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\begin{document}
\title{Check List for Particle : \boldmath{ $D_s^+$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &431 & & & Mass & 1968.2& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: D_s+: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0.00015$~m.& & &   & & &\\ 
Length & & & & & & &\\ 
\hline 
\end{tabular} 
\end{center} 
\vspace{2cm}
\begin{center}
\begin{tabular}{|c|c|c|c|c|c|c|c|}
\hline
Latex Name  & $D_s^+ $ \ \ \ \ \ \ \ \ \ \ \ \ & 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 &s034 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $D_s^+$ is the lightest meson containing a charm and a strange quark, it decays weakly. The mass and lifetime are well measured but the decay modes aren't as well known. The mass and lifetime are taken from \cite{Yao:2006px}. We take the majority of the decay modes from \cite{Yao:2006px} together with the addition of some additional modes, about 10\% of the branching ratio, to saturate the 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 $D_s^+$ (continues).}
\endfoot
\caption{The decay modes of the $D_s^+$.}
\endlastfoot
\label{tab:431decaymodes}
0.131000 & $*****$ & $\eta$, $\rho^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.122000 & $*****$ & $\eta'$, $\rho^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.082000 & $*****$ & $\phi$, $\rho^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.071700 & $*****$ & $\tau^+$, $\nu_\tau$ & & Herwig::PScalarLeptonNeutrino::PScalarlnu& \\ 
& & & & & \\ \hline
0.070000 & $*****$ & $K^{*+}$, $\bar{K}^{*0}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.053000 & $*****$ & $K^{*+}$, $\bar{K}^0$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.047000 & $*****$ & $\eta'$, $\pi^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.044000 & $*****$ & $\phi$, $\pi^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.044000 & $*****$ & $K^+$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.037500 & $*****$ & $K^+$, $\bar{K}^{*0}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.031500 & $*****$ & $\eta$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.030500 & $*****$ & $\eta$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.029000 & $*****$ & $a_1^+(1260)$, $\phi$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.024700 & $*****$ & $\phi$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.023300 & $*****$ & $\phi$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.021100 & $*****$ & $\eta$, $\pi^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.011100 & $*****$ & $\eta'$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.010500 & $*****$ & $\eta'$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.010000 & $**$ & $\eta$, $a_1^+(1260)$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.009000 & $**$ & $K^0$, $\rho^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.008000 & $***$ & $f_0(980)$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.007600 & $***$ & $\pi^+$, $\pi^+$, $\pi^+$, $\pi^-$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.007400 & $****$ & $\mu^+$, $\nu_\mu$ & & Herwig::PScalarLeptonNeutrino::PScalarlnu& \\ 
& & & & & \\ \hline
0.007200 & $****$ & $K^+$, $\bar{K}^{*0}_0(1430)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005000 & $**$ & $\rho^0(1450)$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005000 & $**$ & $f_0(1370)$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004500 & $**$ & $K^0$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004500 & $**$ & $K^0$, $a_1^+(1260)$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.004200 & $**$ & $K^{*0}$, $\rho^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.003400 & $****$ & $\omega$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002600 & $****$ & $K^+$, $\rho^0$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.002500 & $*$ & $K^+_1(1400)$, $\bar{K}^{*0}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002500 & $**$ & $K^+$, $\rho^0(1450)$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002500 & $*$ & $K^+_1(1400)$, $\bar{K}^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002500 & $*$ & $K^+$, $\bar{K}_1(1400)^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002500 & $*$ & $K^{*+}$, $\bar{K}_1(1400)^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002200 & $**$ & $K^0$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.002200 & $**$ & $K^0$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.002100 & $****$ & $f_2(1270)$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002100 & $****$ & $K^{*0}$, $\pi^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.002100 & $**$ & $K^{*0}$, $a_1^+(1260)$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.001230 & $**$ & $K^+$, $K^-$, $\pi^+$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001220 & $**$ & $K^0$, $K^-$, $\pi^+$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001220 & $**$ & $K^+$, $\bar{K}^0$, $\pi^+$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001220 & $**$ & $K^0$, $\bar{K}^0$, $\pi^+$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $K^+$, $\pi^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\phi$, $K^{*+}$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001000 & $*****$ & $K^{*0}$, $e^+$, $\nu_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\eta$, $K^{*+}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\eta'$, $K^{*+}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\eta'$, $K^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $\eta$, $K^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.000970 & $*****$ & $K^{*0}$, $\mu^+$, $\nu_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.000750 & $**$ & $K^{*0}_0(1430)$, $\pi^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000320 & $***$ & $K^+$, $K^-$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000300 & $**$ & $\phi$, $K^+$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.000270 & $**$ & $K^+$, $K^+$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
