2002
DOI: 10.1103/physrevb.65.165313
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Localized states in two-dimensional semiconductors doped with magnetic impurities in a quantizing magnetic field

Abstract: A theory of magnetic impurities in a two-dimensional electron gas quantized by a strong magnetic field is formulated in terms of Friedel-Anderson theory of resonance impurity scattering. It is shown that this scattering results in an appearance of bound Landau states with zero angular moment between the Landau subbands. The resonance scattering is spin selective, and it results in a strong spin polarization of Landau states, as well as in a noticeable magnetic field dependence of the g factor and the crystal f… Show more

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Cited by 12 publications
(12 citation statements)
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“…Since the nuclear spin of the impurity interacts with the localized electron which in our case is s function (m ¼ 0) [10], we would expect the important interaction to be with the localized phonons acting as a breathing modes distortion up to few nearest-neighbor shell around the impurity [11]. The electron-phonon interaction is…”
Section: Nuclear Spin Relaxation Ratementioning
confidence: 98%
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“…Since the nuclear spin of the impurity interacts with the localized electron which in our case is s function (m ¼ 0) [10], we would expect the important interaction to be with the localized phonons acting as a breathing modes distortion up to few nearest-neighbor shell around the impurity [11]. The electron-phonon interaction is…”
Section: Nuclear Spin Relaxation Ratementioning
confidence: 98%
“…[10]. We have shown there that the resonance impurity scattering results in appearance of bound Landau states with zero momentum between the Landau subbands.…”
Section: Introductionmentioning
confidence: 94%
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