We develop a quasiclassical method based on the path integral formalis
m, to study the influence of disorder on magnetooscillations of the de
nsity of states and conductivity. The treatment is appropriate for ele
ctron systems in the presence of a random potential with large correla
tion length or a random magnetic field, which are characteristic featu
res of various 2D electronic systems presently studied in experiment.
In particular, we study the system of composite fermions in the fracti
onal quantum Hall effect device, which are coupled to the Chern-Simons
field and subject to a long-range random potential.