2007
DOI: 10.1103/physreva.75.013406
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Diffraction-limited optics for single-atom manipulation

Abstract: We present an optical system designed to capture and observe a single neutral atom in an optical dipole trap, created by focussing a laser beam using a large numerical aperture (N.A. = 0.5) aspheric lens. We experimentally evaluate the performance of the optical system and show that it is diffraction limited over a broad spectral range (∼ 200 nm) with a large transverse field (±25 µm). The optical tweezer created at the focal point of the lens is able to trap single atoms of 87 Rb and to detect them individual… Show more

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Cited by 102 publications
(99 citation statements)
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“…Thus, it is instructive to show independently that the barrier penetrability for bosons increases due to symmetrization of the wave function. Before turning to this task, we note that this fact might be demonstrated experimentally by modern techniques, that allow the preparation of Bose condensates as well as single atoms in double well traps (see, e.g., [10,11,12,13]). To do this, an initial state of a single boson in one well and Bose condensate in the other well should be formed.…”
Section: Probability Of Stimulated α Decaymentioning
confidence: 99%
“…Thus, it is instructive to show independently that the barrier penetrability for bosons increases due to symmetrization of the wave function. Before turning to this task, we note that this fact might be demonstrated experimentally by modern techniques, that allow the preparation of Bose condensates as well as single atoms in double well traps (see, e.g., [10,11,12,13]). To do this, an initial state of a single boson in one well and Bose condensate in the other well should be formed.…”
Section: Probability Of Stimulated α Decaymentioning
confidence: 99%
“…However, limited by the technology, it is difficult to make the focus small enough. At present, by using diffraction-limited optics based on the combination of a large numerical aperture aspheric lens (NA = 0.5) placed inside the vacuum chamber and a few standard lenses placed outside, a waist of w 0 = (1.03±0.01) μm at 850 nm and a radial oscillation frequency of ν r = (160±3) kHz with a trap depth U 0 = 2.8 mK have been obtained [28,58]. If stronger confinement is required and at the same time a lower red detuned potential depth is desired, a different method must be used.…”
Section: Combining Red and Blue Detuned Optical Potentials To Form A mentioning
confidence: 99%
“…It allows us to adjust the radial oscillation frequency continuously by changing the blue detuned potential depth. Furthermore, we can optimize our scheme by using a diffraction-limited optics as in [58].…”
Section: Experimental Demonstration For the Lamb-dicke Trapmentioning
confidence: 99%
“…We trap lasercooled rubidium 87 atoms in a microscopic dipole trap produced by focusing a laser beam at 957 nm with a large-numerical-aperture aspheric lens, as described in Ref. [26]. The 1/e 2 radius of the gaussian spot is w = 1.6 µm.…”
Section: Experimental Set-up and Proceduresmentioning
confidence: 99%
“…We find that the heating rate R(t), which amounts initially to R(0) = 22 s −1 , drops very rapidly and has very little influence on the evaporation. For the one-body loss rate, we plug in the simulation the value K 1 = 0.1 s −1 corresponding to the measured 10 s vacuum-limited lifetime of a single atom in the microscopic trap [26]. Also, we take for the three-body loss rate the value that we measured in a separate experiment, K 3 = 4 × 10 −29 cm 6 .s −1 [46].…”
Section: Evaporation Dynamicsmentioning
confidence: 99%