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Localized states in two-dimensional semiconductors doped with magnetic impurities in a quantizing magnetic field

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Fleurov,  V.
High Magnetic Field Laboratory, Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;

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Kikoin,  K.
Department Solid State Spectroscopy (Bernhard Keimer), Max Planck Institute for Solid State Research, Max Planck Society;

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Vagner,  I. D.
High Magnetic Field Laboratory, Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;

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Citation

Dahan, P., Fleurov, V., Kikoin, K., & Vagner, I. D. (2002). Localized states in two-dimensional semiconductors doped with magnetic impurities in a quantizing magnetic field. Physical Review B, 65(16): 165313.


Cite as: https://hdl.handle.net/21.11116/0000-000E-F3AD-D
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 field splitting of the impurity d levels.