Local origin of the pseudogap in the attractive Hubbard model

TL;DR

This paper offers a new local excitation perspective on the pseudogap phenomenon in the attractive Hubbard model, emphasizing the role of local physics and incoherent hopping at finite temperatures.

Contribution

It demonstrates that pseudogap physics can be explained by local excitations causing quasiparticle peak splitting, using dynamical mean field theory with a momentum-independent self-energy.

Findings

Pseudogap arises from local excitations leading to quasiparticle peak splitting.

Pseudogap physics is prominent at intermediate and high temperatures with incoherent hopping.

Predictions are testable with ultracold atom experiments in optical lattices.

Abstract

We provide a new perspective on the pseudogap physics for attractive fermions as described by the three-dimensional Hubbard model. The pseudogap in the single-particle spectral function, which occurs for temperatures above the critical temperature $T_c$ of the superfluid transition, is often interpreted in terms of preformed, uncondensed pairs. Here we show that the occurrence of pseudogap physics can be consistently understood in terms of local excitations which lead to a splitting of the quasiparticle peak for sufficiently large interaction. This effect becomes prominent at intermediate and high temperatures when the quantum mechanical hopping is incoherent. We clarify the existence of a conjectured temperature below which pseudogap physics is expected to occur. Our results are based on approximating the physics of the three-dimensional Hubbard model by dynamical mean field theory calculations and a momentum independent self-energy. Our predictions can be tested with ultracold atoms in optical lattices with currently available temperatures and spectroscopic techniques.