# Magnetization, d-wave superconductivity and non-Fermi liquid behavior in a crossover from dispersive to flat bands

## TL;DR

This paper investigates how inhomogeneity affects electronic phases in a 2D Hubbard model, revealing a transition from Fermi-liquid to non-Fermi-liquid behavior and the suppression of d-wave superconductivity with increased inhomogeneity.

## Contribution

It demonstrates the impact of inhomogeneity on electronic properties, including the emergence of non-Fermi-liquid behavior and the suppression of d-wave superconductivity in a Hubbard model.

## Key findings

- Crossover from Fermi-liquid to non-Fermi-liquid behavior at moderate inhomogeneity.
- Emergence of non-Fermi-liquid coincides with quasi-flat band formation.
- d-wave superconductivity is suppressed with increasing inhomogeneity.

## Abstract

We explore the effect of inhomogeneity on electronic properties of the two-dimensional Hubbard model on a square lattice using dynamical mean-field theory (DMFT). The inhomogeneity is introduced via modulated lattice hopping such that in the extreme inhomogeneous limit the resulting geometry is a Lieb lattice, which exhibits a flat-band dispersion. The crossover can be observed in the uniform sublattice magnetization which is zero in the homogeneous case and increases with the inhomogeneity. Studying the spatially resolved frequency-dependent local self-energy, we find a crossover from Fermi-liquid to non-Fermi-liquid behavior happening at a moderate value of the inhomogeneity. This emergence of a non-Fermi liquid is concomitant of a quasi-flat band. For finite doping the system with small inhomogeneity displays $d$-wave superconductivity coexisting with incommensurate spin-density order, inferred from the presence of oscillatory DMFT solutions. The $d$-wave superconductivity gets suppressed for moderate to large inhomogeneity for any finite doping while the incommensurate spin-density order still exists.