Abstract
The electron-hole exchange interaction in semiconductors is analyzed in the framework of the empirical tight-binding method. It is demonstrated that intra-atomic and interatomic contributions to the long-range exchange interaction enter in an inequivalent way. In particular, for the Γ6×Γ7 exciton in a spherical nanocrystal with a cubic lattice, the dipole-dipole contribution associated only with the intra-atomic (or intra-site) transitions does not lead to singlet-triplet splitting of the exciton level. The interatomic transitions, for example, anion-to-cation transitions between the nearest neighbors in binary semiconductor compounds, determine the so-called monopole-monopole contribution to the exchange splitting of the Γ6×Γ7 exciton, and this contribution does not vanish in a spherical nanocrystal.
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Translated from Fizika Tverdogo Tela, Vol. 43, No. 10, 2001, pp. 1791–1798.
Original Russian Text Copyright © 2001 by Goupalov, Ivchenko.
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Goupalov, S.V., Ivchenko, E.L. A tight-binding representation of electron-hole exchange interaction in semiconductors. Phys. Solid State 43, 1867–1875 (2001). https://doi.org/10.1134/1.1410624
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DOI: https://doi.org/10.1134/1.1410624