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\title{\boldmath{ $\bar{D}^0$}\ \ \ \ \ \ \ $****$}
\maketitle
 The $\bar{D}^0$ is the lightest charm meson, its mass and lifetime are accurately measured but the decay modes are less wel known.
The $\bar{D}^0$ has mass $1864.5$~MeV and is unstable. The $\bar{D}^0$ has spin $0$, charge $0$ and is colour neutral.
 The $\bar{D}^0$ 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 $0.000123$~m. The PDG code is -421.
\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 $\bar{D}^0$ (continues).}
\endfoot
\caption{The decay modes of the $\bar{D}^0$.}
\endlastfoot
\label{tab:-421decaymodes}
0.141000 & $*****$ & on & $ K^+, \pi^-, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::DtoKPiPiCLEO::DKPiPiCLEO \\ 
\hline
0.075000 & $****$ & on & $ K^+, a_1^-(1260) $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.064000 & $****$ & on & $ K^{*+}, \rho^- $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.038000 & $*****$ & on & $ K^+, \pi^- $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.034400 & $*****$ & on & $ K^+, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px} including a phase-space factor of 1.033 for the ratio of the two modes.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.033300 & $*****$ & on & $ K^+, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px} including a phase-space factor of 1.033 for the ratio of the two modes.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.029000 & $*****$ & on & $ K^0_S, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::DtoKPiPiCLEO::DKPiPiCLEO \\ 
\hline
0.029000 & $*****$ & on & $ K^0_L, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::DtoKPiPiCLEO::DKPiPiCLEO \\ 
\hline
0.023000 & $***$ & on & $ K^+, \pi^-, \omega $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the $\bar{K}^{*0}\omega$ mode has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.022000 & $***$ & on & $ K^0, \pi^-, \pi^+, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the non-resonant component.   & Herwig::Mambo::Mambo \\ 
\hline
0.021400 & $*****$ & on & $ K^{*+}, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px} including a phase-space factor of 1.055 for the ratio of the two modes.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.020300 & $*****$ & on & $ K^{*+}, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the electron and muon modes from \cite{Yao:2006px} including a phase-space factor of 1.055 for the ratio of the two modes.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.018200 & $****$ & on & $ K^0, \eta' $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.016599 & $*$ & on & $ K^0, \pi^0, \pi^0, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.016599 & $*$ & on & $ K^0, \pi^-, \pi^+, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.016599 & $*$ & on & $ K^+, \pi^-, \pi^0, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.016598 & $*$ & on & $ K^0, \pi^0, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to saturate the branching ratio   & Herwig::Mambo::Mambo \\ 
\hline
0.016598 & $*$ & on & $ K^+, \pi^-, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to saturate the branching ratio   & Herwig::Mambo::Mambo \\ 
\hline
0.015500 & $***$ & on & $ K^+, \pi^-, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the non-resonant component lowed to avoid oversaturating the mode.   & Herwig::Mambo::Mambo \\ 
\hline
0.015000 & $****$ & on & $ K^{*0}, \rho^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.014600 & $***$ & on & $ K^{*0}, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.012600 & $***$ & on & $ \pi^0,[K^{*0} \to K^0, \pi^0] $  & Decay of $\bar{D}^0$ with decay mode of $\bar{K}^{*0}$ specified to give piece not included in the Dalitz mode.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.011700 & $***$ & on & $ K^0, a^0_0(980) $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} including the decay $a^0_0\to\eta\pi^0$.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.011400 & $*****$ & on & $ K^0_S, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.011400 & $*****$ & on & $ K^0_L, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.011200 & $****$ & on & $ K_1^+(1270), \pi^- $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::ISGW2Hadronic \\ 
\hline
0.011000 & $****$ & on & $ K^0_S![\omega \to \pi^+, \pi^-] $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.    & Herwig::Hw64::DecayME0 \\ 
\hline
0.011000 & $****$ & on & $ K^0_L![\omega \to \pi^+, \pi^-] $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.
