Extremal positions in experimental recordings of the transverse magnetophonon resonance effect are usually phase-shifted with respect to magnetic field from the simple expression omega c = omega opt /n. This phase shift arises from the variation in amplitude of the resonance peaks, and is examined as a feature of both differentiated and undifferentiated recordings of the phenomenon; it is greater in the former case. Tables are presented that quote this shift both for power law and exponential amplitude functions.
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Blakemore et al. (1975) studied this question.
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