We show that an n-doped parabolic quantum well absorbs far infrared radiation at the bare harmonic-oscillator frequency ω₀ independently of the electron-electron interaction and the number of electrons in the well. In the presence of a magnetic field tilted with respect to the plane of the quantum well, we find that the cyclotron resonance becomes coupled to this ω₀ frequency mode. The absorption then occurs at two frequencies, which are again independent of the electron-electron interaction and the fractional filling of the well.
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Brey et al. (1989) studied this question.
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