Abstract
At the fundamental bandgap E0 we have for Q2D systems generally a mixing of heavy and light–hole states. In this case, the dipole matrix elements between a valence–band state ψh i ,k∥ (r) and a conduction–band state ψ cj ,k∥ (r) is given by
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© 2006 Springer
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Schüller, C. (2006). Kronecker Products of Dipole Matrix Elements II. In: Inelastic Light Scattering of Semiconductor Nanostructures. Springer Tracts in Modern Physics, vol 219. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-36526-5_10
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DOI: https://doi.org/10.1007/3-540-36526-5_10
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-36525-9
Online ISBN: 978-3-540-36526-6
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