Fermi-edge-induced magnetophotoluminescence in high-carrier-density single heterojunctions

F. A. J. M. Driessen, S. M. Olsthoorn, T. T. J. M. Berendschot, L. J. Giling, D. M. Frigo, G. A. C. Jones, D. A. Ritchie, and J. E. F. Frost
Phys. Rev. B 47, 1282 – Published 15 January 1993
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Abstract

Fermi-edge-induced excitonic magnetophotoluminescence (MPL) of second (nc=2)-subband electrons and photoexcited holes X(nc=2,h) is reported in high-carrier-density GaAs/AlxGa1xAs single heterojunctions for two-dimensional carrier densities in the range (6.6–16.2)×1015 m2. The MPL shows magneto-oscillatory behavior of intensity, photon energy, and peak width. Furthermore, nc=2 subband recombination with light holes X(nc=2,l) is reported. A splitting of the X(nc=2,h) is reported at low carrier density, which results from the separate interaction of the two spin-split states of the nc=1 Landau level in which the Fermi level resides on the second subband. The dependence of the spectra on both excitation density and temperature indicates strongly that photoluminescence (PL) from the nc=3 subband occurs. PL originating from the two-dimensional electron gas (2DEG) and that from the GaAs buffer layer could be distinguished by excitation below and above the GaAs band gap. In the highest-carrier-density sample, evidence is found for the formation of a band of localized states betwen the spin components of a Landau level. Recombination occurs between the exponentially decaying tails of the photoexcited holes, which relax to the flat-band region of the GaAs. Additional information on the 2DEG was obtained via resonant-excitation experiments. Phonon replicas of both the second-subband exciton and the unpopulated third subband are observed. The latter very sharp replica appears if a nonequilibrium electron concentration is created in the resonantly excited third subband. Resonant excitation also reveals the recombination of electrons in the nc=2 subband with holes located at neutral acceptors. Strong indications were found for PL of the nc=1 lowest Landau level upon resonantly exciting the X(nc=2,h) transition in the lowest-carrier-density sample.

  • Received 7 August 1992

DOI:https://doi.org/10.1103/PhysRevB.47.1282

©1993 American Physical Society

Authors & Affiliations

F. A. J. M. Driessen and S. M. Olsthoorn

  • Department of Experimental Solid State Physics, Research Institute for Materials, University of Nijmegen, Toernooiveld, NL 6525 ED Nijmegen, The Netherlands

T. T. J. M. Berendschot

  • High Field Magnet Laboratory, University of Nijmegen, Toernooiveld, NL 6525 ED Nijmegen, The Netherlands

L. J. Giling

  • Department of Experimental Solid State Physics, Research Institute for Materials, University of Nijmegen, Toernooiveld, NL 6525 ED Nijmegen, The Netherlands

D. M. Frigo

  • Billiton Research B.V., P.O. Box 40, NL 6800 AA Arnhem, The Netherlands

G. A. C. Jones, D. A. Ritchie, and J. E. F. Frost

  • Cavendish Laboratory, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom

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Issue

Vol. 47, Iss. 3 — 15 January 1993

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