CHARMED MESONS($\boldsymbol C$ = $\pm1$) ${{\mathit D}^{+}}$ = ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit d}}}$, ${{\mathit D}^{0}}$ = ${\mathit {\mathit c}}$ ${\mathit {\overline{\mathit u}}}$, ${{\overline{\mathit D}}^{0}}$ = ${\mathit {\overline{\mathit c}}}$ ${\mathit {\mathit u}}$, ${{\mathit D}^{-}}$ = ${\mathit {\overline{\mathit c}}}$ ${\mathit {\mathit d}}$, similarly for ${{\mathit D}^{*}}$'s INSPIRE search

# ${{\boldsymbol D}^{0}}$ $I(J^P)$ = $1/2(0^{-})$

 See related review: ${{\mathit D}^{0}}$ $-$ ${{\overline{\mathit D}}^{0}}$ Mixing
 ${{\mathit D}^{0}}$ MASS $1864.83 \pm0.05$ MeV
 ${\mathit m}_{{{\mathit D}^{\pm}}}–{\mathit m}_{{{\mathit D}^{0}}}$ $4.822 \pm0.015$ MeV
 ${{\mathit D}^{0}}$ MEAN LIFE $(4.101 \pm0.015) \times 10^{-13}$ s
 $\vert{}{\mathit m}_{{{\mathit D}_{{1}}^{0}}}–{\mathit m}_{{{\mathit D}_{{2}}^{0}}}\vert{}$ = $x$ $\Gamma$ $(95 {}^{+41}_{-44}) \times 10^{8}$ $\hbar{}$ s${}^{-1}$
 ($\Gamma _{{{\mathit D}_{{1}}^{0}}}$ $-$ $\Gamma _{{{\mathit D}_{{2}}^{0}}})/\Gamma$ = 2$\mathit y$ $0.0129 {}^{+0.0014}_{-0.0018}$
 $\vert$q/p$\vert$ $0.92 {}^{+0.12}_{-0.09}$
 A$_{\Gamma }$ $-0.000125 \pm0.000526$
 $\phi {}^{ {{\mathit K}_S^0} {{\mathit \pi}} {{\mathit \pi}} }$ $-0.09 {}^{+0.10}_{-0.13}$
 cos $\delta$ $0.97 \pm0.11$
 ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$ COHERENCE FACTOR $\mathit R_{ {{\mathit K}} {{\mathit \pi}} {{\mathit \pi}^{0}} }$ $0.82 \pm0.06$
 ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{ {{\mathit K}} {{\mathit \pi}} {{\mathit \pi}^{0}} }$ $199 \pm14$ $^\circ{}$
 ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{+}}$ COHERENCE FACTOR $\mathit R_{ {{\mathit K}}3 {{\mathit \pi}} }$ $0.53 {}^{+0.18}_{-0.21}$
 ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{-}}$2 ${{\mathit \pi}^{+}}$ AVERAGE RELATIVE STRONG PHASE $\delta {}^{ {{\mathit K}}3 {{\mathit \pi}} }$ $125 {}^{+22}_{-14}$ $^\circ{}$
 ${{\mathit D}^{0}}$ $\rightarrow$ ${{\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 $\delta {}^{ {{\mathit K}^{*}} {{\mathit K}} }$ $-17 \pm18$ $^\circ{}$
${{\boldsymbol D}^{0}}$ $\boldsymbol CP$-VIOLATING ASYMMETRY DIFFERENCES
 $\Delta \mathit A_{CP}$ = $\mathit A_{CP}$( ${{\mathit K}^{+}}{{\mathit K}^{-}}$ ) $−$ $\mathit A_{CP}$( ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) $-0.00154 \pm0.00029$
${{\boldsymbol D}^{0}}$ $\boldsymbol CPT$-VIOLATING DECAY-RATE ASYMMETRIES
 $\mathit A_{\mathit CPT}({{\mathit K}^{\mp}}{{\mathit \pi}^{\pm}}$) in ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}$ , ${{\overline{\mathit D}}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ $0.008 \pm0.008$
Amplitude analyses
 ${{\mathit D}}$ $\rightarrow$ ${{\mathit K}}{{\mathit \pi}}{{\mathit \pi}}{{\mathit \pi}}$ , ${{\mathit D}}$ $\rightarrow$ ${{\mathit K}}{{\mathit K}}{{\mathit \pi}}{{\mathit \pi}}$ partial wave analyses
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$~\Gamma ({{\mathit K}_S^0}$ ) = $\Gamma ({{\overline{\mathit K}}^{0}}$).
 constrained fit information