LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT

We study the two-dimensional electron gas in the presence of a random perpendicular magnetic field. We examine, in particular, the limit in which the correlation length of the random field is large compared to the typical magnetic length. In this limit, a semiclassical approach can be used to unders...

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Main Authors: Lee, D, Chalker, J, Ko, D
Format: Journal article
Language:English
Published: 1994
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author Lee, D
Chalker, J
Ko, D
author_facet Lee, D
Chalker, J
Ko, D
author_sort Lee, D
collection OXFORD
description We study the two-dimensional electron gas in the presence of a random perpendicular magnetic field. We examine, in particular, the limit in which the correlation length of the random field is large compared to the typical magnetic length. In this limit, a semiclassical approach can be used to understand a large part of the energy spectrum. To investigate localization, we introduce a simplified model, in which electrons propagate coherently on a random network derived from the classical trajectories. The same network model (with different parameters) also represents electron motion in a uniform magnetic field and a random scalar potential, in a spin-degenerate Landau level. Requiring that the global phase diagram of our model be consistent with Khmelnitskii's scaling flow for the quantum Hall effect, we argue that all electron states in a random magnetic field are localized in the semiclassical limit. We present the results of numerical simulations of the model in support of this conclusion. © 1994 The American Physical Society.
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spelling oxford-uuid:f4e2c2c2-e093-4338-968e-f5231767e0c62022-03-27T12:23:06ZLOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMITJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:f4e2c2c2-e093-4338-968e-f5231767e0c6EnglishSymplectic Elements at Oxford1994Lee, DChalker, JKo, DWe study the two-dimensional electron gas in the presence of a random perpendicular magnetic field. We examine, in particular, the limit in which the correlation length of the random field is large compared to the typical magnetic length. In this limit, a semiclassical approach can be used to understand a large part of the energy spectrum. To investigate localization, we introduce a simplified model, in which electrons propagate coherently on a random network derived from the classical trajectories. The same network model (with different parameters) also represents electron motion in a uniform magnetic field and a random scalar potential, in a spin-degenerate Landau level. Requiring that the global phase diagram of our model be consistent with Khmelnitskii's scaling flow for the quantum Hall effect, we argue that all electron states in a random magnetic field are localized in the semiclassical limit. We present the results of numerical simulations of the model in support of this conclusion. © 1994 The American Physical Society.
spellingShingle Lee, D
Chalker, J
Ko, D
LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title_full LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title_fullStr LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title_full_unstemmed LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title_short LOCALIZATION IN A RANDOM MAGNETIC-FIELD - THE SEMICLASSICAL LIMIT
title_sort localization in a random magnetic field the semiclassical limit
work_keys_str_mv AT leed localizationinarandommagneticfieldthesemiclassicallimit
AT chalkerj localizationinarandommagneticfieldthesemiclassicallimit
AT kod localizationinarandommagneticfieldthesemiclassicallimit