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Regimes of classical transport of cold gases in a two-dimensional anisotropic disorder

Luca PezzèLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FranceMartin Robert-De-Saint-Vincentlaboratoire Charles Fabry de l'Institut d'Optique / Optique atomique (France)Thomas BourdelLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FranceJ-P Brantutlaboratoire Charles Fabry de l'Institut d'Optique / Optique atomique (France)Bruno AllardLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FranceThomas PlissonLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FranceAlain AspectLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FrancePhilippe BouyerLaboratoire Charles Fabry—UMR 8501, Institut d'Optique, CNRS, Univ Paris-Sud 11, 2 avenue Augustin Fresnel, F-91127 Palaiseau cedex, FranceLaurent Sanchez-Palencialaboratoire Charles Fabry de l'Institut d'Optique / Optique atomique (France)
2011en
ABI

Аннотация

We numerically study the dynamics of cold atoms in a two-dimensional disordered potential. We consider an anisotropic speckle potential and focus on the classical dynamics, which is relevant to some recent experiments. Firstly, we study the behavior of particles with a fixed energy and identify different transport regimes. For low energy, the particles are classically localized due to the absence of a percolating cluster. For high energy, the particles undergo normal diffusion and we show that the diffusion coefficients scale algebraically with the particle energy, with an anisotropy factor which significantly differs from that of the disordered potential. For intermediate energy, we find a transient sub-diffusive regime, which is relevant to the time scale of typical experiments. Secondly, we study the behavior of a cold-atomic gas with an arbitrary energy distribution, using the above results as a groundwork. We show that the density profile of the atomic cloud in the diffusion regime is strongly peaked and, in particular, that it is not Gaussian. Its behavior at large distances allows us to extract the energy-dependent diffusion coefficients from experimental density distributions. For a thermal cloud released into the disordered potential, we show that our numerical predictions are in agreement with experimental findings. Not only does this work give insights to recent experimental results, but it may also serve interpretation of future experiments searching for

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