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Physica

Modulation phenomena in resonance fluorescence

George William Series

Published Jan 1, 1967• 15 citations
Publisher
DOI
10.1016/0031-8914(67)90265-0

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The joint probability P 12 of detecting two photons at two different positions in the interference of a classical field with the resonance fluorescence field from a coherently driven two-level atom is investigated. We find that P 12 shows a stronger modulation with detector separation than is predicted by a classical wave theory. Under stationary conditions and if the driving field is strong enough to saturate the atomic transition, the relative modulation amplitude a of the P 12 pattern reaches its maximum possible value a = 1 for E → 0 (where E is the classical field amplitude), but simultaneously the whole phenomena vanishes, P 12 → 0. For equal intensities of the classical and the resonance fluorescent field we have a = ⅔. Compared with this, a classical wave theory predicts a possible maximum value of a = ½.

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The joint probability P 12 of detecting two photons at two different positions in the interference of a classical field with the resonance fluorescence field from a coherently driven two-level atom is investigated. We find that P 12 shows a stronger modulation with detector separation than is predicted by a classical wave theory. Under stationary conditions and if the driving field is strong enough to saturate the atomic transition, the relative modulation amplitude a of the P 12 pattern reaches its maximum possible value a = 1 for E → 0 (where E is the classical field amplitude), but simultaneously the whole phenomena vanishes, P 12 → 0. For equal intensities of the classical and the resonance fluorescent field we have a = ⅔. Compared with this, a classical wave theory predicts a possible maximum value of a = ½.