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arXiv:cond-mat/0210022 · Physical Review A

Anomalous diffusion and Tsallis statistics in an optical lattice

Eric Lutz

Published May 27, 2003• 156 citations
arXivHTMLPDF

Abstract

We point out a connection between anomalous transport in an optical lattice and Tsallis' generalized statistics. Specifically, we show that the momentum equation for the semiclassical Wigner function which describes atomic motion in the optical potential, belongs to a class of transport equations recently studied by Borland [Phys. Lett. A 245, 67 (1998)]. The important property of these ordinary linear Fokker-Planck equations is that their stationary solutions are exactly given by Tsallis distributions. An analytical expression of the Tsallis index q in terms of the microscopic parameters of the quantum-optical problem is given and the spatial coherence of the atomic wave packets is discussed.

DOI
10.1103/physreva.67.051402

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We point out a connection between anomalous transport in an optical lattice and Tsallis' generalized statistics. Specifically, we show that the momentum equation for the semiclassical Wigner function which describes atomic motion in the optical potential, belongs to a class of transport equations recently studied by Borland [Phys. Lett. A 245, 67 (1998)]. The important property of these ordinary linear Fokker-Planck equations is that their stationary solutions are exactly given by Tsallis distributions. An analytical expression of the Tsallis index q in terms of the microscopic parameters of the quantum-optical problem is given and the spatial coherence of the atomic wave packets is discussed.
We study theoretically the spatial diffusion (transport) of two-level atoms in one- and two-dimensional optical molasses derived from counterpropagating laser beams. We use both quantum Monte Carlo and semiclassical methods to study the microscopic characteristics of the atomic motion and their effect on the macroscopic behavior of the spatial distribution. We find that there exists a certain critical depth of the optical potential below which the atomic trajectories show L\'evy flights in space that last on a definite time scale (L\'evy walks). This behavior leads to a transition from Gaussian spatial diffusion to anomalous diffusion while crossing this critical potential depth. We show that only atoms with very high momentum are responsible for these L\'evy walks. This observation allows us to predict the critical parameters via a semiclassical Fokker-Planck equation approach. \textcopyright{} 1996 The American Physical Society.
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A semiclassical theory of chaotic atomic transport in a one-dimensional nondissipative optical lattice, when the standing-wave field and center-of-mass motion are treated classically, is developed. Using the basic equations of motion for the Bloch and translational atomic variables, we derive a stochastic map for the synchronized component of the atomic dipole moment that determines the center-of-mass motion. We find the analytical relations between the atomic and lattice parameters under which atoms typically alternate between flying through the lattice and being trapped in the wells of the optical potential. We use the stochastic map to derive formulas for the probability density functions (PDFs) for the flight and trapping events. Statistical properties of chaotic atomic transport strongly depend on the relations between the atomic and lattice parameters. We show that there is a good quantitative agreement between the analytical PDFs and those computed with the stochastic map and the basic equations of motion for different ranges of the parameters. Typical flight and trapping PDFs are shown to be broad distributions with power law segments with the slope $\ensuremath{-}1.5$ and exponential ``tails.'' The lengths of the power law and exponential segments of the PDFs depend on the values of the parameters. We find analytical conditions under which deterministic atomic transport has fractal properties and explain a hierarchical structure of the dynamical fractals.
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Quantum-mechanical transport of atoms in an optical lattice in one dimension is described in an exactly solvable model. The atoms are tightly bound and they are sufficiently cooled so that they are restricted only to the lowest Bloch band in a single adiabatic potential. The coherent spreading of an atomic wave packet by tunneling is counteracted by the localizing effect of photon emission that accompanies optical pumping. The time evolution of the quasimomentum distribution, the coherence length, and the spatial width of the atomic state are evaluated analytically. These quantities depend strongly on the statistics of photon emissions.