We present a treatment of an interacting two-dimensional electron system mo
ving in a bidirectionally periodic potential and a perpendicular magnetic f
ield. Employing symmetry considerations based on the ray-group of magnetotr
anslation operators and a canonical coordinate transformation, we derive an
efficient scheme for calculating energy levels and states in arbitrary 'ra
tional' magnetic fields. Applying this scheme to a superlattice of strongly
localized antidots we reveal the possibility to split off an isolated and
sufficiently broad cluster of subbands from a Landau band. The implications
of the existence of such subbands to the experimental detection of the sub
band structure and in particular quantum Hall effect measurements in period
ic superlattices are discussed.