2014
DOI: 10.1103/physreva.89.063409
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Atom trapping and spectroscopy in cavity-generated optical potentials

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Cited by 16 publications
(13 citation statements)
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“…Unfortunately, these systems are experimentally demanding due to the need of ultra-high-reflectivity coatings and sophisticated techniques to trap single atoms in these short cavities. However, the notion that short cavities with high finesse are inevitable has been challenged by efforts to use a particular cavity geometry, a (near-)concentric cavity, to implement cavity QED with long cavities of low finesse [6][7][8][9][10][11][12][13]. A cavity is concentric when the separation of the two mirrors l cav matches twice the radius of curvature of the mirrors R C .…”
mentioning
confidence: 99%
“…Unfortunately, these systems are experimentally demanding due to the need of ultra-high-reflectivity coatings and sophisticated techniques to trap single atoms in these short cavities. However, the notion that short cavities with high finesse are inevitable has been challenged by efforts to use a particular cavity geometry, a (near-)concentric cavity, to implement cavity QED with long cavities of low finesse [6][7][8][9][10][11][12][13]. A cavity is concentric when the separation of the two mirrors l cav matches twice the radius of curvature of the mirrors R C .…”
mentioning
confidence: 99%
“…In possible future experimental work, an ultra-deep Rydberg-atom lattice with a depth of 2V 0 = h × 3 GHz, as considered in this section, could be achieved by focusing two counter-propagating laser beams, each with a power of 200 W, into a confocal spot with w 0 = 20 µm. Such a lattice can be prepared, for instance, by using a near-concentric field enhancement cavity [40], with the Rydberg atoms loaded into the focal spot of the cavity.…”
Section: A An Implementation Of a Strong Optical Latticementioning
confidence: 99%
“…1. We load 85 Rb atoms from a MOT, initially prepared in the F = 3 ground-state hyperfine level, into the near-perfect TEM 00 mode of a near-concentric field-enhancement cavity with a finesse of ≈ 600 at λ = 1064 nm [27][28][29]. After loading, the lattice is adiabatically ramped to a maximum depth of ∼ 10 5 E r , where E r = h × 2.076 kHz is the photon recoil for 85 Rb at 1064 nm.…”
Section: Simulationmentioning
confidence: 99%