2012
DOI: 10.1103/physreva.85.033605
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Fast transitionless expansion of cold atoms in optical Gaussian-beam traps

Abstract: We study fast expansions of cold atoms in a three-dimensional Gaussian-beam optical trap. Three different methods to avoid final motional excitation are compared: inverse engineering using Lewis-Riesenfeld invariants, which provides the best overall performance, a bang-bang approach, and a fast adiabatic approach. We analyze the excitation effect of anharmonic terms, radial-longitudinal coupling, and radial-frequency mismatch. In the inverse-engineering approach these perturbations can be suppressed or mitigat… Show more

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Cited by 75 publications
(96 citation statements)
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“…These are exactly the forms obtained by Muga and collaborators [30] and despite the decoupling of the radial and axial coordinates, ω 2 r (t) and ω…”
Section: Extensions To Optical Dipole Trapping Using Gaussian Beamssupporting
confidence: 83%
See 1 more Smart Citation
“…These are exactly the forms obtained by Muga and collaborators [30] and despite the decoupling of the radial and axial coordinates, ω 2 r (t) and ω…”
Section: Extensions To Optical Dipole Trapping Using Gaussian Beamssupporting
confidence: 83%
“…We shall take the minimum Rayleigh length that permits paraxial approximation, z R = 2w 0 (typically z R is much larger, for example z R = 24w 0 in [30]). Also we choose the small beam waist of w 0 =20 and 200 harmonic oscillator lengths, based on the fact that the size of a typical beam waist can range from w 0 = 8µm (as in [30] which is of the order 53 harmonic oscillator lengths for 87 Rb atoms) to sizes of order 0.3 mm (corresponding to roughly 2, 000 harmonic oscillator lengths). Figure 3 shows the Π vs. ρ phase diagram, where the top row presents the phase space diagram for the radial variables Π r and ρ r and the bottom row is for the axial variables Π z and ρ z .…”
Section: Extensions To Optical Dipole Trapping Using Gaussian Beamsmentioning
confidence: 99%
“…Among other approaches let us mention (i) a transitionless tracking algorithm or "counterdiabatic" approach that adds to the original Hamiltonian extra terms to cancel transitions in the adiabatic or superadiabatic bases [8][9][10][11][12][13]; (ii) inverse engineering of the external driving [3,4,6,[21][22][23][24][25][26] based on Lewis-Riesenfeldt invariants [27], which has been applied in several expansion experiments [25,26]; (iii) optimal control (OC) methods [5,7,14,16], sometimes combined with other methods to enhance their performance [4,5,7]; (iv) the fast-forward (FF) approach advocated by Masuda and Nakamura [19,28]; (v) parallel adiabatic passage [29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…Torrontegui et al [15] studied the fast expansions of cold atoms in a three-dimensional Gaussian-beam optical trap. The radial and axial frequencies are coupled and as a consequence some shortcut schemes that work in 1D were in fact restricted to certain parameter domains, and others failed completely.…”
Section: Introductionmentioning
confidence: 99%