2010
DOI: 10.1103/physreva.81.031402
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Trapping ultracold atoms in a time-averaged adiabatic potential

Abstract: We report an experimental realization of ultracold atoms confined in a time-averaged, adiabatic potential (TAAP). This trapping technique involves using a slowly oscillating (∼kHz) bias field to time-average the instantaneous potential given by dressing a bare magnetic potential with a high-frequency (∼MHz) magnetic field. The resultant potentials provide a convenient route to a variety of trapping geometries with tunable parameters. We demonstrate the TAAP trap in a standard time-averaged orbiting potential t… Show more

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Cited by 35 publications
(41 citation statements)
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“…This configuration can be implemented in an effectively 2D BEC using a set of attractive (red-detuned) laser sheets and/or blue-detuned repelling sheet pairs [25], or in BEC layers isolated by a strong-standing optical wave [26], that can also be combined with magnetic trapping fields [27]. It is also possible to use the techniques allowing one to "paint" complex potential landscapes (in fact, even more complex than the H-shaped ones that we aim to consider) by rapidly moving laser beams [28], or induce time-averaged adiabatic landscapes created by means of variable magnetic fields [29]. Essentially the same effective potentials can be created in nonlinear optics using properly patterned photonic-crystal media [5] or a transverse trapping structure permanently written in bulk silica [30].…”
Section: Below)mentioning
confidence: 99%
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“…This configuration can be implemented in an effectively 2D BEC using a set of attractive (red-detuned) laser sheets and/or blue-detuned repelling sheet pairs [25], or in BEC layers isolated by a strong-standing optical wave [26], that can also be combined with magnetic trapping fields [27]. It is also possible to use the techniques allowing one to "paint" complex potential landscapes (in fact, even more complex than the H-shaped ones that we aim to consider) by rapidly moving laser beams [28], or induce time-averaged adiabatic landscapes created by means of variable magnetic fields [29]. Essentially the same effective potentials can be created in nonlinear optics using properly patterned photonic-crystal media [5] or a transverse trapping structure permanently written in bulk silica [30].…”
Section: Below)mentioning
confidence: 99%
“…7, but for the 1D model with the Gaussian profile of the mixed linear-nonlinear coupling, based on Eq (33),. and the variational ansatz(29). The width of the Gaussian profile is y 0 = 0.25 (squares), 0.125 (stars), and 0.05 (balls), respectively.…”
mentioning
confidence: 99%
“…A detailed discussion of the TAAP loading scheme is presented in [18]. Briefly, a typical experimental sequence begins with 5 × 10 6 atoms of 87 Rb at 1 µK confined in the |F = 1,m F = −1 hyperfine state, in an axially symmetric time-averaged orbiting potential (TOP) trap (ω T = 2π × 7 kHz) where B T = 3.2 G and B q = 84 G/cm.…”
Section: Implementation and Resultsmentioning
confidence: 99%
“…The positioning of the magnet coil several centimeters from the atoms gives rise to very smooth potentials that allow the preservation of the atomic phase coherence during changes to the confinement. In the first successful trapping of atoms in a TAAP trap reported in [2], cold atoms were loaded into a vertically offset double-well potential which could be adiabatically transformed into an anisotropic shell potential. Building on this work a successful technique was developed to trap atoms in a horizontally orientated, ring-shaped TAAP with a continuously adjustable ring radius [3].…”
Section: Introductionmentioning
confidence: 99%