   & Herwig::Hw64::DecayME0 \\ 
\hline
0.011000 & $****$ & on & $ K^{*0}, \omega $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.010200 & $**$ & on & $ K^{*+}, a_1^-(1260) $  & Decay of $\bar{D}^0$ with branching ratio from the $K^{*-}\rho^0\pi^+$ mode assuming this is from $a_1$.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.010000 & $*$ & on & $ K_1^+(1270), \rho^- $  & Decay of $\bar{D}^0$ added to ensure the branching ratios sum to one.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.009000 & $*$ & on & $ K^{*+}, \pi^-, \pi^0, \pi^0, \pi^0 $  & Decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.009000 & $*$ & on & $ K^{*+}, \pi^-, \pi^-, \pi^+, \pi^0 $  & Decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.009000 & $*$ & on & $ K^{*0}, \pi^-, \pi^+, \pi^0, \pi^0 $  & Decay of $\bar{D}^0$ which is added to saturate the branching ratio.   & Herwig::Mambo::Mambo \\ 
\hline
0.009000 & $***$ & on & $ K^{*0}, \eta $  & Hadronic dcay of $\bar{D}^0$ with branching ratio from the contribution to the $K^0_s\eta\pi^0$ mode from \cite{Yao:2006px}.    & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.008780 & $***$ & on & $ \pi^+, a_1^-(1260) $  & Decay of $\bar{D}^0$ with branching ratio obtained by multiplying the branching ratio for $\pi^+\pi^+\pi^-\pi^-$ by the fit fraction from \cite{Link:2007fi}    & Herwig::ScalarMesonFactorized::ISGW2Hadronic \\ 
\hline
0.008600 & $****$ & on & $ K^0, \phi $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the $\phi\toK^+K^-$ mode.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.008500 & $***$ & on & $ K^+, \pi^-, \pi^-, \pi^+, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the resonant modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.008400 & $***$ & on & $ K^0, \pi^0, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the non-resonant component.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.008000 & $***$ & on & $ K^{*0}, a_1^0(1260) $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the $\bar{K}^{*0}\eta$ and $\bar{K}^{*0}\omega$ modes have been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.007600 & $****$ & on & $ K^0, \eta $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.007500 & $***$ & on & $ \rho^-, \pi^+ $  & Unobserved decay of $\bar{D}^0$ wwith branching ratio from \cite{Yao:2006px} scaled down to avoid over-saturating the $\pi^+\pi^-\pi^0$ mode.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.006500 & $***$ & on & $ K^+, \pi^-, \eta' $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after our assumed $\bar{K}^{*0}\eta'$ contribution has been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005400 & $***$ & on & $ \bar{K}^0, K^0, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the $\phi\rho^0$ mode has been subtracted. This is significantly higher than the value used in EvtGen.   & Herwig::Mambo::Mambo \\ 
\hline
0.005000 & $*$ & on & $ K^+_1(1400), \pi^- $  & Decay of $\bar{D}^0$ added to ensure the branching ratios sum to one.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.005000 & $*$ & on & $ K^+_1(1400), \rho^- $  & Decay of $\bar{D}^0$ added to ensure the branching ratios sum to one.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.004900 & $***$ & on & $ K^+, \pi^-, \rho^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the non-resonant piece.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003900 & $***$ & on & $ K^+, \pi^0, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$. This mode is included to ensure that the total semi-leptonic branching ratio is $6.71\%$ from \cite{Yao:2006px}. The excess after the exclusive modes is split into $K\pi$ modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.003900 & $***$ & on & $ K^+, \pi^0, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$. This mode is included to ensure that the total semi-leptonic branching ratio is $6.71\%$ from \cite{Yao:2006px}. The excess after the exclusive modes is split into $K\pi$ modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.003840 & $****$ & on & $ K^-, K^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003800 & $***$ & on & $ K^0, K^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the resonant modes have been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.003700 & $****$ & on & $ K^{*-}, K^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.003200 & $****$ & on & $ \rho^+, \pi^- $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} but scaled down to give the correct $\pi^+\pi^-\pi^0$ rate.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.003100 & $***$ & on & $ K^+, K^-, \pi^-, \pi^+, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}. This is not included in EvtGen.   & Herwig::Mambo::Mambo \\ 
\hline
