  We formulate the massive overlap fermions on anisotropic lattices.
  We find that the dispersion relation for the overlap fermion resembles the
continuum form in the low-momentum region once the bare parameters are properly
tuned. The quark self-energy and the quark field renormalization constants are
calculated to one-loop in bare lattice perturbation theory.
  We argue that massive domain wall quarks might be helpful in lattice QCD
studies on heavy-light hadron spectroscopy.
