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Thermally activated deviations from quantum Hall plateaux

The Hall conductivity σ xy of a two-dimensional electron system is quantized in units of e 2 h when the Fermi level is located in the gap between two Landau levels. We consider the deviation of σ xy from a quantized value caused by the thermal activation of electrons to the extended states for the c...

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Bibliographic Details
Published in:Solid state communications 1995, Vol.94 (7), p.503-507
Main Authors: Fogler, M.M., Shklovskii, B.I.
Format: Article
Language:English
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Summary:The Hall conductivity σ xy of a two-dimensional electron system is quantized in units of e 2 h when the Fermi level is located in the gap between two Landau levels. We consider the deviation of σ xy from a quantized value caused by the thermal activation of electrons to the extended states for the case of a long range random potential. This deviation is of the form σ xy ∗ exp( −Δ T ) . The prefactor σ xy ∗ is equal to e 2 h at temperatures above a characteristic value T 2. Below T 2, σ xy ∗ decays according to a power law: σ xy ∗ = e 2 h ( T T 2 ) γ . The generalization to fractional Hall plateaux is discussed.
ISSN:0038-1098
1879-2766
DOI:10.1016/0038-1098(95)00119-0