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We present a theory of the Hall effect in a quantum dot coupled to Hall and current leads by narrow constrictions. A magnetic-diffraction effect is described which results in a series of deep minima in the Hall resistance persisting temperatures T>1 K, robustness that is unique among mesoscopic quantum interference phenomena. At higher T, phase-breaking casues an anomalous ``last'' Hall plateau at RH=h/4e² and, at higher B, a plateau near the single-mode quantum Hall value RH=h/2e². We explain the surprising behavior of the Hall resonances observed by Ford et al. (preceding paper) in quantum-wire junctions.
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Kirczenow et al. (1991) studied this question.
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