Universal thermodynamics of the one-dimensional attractive Hubbard model

TL;DR

This paper investigates the universal thermodynamics, quantum criticality, and magnetism of the 1D attractive Hubbard model using the thermodynamic Bethe ansatz, revealing two free quantum fluids and phase boundary mappings.

Contribution

It provides a comprehensive analysis of the 1D attractive Hubbard model's thermodynamics and quantum critical behavior, highlighting the existence of two free quantum fluids and phase boundary characterization.

Findings

Compressibility and susceptibility obey additivity rules at low temperatures.

Identification of three magnetic regions: quantum fluids, non-Fermi liquid, and crossover.

Dimensionless Wilson ratio maps phase boundaries and characterizes free fluids.

Abstract

The one-dimensional (1D) Hubbard model, describing electrons on a lattice with an on-site repulsive interaction, provides a paradigm for the physics of quantum many-body phenomena. Here by solving the thermodynamic Bethe ansatz equations we study the universal thermodynamics, quantum criticality and magnetism of the 1D attractive Hubbard model. We show that the compressibility and the susceptibility of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO)-like state obey simple additivity rules at low temperatures, indicating an existence of two free quantum fluids. The magnetic properties, such as magnetization and susceptibility, reveal three physical regions: quantum fluids at low temperatures, a non-Fermi liquid at high temperatures and the quantum fluid to non-Fermi liquid crossover in between. The lattice interaction is seen to significantly influence the nature of the FFLO-like state in 1D. Furthermore, we show that the dimensionless Wilson ratio provides an ideal parameter to map out the various phase boundaries and to characterize the two free fluids of the FLLO-like state. The quantum scaling functions for the thermal and magnetic properties yield the same dynamic critical exponent $z=2$ and correlation critical exponent $\nu=1/2$ in the quantum critical region whenever a phase transition occurs. Our results provide a rigorous understanding of quantum criticality and free fluids of many-body systems on a 1D lattice.