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

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

See related review:
Review of Multibody Charm Analyses
${{\mathit D}^{\pm}}$ MASS   $1869.65 \pm0.05$ MeV 
${{\mathit D}^{\pm}}$ MEAN LIFE   $(1.040 \pm0.007) \times 10^{-12}$ s 
$\boldsymbol CP$ VIOLATING ASYMMETRIES OF $\boldsymbol P$-ODD ($\boldsymbol T$-ODD) MOMENTS
$\mathit A_{\mathit Tviol}$( ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ ) in ${{\mathit D}^{\pm}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$   $-0.012 \pm0.011$  
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$~\Gamma ({{\mathit K}_S^0}$ ) = $\Gamma ({{\overline{\mathit K}}^{0}}$).
$\Gamma_{142}$ Unaccounted decay modes $(63.7\pm{0.6})\%$S=1.6 
    constrained fit information