The transition from the quantum Hall state to the insulator is considered f
or non-interacting electrons in a two-dimensional disordered lattice model
with perpendicular magnetic field. Using correlated random disorder potenti
als the floating up of the critical states can be observed in a similar way
as in the continuum model. Thus, the peculiar behaviour of the lattice mod
els reported previously originates in the special choice of uncorrelated ra
ndom disorder potentials. (C) 2001 Elsevier Science B.V. All rights reserve
d.