ζ(2230)May Be a(qs)3*−(q¯s¯)3Baryonium or anss¯gHybrid State

Possible interpretations for the $\zeta \mathrm{}\left(2230\right)\mathrm{}$ are discussed in accordance with new data from Baltrusaitis et al., Aston et al., and Binon et al., and it is argued that the $\zeta \mathrm{}\left(2230\right)\mathrm{}$ is likely to be a ${\mathrm{}\left(\mathrm{qs}\right)\mathrm{}}_{3*}-{\left(\overline{q}\overline{s}\right)}_3\mathrm{}(q=u,d)\mathrm{}$ baryonium state, which couples strongly to $\Lambda \Lambda$ and decays to $K\overline{K}$, $K{\overline{K}}^{*}$, ${\overline{K}}^{*}{K}^{*}$, $\eta \eta ,\eta {\eta }^{\prime }$, ${\eta }^{\prime }{\eta }^{\prime }$, and $\omega \phi$, via quark rearrangement, and also to $\pi \pi$, $\omega \omega$, and $\phi \phi$ via quark annihilation, and therefore has a narrow width. A possible $s\overline{s}g$ hybrid state, which can decay to $\phi \phi$, $\omega \phi$, and other mesons, is also suggested.