Abstract
A Green's-function method is used to calculate the shape of the magnetophonon-oscillation line of the differential susceptibility of a semiconductor in a quantizing magnetic field. The amplitude of the resonant peak is shown to be proportional to g2/3 (where g is the electron-phonon interaction constant), while the peak width is proportional to g4/3.
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D. I. Sirota, Z. I. Uritskii, and G. V. Shuster, Zh. Éksp. Teor. Fiz. Pis. Red., 1, No. 5 (1965).
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Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 1, pp. 33–37, January, 1971.
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Sirota, D.I. Magnetophonon oscillations of the differential susceptibility of semiconductors in a quantizing magnetic field. Soviet Physics Journal 14, 21–24 (1971). https://doi.org/10.1007/BF00819854
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DOI: https://doi.org/10.1007/BF00819854