Bimodal momentum distribution of laser-cooled atoms in optical lattices
arXiv:1604.03374 · doi:10.1103/PhysRevA.93.053416
Abstract
We study, numerically and experimentally, the momentum distribution of atoms cooled in optical lattices. Using semi-classical simulations, we show that this distribution is bimodal, made up of a central feature corresponding to "cold", trapped atoms, with tails of "hot", untrapped atoms, and that this holds true also for very shallow potentials. Careful analysis of the distribution of high-momentum untrapped atoms, both from simulations and experiments, shows that the tails of the distribution does not follow a normal law, hinting at a power-law distribution and non-ergodic behavior. We also revisit the phenomenon of décrochage, the potential depth below which the temperature of the atoms starts increasing.
References in corpus (10)
- Laser Cooling of Molecular Anions
- Efficient all-optical production of large Li quantum gases using D gray-molasses cooling
- Simultaneous sub-Doppler laser cooling of fermionic Li and K on the D line: Theory and Experiment
- Analysis of self-organized criticality in Ehrenfest's dog-flea model
- All optical cooling of K to Bose Einstein condensation
- Deviations from Boltzmann-Gibbs equilibrium in confined optical lattices
- Cold atoms: A field enabled by light
- Proposal for laser-cooling of rare-earth ions
- Time dependence of laser cooling in optical lattices
- Simulations of Sisyphus cooling including multiple excited states