Abstract

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. At low energy, the particles are classically localized due to the absence of a percolating cluster. At high energy, the particles undergo normal diffusion, and we show that the diffusion coefficients scale algebraically with the particle energy, with an anisotropy factor that is significantly different from that of the disordered potential. At 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 the 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 paper give insights into recent experimental results, but it may also help in the interpretation of future experiments searching for deviation from classical diffusion and traces of Anderson localization.

Highlights

  • Germany. 2 Current address: Institute for Quantum Electronics, ETH Zürich, Hönggerberg, CH-8093 Zürich, Switzerland. 3 Author to whom any correspondence should be addressed

  • We study some topographic properties of the 2D speckle potential that are relevant for understanding the transport regimes of classical particles

  • Upon proper rescaling, the atomic dynamics can be parameterized by the energy as the sole relevant quantity

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Summary

Introduction

With a view to searching for localization effects in cold atomic gases, characterization of classical transport regimes is a central task. It is of special interest in dimension two (2D), which is the marginal dimension for return probability in Brownian motion and for Anderson localization [71]. Where σR is the characteristic length scale of the disordered potential, λdB is the atomic de Broglie wavelength, lB is the Boltzmann (transport) mean free path, L is the system size and Lloc is the localization length. Instead we consider the opposite condition λdB σR, meaning that the atoms scatter in the disordered potential as purely classical particles, satisfying the Newton equations of motion. An additional aim is to use these results to determine the behavior of atomic clouds with a broad energy distribution, as is relevant to cold-atom experiments

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