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${{\mathit D}^{0}}$ MASS
$1864.84 \pm0.04$ MeV
${\mathit m}_{{{\mathit D}^{\pm}}}{\mathit m}_{{{\mathit D}^{0}}}$
$4.822 \pm0.015$ MeV
${{\mathit D}^{0}}$ MEAN LIFE
$(4.103 \pm0.010) \times 10^{-13}$ s
$\vert{}{\mathit m}_{{{\mathit D}_{{{1}}}^{0}}}{\mathit m}_{{{\mathit D}_{{{2}}}^{0}}}\vert{}$ = $x$ $\Gamma $
$(99.7 \pm11.6) \times 10^{8}$ $\hbar{}$ s${}^{-1}$
($\Gamma _{{{\mathit D}_{{{1}}}^{0}}}$ $-$ $\Gamma _{{{\mathit D}_{{{2}}}^{0}}})/\Gamma $ = 2$\mathit y$
$0.01394 \pm0.00056$
$\vert $q/p$\vert $
$0.995 \pm0.016$
A$_{\Gamma }$
$0.000089 \pm0.000113$
$\phi {}^{{{\mathit K}_S^0} {{\mathit \pi}} {{\mathit \pi}}}$
$0.02 {}^{+0.04}_{-0.05}$
cos $ \delta $
$0.990 \pm0.025$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$ COHERENCE FACTOR $\mathit R_{{{\mathit K}} {{\mathit \pi}} {{\mathit \pi}^{0}}}$
$0.792 \pm0.033$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{{{\mathit K}} {{\mathit \pi}} {{\mathit \pi}^{0}}}$
$198 \pm10$ $^\circ{}$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{+}}$ COHERENCE FACTOR $\mathit R_{{{\mathit K}}3 {{\mathit \pi}}}$
$0.52 {}^{+0.10}_{-0.09}$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{+}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{{{\mathit K}}3 {{\mathit \pi}}}$
$149 {}^{+26}_{-16}$ $^\circ{}$ (S = 1.4)
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{+}}$, $\mathit R_{{{\mathit K}}3 {{\mathit \pi}}}$ (y cos $\delta {}^{{{\mathit K}}3 {{\mathit \pi}}}$ $−$ x sin$\delta {}^{{{\mathit K}}3 {{\mathit \pi}}}$)
$-0.0030 \pm0.0007$ TeV${}^{-1}$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ COHERENCE FACTOR R$_{{{\mathit K}_S^0} {{\mathit K}} {{\mathit \pi}}}$
$0.70 \pm0.08$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{{{\mathit K}_S^0} {{\mathit K}} {{\mathit \pi}}}$
$0 \pm16$ $^\circ{}$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{*}}{{\mathit K}}$ COHERENCE FACTOR R$_{{{\mathit K}^{*}} {{\mathit K}}}$
$0.94 \pm0.12$
${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{*}}{{\mathit K}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{{{\mathit K}^{*}} {{\mathit K}}}$
$-17 \pm18$ $^\circ{}$
$\Delta \mathit A_{CP}$ = $\mathit A_{CP}({{\mathit K}^{+}}{{\mathit K}^{-}}$) $−$ $\mathit A_{CP}({{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$)
$-0.00154 \pm0.00029$
$\mathit A_{\mathit CPT}({{\mathit K}^{\mp}}{{\mathit \pi}^{\pm}}$) in ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}$, ${{\overline{\mathit D}}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$
$-1.46 \times 10^{-4}\text{ to }6.6 \times 10^{-5} $ CL=95.0%
Most decay modes (other than the semileptonic modes) that involve a neutral ${{\mathit K}}$ meson are now given as ${{\mathit K}_S^0}$ modes, not as ${{\overline{\mathit K}}^{0}}$ modes. Nearly always it is a ${{\mathit K}_S^0}$ that is measured, and interference between Cabibbo-allowed and doubly Cabibbo-suppressed modes can invalidate the assumption that 2$~\Gamma ({{\mathit K}_S^0}$ ) = $\Gamma ({{\overline{\mathit K}}^{0}}$).