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Excitons in motion in II–VI semiconductors
Author(s) -
Davies J. J.,
Smith L. C.,
Wolverson D.,
Kochereshko V. P.,
Cibert J.,
Mariette H.,
Boukari H.,
Wiater M.,
Karczewski G.,
Wojtowicz T.,
Gust A.,
Kruse C.,
Hommel D.
Publication year - 2010
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200983167
Subject(s) - exciton , bohr radius , condensed matter physics , diamagnetism , hamiltonian (control theory) , biexciton , physics , wave function , semiconductor , bohr model , chemistry , atomic physics , magnetic field , quantum mechanics , mathematical optimization , mathematics
Abstract We have shown recently that the magnetic properties of excitons change significantly as the excitons acquire kinetic energy. In particular, the exciton magnetic moments are enhanced considerably, whilst the diamagnetism decreases. The behaviour can be investigated through spectroscopic studies of excitons confined in quantum wells of large width (greater than five times the exciton Bohr radius) and these motion‐induced changes in the magnetic properties have now been observed for CdTe, ZnSe, ZnTe and GaAs. The present paper summarises these phenomena, with particular focus on CdTe and ZnSe, and shows that the changes can be accounted for by motion‐induced mixing between the exciton ground and higher lying states. The mixing is caused by the γ 3 term in the Luttinger Hamiltonian which describes the dispersion curves for the valence band and, as a result, the form of the exciton wavefunction becomes motion‐dependent. For both materials, excellent agreement is obtained between experiment and the results predicted by this mechanism.