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Annual Meeting Optical Society of America

Sub-μK cesium by adiabatic cooling in an optical lattice

R. J. C. Spreeuw, Poul Jessen, Anders Kastberg, William D. Phillips, S. L. Rolston

Published Jan 1, 1993• 0 citations
Publisher

Abstract

Cesium atoms are confined to a lattice of optical potential wells, created by four intersecting laser beams. As the light intensity is slowly reduced, the atoms adiabatically cool to a 3D temperature well below 1 μK.
DOI
10.1364/oam.1993.pdp.4

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We localize Cs atoms in wavelength-sized potential wells of an optical lattice, and cool them to a three-dimensional temperature of 700 nK by adiabatic expansion. In the optical lattice we precool the atoms to $\ensuremath{\approx}1\ensuremath{\mu}\mathrm{K}$. We then reduce the trapping potential in a few hundred $\ensuremath{\mu}$s, causing the atomic center-of-mass distribution to expand and the temperature to decrease by an amount which agrees with a simple 3D band theory. These are the lowest 3D kinetic temperatures ever measured.
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A complete laser cooling setup was built, with focus on threedimensional near-resonant optical lattices for cesium. These consist of regularly ordered micropotentials, created by the interference of four laser beams. One key feature of optical lattices is an inherent ”Sisyphus cooling” process. It efficiently extracts kinetic energy from the atoms, leading to equilibrium temperatures of a few µK. The corresponding kinetic energy is lower than the depth of the potential wells, so that atoms can be trapped.We performed detailed studies of the cooling processes in optical lattices by using the time-of-flight and absorption-imaging techniques. We investigated the dependence of the equilibrium temperature on the optical lattice parameters, such as detuning, optical potential and lattice geometry. The presence of neighbouring transitions in the cesium hyperfine level structure was used to break symmetries in order to identify, which role “red” and “blue” transitions play in the cooling. We also examined the limits for the cooling process in optical lattices, and the possible difference in steady-state velocity distributions for different directions. Moreover, in collaboration with ´Ecole Normale Sup´erieure in Paris, numerical simulations were performed in order to get more insight in the cooling dynamics of optical lattices.Optical lattices can keep atoms almost perfectly isolated from the environment and have therefore been suggested as a platform for a host of possible experiments aimed at coherent quantum manipulations, such as spin-squeezing and the implementation of quantum logic-gates. We developed a novel way to trap two different cesium ground states in two distinct, interpenetrating optical lattices, and to change the distance between sites of one lattice relative to sites of the other lattice. This is a first step towards the implementation of quantum simulation schemes in optical lattices.
Recently, great progress has been made in the cooling and trapping of atoms. It is now possible to create a collection of atoms with a number density in excess of 1011cm-3 and a kinetic temperature of the order of 10 μK. At such low temperatures the mean atomic velocity is of the order of 10cm/sec and the resulting Doppler width of the atomic transition is much lower than the homogeneous width. Furthermore, it has been shown that a substantial fraction of the atoms are localized inside wavelength-scale potential wells due to light-shifts[1]. Such a collection of essentially stationary atoms provide a reasonably large nonlinear susceptibility that can be exploited for the study of various nonlinear optical interactions [2].
A complete laser cooling setup was built, with focus on threedimensional near-resonant optical lattices for cesium. These consist of regularly ordered micropotentials, created by the interference of four laser beams. One key feature of optical lattices is an inherent ”Sisyphus cooling” process. It efficiently extracts kinetic energy from the atoms, leading to equilibrium temperatures of a few µK. The corresponding kinetic energy is lower than the depth of the potential wells, so that atoms can be trapped. We performed detailed studies of the cooling processes in optical lattices by using the time-of-flight and absorption-imaging techniques. We investigated the dependence of the equilibrium temperature on the optical lattice parameters, such as detuning, optical potential and lattice geometry. The presence of neighbouring transitions in the cesium hyperfine level structure was used to break symmetries in order to identify, which role “red” and “blue” transitions play in the cooling. We also examined the limits for the cooling process in optical lattices, and the possible difference in steady-state velocity distributions for different directions. Moreover, in collaboration with ´Ecole Normale Sup´erieure in Paris, numerical simulations were performed in order to get more insight in the cooling dynamics of optical lattices. Optical lattices can keep atoms almost perfectly isolated from the environment and have therefore been suggested as a platform for a host of possible experiments aimed at coherent quantum manipulations, such as spin-squeezing and the implementation of quantum logic-gates. We developed a novel way to trap two different cesium ground states in two distinct, interpenetrating optical lattices, and to change the distance between sites of one lattice relative to sites of the other lattice. This is a first step towards the implementation of quantum simulation schemes in optical lattices.
Laser-cooled 7Li^{7}\mathrm{Li}7Li atoms have been confined in three-dimensional spatially periodic potentials that are nearly conservative. The potentials were formed from the intersection of four laser beams far-detuned from the optical resonance. By adjusting the relative orientations of the beams, lattices with primitive translation vectors larger than the laser light wavelength were created. We achieved an effective temperature of \ensuremath{\sim}80 \ensuremath{\mu}K through adiabatic reduction of the confining potential strength, and prepared ensembles with effective temperatures of \ensuremath{\sim}1.8 \ensuremath{\mu}K by initially confining atoms in weak potentials.