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

TL;DR

This paper rigorously derives the correlation energy formula for a two-dimensional mean-field Fermi gas, including Coulomb interactions, using an approximate bosonization approach focused on low-energy excitations.

Contribution

It provides a new rigorous derivation of the correlation energy for 2D Fermi gases with Coulomb-like potentials, employing a refined bosonization technique.

Findings

Established a formula for the correlation energy in 2D Fermi gases.

Extended the analysis to include Coulomb potentials.

Developed a refined low-energy excitation analysis.

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 $\hat{V}(\cdot)^2 | \cdot |^{1 + \varepsilon} \in \ell^1$, 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.