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\begin{document}
\title{Check List for Particle : \boldmath{ $\Xi_c^0$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &4132 & & & Mass & 2471& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: Xi_c0: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $3.36\times10^{-5}$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $\Xi_c^0 $ \ \ \ \ \ \ \ \ \ \ \ \ & 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 &s048 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $\Xi_c^0$ is the neutral $\Xi_c$ member of the lightest $\Xi_c$ multiplet. The mass and lifetime have been measured and are taken from \cite{Yao:2006px}. 

No absolute branching ratio measurements have been made and only a few ratios of branching fractions are known. We have chosen to normalise these inclusive modes to the value of the $\Xi^-\pi^+$ rate from \cite{Korner:1992wi}  and include the observed modes and other modes predicted in \cite{Korner:1992wi} . 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. The partonic semi-leptonic modes have been replaced with multi-body modes due to problems with the hadronization of the partonic decays.
\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 $\Xi_c^0$ (continues).}
\endfoot
\caption{The decay modes of the $\Xi_c^0$.}
\endlastfoot
\label{tab:4132decaymodes}
0.394200 & $**$ & $\bar{d}$, $u$, $s$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.108400 & $**$ & $\bar{d}$, $s$, $u$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.033000 & $**$ & $\Xi^-$, $\pi^+$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.032000 & $**$ & $\Xi^-$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy3& \\ 
& & & & & \\ \hline
0.032000 & $*****$ & $e^+$, $\nu_e$, $\pi^-$, $\Xi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.032000 & $*****$ & $\mu^+$, $\nu_\mu$, $\pi^-$, $\Xi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.032000 & $**$ & $\Xi^-$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy3& \\ 
& & & & & \\ \hline
0.029800 & $**$ & $\bar{d}$, $u$, $d$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.029800 & $**$ & $\bar{s}$, $u$, $s$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.023300 & $**$ & $\Xi^0$, $\omega$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.022000 & $**$ & $\Sigma^{*+}$, $K^{*-}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.018000 & $**$ & $\Xi^-$, $\rho^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.018000 & $**$ & $\Xi^{*-}$, $\rho^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.017000 & $**$ & $\Xi^0$, $\rho^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.016000 & $**$ & $e^+$, $\nu_e$, $\pi^0$, $\Xi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.016000 & $**$ & $\mu^+$, $\nu_\mu$, $\pi^0$, $\Xi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.012000 & $**$ & $\Sigma^0$, $\bar{K}^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.011000 & $**$ & $\Lambda^0$, $\bar{K}^{*0}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.011000 & $**$ & $\Sigma^{*0}$, $\bar{K}^{*0}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.010000 & $**$ & $\Xi^-$, $\pi^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.009900 & $**$ & $\bar{d}$, $d$, $u$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.009900 & $**$ & $\bar{s}$, $s$, $u$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.009200 & $**$ & $\Xi^{*0}$, $\rho^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.008500 & $**$ & $\Xi^0$, $\eta'$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.008400 & $**$ & $\Xi^{*0}$, $\omega$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.006200 & $**$ & $\Sigma^0$, $\bar{K}^{*0}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.005600 & $**$ & $\Xi^{*-}$, $\pi^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.005000 & $**$ & $\Sigma^{*+}$, $K^-$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.004200 & $**$ & $\Lambda^0$, $\bar{K}^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.004000 & $**$ & $\mu^+$, $\nu_\mu$, $d$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.004000 & $**$ & $e^+$, $\nu_e$, $d$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.004000 & $**$ & $\Sigma^+$, $K^{*-}$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.003400 & $**$ & $\Lambda^0$, $K^-$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003000 & $**$ & $\Omega^-$, $K^+$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.002800 & $**$ & $\Xi^{*0}$, $\pi^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.002500 & $**$ & $\Sigma^{*0}$, $\bar{K}^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.002400 & $**$ & $\Xi^0$, $\eta$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.002100 & $**$ & $p^+$, $K^-$, $\bar{K}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002000 & $**$ & $p^+$, $K^-$, $K^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001800 & $**$ & $\Xi^0$, $\phi$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.001600 & $**$ & $\bar{s}$, $u$, $d$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.001200 & $**$ & $\Sigma^+$, $K^-$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
0.000500 & $**$ & $\bar{s}$, $d$, $u$, $(sd)_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000300 & $**$ & $\Xi^0$, $\pi^0$ & & Herwig::KornerKramerCharm::CharmBaryon1& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

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