Density functional theory of the trapped Fermi gas in the unitary regime

Abstract

We investigate a density-functional theory (DFT) approach for an unpolarized trapped dilute Fermi gas in the unitary limit . A reformulation of the recent work of T. Papenbrock [Phys. Rev. A, {\bf 72}, 041602(R) (2005)] in the language of fractional exclusion statistics allows us to obtain an estimate of the universal factor, ${\xi }_{3D}$, in three dimensions (3D), in addition to providing a systematic treatment of finite-$N$ corrections. We show that in 3D, finite-$N$ corrections lead to unphysical values for ${\xi }_{3D}$, thereby suggesting that a simple DFT applied to a small number of particles may not be suitable in 3D. We then perform an analogous calculation for the two-dimensional (2D) system in the infinite-scattering length regime, and obtain a value of ${\xi }_{2D}=1$. Owing to the unique properties of the Thomas-Fermi energy density-functional in 2D our result, in contrast to 3D, is {\em exact} and therefore requires no finite-$N$ corrections.

References in corpus (4)

• Observation of the Pairing Gap in a Strongly Interacting Fermi Gas
• Critical Temperature and Thermodynamics of Attractive Fermions at Unitarity
• Fermi gas near unitarity around four and two spatial dimensions
• Density-functional theory for fermions in the unitary regime