The analytical solution for the spectrum of resonance fluorescence from a collective system of two atoms is presented. It is shown that the spectrum is a decreasing function of frequency in the neighborhood ω-ωL=±2Ω (Ω is the Rabi frequency) for moderately large Ω and exhibits resonant structure only for extremely large Ω≈100γ. For moderately large Ω the resonant contributions at ω-ωL=±2Ω are destroyed by the nonresonant contributions; hence the additional structures at ±2Ω can be resolved only by filtering the nonresonant contributions.
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Agarwal et al. (1980) studied this question.
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