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Optics Communications

Force pattern on atoms in a monochromatic light field with arbitrary polarization

A. V. Bezverbnyĭ, Gerard Nienhuis, Anatolii M Tumaikin

Published Mar 1, 1998• 12 citations
Publisher
DOI
10.1016/s0030-4018(97)00697-4

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Light-induced force on atoms in a monochromatic light field with arbitrary polarization

A. V. Bezverbnyĭ, Gerard Nienhuis, Anatolii M Tumaikin

The light force on slow atoms in a light field with arbitrary polarization distribution is explicitly evaluated in the case of an atomic transition J yields J with half-integer J values. The expression of the force is based on an exact analytical expression for the steady-state density matrix of the atoms. The force is naturally separated in contributions resulting from gradients of the field intensity, the polarization ellipticity, and the phase. In addition to a conservative part this force also contains a vortex component. In areas of spatial localization, where the total force vanishes, the atomic motion is governed by a potential, which in general is not harmonic for J greater than 1/2. Simple model of the formation of a one- or two-dimensional spatial atomic grating in a specific light field configuration illustrates the results.

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Steady state of atoms in a monochromatic elliptically polarized light field

Gerard Nienhuis, А. В. Тайченачев, Anatolii M Tumaikin +1 more

An analytical and invariant expression is given for the steady-state density matrix of free atoms in a monochromatic radiation field with arbitrary intensity and arbitrary elliptical polarization. The field drives the closed transition F → F + 1, with arbitrary values of F . This is the only class of transitions where a closed analytical expression for the steady state was lacking. Some applications of this result are indicated.

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Light Forces on Atoms

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Springer series on atomic, optical, and plasma physics•Jan 1, 2001•0 citations
The light force on slow atoms in a light field with arbitrary polarization distribution is explicitly evaluated in the case of an atomic transition J yields J with half-integer J values. The expression of the force is based on an exact analytical expression for the steady-state density matrix of the atoms. The force is naturally separated in contributions resulting from gradients of the field intensity, the polarization ellipticity, and the phase. In addition to a conservative part this force also contains a vortex component. In areas of spatial localization, where the total force vanishes, the atomic motion is governed by a potential, which in general is not harmonic for J greater than 1/2. Simple model of the formation of a one- or two-dimensional spatial atomic grating in a specific light field configuration illustrates the results.