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DOI: 10.1209/epl/i1997-00505-4


Europhys. Lett, 40 (5), pp. 557-562 (1997)

Narrow-resonance states of 2D magnetic spin-exciton
in periodically modulated fields

Yu. A. Bychkov tex2html_wrap_inline325, T. Maniv tex2html_wrap_inline327, I. D. Vagner tex2html_wrap_inline329 and P. Wyder tex2html_wrap_inline331

tex2html_wrap_inline333 L. D. Landau Institute for Theoretical Physics - Kosygina 2, Moscow, Russia
tex2html_wrap_inline331High Magnetic Field Laboratory, Max-Planck-Institut für Festkörperforschung
Centre National de la Recherche Scientifique - BP 166, F-38042 Grenoble, Cedex 9, France
tex2html_wrap_inline337 Department of Chemistry, Technion-Israel Institute of Technology - Haifa 32000, Israel
tex2html_wrap_inline339 Solid State Institute, Technion-Israel Institute of Technology - Haifa 32000, Israel

(received 5 May 1997; accepted in final form 17 October 1997)

PACS. 73.50Jt - Galvanomagnetic and other magnetotransport effects (including thermomagnetic effects).
PACS. 71.35tex2html_wrap_inline341 - Excitons and related phenomena.
PACS. 76.60tex2html_wrap_inline343 - Nuclear magnetic resonance and relaxation.

Abstract:

Two-dimensional electron gas (2DEG) under a strong perpendicular magnetic field in periodically modulated fields exhibits a peculiar discrete spectrum near the bottom of the spin-exciton band. The combined effect of the electrostatic modulation potential, and the e-h Coulomb attraction under the magnetic field, leads to nearly bound relative e-h oscillations perpendicular to the modulation axis, which have a characteristic Rydberg-like spectrum near the edge of the spin-exciton band. This low-lying, very narrow excitonic lines may significantly affect the spin and the charge transport in the thermally activated regime.


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