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Physica Scripta

Manipulation of the atomic localization via resonance fluorescence

Nelly Ciobanu, N. A. Enaki, Miguel Orszag

Published Mar 1, 2013• 0 citations
Publisher

Abstract

The possibility of manipulating the position of atoms dressed in the standing field of the cavity, based on the resonance fluorescence emission, is discussed. Stark dynamics modification and the strong coupling between two undistinguishable radiators situated in non-symmetric positions of the anti-nodes are investigated. The fluorescent spectrum is shown versus the second atom localization and external field parameters. We describe the conditions in which the Rabi frequencies of atoms change their correlations and cooperative emission.

DOI
10.1088/0031-8949/2013/t153/014011

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The possibility of manipulating the position of atoms dressed in the standing field of the cavity, based on the resonance fluorescence emission, is discussed. Stark dynamics modification and the strong coupling between two undistinguishable radiators situated in non-symmetric positions of the anti-nodes are investigated. The fluorescent spectrum is shown versus the second atom localization and external field parameters. We describe the conditions in which the Rabi frequencies of atoms change their correlations and cooperative emission.
The resonance fluorescence emitted by two three-level atoms dressed in a strong laser field is studied. A stark dynamics shift based on photon statistics is discussed. The appearance of coherent Rabi oscillations (quantum beats) of the atoms located in the non-symmetric positions of the anti-nodes and the modification of the quantum correlations at the Stokes and anti-Stokes cooperative emission are described. For some positions of the atoms, we observed the violation of the Cauchy–Schwarz inequality, finding antibunching in the scattered light. We present a scheme to control the position of atoms dressed with the standing field via the resonance fluorescence. (Some figures may appear in colour only in the online journal)
The influence of the standing wave amplitude on the resonance fluorescence of a three-level system of radiators is discussed. Great attention is devoted to the peculiarities of dressed states in the standing wave and the exchange integrals between two atoms situated in the anti-nodes or the nodes. The correlation functions of emitted photons at two dressed frequencies were obtained. It is shown that in the case when the distance between two atoms is smaller than the wavelength of the field, the emitted photons are strongly correlated. As was observed, for large values of laser field intensity, the control of spontaneous emission is possible at two frequencies as well as the atom–atom interaction process. The dependence of the fluorescent light spectrum as a function of the position of two atoms dressed in the standing wave is investigated.
We investigate the resonance fluorescence spectrum from two identical atoms driven by a strong standing-wave field. We find interesting modifications of the Mollow spectrum, caused by interferences between the two atoms, and in particular a succession of ``dark'' and ``bright'' states as one of the atoms is moved to successive nodes of the field. Large enough separation between the atoms leads to their decorrelation and the disappearance of these interferences, the atoms acting then as independent radiators. From a technical viewpoint, we also illustrate how the use of superoperators in Liouville space keeps the discussion transparent and provides a convenient tool for numerical calculations.
We have investigated the resonance fluorescence spectrum from two identical atoms driven by a strong standing wave field. We found interesting modifications of the Mollow spectrum, caused by interferences between the two atoms, and in particular a succession of dark and bright states as one of the atoms is moved to successive nodes of the field. Large enough separation between the atoms leads to the disappearance of these interferences, and the atoms act then as independent radiators, the fluorescence spectrum becoming then independent of the interatomic distance. From the point of view advocated by E. Wolf,1 one can interpret these modifications as caused by source correlations. For instance, we obtain new sidebands which are altered as the separation between atoms is modified. When these sidebands eventually cross, the fluorescence spectrum displays interesting properties such as “dark” and “bright” states. These investigations lay the foundations for a discussion of the influence of particle statistics on spectral properties of atoms cooled and trapped in optical molasses. The next step in this direction will include the effects of translational motion on these spectra.2 This program will eventually lead to a full-fledged field theoretical description of the spectral and translational correlation properties of an ensemble of cooled and trapped atoms.