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\begin{document}
\title{\boldmath{ $D^+$}\ \ \ \ \ \ \ $****$}
\maketitle
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.
The $D^+$ has mass $1869.3$~MeV and is unstable. The $D^+$ has spin $0$, charge $1$ and is colour neutral.
 The $D^+$ is a meson and is from the $1^1S_0$ multiplet.The properties of the particle and its antiparticle are taken to be charge-conjugate to each other.
 The decay length is $0.0003118$~m. The PDG code is 411.
\setlongtables
\begin{longtable}[t]{|c|c|c|p{1in}|p{2.5in}|c|}
\hline
Branching & Rating & On/ & Outgoing  & Description & Decayer  \\ 
Ratio     &                                 & Off & 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 & $****$ & on & $ \bar{K}^0, \pi^+, \pi^0 $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::DtoKPiPiMarkIII::DtoKPiPiMarkIII \\ 
\hline
0.095100 & $****$ & on & $ K^-, \pi^+, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::DtoKPiPiE691::DKPiPiE691 \\ 
\hline
0.089200 & $*****$ & on & $ \bar{K}^0, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio from averaging the rates from \cite{Yao:2006px} including a phase-space factor of 1.031 for the electron mode relative to the electron mode.    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.086500 & $*****$ & on & $ \bar{K}^0, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio from averaging the rates from \cite{Yao:2006px} including a phase-space factor of 1.031 for the electron mode relative to the electron mode.    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.072000 & $****$ & on & $ \bar{K}^0, a_1^+(1260) $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.056600 & $*****$ & on & $ \bar{K}^{*0}, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio from averaging the rates from \cite{Yao:2006px} including a phase-space factor of 1.057 for the electron mode relative to the electron mode.    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.053600 & $*****$ & on & $ \bar{K}^{*0}, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio from averaging the rates from \cite{Yao:2006px} including a phase-space factor of 1.057 for the electron mode relative to the electron mode.    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.043000 & $****$ & on & $ \bar{K}_1(1400)^0, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::ISGW2Hadronic \\ 
\hline
0.036000 & $***$ & on & $ \bar{K}^{*0}, \pi^+, \pi^0 $  & Hadronic decay of $D^+$ with branching ratio reduced from that in \cite{Yao:2006px} to avoid oversaturating the $K^-\pi^+\pi^+\pi$ mode.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.032000 & $****$ & on & $ K^{*+}, \bar{K}^0 $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.029600 & $*****$ & on & $ \bar{K}^0, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.026000 & $****$ & on & $ K^{*+}, \bar{K}^{*0} $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.023000 & $***$ & on & $ \phi, \pi^+, \pi^0 $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px},.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.018800 & $***$ & on & $ \bar{K}^0, \bar{K}^0, K^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.018000 & $***$ & on & $ \bar{K}^{*0}, \rho^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.018000 & $***$ & on & $ K^{*-}, \pi^+, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio 1$\sigma$ below that in \cite{Yao:2006px} to avoid over-saturating the $\bar{K}^0\pi^+\pi^+\pi^-$ mode.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.011000 & $***$ & on & $ \pi^+, \pi^+, \pi^-, \pi^0 $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px} after the resonant modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.010000 & $***$ & on & $ K^-, \pi^+, \pi^+, \pi^0 $  & Decay of $D^+$ to $K^-$ and three pions with branching ratio from \cite{Yao:2006px} for the non-resonant contribution.    & Herwig::Mambo::Mambo \\ 
\hline
0.009400 & $****$ & on & $ \bar{K}^{*0}, a_1^+(1260) $  & Decay of $D^+$ to $K^{*0}$ and the $a_1$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.009300 & $***$ & on & $ K^+, K^-, \pi^+, \pi^0 $  & Decay of $D^+$ with branching ratio reduced from that in \cite{Yao:2006px} for the resonant modes and due to the large error.   & Herwig::Mambo::Mambo \\ 
\hline
0.009000 & $***$ & on & $ K^-, \rho^+, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px} for the 3-body component.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.007400 & $***$ & on & $ \bar{K}^0, \pi^+, \pi^+, \pi^- $  & Decay of $D^+$ with branching  ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.006500 & $****$ & on & $ \phi, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005920 & $****$ & on & $ K^+, \bar{K}^0 $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005550 & $***$ & on & $ \bar{K}^{*0}_0(1430), K^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px} including the $K^-\pi^+$ mode of the $\bar{K}^{*0}_0$   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005300 & $**$ & on & $ \pi^+![\bar{K}^{*0}(1680) \to K^-, \pi^+] $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005300 & $****$ & on & $ \eta', \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.004530 & $****$ & on & $ K^+, \bar{K}^{*0} $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px} including the $K^-\pi^+$ mode of the $\bar{K}^{*0}$.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.004400 & $****$ & on & $ \pi^0, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.004400 & $****$ & on & $ \pi^0, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.004400 & $***$ & on & $ \bar{K}^0, \rho^0, \pi^+ $  & Decay of the $D^+$ with branching ratio from \cite{Yao:2006px} for the three-body component.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003700 & $***$ & on & $ \pi^+, \pi^0, \pi^0 $  & Decay of $D^+$ to with branching ratio from \cite{Yao:2006px} after the resonant modes have been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003500 & $****$ & on & $ \eta, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.003000 & $*$ & on & $ \pi^+, \pi^0, \pi^0, \pi^0 $  & Mode added to produce four pion modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.003000 & $*$ & on & $ \pi^+, \pi^+, \pi^-, \pi^0, \pi^0 $  & Mode added to produce five pion modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.003000 & $*$ & on & $ \pi^+, \pi^0, \pi^0, \pi^0, \pi^0 $  & Mode added to produce five pion modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.002440 & $****$ & on & $ \rho^0, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px}.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.002440 & $****$ & on & $ \rho^0, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px}.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.002300 & $***$ & on & $ \sigma, \pi^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002100 & $**$ & on & $ K^-, \pi^+, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio set to the value from \cite{Yao:2006px} for the muon mode.   & Herwig::Mambo::Mambo \\ 
