We investigate the effect of reabsorption of photons in laser cooling of trapped atoms, in view of a possible achievement of Bose-Einstein condensation by purely optical means. Reabsorption can be strongly suppressed by using strongly deformed traps and by reducing the fluorescence rate to a value smaller than the trap frequencies.
Optical trapping and cooling of atoms at high densities is limited by strong absorption of both the incident laser light and the emitted fluorescence. Reabsorption of the emitted fluorescence gives rise to repulsive forces between the trapped atoms and also to additional heating thus limiting both density and ultimate temperature. We have recently demonstrated a method to avoid these effects by shelving most of the atoms being trapped or cooled in a dark hyperfine state. At any instant, about one percent of the atoms are in the bright state where the trapping and cooling forces are exerted. This scheme ensures transparency of the atom cloud at very high optical densities.
Reabsorption, the multiple scattering of spontaneously emitted photons in optically thick gases, is a major limitation to efficient optical pumping and laser cooling in ultracold gases. We report mitigation of reabsorption using spatial and frequency modulation of laser light illuminating such gases. We developed a semiclassical model that successfully describes the reabsorption process when frequency-modulated light is present. It was necessary to extend the treatment in the model beyond a simple two-atom picture in order to reproduce our experimental results.
We study the optical loading of a trapped Bose-Einstein condensate by spontaneous emission of atoms in excited electronic state in the boson accumulation regime. We generalize the previous simplified analysis of Cirac and Lewenstein ( Phys. Rev. A , 53 (1996) 2466), to a 3D case in which more than one trap level of the excited-state trap is considered. By solving the corresponding quantum many-body master equation, we demonstrate that also for this general situation the photon reabsorption can help to increase the condensate fraction. Such effect could be employed to realize a continuous atom laser, and to overcome condensate losses.
We analyze the continuous pumping of atoms into a Bose-Einstein condensate via spontaneous emission from a thermal reservoir of atoms. We consider the case of atoms with a three-level $\ensuremath{\Lambda}$ scheme, in which one of the atomic transitions has a very much shorter lifetime than the other one. We found that in such a scenario the photon reabsorption in dense clouds at the frequency of the narrow transition can be considered negligible. If, in addition, inelastic processes can be kept negligible, we find that optical pumping can be used to continuously load and refill Bose-Einstein condensates, i.e., it provides a possible way to achieve a continuous atom laser.
The laser cooling and trapping of 87Rb atoms in pure-optical two frequency trap is studied in details. The parameter ranges in which optimal laser cooling is achieved were studied for the first time. The atoms can be simultaneously cooled and trapped by bichromatic laser field that opens up possibility to realize principally new type of pure optical trap. The depth of our trap is hundreds of spontaneous relaxation frequencies which corresponds to the depth of the magneto-optical traps used in the experiments.