Ground-state energy, density profiles, and momentum distribution of attractively interacting 1D Fermi gases with hard-wall boundaries: a Monte Carlo study

TL;DR

This study uses Monte Carlo simulations to analyze the ground-state properties of attractively interacting 1D Fermi gases with hard-wall boundaries, revealing detailed density, momentum, and correlation characteristics relevant to ultracold atom experiments.

Contribution

It provides a comprehensive Monte Carlo analysis of ground-state energy, density profiles, and momentum distribution in 1D attractive Fermi gases with hard walls, including a simple parametrization of density profiles.

Findings

Density profiles exhibit Friedel oscillations influenced by interactions.

Momentum distribution shows a robust discontinuity at the Fermi surface.

Tan's contact density and total contact are determined from correlations.

Abstract

Motivated by the realization of hard-wall boundary conditions in experiments with ultracold atoms, we investigate the ground-state properties of spin-1/2 fermions with attractive interactions in a one-dimensional box. We use lattice Monte Carlo methods to determine essential quantities like the energy, which we compute as a function of coupling strength and particle number in the regime from few to many particles. Many-fermion systems bound by hard walls display non-trivial density profiles characterized by so-called Friedel oscillations (which are similar to those observed in harmonic traps). In non-interacting systems, the characteristic length scale of the oscillations is set by (2 kF)^(-1), where kF is the Fermi momentum, while repulsive interactions tend to generate Wigner-crystal oscillations of period (4 kF)^(-1). Based on the non-interacting result, we find a remarkably simple parametrization of the density profiles of the attractively interacting case, which we generalize to the one-body density matrix. While the total momentum is not a conserved quantity in the presence of hard walls, the magnitude of the momentum does provide a good quantum number. We are therefore able to provide a detailed characterization of the (quasi-)momentum distribution, which displays rather robust discontinuity at the Fermi surface. In addition, we determine the spatially varying on-site density-density correlation, which in turn yields Tan's contact density and, upon integration, Tan's contact. As is well known, the latter fully determines the short-range correlations and plays a crucial role in a multitude of equilibrium and non-equilibrium sum rules.