  The spectrum of tetraquark states with hidden charm is studied within an
effective QCD Coulomb gauge Hamiltonian approach. Of the four independent color
schemes, two are investigated, the $(q\bar{c})_1(c\bar{q})_1$ singlet-singlet
(molecule) and the $(qc)_3(\bar{q}\bar{c})_3$ triplet-triplet (diquark), for
selected $J^{PC}$ states using a variational method. The predicted masses of
triplet-triplet tetraquarks are roughly a GeV heavier than the singlet-singlet
states. There is also an interesting flavor dependence with
$(q\bar{q})_1(c\bar{c}_1)$ states about half a GeV lighter than
$(q\bar{c})_1(\bar{q}c)_1$. The lightest $1^{++}$ and $1^{--}$ predictions are
in agreement with the observed X(3872) and Y(4008) masses, respectively,
suggesting they both have a $\omega J/ \psi$ rather than $D^*\bar D^*$
molecular type structure. This is consistent with observed $X$, $Y$ decays to
$\pi^\pm J/ \psi$ and not $D^*\bar D^*$ .
