Abstract
First, the theory for the bulk crystals [1-3] is described. According to Bloch’s theorem, a single-body state of an electron in a solid crystal of volume V takes the following form:
where b labels bands (conduction band, heavy-hole band, and so on), and Ubk is the cell-periodic function. The spin index is omitted for the sake of simplicity.
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Shimizu, A. (1998). Theory of Electron-Photon Interaction. In: Ando, T., Arakawa, Y., Furuya, K., Komiyama, S., Nakashima, H. (eds) Mesoscopic Physics and Electronics. NanoScience and Technology. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-71976-9_19
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DOI: https://doi.org/10.1007/978-3-642-71976-9_19
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