  We study the $D^{*}_s \bar D^*$ system in connection with the $J/\psi K^*$ in
coupled channels and observe that, within reasonable values of the cut-off used
to regularize the loops, the system does not develop a bound state. However,
the $J^P = 2^+$ channel has enough attraction to create a strong cusp structure
that shows up in the $J/\psi K^+$ invariant mass distribution in the $B^+ \to
J/\psi \phi K^+$ decay at the $D^*_s \bar D^*$ threshold. Such structure is
visible in the experimental $B^+ \to J/\psi \phi K^+$ and $\bar B^0 \to J/\psi
K^+ K^-$ decays, with small statistics, and our results should stimulate
further measurements around this region, given the fact that cusp effects
provide as valuable information on hadron dynamics as resonances themselves.
