The transition between localized and extended eigenstates in the integral quantum Hall regime is observable as a scaling phenomenon in the magnetoresistance tensor as a function of temperature and applied magnetic field strength. Field-theoretic studies on the quantum Hall effect are used to derive the scaling functions. The scaling behavior is shown to involve only a single critical exponent (μ) which is the ratio between the inelastic-scattering exponent (p) and twice the localization length exponent (ν). The results have recently been confirmed experimentally.
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A. M. M. Pruisken (1988) studied this question.
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