The Ground State Energy of a Mean-Field Fermi Gas in Two Dimensions

Abstract

We rigorously establish a formula for the correlation energy of a two-dimensional Fermi gas in the mean-field regime for potentials whose Fourier transform $\hat{V}$ satisfies $\hat{V}(\cdot )|\cdot |\in {\ell }^1$. Further, we establish the analogous upper bound for $\hat{V}(\cdot {)}^2|\cdot {|}^{1+\epsilon }\in {\ell }^1$, which includes the Coulomb potential $\hat{V}(k)\sim |k{|}^{-2}$. The proof is based on an approximate bosonization using slowly growing patches around the Fermi surface. In contrast to recent proofs in the three-dimensional case, we need a refined analysis of low-energy excitations, as they are less numerous, but carry larger contributions.

46 pages, 6 figures