Landauer-type formulas are derived for two-dimensional quantum-Hall transport in the extreme quantum limit ({}ωc{→}{∞}) for an arbitrary current through an electron system confined to a channel. For narrow channels the problem is mapped into a one-dimensional ordinary (B=0) transport problem. An expression for the critical current and a description of the breakdown of the dissipationless transport are obtained. We find that it is possible to have quantization of the Hall resistance even when the magnetoresistance is nonzero.
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Jain et al. (1988) studied this question.
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