Density Functional of a Two-Dimensional Gas of Dipolar Atoms: Thomas-Fermi-Dirac Treatment
arXiv:1008.1163 · doi:10.1103/PhysRevA.83.052517
Abstract
We derive the density functional for the ground-state energy of a two-dimensional, spin-polarized gas of neutral fermionic atoms with magnetic-dipole interaction, in the Thomas-Fermi-Dirac approximation. For many atoms in a harmonic trap, we give analytical solutions for the single-particle spatial density and the ground-state energy, in dependence on the interaction strength, and we discuss the weak-interaction limit that is relevant for experiments. We then lift the restriction of full spin polarization and account for a time-independent inhomogeneous external magnetic field. The field strength necessary to ensure full spin polarization is derived.
12 pages, 4 figures, 1 table
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- Leading gradient correction to the kinetic energy for two-dimensional fermion gases
- Systematic corrections to the Thomas-Fermi approximation without a gradient expansion
- Airy-averaged gradient corrections for two-dimensional fermion gases
- Density-functional theory for the crystalline phases of a two-dimensional dipolar Fermi gas
- Kohn-Sham theory of rotating dipolar Fermi gas in two dimensions
- Collective excitations of a harmonically trapped, two-dimensional, spin-polarized dipolar Fermi gas in the hydrodynamic regime
- Ground state of a two component dipolar Fermi gas in a harmonic potential
- Kohn-Sham approach to Fermi gas superfluidity: the bilayer of fermionic polar molecules
- Self-consistent field theory of polarized BEC: dispersion of collective excitation
- Energy functionals of single-particle densities: A unified view
- Testing the nonlocal kinetic energy functional of an inhomogeneous, two-dimensional degenerate Fermi gas within the average density approximation
- Ordered phases in a bilayer system of dipolar fermions