Antiferromagnetic pseudogap in the two-dimensional Hubbard model deep in the renormalized classical regime
Y.M. Vilk, Camille Lahaie, A.-M.S. Tremblay

TL;DR
This paper investigates the emergence of a pseudogap in the two-dimensional Hubbard model within the renormalized classical regime, revealing how spin fluctuations influence spectral properties and gap formation at finite temperatures.
Contribution
It introduces a generalized two-particle self-consistent approach with a special algorithm to accurately describe the pseudogap regime in the 2D Hubbard model, including quantum corrections.
Findings
Pseudogap appears at higher temperatures than previously thought.
Results agree with quantum Monte Carlo benchmarks at high temperature.
Quantum corrections modify the zero-temperature antiferromagnetic gap.
Abstract
Long-wavelength spin fluctuations prohibit antiferromagnetic long-range order at finite temperature in two dimensions. Nevertheless, the correlation length starts to grow rapidly at a crossover temperature, leading to critical slowing down and to a renormalized-classical regime over a wide range of temperature, between a fraction of the mean-field transition temperature and the zero-temperature ordered state. This leads to a single-particle pseudogap of the kind observed in electron-doped cuprates. Very few theoretical methods can claim an accurate description of this regime. The challenge is that in this regime Fermi-liquid quasiparticles are already destroyed and new quasiparticles of the ordered state are not fully formed yet. Here, we study this problem for the two-dimensional Hubbard model by first generalizing the two-particle self-consistent approach. Using a special algorithm,…
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