Abstract

Abstract The quantum localization is known to be responsible for the deep conductivity minima of the quantum Hall effect. In this paper we calculate the localization length ξ as a function of magnetic field B at such minima for several models of disorder (“white-noise”, short-range, and long-range random potentials). We find that ξ∝B−α with the exponent α between one and 10 3 , depending on the model. In particular, for the “white-noise” random potential ξ roughly coincides with the classical cyclotron radius. Our results are in agreement with available experimental data.

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