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An optimal lower bound for the low density Fermi gas in three dimensions

Emanuela L. Giacomelli

TL;DR

The paper addresses the problem of rigorously deriving a Huang–Yang–type second-order lower bound for the ground state energy density of a dilute three-dimensional Fermi gas with spin-1/2 in the thermodynamic limit, for a broad class of positive, radial, compactly supported interactions. The authors develop a two-stage unitary transformation strategy—first a particle-hole map to separate correlations, then two quasi-bosonic Bogoliubov-type transformations near the Fermi surface—to isolate and control the relevant correlations responsible for the HY correction. They show that the energy density admits the HY-scale expansion $e(\rho_\uparrow,\rho_\downarrow) = \frac{3}{5}(6\pi^2)^{2/3}(\rho_\uparrow^{5/3}+\rho_\downarrow^{5/3}) + 8\pi a\rho_\uparrow\rho_\downarrow + \mathcal{O}(\rho^{7/3})$, with the error term optimal in order, and provide refined bounds on excitations outside the Fermi ball. The results extend previous upper-bound analyses, clarify the role of opposite-spin correlations in the HY term, and advance the rigorous understanding of low-density Fermi liquids by combining scattering-cancellation arguments with Bogoliubov-type decoupling and detailed propagation estimates.

Abstract

We consider the dilute Fermi gas in three dimensions interacting through a positive, radially symmetric, compactly supported and integrable potential in the thermodynamic limit. We establish a second order lower bound for the ground state energy density with an error term which is optimal in the sense that it matches the order of the next correction term conjectured by Huang-Yang in 1957.

An optimal lower bound for the low density Fermi gas in three dimensions

TL;DR

The paper addresses the problem of rigorously deriving a Huang–Yang–type second-order lower bound for the ground state energy density of a dilute three-dimensional Fermi gas with spin-1/2 in the thermodynamic limit, for a broad class of positive, radial, compactly supported interactions. The authors develop a two-stage unitary transformation strategy—first a particle-hole map to separate correlations, then two quasi-bosonic Bogoliubov-type transformations near the Fermi surface—to isolate and control the relevant correlations responsible for the HY correction. They show that the energy density admits the HY-scale expansion , with the error term optimal in order, and provide refined bounds on excitations outside the Fermi ball. The results extend previous upper-bound analyses, clarify the role of opposite-spin correlations in the HY term, and advance the rigorous understanding of low-density Fermi liquids by combining scattering-cancellation arguments with Bogoliubov-type decoupling and detailed propagation estimates.

Abstract

We consider the dilute Fermi gas in three dimensions interacting through a positive, radially symmetric, compactly supported and integrable potential in the thermodynamic limit. We establish a second order lower bound for the ground state energy density with an error term which is optimal in the sense that it matches the order of the next correction term conjectured by Huang-Yang in 1957.

Paper Structure

This paper contains 19 sections, 19 theorems, 367 equations.

Key Result

Theorem 2.1

Let $V, V_\infty$ be as in Assumption asu: potential V. As $\rho\rightarrow 0$, it holds that where $a$ is the scattering length of the interaction potential $V_\infty$.

Theorems & Definitions (40)

  • Theorem 2.1: Optimal energy asymptotics
  • Theorem 2.2: Excitation estimates
  • Remark 2.3: Hard core interaction
  • Remark 2.4: Filled Fermi sea
  • Definition 2.5: Particle-hole transformation
  • Proposition 2.6: Conjugation by $R$
  • Definition 2.7: Approximate ground state
  • Lemma 2.8: A priori bound for $\mathbb{H}_0, \mathbb{Q}_4, \mathbb{Q}_4^{\sigma, \sigma^\prime}, \mathcal{N}$
  • Remark 2.9: Comparison with Gia1
  • Lemma 2.10: Bounds for $\varphi$
  • ...and 30 more