Properties incompatible with a ${{\mathit q}}{{\overline{\mathit q}}}$ structure (exotic state). See the review on "Heavy Non-${{\mathit q}}{{\overline{\mathit q}}}$ Mesons." Seen by AAIJ 2021E in ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit T}_{{{c {{\overline{\mathit c}}} {{\overline{\mathit s}}} 1}}}{(4000)}^{+}}{{\mathit \phi}}$ with ${{\mathit T}_{{{c {{\overline{\mathit c}}} {{\overline{\mathit s}}} 1}}}{(4000)}^{+}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit K}^{+}}$ using an amplitude analysis of ${{\mathit B}^{+}}$ $\rightarrow$ ${{\mathit J / \psi}}{{\mathit \phi}}{{\mathit K}^{+}}$ with a significance (accounting for systematic uncertainties) of 15 $\sigma $. The $\mathit J{}^{P} = 1{}^{+}$ assignment is favored with high significance. ABLIKIM 2021G also reports a $\mathit J{}^{P} = 1{}^{+}$ ${{\mathit Z}_{{{cs}}}}$ state in this mass region using ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{+}}$( ${{\mathit D}_{{{s}}}^{-}}{{\mathit D}^{*0}}{+}$ ${{\mathit D}_{{{s}}}^{*-}}{{\mathit D}^{0}}$) with a significance of 5.3 $\sigma $. The incompatible values for the widths reported by AAIJ 2021E and ABLIKIM 2021G could either indicate the existence of two separate states or possibly be explained in a coupled channel model (see ORTEGA 2021).