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

${{\boldsymbol D}_{{3}}^{*}{(2750)}}$ $I(J^P)$ = $1/2(3^{-})$ 

$\mathit J{}^{P}$ determined by AAIJ 2015Y from the Dalitz plot analysis of ${{\mathit B}^{0}}$ $\rightarrow$ ${{\overline{\mathit D}}^{0}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ decays. $\mathit J{}^{P}$ consistent with natural parity (AAIJ 2013CC).
${{\mathit D}_{{3}}^{*}{(2750)}}$ MASS   $2763.5 \pm3.4$ MeV (S = 2.2)
${{\mathit D}_{{3}}^{*}{(2750)}}$ WIDTH   $66 \pm5$ MeV 
${{\mathit D}_{{3}}^{*}{(2750)}}$ POLARIZATION AMPLITUDE A$_{{{\mathit D}}}$
$\Gamma_{1}$ ${{\mathit D}}{{\mathit \pi}}$  seen 744
$\Gamma_{2}$ ${{\mathit D}^{+}}{{\mathit \pi}^{-}}$  seen 740
$\Gamma_{3}$ ${{\mathit D}^{0}}{{\mathit \pi}^{\pm}}$  seen 743
$\Gamma_{4}$ ${{\mathit D}^{*}}{{\mathit \pi}}$  seen 640
$\Gamma_{5}$ ${{\mathit D}^{*+}}{{\mathit \pi}^{-}}$  seen 639