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International Conference Laser Optics (ICLO)

Cooperative properties of an atomic cluster in a charged Fabry-Perot microcavity

A. S. Kuraptsev, Igor M. Sokolov

Published Jun 1, 2018• 0 citations
Publisher

Abstract

We study the cooperative spontaneous decay and cooperative Lamb shift caused by the dipole-dipole interatomic interaction in an atomic cluster located in a Fabry-Perot microcavity with charged mirrors. The results are compared with the case when the mirrors are not charged as well as with the case of absence of the cavity, and the differences are discussed.

DOI
10.1109/lo.2018.8435469

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We study the cooperative spontaneous decay and cooperative Lamb shift caused by the dipole-dipole interatomic interaction in an atomic cluster located in a Fabry-Perot microcavity with charged mirrors. The results are compared with the case when the mirrors are not charged as well as with the case of absence of the cavity, and the differences are discussed.
We report the investigation of the peculiarities of excitation trapping caused by the cooperative effects in a disordered ensemble of point-like impurity centers (atoms) embedded in a transparent dielectric and located in a Fabry-Perot cavity. On the basis of the general quantum microscopic theory we have calculated cooperative spontaneous decay of an excited atom located in the center of a sample. It is shown that in the case when the distance between the mirrors of a cavity d is less or comparable with resonant wavelength of the atomic transition λ 0 , the character of cooperative effects in a cavity essentially differs from one without a cavity. For the opposite case d ≫ λ 0 cooperative effects in a cavity manifest themselves almost like in the case of absence of a cavity.
Abstract On the basis of a quantum microscopic approach, we study the excitation dynamics of two motionless point atoms located in fixed positions near a perfectly conductive charged surface. We analyze the spontaneous decay rate of individual atoms near the plate, as well as the strength of the dipole–dipole interaction between different atoms. It is shown that the spontaneous decay rate of an excited atom depends to a significant extent on its distance from the mirror. In the case where the interatomic separation is smaller than or comparable to the wavelength of the resonant radiation, the spontaneous decay dynamics of an excited atom is cooperative, so it is described by a multi-exponential law. It is shown that an electrostatic field caused by the charged plate modifies the character of the dipole–dipole interaction.
Abstract On the basis of the general quantum microscopic theory we study the process of spontaneous decay of an excited atom in a dense and disordered ensemble of point-like impurity atoms embedded into transparent dielectric and located near a charged perfectly conducting surface. We have analyzed the simultaneous influence of the modified spatial structure of field modes near the conductive surface and the electric field on the character of interatomic dipole-dipole interaction. This leads to the modification of the transition spectrum of an excited atom inside an ensemble and the spontaneous decay dynamics. We have shown that the electric field changes the cooperative Lamb shift, as well as the character of sub- and superradiant decay.
We report the development of quantum microscopic theory of quasiresonant dipole-dipole interaction in the ensembles of impurity atoms imbedded into transparent dielectric and located in a Fabry-Perot cavity. On the basis of the general approach we study the simultaneous influence of the cavity and resonant dipole-dipole interaction on the shape of the line of atomic transition as well as on light trapping in dense impurity ensembles. We analyze this influence depending on the size of the ensemble, its density, as well as on rms deviation of the transition frequency shifts caused by the symmetry disturbance of the internal fields of the dielectric medium. Obtained results are compared with the case when the cavity is absent. We show that the cavity can essentially modify cooperative polyatomic effects.