  We study a generic two-dimensional hopping model on a honeycomb lattice with
strong spin-orbit coupling, without the requirement that the half-filled
lattice be a Topological Insulator. For quarter-(or three-quarter) filling, we
show that a state with a quantized Hall conductance generically arises in the
presence of a Zeeman field of sufficient strength. We discuss the influence of
Hubbard interactions and argue that spontaneous ferromagnetism (which breaks
time-reversal) will occur, leading to a quantized anomalous Hall effect.
