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\begin{document}
\title{Check List for Particle : \boldmath{ $D^-$}}
\maketitle
\begin{center}
\begin{tabular}{|c|c|c|c||c|c|c|c|}
\hline
Quantity &\ \ \  Us \ \ \ &\ \ \ PDG \ \ \ &\ \ \  EvtGen \ \ \ & Quantity & \ \ \ Us \ \ \ & \ \ \ PDG \ \ \ & \ \ \ EvtGen \ \ \ \\ 
\hline
PDG  &-411 & & & Mass & 1869.3& &\\ 
Code & & & &      & & &\\ 
\hline 
Width  & 0& & & Gen  & \verb: D-: & &\\ 
       & & & & Name & & &\\ 
\hline
Decay  & $0.0003118$~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^- $ \ \ \ \ \ \ \ \ \ \ \ \ & 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 &s031 & & \\ 
\hline 
\end{tabular} 
\end{center} 
\begin{itemize}
\item Is the description present and correct?

The $D^-$ is the the lightest charged D meson. It mass and lifetime are well measured but the decay modes are less well known. The mass and width are taken from \cite{Yao:2006px}.
The majority of the decay modes are taken from \cite{Yao:2006px} together with additional modes, approximately 10\%, added to saturate the branching ratios.
\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 $D^-$ (continues).}
\endfoot
\caption{The decay modes of the $D^-$.}
\endlastfoot
\label{tab:-411decaymodes}
0.140000 & $****$ & $K^0$, $\pi^-$, $\pi^0$ & & Herwig::DtoKPiPiMarkIII::DtoKPiPiMarkIII& \\ 
& & & & & \\ \hline
0.095100 & $****$ & $K^+$, $\pi^-$, $\pi^-$ & & Herwig::DtoKPiPiE691::DKPiPiE691& \\ 
& & & & & \\ \hline
0.089200 & $*****$ & $K^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.086500 & $*****$ & $K^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.072000 & $****$ & $K^0$, $a_1^-(1260)$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.056600 & $*****$ & $K^{*0}$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.053600 & $*****$ & $K^{*0}$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.043000 & $****$ & $K^0_1(1400)$, $\pi^-$ & & Herwig::ScalarMesonFactorized::ISGW2Hadronic& \\ 
& & & & & \\ \hline
0.036000 & $***$ & $K^{*0}$, $\pi^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.032000 & $****$ & $K^{*-}$, $K^0$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.029600 & $*****$ & $K^0$, $\pi^-$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.026000 & $****$ & $K^{*-}$, $K^{*0}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.023000 & $***$ & $\phi$, $\pi^-$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.018800 & $***$ & $K^0$, $K^0$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.018000 & $***$ & $K^{*0}$, $\rho^-$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.018000 & $***$ & $K^{*+}$, $\pi^-$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.011000 & $***$ & $\pi^-$, $\pi^-$, $\pi^+$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.010000 & $***$ & $K^+$, $\pi^-$, $\pi^-$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.009400 & $****$ & $K^{*0}$, $a_1^-(1260)$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.009300 & $***$ & $K^-$, $K^+$, $\pi^-$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.009000 & $***$ & $K^+$, $\rho^-$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.007400 & $***$ & $K^0$, $\pi^-$, $\pi^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.006500 & $****$ & $\phi$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005920 & $****$ & $K^-$, $K^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005550 & $***$ & $K^{*0}_0(1430)$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005300 & $**$ & $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.005300 & $****$ & $\eta'$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004530 & $****$ & $K^-$, $K^{*0}$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.004400 & $****$ & $\pi^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.004400 & $***$ & $K^0$, $\rho^0$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.004400 & $****$ & $\pi^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.003700 & $***$ & $\pi^-$, $\pi^0$, $\pi^0$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.003500 & $****$ & $\eta$, $\pi^-$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.003000 & $*$ & $\pi^-$, $\pi^0$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.003000 & $*$ & $\pi^-$, $\pi^0$, $\pi^0$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.003000 & $*$ & $\pi^-$, $\pi^-$, $\pi^+$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002440 & $****$ & $\rho^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.002440 & $****$ & $\rho^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.002300 & $***$ & $\sigma$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.002100 & $**$ & $K^+$, $\pi^-$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002100 & $**$ & $K^+$, $\pi^-$, $e^-$, $\bar{\nu}_e$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.002000 & $**$ & $K_1^0(1270)$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.002000 & $**$ & $K_1^0(1270)$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001680 & $***$ & $\pi^-$, $\pi^-$, $\pi^-$, $\pi^+$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001614 & $*$ & $K^+$, $\pi^-$, $\pi^-$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^{*0}$, $\pi^-$, $\pi^0$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^{*0}$, $\pi^-$, $\pi^-$, $\pi^+$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^0$, $\pi^-$, $\pi^0$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^{*+}$, $\pi^-$, $\pi^-$, $\pi^0$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^{*+}$, $\pi^-$, $\pi^-$, $\pi^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001613 & $*$ & $K^0$, $\pi^-$, $\pi^-$, $\pi^+$, $\pi^0$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001600 & $***$ & $\omega$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001600 & $***$ & $\omega$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001290 & $***$ & $\eta$, $e^-$, $\bar{\nu}_e$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001290 & $***$ & $\eta$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::SemiLeptonicScalar::ISGW2& \\ 
& & & & & \\ \hline
0.001280 & $****$ & $\pi^0$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.001200 & $***$ & $\tau^-$, $\bar{\nu}_\tau$ & & Herwig::PScalarLeptonNeutrino::PScalarlnu& \\ 
& & & & & \\ \hline
0.001070 & $****$ & $\rho^0$, $\pi^-$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $K^0$, $\pi^0$, $e^-$, $\bar{\nu}_e$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.001000 & $**$ & $K^0$, $\pi^0$, $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000850 & $****$ & $f_2(1270)$, $\pi^-$ & & Herwig::ScalarMesonTensorScalar::STSDecayer& \\ 
& & & & & \\ \hline
0.000550 & $***$ & $K^+$, $\rho^0$, $\pi^-$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000480 & $***$ & $K^-$, $K^+$, $K^0$, $\pi^-$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000450 & $***$ & $\bar{K}^{*0}$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000440 & $****$ & $\mu^-$, $\bar{\nu}_\mu$ & & Herwig::PScalarLeptonNeutrino::PScalarlnu& \\ 
& & & & & \\ \hline
0.000410 & $***$ & $K^+$, $\pi^-$, $\pi^-$, $\pi^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000400 & $***$ & $f_0(980)$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000250 & $***$ & $K^-$, $\rho^0$ & & Herwig::ScalarMesonFactorized::WSBHadronic& \\ 
& & & & & \\ \hline
0.000230 & $***$ & $K^-$, $K^+$, $\pi^-$, $\pi^-$, $\pi^+$ & & Herwig::Mambo::Mambo& \\ 
& & & & & \\ \hline
0.000090 & $***$ & $f_0(980)$, $K^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000090 & $**$ & $K^-$, $K^-$, $K^+$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
0.000078 & $***$ & $\bar{K}_2^{*0}(1430)$, $\pi^-$ & & Herwig::Hw64::DecayME0& \\ 
& & & & & \\ \hline
\end{longtable}Total branching ratio is $1$.
\bibliography{particles}

\end{document}
