Kelvin-Helmholtz instability in two-component Bose gases on a lattice
arXiv:1111.2175 · doi:10.1103/PhysRevA.85.023628
Abstract
We explore the stability of the interface between two phase-separated Bose gases in relative motion on a lattice. Gross-Pitaevskii-Bogoliubov theory and the Gutzwiller ansatz are employed to study the short- and long-time stability properties. The underlying lattice introduces effects of discreteness, broken spatial symmetry, and strong correlations, all three of which are seen to have considerable qualitative effects on the Kelvin-Helmholtz instability. Discreteness is found to stabilize low flow velocities, because of the finite energy associated with displacing the interface. Broken spatial symmetry introduces a dependence not only on the relative flow velocity, but on the absolute velocities. Strong correlations close to a Mott transition will stop the Kelvin-Helmholtz instability from affecting the bulk density and creating turbulence; instead, the instability will excite vortices with Mott-insulator filled cores.
11 pages, 11 figures
References in corpus (7)
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- Characteristic temperature for the immiscible-miscible transition of binary condensates in optical lattices
- Segregated quantum phases of dipolar bosonic mixtures in two-dimensional optical lattices
- Quantum droplet of a two-component Bose gas in an optical lattice near the Mott insulator transition
- Suppression of the superfluid Kelvin-Helmholtz instability due to massive vortex cores, friction and confinement
- Number-conserving approaches to -component Bose-Einstein condensates
- Emergence of spiral dark solitons in the merging of rotating Bose-Einstein condensates
- Kelvin-Helmholtz instability of AB interface in superfluid 3He