Properties incompatible with a ${{\mathit q}}{{\overline{\mathit q}}}$ structure (exotic state). See the review on non- ${{\mathit q}}{{\overline{\mathit q}}}$ states. Charged ${{\mathit X}{(4020)}}$ seen by ABLIKIM 2013X from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit h}_{{c}}{(1P)}}$ at c.m. energy from 3.90 to 4.42 GeV as a peak in the invariant mass distribution of the ${{\mathit \pi}^{\pm}}{{\mathit h}_{{c}}{(1P)}}$ system, and by ABLIKIM 2014B from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ( ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}){}^{+-}{{\mathit \pi}^{\mp}}$ events in ( ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ )${}^{+-}$ mass. A neutral ${{\mathit X}{(4020)}}$ seen by ABLIKIM 2014P at three c.m. energies in the same range in ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \pi}^{0}}{{\mathit \pi}^{0}}{{\mathit h}_{{c}}{(1P)}}$ as a peak in the larger of the two masses recoiling against a ${{\mathit \pi}^{0}}$. ABLIKIM 2015AA observes a 5.9 $\sigma $ signal in ( ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ )${}^{0}$ in ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ( ${{\mathit D}^{*}}{{\overline{\mathit D}}^{*}}$ )${}^{0}{{\mathit \pi}^{0}}$ events using collisions at two c.m. energies. Production rates and mass values support grouping neutral and charged ${{\mathit X}{(4020)}}$ together as manifestations of a single $\mathit I = $ particle.