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

${{\boldsymbol D}_{{2}}^{*}{(2460)}^{0}}$ $I(J^P)$ = $1/2(2^{+})$ 

$\mathit J{}^{P} = 2{}^{+}$ assignment strongly favored (ALBRECHT 1989B, ALBRECHT 1989H), natural parity confirmed by the helicity analysis (DEL-AMO-SANCHEZ 2010P). AAIJ 2013CC confirms $\mathit J{}^{P} = 2{}^{+}$ and natural parity.
${{\mathit D}_{{2}}^{*}{(2460)}}$0 MASS   $2460.7 \pm0.4$ MeV (S = 3.1)
${\mathit m}_{{{\mathit D}_{{2}}^{*0}}}–{\mathit m}_{{{\mathit D}^{+}}}$   $591.0 \pm0.4$ MeV (S = 2.9)
${\mathit m}_{{{\mathit D}_{{2}}^{*0}}}–{\mathit m}_{{{\mathit D}^{*+}}}$   $450.4 \pm0.4$ MeV (S = 2.9)
${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$ WIDTH   $47.5 \pm1.1$ MeV (S = 1.8)
${{\mathit D}_{{2}}^{*}{(2460)}^{0}}$ POLARIZATION AMPLITUDE A$_{{{\mathit D}_{{2}}}}$
${{\overline{\mathit D}}_{{2}}^{*}{(2460)}^{0}}$ modes are charge conjugates of modes below.
$\Gamma_{1}$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$  seen 505
$\Gamma_{2}$ ${{\mathit D}^{*}{(2010)}^{+}}{{\mathit \pi}^{-}}$  seen 389
$\Gamma_{3}$ ${{\mathit D}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  not seen 462
$\Gamma_{4}$ ${{\mathit D}^{*0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  not seen 324