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Quantum Electronics and Laser Science Conference

Spontaneous and stimulated photon emission and transverse quantum correlations in the optical microscopic cavity

F. De Martini

Published May 12, 1991• 0 citations
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Anomalous quantum processes in the context of spontaneous emission (SpE)1,2 and stimulated emission (StE)3,4, which are closely related to the fundamental dynamics of photon emission and to the related plane-wave quantum photon delocalization process4,5 were studied by our laboratory by use of the optical microcavity. The most efficient method we adopt in our present studies consists of a detailed investigation of the Bose-Einstein (BE) transverse quantum correlation process established within the microcavity active plane between two identical cylindrical microlasers (with diameter δ≈30 μm) excited by two identical focused pump beams (at wavelength λ p = 0.53 μm when working within nanosecond exciting pulse-duration (Δτ) conditions, SHG by an unstable-cavity Nd-YAG laser) and coupled to the same and common microcavity plane-wave, forward k-mode. Our investigation of the quantum coupling process consists of the determination of the thresholdless laser-gain (g) of the overall active device as a function of the radial distance s between the microlasers and determined by the position of the pump focused beams. The solution of the detailed QED intermicrolaser coupling equations leads to the determination of the s-dependence of the relevant dynamical quantity α(s), the degree of BE transverse quantum correlation by assuming the microcavity spacing d = d ¯ N , d ¯ ≡ λ / 2 as a relevant parameter. The overall laser output radiation is detected by a high quantum efficiency, cooled photomultiplier by previous focusing onto a 20-μm pinhole, making a spatial filter that dis criminates efficiently against detection of radiation emitted on FP-cavity modes other than the forward-mode.4

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Transverse quantum correlations in the active microscopic cavity

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A microcavity technique is adopted to investigate, we believe for the first time, the process of transverse interatom quantum correlations taking place after photon emission, according to the plane-wave QED photon-delocalization model. We find that the QED model is indeed verified, but that it is generally limited by the nonideal cavity properties. The concept introduced here of ``transverse quantum-correlation length'' is of fundamental relevance to all kinds of Casimir-type vacuum-confinement processes, including ``anomalous'' QED effects in spontaneous emission. It also sets a fundamental limitation on the performance of the ``thresholdless laser,'' a device of actual scientific and technological interest.

Physical Review Letters•Oct 1, 1990•83 citations
Anomalous quantum processes in the context of spontaneous emission (SpE)1,2 and stimulated emission (StE)3,4, which are closely related to the fundamental dynamics of photon emission and to the related plane-wave quantum photon delocalization process4,5 were studied by our laboratory by use of the optical microcavity. The most efficient method we adopt in our present studies consists of a detailed investigation of the Bose-Einstein (BE) transverse quantum correlation process established within the microcavity active plane between two identical cylindrical microlasers (with diameter δ≈30 μm) excited by two identical focused pump beams (at wavelength λ p = 0.53 μm when working within nanosecond exciting pulse-duration (Δτ) conditions, SHG by an unstable-cavity Nd-YAG laser) and coupled to the same and common microcavity plane-wave, forward k-mode. Our investigation of the quantum coupling process consists of the determination of the thresholdless laser-gain (g) of the overall active device as a function of the radial distance s between the microlasers and determined by the position of the pump focused beams. The solution of the detailed QED intermicrolaser coupling equations leads to the determination of the s-dependence of the relevant dynamical quantity α(s), the degree of BE transverse quantum correlation by assuming the microcavity spacing d = d ¯ N , d ¯ ≡ λ / 2 as a relevant parameter. The overall laser output radiation is detected by a high quantum efficiency, cooled photomultiplier by previous focusing onto a 20-μm pinhole, making a spatial filter that dis criminates efficiently against detection of radiation emitted on FP-cavity modes other than the forward-mode.4
A microcavity technique is adopted to investigate, we believe for the first time, the process of transverse interatom quantum correlations taking place after photon emission, according to the plane-wave QED photon-delocalization model. We find that the QED model is indeed verified, but that it is generally limited by the nonideal cavity properties. The concept introduced here of ``transverse quantum-correlation length'' is of fundamental relevance to all kinds of Casimir-type vacuum-confinement processes, including ``anomalous'' QED effects in spontaneous emission. It also sets a fundamental limitation on the performance of the ``thresholdless laser,'' a device of actual scientific and technological interest.