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\title{Check List for Particle : \boldmath{ $\Omega^0_c$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &4332 & & & Mass & 2697.5& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: Omega_c0: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $2.1\times10^{-5}$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $\Omega^0_c $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:: \ \ & Width Gen.  & \verb:: \ \ & Type        & baryon \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $1/2$& Charge & $0$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 0& Upper cut & 0& PDG link &s047 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The lightest $\Omega_c$ state. The mass and liftime have been measured and taken from \cite{Yao:2006px}. No absolute branching ratios have been measured and only a few ratios of branching ratios are known, usually the rate relative to the $\Omega\pi$ mode.

 We therefore include a few of these exclusive modes and model the rest of the decays as partonic decays. The partonic decays are calculated assuming an 8\% branching ratio for the semileptonic decay $c\to s\ell\nu$. The remaining leptonic modes are calculated using the ratio of the CKM matrix elements. The hadronic decays are calculated by including the normal decays and the colour exchanged decays with a factor of $1/3$ the direct decay. The CKM factors are used to calculated the rates for the different quarks produced in the weak decays. The exclusive modes are then subtracted from the relevant partonic mode.
\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 $\Omega^0_c$ (continues).}
\endfoot
\caption{The decay modes of the $\Omega^0_c$.}
\endlastfoot
\label{tab:4332decaymodes}
0.531900 & $**$ & $\bar{d}$, $u$, $s$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.160600 & $**$ & $\bar{d}$, $s$, $u$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.066000 & $**$ & $e^+$, $\nu_e$, $s$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.066000 & $**$ & $\mu^+$, $\nu_\mu$, $s$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.029800 & $**$ & $\bar{d}$, $u$, $d$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.029800 & $**$ & $\bar{s}$, $u$, $s$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.025000 & $**$ & $\Omega^-$, $\rho^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.014000 & $**$ & $\Omega^-$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy3& \\ 
& & & & & \\ \hline
0.014000 & $**$ & $\Omega^-$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy3& \\ 
& & & & & \\ \hline
0.012000 & $**$ & $\Xi^0$, $\bar{K}^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.009900 & $**$ & $\bar{d}$, $d$, $u$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.009900 & $**$ & $\bar{s}$, $s$, $u$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.007800 & $**$ & $\Xi^{*0}$, $\bar{K}^{*0}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.005900 & $**$ & $\Omega^-$, $\pi^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.005900 & $**$ & $\Xi^0$, $\bar{K}^{*0}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.004000 & $**$ & $e^+$, $\nu_e$, $d$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.004000 & $**$ & $\mu^+$, $\nu_\mu$, $d$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.001600 & $**$ & $\bar{s}$, $u$, $d$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.001400 & $**$ & $\Xi^{*0}$, $\bar{K}^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.000500 & $**$ & $\bar{s}$, $d$, $u$, $(ss)_1$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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