We study the AC properties of a two-dimensional electron gas in high-mobili
ty samples at half-filling of the lowest Landau level within the framework
of the composite-fermion (CF) theory. We have shown that the low-frequency
behavior of the AC conductivity sigma (xx)(omega) in the presence of smooth
disorder is governed by quasiclassical memory effects that are related to
return processes neglected in Boltzmann transport theory. We have demonstra
ted that the fictitious random magnetic field acting on CFs strongly enhanc
es this anomalous contribution to sigma (xx)(omega); specifically, the retu
rn-induced correction to Re sigma (xx)(omega) shows a pronounced cusp propo
rtional to/omega/ . This anomaly is of quasiclassical origin and dominates
(compared to quantum corrections proportional to ln omega) in a wide freque
ncy range, provided k(F)d much greater than 1, where k(F) is the CF Fermi w
ave vector, d the correlation radius of disorder. The prefactor of the /ome
ga/ term is proportional to d/l (l is the mean free path of the CFs). (C) 2
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