1990
DOI: 10.1007/978-1-4684-7412-1_8
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Magnetoquantum Oscillations in a Lateral Superlattice

Abstract: The low temperature magnetoresistance of a high mobility two-dimensional electron gas is dominated by Shubnikov-de Haas oscillations, reflecting the discrete nature of the electron energy spectrum. When a weak one-or two-dimensional periodic potential is superimposed on the two-dimensional electron gas a novel type of oscillations occurs which reflects the commensurability of the relevant lengths in these systems -the cyclotron orbit diameter at the Fermi energy and the period a of the periodic potential. In a… Show more

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Cited by 3 publications
(2 citation statements)
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“…1.2 Weiss oscillations and the ν = 1/2 state Here, we study theoretically commensurability oscillations in the magnetoresistance near ν = 1/2, focusing on those oscillations that result from the presence of a periodic onedimensional static potential [9]. These commensurability oscillations are commonly known as Weiss oscillations [25][26][27][28]. For a free two-dimensional Fermi gas, the locations of the Weiss oscillation minima, say, as a function of the transverse magnetic field b, satisfy…”
Section: Motivationmentioning
confidence: 99%
“…1.2 Weiss oscillations and the ν = 1/2 state Here, we study theoretically commensurability oscillations in the magnetoresistance near ν = 1/2, focusing on those oscillations that result from the presence of a periodic onedimensional static potential [9]. These commensurability oscillations are commonly known as Weiss oscillations [25][26][27][28]. For a free two-dimensional Fermi gas, the locations of the Weiss oscillation minima, say, as a function of the transverse magnetic field b, satisfy…”
Section: Motivationmentioning
confidence: 99%
“…Weiss oscillations [3][4][5] are quantum oscillations that occur because of the presence of a periodic scalar or vector potential. The length scale provided by the period of the imposed potential allows additional oscillations to occur when the cyclotron radius is (approximately) commensurate with the period [6]. These oscillations occur at magnetic field values B(p) satisfying ℓ 2 B(p) = d 2k F p − φ , p = 1, 2, 3, .…”
Section: Introductionmentioning
confidence: 99%