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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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Published in: | Solid state communications 1995, Vol.94 (7), p.503-507 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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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. |
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ISSN: | 0038-1098 1879-2766 |
DOI: | 10.1016/0038-1098(95)00119-0 |