  We calculate the masses of $\chi_{\rm c}(2P)$ and $\chi_{\rm b}(3P)$ states
with threshold corrections in a coupled-channel model. Here, the meson
quarkonium core is augmented by higher Fock components due to pair-creation
effects. According to our results, we interpret the resonances characterized by
very small threshold corrections, like $\chi_{\rm b}(3P)$'s, as almost pure
quarkonia, and those states characterized by non-negligible threshold
corrections, like the $X(3872)$, as quarkonium cores plus meson-meson
components. We also study the $J/\psi \rho$ and $J/\psi \omega$ hidden-flavor
strong decays of the $X(3872)$. The decays are calculated as the dissociation
of one of these components ($D^0 \bar D^{0*}$) into a $c \bar c$ state
($J/\psi$) plus a light meson ($\rho$ or $\omega$) in a potential model. In
particular, our result for the ratio between the $X(3872) \rightarrow J/\psi
\omega$ and $J/\psi \rho$ widths (0.6) is compatible with the present
experimental data ($0.8\pm0.3$) within the experimental error.
