Abstract
A theory of optical anisotropy for zinc-blende semiconductors in an electric field is derived by extending the formalism of Luttinger and Kohn [Phys. Rev. 97, 869 (1955)] to higher order. This resolves a recent controversy over the correct form of the Hamiltonian for the degenerate valence bands. © 2000 The American Physical Society.
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CITATION STYLE
APA
Foreman, B. A. (2000). Optical anisotropy of zinc-blende semiconductors in an electric field. Physical Review Letters, 84(11), 2505–2508. https://doi.org/10.1103/PhysRevLett.84.2505
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