2013
DOI: 10.1088/0953-4075/46/21/215003
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Trapping of85Rb atoms by optical pumping between metastable hyperfine states

Abstract: We describe an atom trapping mechanism based upon differential optical pumping between metastable hyperfine states by partially-displaced laser beams in the absence of a magnetic field. With realistic laser powers, trap spring constants should match or exceed those typical of magneto-optical traps, and highly flexible tailored trap shapes should be achievable. In a proof-of-principle experiment, we have combined a 1D implementation with magneto-optical trapping in the orthogonal directions, capturing ∼ 10 4 85… Show more

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Cited by 4 publications
(3 citation statements)
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“…Second, position and velocity dependent optical pumping effects, that can give rise to spatial confinement (e.g. [19,20]), are minimized. This is because all laser beams drive the same σ − -transitions with respect to a 'universal' quantization axis (except for a small contribution of σ + -transitions).…”
Section: Trapping Mechanismmentioning
confidence: 99%
“…Second, position and velocity dependent optical pumping effects, that can give rise to spatial confinement (e.g. [19,20]), are minimized. This is because all laser beams drive the same σ − -transitions with respect to a 'universal' quantization axis (except for a small contribution of σ + -transitions).…”
Section: Trapping Mechanismmentioning
confidence: 99%
“…In order to determine the influence of these 'equilibrium state' atoms on the spectroscopic signals, we adopt a similar approach to that presented in previous work on atom trapping using optical pumping effects 35 , developing a rate-equation based model in which we consider the six-level system shown in figure 1(b). For convenience, we label the F=3 and F=4 hyperfine states of the 6S 1/2 level as 'A' and 'B' respectively, while the F =2 through F =4 hyperfine states of the 6P 3/2 level will be denoted by 'C' to 'F' respectively.…”
Section: Theoretical Modelmentioning
confidence: 99%
“…First, we only consider initial states of the atom with no angular momentum. For atoms with just one electron in its last orbital, which are commonly used for atomic trapping [9,26,29], we can approximate the wave function as that of the hydrogen atom by adding a correction term to the principal quantum number [23]; this approximation is especially accurate for Rydberg atoms [15].…”
Section: Decoherence By Scatteringmentioning
confidence: 99%