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Quantum Electronics and Laser Science Conference

Two-dimensional Tight Confinement Of Cold Cesium Atoms In A Far-detuned Dipole Trap

Denis Boiron, A. Michaud, Ch Salomon

Published Jan 1, 1997• 0 citations
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Received 4 November 1997We study the behavior of cesium atoms confined in far-detuned laser traps and submitted to blue Sisyphuscooling. First, in a single focused yttrium aluminum garnet YAG beam, the atomic cloud has a rod shape witha6- 3mtransverse waist radius, a temperature of 2 K, and a transient density of 10

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We study the behavior of cesium atoms confined in far-detuned laser traps and submitted to blue Sisyphus cooling. First, in a single focused yttrium aluminum garnet (YAG) beam, the atomic cloud has a rod shape with a $6\ensuremath{-}\ensuremath{\mu}\mathrm{m}$ transverse waist radius, a temperature of $2\ensuremath{\mu}\mathrm{K}$, and a transient density of 10${}^{12}{\phantom{\rule{0ex}{0ex}}\mathrm{a}\mathrm{t}\mathrm{o}\mathrm{m}\mathrm{s}/\mathrm{c}\mathrm{m}}^{3}$. For this sample, we have not detected any influence of photon multiple scattering on the atomic temperature, in contrast to previous measurements in isotropic samples. Second, the YAG laser is used to produce a $29\ensuremath{-}\ensuremath{\mu}\mathrm{m}$ period hexagonal optical lattice in which we directly observe the localization of the atoms by absorption imaging. Equilibrium densities on the order of ${10}^{13}{\phantom{\rule{0ex}{0ex}}\mathrm{a}\mathrm{t}\mathrm{o}\mathrm{m}\mathrm{s}/\mathrm{c}\mathrm{m}}^{3}$ are achieved in this structure.

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Towards implementation of a magic optical-dipole trap for confining ground-state and Rydberg-state cesium cold atoms

Jiandong Bai, Shuo Liu, Jun He +1 more

Abstract Long ground-Rydberg coherence lifetime is interesting for implementing high-fidelity quantum logic gates, many-body physics, and other quantum information protocols. However, the potential formed by a conventional far-off-resonance red-detuned optical-dipole trap (ODT) is usually repulsive for Rydberg atoms, which will result in fast atom loss and low repetition rate of the experimental sequence. These issues can be addressed by a magic ODT. We performed the calculation of ODT’s magic detuning for confinement of ground-state and Rydberg-state cesium atoms with the same potential well. We used a sum-over-states method to calculate the dynamic polarizabilities of 6S 1/2 ground state and highly-excited ( n S 1/2 and n P 3/2 ) Rydberg state of cesium atoms, and identify corresponding magic detuning for optical wavelengths in the range of 850–1950 nm. We estimated the trapping lifetime of cesium Rydberg atoms confined in the magic ODT by including different dissipative mechanisms. Furthermore, we have experimentally realized an 1879.43 nm single-frequency laser system with a watt-level output power for setting up the magic ODT for 6S 1/2 ground-state and 84P 3/2 Rydberg-state cesium cold atoms.

arXiv:2001.05698•Journal of Physics B Atomic Molecular and Optical Physics•May 11, 2020•10 citations
We study the behavior of cesium atoms confined in far-detuned laser traps and submitted to blue Sisyphus cooling. First, in a single focused yttrium aluminum garnet (YAG) beam, the atomic cloud has a rod shape with a $6\ensuremath{-}\ensuremath{\mu}\mathrm{m}$ transverse waist radius, a temperature of $2\ensuremath{\mu}\mathrm{K}$, and a transient density of 1012atoms/cm3{}^{12}{\phantom{\rule{0ex}{0ex}}\mathrm{a}\mathrm{t}\mathrm{o}\mathrm{m}\mathrm{s}/\mathrm{c}\mathrm{m}}^{3}12atoms/cm3. For this sample, we have not detected any influence of photon multiple scattering on the atomic temperature, in contrast to previous measurements in isotropic samples. Second, the YAG laser is used to produce a $29\ensuremath{-}\ensuremath{\mu}\mathrm{m}$ period hexagonal optical lattice in which we directly observe the localization of the atoms by absorption imaging. Equilibrium densities on the order of 1013atoms/cm3{10}^{13}{\phantom{\rule{0ex}{0ex}}\mathrm{a}\mathrm{t}\mathrm{o}\mathrm{m}\mathrm{s}/\mathrm{c}\mathrm{m}}^{3}1013atoms/cm3 are achieved in this structure.
Abstract Long ground-Rydberg coherence lifetime is interesting for implementing high-fidelity quantum logic gates, many-body physics, and other quantum information protocols. However, the potential formed by a conventional far-off-resonance red-detuned optical-dipole trap (ODT) is usually repulsive for Rydberg atoms, which will result in fast atom loss and low repetition rate of the experimental sequence. These issues can be addressed by a magic ODT. We performed the calculation of ODT’s magic detuning for confinement of ground-state and Rydberg-state cesium atoms with the same potential well. We used a sum-over-states method to calculate the dynamic polarizabilities of 6S 1/2 ground state and highly-excited ( n S 1/2 and n P 3/2 ) Rydberg state of cesium atoms, and identify corresponding magic detuning for optical wavelengths in the range of 850–1950 nm. We estimated the trapping lifetime of cesium Rydberg atoms confined in the magic ODT by including different dissipative mechanisms. Furthermore, we have experimentally realized an 1879.43 nm single-frequency laser system with a watt-level output power for setting up the magic ODT for 6S 1/2 ground-state and 84P 3/2 Rydberg-state cesium cold atoms.