Magnetic properties and temperature variation of spectra in the Hubbard model

TL;DR

This study uses the strong coupling diagram technique to analyze magnetic and spectral properties of the 2D Hubbard model across various temperatures, interactions, and electron concentrations, aligning well with Monte Carlo results.

Contribution

It introduces a comprehensive approach that accounts for electron interactions with spin and charge fluctuations, fulfilling the Mermin-Wagner theorem and detailing temperature-dependent spectral behaviors.

Findings

Magnetic susceptibility and double occupancy agree with Monte Carlo data.

Three distinct temperature regimes of the electron spectrum are identified.

Spectral evolution includes band merging and formation of spin-polaron bands.

Abstract

Using the strong coupling diagram technique, magnetic and spectral properties of the two-dimensional repulsive Hubbard model are investigated in the ranges of repulsions $t\leq U\leq 10t$, temperatures $0.1t\lesssim T\lesssim 4t$ and electron concentrations $0.6\lesssim\bar{n}\leq 1$ with $t$ the hopping constant. The approach takes into account interactions of electrons with spin and charge fluctuations of all ranges and fulfils the Mermin-Wagner theorem. Temperature and concentration dependencies of the uniform magnetic susceptibility, the variation of the double occupancy with the repulsion and the temperature dependence of the square of the site spin are in satisfactory agreement with Monte Carlo results. Three types of the temperature variation of the electron energy spectrum can be distinguished at half-filling. For $U\lesssim 3t$, at low temperatures, there are two nonintersecting bands, which approach each other on the boundary of the magnetic Brillouin zone. With increasing $T$ these bands merge into one band crossing the Fermi level. For $4t\lesssim U \lesssim 6t$, the low-temperature picture described above is supplemented with a low-intensity spin-polaron band located near the Fermi level. As its counterpart in the strong-correlation case, the band is formed by bound states of electrons and spin excitations. However, in contrast to the former case, the band exists even at half-filling and occupies the entire Brillouin zone. As for lower $U$, with increasing temperature, all bands coalesce into a single band. For $U\gtrsim 7t$ and low temperatures the spectrum has a pronounced four-band structure, which with increasing $T$ transforms into two Hubbard subbands.