\hline
0.002100 & $**$ & on & $ K^-, \pi^+, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio set to the value from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.002000 & $**$ & on & $ \bar{K}_1(1270)^0, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio calculated from the rate for the $D^0$ mode from \cite{Artuso:2007wa}  and assuming the partial widths are equal.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.002000 & $**$ & on & $ \bar{K}_1(1270)^0, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio calculated from the rate for the $D^0$ mode from \cite{Artuso:2007wa}  and assuming the partial widths are equal.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001680 & $***$ & on & $ \pi^+, \pi^+, \pi^+, \pi^-, \pi^- $  & Decay of $D^+$ to five charged pions with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.001614 & $*$ & on & $ K^-, \pi^+, \pi^+, \pi^0, \pi^0 $  & Decay of $D^+$ added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ \bar{K}^0, \pi^+, \pi^+, \pi^-, \pi^0 $  & Decay of $D^+$ added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ \bar{K}^0, \pi^+, \pi^0, \pi^0, \pi^0 $  & Decay of $D^+$ added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ \bar{K}^{*0}, \pi^+, \pi^+, \pi^-, \pi^0 $  & Multi-body decay mode added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ \bar{K}^{*0}, \pi^+, \pi^0, \pi^0, \pi^0 $  & Multi-body decay mode added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ K^{*-}, \pi^+, \pi^+, \pi^+, \pi^- $  & Multi-body decay mode added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001613 & $*$ & on & $ K^{*-}, \pi^+, \pi^+, \pi^0, \pi^0 $  & Multi-body decay mode added to ensure the branching ratios sum to one.   & Herwig::Mambo::Mambo \\ 
\hline
0.001600 & $***$ & on & $ \omega, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Yao:2006px} for the electron mode.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001600 & $***$ & on & $ \omega, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Yao:2006px} for the electron mode.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001290 & $***$ & on & $ \eta, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Gao:2006talk}    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001290 & $***$ & on & $ \eta, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio from \cite{Gao:2006talk}    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001280 & $****$ & on & $ \pi^0, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001200 & $***$ & on & $ \tau^+, \nu_\tau $  & Leptonic decay of the $D^+$. The branching ratio is calculated using the matrix element and the value for the muon mode.   & Herwig::PScalarLeptonNeutrino::PScalarlnu \\ 
\hline
0.001070 & $****$ & on & $ \rho^0, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.001000 & $**$ & on & $ \bar{K}^0, \pi^0, \mu^+, \nu_\mu $  & Semi-leptonic decay of $D^+$ with branching ratio taken to be half the $K^-\pi^+$ value.   & Herwig::Mambo::Mambo \\ 
\hline
0.001000 & $**$ & on & $ \bar{K}^0, \pi^0, e^+, \nu_e $  & Semi-leptonic decay of $D^+$ with branching ratio taken to be half the $K^-\pi^+$ value.   & Herwig::Mambo::Mambo \\ 
\hline
0.000850 & $****$ & on & $ f_2(1270), \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonTensorScalar::STSDecayer \\ 
\hline
0.000550 & $***$ & on & $ K^-, \rho^0, \pi^+, \pi^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000480 & $***$ & on & $ K^+, K^-, \bar{K}^0, \pi^+ $  & Hadronic decay of $D^+$ with branching ratio from \cite{Yao:2006px}. This mode is not included in EvtGen.   & Herwig::Mambo::Mambo \\ 
\hline
0.000450 & $***$ & on & $ K^{*0}, \pi^+ $  & Doubly cabibbo supressed modes with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000440 & $****$ & on & $ \mu^+, \nu_\mu $  & Leptonic decay of the $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::PScalarLeptonNeutrino::PScalarlnu \\ 
\hline
0.000410 & $***$ & on & $ K^-, \pi^+, \pi^+, \pi^+, \pi^- $  & Non-resonant mode with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000400 & $***$ & on & $ f_0(980), \pi^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000250 & $***$ & on & $ K^+, \rho^0 $  & Doubly cabibbo supressed modes with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.000230 & $***$ & on & $ K^+, K^-, \pi^+, \pi^+, \pi^- $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000090 & $***$ & on & $ f_0(980), K^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px}. 
   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000090 & $**$ & on & $ K^+, K^+, K^- $  & Doubly cabibbo supressed modes with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000078 & $***$ & on & $ K_2^{*0}(1430), \pi^+ $  & Decay of $D^+$ with branching ratio from \cite{Yao:2006px} including the $K^-\pi^+$ mode of the $K^*_2$   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $D^+$ decay modes are given in Table~\ref{tab:411decaymodes} and the total branching ratio is $1$.


 There is no mass generator for the $D^+$.
 There is no width generator for the $D^+$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 16:20:13 on the 15th of May 2008. The most recently changed decay mode was modified at 19:14:56 on the 10th of May 2008. The particle data was last modified at 21:34:27 on the 22nd of August 2007.

\end{document}
