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arXiv cond-mat/0106339cond-mat.mes-hall
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量子化磁场中二维磁性杂质掺杂半导体的局域态

Localized states in 2D semiconductors doped with magnetic impurities in quantizing magnetic field

P. Dahan, V. Fleurov, K. Kikoin, I. D. Vagner

摘要:

根据Friedel-Anderson共振杂质散射理论,建立了强磁场量子化二维电子气中磁性杂质的理论。结果表明,这种散射的结果在外观的束缚朗道子带之间的零角动量的朗道态。共振散射是自旋选择性的,并且它导致朗道态的强自旋极化,以及杂质$d$能级的$g$因子和晶场分裂的显著磁场依赖性。

英文摘要:

A theory of magnetic impurities in a 2D 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 field splitting of the impurity $d$ levels.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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