The magnetophonon effect in nonpolar nondegenerate semiconductors is investigated by solving the Boltzmann equation exactly in the Ohmic limit for combined optical- and acousticphonon scattering of carriers in parallel electric and magnetic fields. The solution is used in computing the longitudinal magnetoresistance at several temperatures and ratios of acousticto optical-phonon scattering. As this ratio increases from zero at intermediate temperatures, the Gurevich-Firsov (GF) resonance maxima are found to broaden and shift toward higher magnetic field, with pronounced minima developing at the resonance fields before the magnetophonon structure vanishes at large acoustic-phonon scattering. As the temperature increases, additional (pseudoresonance) minima develop between the GF extrema, and are comparable in amplitude to the latter when kT approximates the optical-phonon energy. At these temperatures the GF extrema are minima, even in the absence of elastic scattering. The results are compared with displaced-Maxwellian computations. The various effects are explained by physical arguments, which suggest that the same effects should occur for polar materials also.
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Robert L. Peterson (1972) studied this question.
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