Abstract

A theoretical analysis of the resonance fluorescence of a two-level atom in a classical monochromatic field with feedback phase switching depending on the fluorescence triplet component which the last spontaneously emitted photon belongs to is presented. The considered feedback loop is a hybrid quantum-classical system. Statistics of photoemissions into the triplet components is investigated as well as correlations between the components. In contrast to the well-known resonance fluorescence of a two-level atom without feedback phase switching, a bunching of photocounts is predicted in each side-band, and successive photoemissions into different side-bands manifest antibunching. The type of the statistics can efficiently be controlled by the frequency detuning of the external field. In many points the considered feedback scheme provides drastically different statistical features of fluorescence when compared with the scheme of frequency-unselective feedback phase switching.

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