2012
DOI: 10.1103/physreva.85.033619
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Dipolar Bose-Einstein condensates with large scattering length

Abstract: A uniform dilute Bose gas of known density has a universal behavior as the atomic scattering length tends to infinity at unitarity while most of its properties are determined by a universal parameter ξ relating the energies of the noninteracting and unitary gases. The usual mean-field equation is not valid in this limit, and beyond mean-field corrections become important. We use a dynamical model including such corrections to investigate a trapped disk-shaped dipolar Bose-Einstein condensate (BEC) and a dipola… Show more

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Cited by 4 publications
(5 citation statements)
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References 67 publications
(111 reference statements)
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“…Stable checkerboard, star, and stripe configurations in dipolar BECs have been identified in a two-dimensional (2D) optical lattice as stable Mott insulator [19] as well as superfluid soliton [20] states. A new possibility of studying universal properties of dipolar BECs at unitarity has been suggested [21].…”
Section: Introductionmentioning
confidence: 99%
“…Stable checkerboard, star, and stripe configurations in dipolar BECs have been identified in a two-dimensional (2D) optical lattice as stable Mott insulator [19] as well as superfluid soliton [20] states. A new possibility of studying universal properties of dipolar BECs at unitarity has been suggested [21].…”
Section: Introductionmentioning
confidence: 99%
“…Distinct stable checkerboard, stripe, and star configurations in dipolar BECs have been identified in a two-dimensional (2D) optical lattice as a stable Mott insulator [17] as well as superfluid soliton [18] states. A new possibility of studying the universal properties of dipolar BECs for large scattering length has been suggested [19]. Many of these features have only been predicted theoretically, although some of them have already been experimentally confirmed.…”
Section: Introductionmentioning
confidence: 99%
“…An approximate variational solution of ( 25) is possible with the following ansatz for density [41] n(ρ) = 1/ πw 2 ρ exp − ρ 2 w 2 ρ , while the width w ρ is determined by solving (16) with w z = d z and κ = w ρ /d z .…”
Section: Approximate Density For Cigar and Disc Shapesmentioning
confidence: 99%
“…With this initial condition ( 35) is solved by real-time propagation [43] to study sound waves. Typical anisotropic sound propagation in θ = 0 (num,n 0 =10 16 /cm 3 ) θ = 0 (ana,n 0 =10 16 /cm 3 ) θ = π/2 (num,n 0 =10 16 /cm 3 ) θ = π/2 (ana,n 0 =10 16…”
Section: Anisotropic Sound Propagation In Uniform Dipolar Fermi Gasmentioning
confidence: 99%
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