2006
DOI: 10.1016/j.physe.2006.03.001
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Angular magnetoresistance oscillations in bilayers in tilted magnetic fields

Abstract: Angular magnetoresistance oscillations (AMRO) were originally discovered in organic conductors and then found in many other layered metals. It should be possible to observe AMRO to semiconducting bilayers as well. Here we present an intuitive geometrical interpretation of AMRO as the Aharonov-Bohm interference effect, both in real and momentum spaces, for balanced and imbalanced bilayers. Applications to the experiments with bilayers in tilted magnetic fields in the metallic state are discussed. We speculate t… Show more

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Cited by 18 publications
(33 citation statements)
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References 34 publications
(58 reference statements)
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“…Using these parameters, we obtained the distance between wave-function maxima d = 170-180 Å for d b = 14 Å barrier sample, which roughly agrees with the expected value ͑see Table I͒. In the last part we reproduce the intuitive geometrical interpretation of the observed oscillatory effects as a manifestation of the Aharonov-Bohm effect in the titled magnetic field, first presented in Ref. 9. Figure 8͑a͒ shows schematically two layers separated by the distance d in a tilted magnetic field.…”
Section: Resultssupporting
confidence: 85%
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“…Using these parameters, we obtained the distance between wave-function maxima d = 170-180 Å for d b = 14 Å barrier sample, which roughly agrees with the expected value ͑see Table I͒. In the last part we reproduce the intuitive geometrical interpretation of the observed oscillatory effects as a manifestation of the Aharonov-Bohm effect in the titled magnetic field, first presented in Ref. 9. Figure 8͑a͒ shows schematically two layers separated by the distance d in a tilted magnetic field.…”
Section: Resultssupporting
confidence: 85%
“…8͑b͒, produces the phase shift between cyclotron orbits in different layers, which leads to the oscillations of the effective interlayer tunneling amplitude. 9 In momentum space in-plane magnetic field introduces the shift of the two Fermi surfaces ⌬k ʈ = eB ʈ d / ប relative to each other, 20 as shown in Fig. 1͑c͒.…”
Section: Resultsmentioning
confidence: 99%
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“…16 AMROs are essentially a geometric resonance involving the cyclotron orbits projected onto the plane parallel to the layers. 17 In this sense, they are similar to geometric commensurability oscillations in magnetoresistance seen for two-dimensional electron gases in semiconductor heterostructures. [18][19][20] In this paper, we present the following results for interlayer magnetotransport in a layered Fermi liquid metal.…”
Section: Introductionmentioning
confidence: 57%