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\begin{document}
\title{Check List for Particle : \boldmath{ $\bar{\Xi}_b^0$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &-5232 & & & Mass & 5789.8& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: Xi_bbar0: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0.000417$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $\bar{\Xi}_b^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 &s060 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The evidence for the existance of $\bar{\Xi}_b^0$ is not strong, although the evidence for the $\Xi_b^-$ is stronger. The mass is obtained using the mass difference from the charm system and the mass of the $\Xi_b^-$. The lifetime is the experimentally measured value from \cite{Yao:2006px}.

The mass is taken from \cite{cdf:2007un} . The lifetime is the experimentally measured value from \cite{Yao:2006px}. 

  No branching ratios have been measured. We have therefore chosen to add a number of two body modes with branching ratios calculated from various theoretical papers and model the remaining modes using partonic decays. The ratios of the partonic decays were calculated using the colour factor for the relative rates of the leptonic and direct $b\to c$ decays, colour exchanged decays were added with one third of the rate for the direct decays. The rates of the different quarks produced in the weak decays were calculated using the CKM matrix elements.

\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 $\bar{\Xi}_b^0$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{\Xi}_b^0$.}
\endlastfoot
\label{tab:-5232decaymodes}
0.221900 & $**$ & $\bar{s}$, $c$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.217850 & $**$ & $\bar{d}$, $u$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.091110 & $**$ & $\bar{c}$, $u$, $\bar{d}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.089460 & $**$ & $\bar{c}$, $c$, $\bar{s}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.073200 & $**$ & $\mu^+$, $\nu_\mu$, $\bar{\Xi}_c^-$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy1& \\ 
& & & & & \\ \hline
0.073200 & $**$ & $e^+$, $\nu_e$, $\bar{\Xi}_c^-$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy1& \\ 
& & & & & \\ \hline
0.032000 & $**$ & $\bar{\Xi}_c^-$, $D_s^{*+}$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.028000 & $**$ & $\bar{\Xi}_c^-$, $a_1^+(1260)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.023000 & $**$ & $e^+$, $\nu_e$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.023000 & $**$ & $\mu^+$, $\nu_\mu$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.021100 & $**$ & $\tau^+$, $\nu_\tau$, $\bar{\Xi}_c^-$ & & Herwig::SemiLeptonicBaryon::BaryonHeavy1& \\ 
& & & & & \\ \hline
0.020000 & $**$ & $\bar{\Xi}_c^-$, $D_s^+$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
0.019000 & $**$ & $\bar{\Xi}_c^-$, $\rho^+$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.012870 & $**$ & $\bar{s}$, $u$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.012630 & $**$ & $\bar{d}$, $c$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.011000 & $**$ & $\tau^+$, $\nu_\tau$, $\bar{c}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.006700 & $**$ & $\bar{\Xi}_c^-$, $\pi^+$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
0.004800 & $**$ & $\bar{c}$, $u$, $\bar{s}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.004800 & $**$ & $\bar{c}$, $c$, $\bar{d}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.002200 & $**$ & $\bar{d}$, $u$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.002200 & $**$ & $\bar{s}$, $c$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.001100 & $**$ & $\bar{\Xi}_c^-$, $D^{*+}(2010)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.001100 & $**$ & $\bar{\Xi}_c^-$, $K^{*+}$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\bar{\Xi}^0$, $J/\psi(1S)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.000840 & $**$ & $\bar{\Xi}^0$, $\psi(2S)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.000800 & $**$ & $e^+$, $\nu_e$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000800 & $**$ & $\mu^+$, $\nu_\mu$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000770 & $**$ & $\bar{\Xi}_c^-$, $D^+$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
0.000530 & $**$ & $\bar{\Xi}_c^-$, $K^+$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
0.000400 & $**$ & $\bar{\Sigma}_c^{-}$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000320 & $**$ & $\bar{\Omega}^0_c$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000300 & $**$ & $\tau^+$, $\nu_\tau$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000300 & $**$ & $\bar{{\Xi'}}_c^0$, $\eta'$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000300 & $**$ & $\bar{\Sigma}_c^0$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000250 & $**$ & $\bar{{\Xi'}}_c^-$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000210 & $**$ & $\bar{{\Xi'}}_c^0$, $\eta$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000200 & $**$ & $\bar{{\Xi'}}_c^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000160 & $**$ & $\bar{\Xi}_c^0$, $\eta$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000140 & $**$ & $\bar{\Lambda}_c^-$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000100 & $**$ & $\bar{d}$, $c$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000100 & $**$ & $\bar{s}$, $u$, $\bar{u}$, $(\bar{s}\bar{u})_0$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.000090 & $**$ & $\bar{\Sigma}^0$, $\bar{D}^{*0}(2007)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.000060 & $**$ & $\bar{\Sigma}^0$, $\bar{D}^0$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
0.000040 & $**$ & $\bar{\Xi}_c^0$, $\eta'$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000030 & $**$ & $\bar{\Xi}_c^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000020 & $**$ & $\bar{\Lambda}^0$, $\bar{D}^{*0}(2007)$ & & Herwig::BaryonFactorized::BottomBaryonVector& \\ 
& & & & & \\ \hline
0.000020 & $**$ & $\bar{\Lambda}^0$, $\bar{D}^0$ & & Herwig::BaryonFactorized::BottomBaryonScalar& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
