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\begin{document}
\title{Check List for Particle : \boldmath{ $B^-_c$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &-541 & & & Mass & 6286& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: B_c-: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0.000138$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $B^-_c $ \ \ \ \ \ \ \ \ \ \ \ \ & Mass Gen.   & \verb:: \ \ & Width Gen.  & \verb:: \ \ & Type        & meson \ \ \ \ \ \\ 
& & & & & & & \\ 
\hline
Type        & normal \ \ \ & Con. Mass   & 0 \ \ \ \ & Rating      &$***$ \ \ \ \ \ \ \ \ \ \ \ \ &Variable    & fixed \\ 
& & & & & & Ratio & \\ 
\hline
Stable & unstable & Spin   & $0$& Charge & $-1$ & Colour & 0\\ 
&&&&&&& \\ 
 \hline
Lower Cut & 0& Upper cut & 0& PDG link &s091 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $B^-_c$ is the lightest meson containing a bottom and a charm quark. It has been observed and the mass and lifetime measured but only one decay mode and no branching ratios are known. The mass and lifetime are taken from \cite{Yao:2006px}. The branching ratios for the exclusive modes are taken from \cite{Kiselev:2003mp} , as in EvtGen. The remaining partonic modes have been add to ensure the branching ratios sum to one and roughly give the totals for the exclusive modes taken from \cite{Kiselev:2003mp} .
\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 $B^-_c$ (continues).}
\endfoot
\caption{The decay modes of the $B^-_c$.}
\endlastfoot
\label{tab:-541decaymodes}
0.202000 & $*$ & $\bar{B}_s^{*0}$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.164000 & $*$ & $\bar{B}_s^{0}$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.072000 & $*$ & $\bar{B}_s^{0}$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.065000 & $*$ & $\bar{B}_s^{*0}$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.050600 & $*$ & $\bar{B}_s^{*0}$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.050600 & $*$ & $\bar{B}_s^{*0}$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.049000 & $*$ & $\bar{c}$, $s$ & & Herwig::Quarkonium::QDecayME0& \\ 
& & & & & \\ \hline
0.040300 & $*$ & $\bar{B}_s^{0}$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.040300 & $*$ & $\bar{B}_s^{0}$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.025700 & $*$ & $\bar{B}^{*0}$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.019800 & $*$ & $B^-$, $K^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.019000 & $*$ & $J/\psi(1S)$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.019000 & $*$ & $J/\psi(1S)$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.016700 & $*$ & $B^{*-}$, $K^{*0}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.016000 & $*$ & $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::PScalarLeptonNeutrino::PScalarlnu& \\ 
& & & & & \\ \hline
0.016000 & $*$ & $B^{*-}$, $K^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.011134 & $*$ & $d$, $\bar{u}$, $c$, $\bar{c}$ & & Herwig::WeakPartonic::WeakPartonic100& \\ 
& & & & & \\ \hline
0.010600 & $*$ & $\bar{B}^0$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.010600 & $*$ & $\bar{B}_s^{0}$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.009600 & $*$ & $\bar{B}^0$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.009500 & $*$ & $\bar{B}^{*0}$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.007500 & $*$ & $\eta_c$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.007500 & $*$ & $\eta_c$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.006700 & $*$ & $J/\psi(1S)$, $D_s^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.005800 & $*$ & $\bar{B}^{*0}$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.005800 & $*$ & $\bar{B}^{*0}$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.004800 & $*$ & $J/\psi(1S)$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.004300 & $*$ & $B^-$, $K^{*0}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.004200 & $*$ & $\eta_c$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.004000 & $*$ & $J/\psi(1S)$, $\rho^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.003700 & $*$ & $\bar{B}_s^{*0}$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.003400 & $*$ & $\bar{B}^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.003400 & $*$ & $\bar{B}^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.002800 & $*$ & $\eta_c$, $D_s^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.002700 & $*$ & $\eta_c$, $D_s^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.002300 & $*$ & $\eta_c$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.002000 & $*$ & $\eta_c$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.001700 & $*$ & $J/\psi(1S)$, $D_s^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.001300 & $*$ & $J/\psi(1S)$, $\pi^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000940 & $*$ & $\psi(2S)$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000940 & $*$ & $\psi(2S)$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000900 & $*$ & $B^{*-}$, $\rho^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000700 & $*$ & $\bar{B}^0$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000580 & $*$ & $\bar{B}^{*0}$, $K^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000550 & $*$ & $\bar{B}^{*0}$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000370 & $*$ & $B^-$, $\pi^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000340 & $*$ & $B^-$, $\rho^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000330 & $*$ & $B^{*-}$, $\pi^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000330 & $*$ & $D^{*-}(2010)$, $D^{*0}(2007)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000280 & $*$ & $J/\psi(1S)$, $D^{*-}(2010)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000220 & $*$ & $J/\psi(1S)$, $K^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000200 & $*$ & $\eta_c(2S)$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000200 & $*$ & $\eta_c(2S)$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000200 & $*$ & $\eta_c$, $K^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000180 & $*$ & $\bar{D}^{*0}(2007)$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000180 & $*$ & $\bar{D}^{*0}(2007)$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000150 & $*$ & $\bar{B}^0$, $K^{*-}$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000150 & $*$ & $\eta_c$, $D^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000130 & $*$ & $\eta_c$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000110 & $*$ & $J/\psi(1S)$, $K^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000100 & $*$ & $\eta_c$, $D^{*-}(2010)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000090 & $*$ & $J/\psi(1S)$, $D^-$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000080 & $*$ & $\psi(2S)$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000080 & $*$ & $\bar{D}^{*0}(2007)$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000075 & $*$ & $D^-$, $D^{*0}(2007)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000053 & $*$ & $D^-$, $D^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000049 & $*$ & $D^{*-}(2010)$, $D^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000040 & $*$ & $\bar{D}^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000040 & $*$ & $\bar{D}^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000026 & $*$ & $D_s^{*-}$, $D^{*0}(2007)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000020 & $*$ & $\bar{D}^0$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000016 & $*$ & $\eta_c(2S)$, $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::SemiLeptonicScalar::KiselevBc& \\ 
& & & & & \\ \hline
0.000007 & $*$ & $D_s^-$, $D^{*0}(2007)$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000005 & $*$ & $D_s^-$, $D^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
0.000005 & $*$ & $D_s^{*-}$, $D^0$ & & Herwig::ScalarMesonFactorized::BcHadronic& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
