtable}[t]{|c|c|c|p{1in}|c|p{2.5in}|}
\hline
Branching & Rating & Outgoing  & Description & Decayer &  EvtGen \\ 
Ratio     &        & Particles &             &         & \\ 
\hline
\endhead
\caption{The decay modes of the $\rho_3^-(1690)$ (continues).}
\endfoot
\caption{The decay modes of the $\rho_3^-(1690)$.}
\endlastfoot
\label{tab:-217decaymodes}
0.235810 & $***$ & $\pi^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.234443 & $***$ & $a_2^-(1320)$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.234443 & $***$ & $a_2^0(1320)$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.160000 & $***$ & $\pi^-$, $\omega$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.081547 & $***$ & $\rho^-$, $\rho^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.018985 & $***$ & $K^{*0}$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.018985 & $***$ & $K^{*-}$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.015787 & $***$ & $K^-$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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