  $J/\Psi$-nuclear bound state energies are calculated for a range of nuclei by
solving the Proca (Klein-Gordon) equation. Critical input for the calculations,
namely the medium-modified $D$ and $D^*$ meson masses, as well as the nucleon
density distributions in nuclei, are obtained from the quark-meson coupling
model. The attractive potential originates from the $D$ and $D^*$ meson loops
in the $J/\Psi$ self-energy in nuclear medium. It appears that $J/\Psi$-nuclear
bound states should produce a clear experimental signature provided that the
$J/\Psi$ meson is produced in recoilless kinematics.
