  We present the first calculation within lattice QCD of excited light meson
resonances with $J^{PC} = 1^{--}$, $2^{--}$ and $3^{--}$. Working with an exact
SU(3) flavor symmetry, for the singlet representation of pseudoscalar-vector
scattering, we find two $1^{--}$ resonances, a lighter broad state and a
heavier narrow state, a broad $2^{--}$ resonance decaying in both $P$- and
$F$-waves, and a narrow $3^{--}$ state. We present connections to experimental
$\omega^\star_J, \phi^\star_J$ resonances decaying into $\pi \rho$,
$K\bar{K}^*$, $\eta \omega$ and other final states.
