Abstract

We present a theoretical study on magneto-photon-phonon interaction in a parabolically confined quantum dot subjected simultaneously to static magnetic field and radiation field. A nonperturbative treatment for electron-photon interaction is proposed by solving analytically the time-dependent Schr\odinger equation in which the magnetic field and the radiation field are included exactly. We employ the energy-balance equation approach on the basis of the Boltzmann equation to evaluate the energy transfer rate induced by optical transition events. It is found that for relatively low radiation levels, two peaks of the cyclotron resonance (CR) appear at two Kohn's frequencies ${\ensuremath{\omega}}_{\ifmmode\pm\else\textpm\fi{}}$, and the strength and the width of the CR increase with radiation intensity. The CR at ${\ensuremath{\omega}}_{+}$ is more prominent than that at ${\ensuremath{\omega}}_{\ensuremath{-}}$. When the radiation become intense, the splitting of the CR peaks can be observed and the splitting increases with radiation intensity. The physics reasons behind these interesting findings are discussed. This study is pertinent to the application of intense terahertz radiation sources such as free-electron lasers in the investigation into low-dimensional semiconductor systems.

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