Abstract
The Stark representation of a strong external resonant field and the third order of perturbation theory of the fluorescence field are used to show that the probability of emission of the (ωa + 4Ω) harmonic (ωa and Ω are the atomic and Rabi frequencies) of collective resonance fluorescence of a pair of two-level atoms is equal to γ2/384, where γ is the width of the spontaneous emission line of a single atom.
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