2008
DOI: 10.1103/physreva.78.013631
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Vortex-lattice formation and melting in a nonrotating Bose-Einstein condensate

Abstract: Numerical simulations of the interference of a three-way segmented nonrotating Bose-Einstein condensate reveal the production of a honeycomb vortex lattice containing significant numbers of vortices and antivortices. If confined within a trap, the lattice subsequently melts, exhibiting a rich assortment of vortex-antivortex interactions. In contrast with nonlinear vortex production mechanisms previously described for Bose-Einstein condensates, the process here is shown to be primarily one of linear superpositi… Show more

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Cited by 21 publications
(32 citation statements)
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“…with J σ = i 2m σ (ψ * σ ∇ψ σ −ψ σ ∇ψ * σ ) being the velocity probability current. The overall vorticity of the system can be quantified via the integrated vorticity [96] Z σ = |Ω σ |dxdy.…”
Section: Observablesmentioning
confidence: 99%
“…with J σ = i 2m σ (ψ * σ ∇ψ σ −ψ σ ∇ψ * σ ) being the velocity probability current. The overall vorticity of the system can be quantified via the integrated vorticity [96] Z σ = |Ω σ |dxdy.…”
Section: Observablesmentioning
confidence: 99%
“…Adiabatic removal of the separating potential provided a statistical prediction of the presence or absence of a vortex in the resulting condensate, depending on the random relative phases of the initial condensate components. In contrast with this experiment, under sufficiently rapid non-adiabatic removal of the separating potential, three colliding condensate fragments have been predicted and demonstrated to form a honeycomb vortex-antivortex lattice, equivalent to two interleaved Abrikosov lattices-one of vortices and the other of antivortices [46,49,50]. Similar honeycomb vortex lattices could also be produced by using aberrated matter wave lensing technique [51,52].…”
Section: Introductionmentioning
confidence: 93%
“…Theê i are Cartesian basis vectors. In comparison, by treating the colliding wave packets as Gaussian functions the interference is described by the wavefunction [46,64] ψ (r, t) = π − 1 2 ∆p…”
Section: A Collision Of Three Scalar Condensatesmentioning
confidence: 99%
“…For vortices to be produced by interference, the contributions from each expanding wavepacket must be approximately equal. This establishes a spatiotemporal condition, which limits the lattice extent and describes its growth by vortex formation within an expanding circular envelope [9]. By evaluating the locations of two adjacent vortices of the same sign within this envelope, we find that the lattice basis vectors [ Fig.…”
mentioning
confidence: 91%
“…The π/2 pulse may be applied either immediately before or after trap removal. The overall translation of each VA lattice depends only on the relative phases of the initial wavepackets [9]. Although intra-component phases are uncontrolled in typical experiments, full control over the inter-component phase may be realized by spatially-localized Raman beam pairs focused on each wavepacket.…”
mentioning
confidence: 99%