0.003000 & $*$ & on & $ \rho^-, \rho^+ $  & Unobserved decay of $\bar{D}^0$ which is seems a reasonable component of the $\pi^+\pi^-\pi^0\pi^0$ mode.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.002900 & $***$ & on & $ \pi^0,[K^{*0}_0(1430) \to K^0, \pi^0] $  & Hadronic decay of $\bar{D}^0$ this is the left over piece of the $\bar{K}^*_0(1430)$ not included in the Dalitz decays.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002750 & $****$ & on & $ \pi^+, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the values for the electron and muon modes from \cite{Yao:2006px} with a relative phase space factor of $1.023$.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.002680 & $***$ & on & $ \pi^-, \pi^-, \pi^+, \pi^+, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the $\omega\pi^+\pi^-$ contribution has been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.002680 & $****$ & on & $ \pi^+, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio calculated by averaging the values for the electron and muon modes from \cite{Yao:2006px} with a relative phase space factor of $1.023$.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.002300 & $***$ & on & $ K_1^-(1270), K^+ $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002200 & $***$ & on & $ \rho^0, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} scaled down to avoid oversaturating the $\pi^+\pi^-\pi^0$ mode.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.002200 & $***$ & on & $ \bar{K}^0, K^+, \pi^- $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the subtraction of the resonant modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.002200 & $***$ & on & $ K^0, \rho^0, \pi^-, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.002000 & $****$ & on & $ K^{*+}, K^- $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.001900 & $***$ & on & $ K^0, \pi^+, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$. This mode is included to ensure that the total semi-leptonic branching ratio is $6.71\%$ from \cite{Yao:2006px}. The excess after the exclusive modes is split into $K\pi$ modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.001900 & $***$ & on & $ K^0, \pi^+, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$. This mode is included to ensure that the total semi-leptonic branching ratio is $6.71\%$ from \cite{Yao:2006px}. The excess after the exclusive modes is split into $K\pi$ modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.001900 & $****$ & on & $ \rho^+, e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001800 & $****$ & on & $ \rho^+, \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} and a small phase-space supression for the muon mode.   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.001790 & $***$ & on & $ \rho^0, \rho^0 $  & Decay of $\bar{D}^0$ with branching ratio obtained by multiplying the branching ratio for $\pi^+\pi^+\pi^-\pi^-$ by the fit fraction from \cite{Link:2007fi} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001710 & $*$ & on & $ \pi^-, \pi^+, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the resonant sub-modes have been subtracted.   & Herwig::Mambo::Mambo \\ 
\hline
0.001600 & $***$ & on & $ \omega, \pi^-, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001500 & $*$ & on & $ K_1^-(1270), K^{*+} $  & Decay of $\bar{D}^0$ added to increase the rate of Cabibbo supressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001500 & $*$ & on & $ K^-_1(1400), K^{*+} $  & Decay of $\bar{D}^0$ added to increase the rate of Cabibbo supressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001480 & $***$ & on & $ \bar{K}^0, K^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for $K^0_SK^0_S$.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001400 & $**$ & on & $ \phi, \omega $  & Decay of $\bar{D}^0$ added to ensure the branching ratio sums to one. The branching ratio is set equal to the observed $\phi\rho^0$ mode.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.001400 & $****$ & on & $ \phi, \rho^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.001364 & $****$ & on & $ \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}. This is lower than the value in EvtGen.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001360 & $***$ & on & $ K^0,[f_0(980) \to \pi^0, \pi^0] $  & Decay of $\bar{D}^0$ for the $\pi^0\pi^0$ component of the $f_0$ as the $\pi^+\pi^-$ component is part of the Dalitz decay.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001320 & $***$ & on & $ K^+, a^-_0(980) $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} including the decay of the $a^+_0$ to kaons.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001200 & $***$ & on & $ K^-_1(1400), K^+ $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001000 & $*$ & on & $ \pi^-, \pi^+, \pi^0, \pi^0, \pi^0 $  & Unobserved decay of $\bar{D}^0$ which is added to increase the rate of the cabibbo surpressed modes.   & Herwig::Mambo::Mambo \\ 
\hline
0.001000 & $**$ & on & $ K^{*0}, \eta' $  & Unobserved decay of $\bar{D}^0$ which is below the experimental limit   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.001000 & $**$ & on & $ K^{*0}, \bar{K}^0 $  & Hadronic decay of $\bar{D}^0$. This mode has not been observed and is added below the experimental limit from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.001000 & $*$ & on & $ \pi^-, \pi^+, \pi^-, \pi^+, \pi^0, \pi^0 $  & Decay of $\bar{D}^0$ added to increase the rate of Cabibbo supressed mode   & Herwig::Mambo::Mambo \\ 
\hline
0.001000 & $*$ & on & $ \pi^-, \pi^+, \pi^0, \pi^0, \pi^0, \pi^0 $  & Decay of $\bar{D}^0$ added to increase the rate of Cabibbo supressed mode   & Herwig::Mambo::Mambo \\ 
\hline
0.000930 & $***$ & on & $ K^0_S, K^0_S, K^0_S $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000900 & $***$ & on & $ \sigma, \pi^-, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio obtained by multiplying the branching ratio for $\pi^+\pi^+\pi^-\pi^-$ by the fit fraction from \cite{Link:2007fi} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000790 & $****$ & on & $ \pi^0, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000760 & $***$ & on & $ K_1^+(1270), e^-, \bar{\nu}_e $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio from \cite{Artuso:2007wa} . 
   & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.000760 & $***$ & on & $ K_1^+(1270), \mu^-, \bar{\nu}_\mu $  & Semi-leptonic decay of $\bar{D}^0$ with branching ratio from \cite{Artuso:2007wa} .    & Herwig::SemiLeptonicScalar::ISGW2 \\ 
\hline
0.000740 & $****$ & on & $ \phi, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.000630 & $***$ & on & $ f_2(1270), \pi^-, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio obtained by multiplying the branching ratio for $\pi^+\pi^+\pi^-\pi^-$ by the fit fraction from \cite{Link:2007fi} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000610 & $***$ & on & $ K^0_S, K^0_S, K^+, \pi^- $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000600 & $**$ & on & $ \bar{K}^{*0}, K^0 $  & Hadronic decay of $\bar{D}^0$. This mode has not been observed and is included below the experimental limit from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000560 & $***$ & on & $ \eta, \pi^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000498 & $**$ & on & $ K^-, a_1^+(1260) $  & Hadronic decay of $\bar{D}^0$ with branching ratio calculated from \cite{Yao:2006px} using the $K^+\pi^+\pi^+\pi^-$ rate and the assumption this is dominated by $a_1$.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000400 & $***$ & on & $ \pi^-, \pi^-, \pi^-, \pi^+, \pi^+, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Mambo::Mambo \\ 
\hline
0.000380 & $***$ & on & $ K^{*0}, K^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000360 & $***$ & on & $ f_0(980), \pi^-, \pi^+ $  & Decay of $\bar{D}^0$ with branching ratio obtained by multiplying the branching ratio for $\pi^+\pi^+\pi^-\pi^-$ by the fit fraction from \cite{Link:2007fi} .   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000319 & $***$ & on & $ K^-, \pi^+, \pi^0 $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} after the resonant contributions have been subtracted.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000310 & $***$ & on & $ K^{*0}, \phi $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.    & Herwig::Hw64::DecayME0 \\ 
\hline
0.000210 & $***$ & on & $ K^+, \pi^-, \pi^-, \pi^-, \pi^+, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.    & Herwig::Mambo::Mambo \\ 
\hline
0.000160 & $***$ & on & $ \bar{K}^{*0}, K^{*0} $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000143 & $****$ & on & $ K^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}. This mode is doubly cabibbo supressed.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000140 & $***$ & on & $ \phi, \eta $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.000100 & $*$ & on & $ K^-_1(1400), \pi^+ $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $*$ & on & $ K_1^-(1270), \pi^+ $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $***$ & on & $ \pi^+,[K^{*-} \to K^-, \pi^0] $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the piece not in the Dalitz decay.   & Herwig::ScalarMesonFactorized::WSBHadronic \\ 
\hline
0.000100 & $*$ & on & $ K^-_1(1400), \rho^+ $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $*$ & on & $ K_1^-(1270), \rho^+ $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $*$ & on & $ K^{*-}, a_1^+(1260) $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $*$ & on & $ K_1^-(1270), a_1^+(1260) $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000100 & $*$ & on & $ K^-_1(1400), a_1^+(1260) $  & Decay of $\bar{D}^0$ added to increase the rate of the doubly cabibbo surpressed modes.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000050 & $***$ & on & $ K^+, K^-, \rho^0 $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the three body component.   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000047 & $***$ & on & $ \phi, \pi^-, \pi^+ $  & Hadronic decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the three-body component   & Herwig::Hw64::DecayME0 \\ 
\hline
0.000032 & $***$ & on & $ K^+, K^-, K^+, \pi^- $  & Decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px} for the non-resonant component.   & Herwig::Mambo::Mambo \\ 
\hline
0.000024 & $***$ & on & $ \phi, \gamma $  & Radiative decay of $\bar{D}^0$ with branching ratio from \cite{Yao:2006px}.   & Herwig::Hw64::DecayME0 \\ 
\hline
\end{longtable}The $\bar{D}^0$ decay modes are given in Table~\ref{tab:-421decaymodes} and the total branching ratio is $1$.


 There is no mass generator for the $\bar{D}^0$.
 There is no width generator for the $\bar{D}^0$.

\bibliography{particles}


 The particle was checked by Peter Richardson at 16:19:30 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 14:51:40 on the 3rd of August 2007.

\end{document}
