The localization behavior of noninteracting two-dimensional electrons in a
random potential and strong magnetic field is of fundamental interest for t
he physics of the quantum Hall effect. In order to understand the emergence
of power-law delocalization near the discrete extended-state energies E-n
= (h) over barw(c)(n + 1/2), we study a generalization of the disorder-aver
aged Liouvillian framework for the lowest Landau level to N flavors of elec
tron densities (N = 1 for the physical case). We find analytically the larg
e-N limit and 1/N corrections for all disorder strengths: at N = infinity t
his gives an estimate of the critical conductivity, and at order 1/N an est
imate of the localization exponent v.