Hidden Bose-Einstein Singularities in Correlated Electron Systems: II. Pseudogap Phase in the Weakly Attractive Hubbard Model
Takafumi Kita

TL;DR
This paper investigates hidden Bose-Einstein singularities in the pseudogap phase of the weakly attractive Hubbard model, revealing their role as a threshold for the pseudogap formation above superconductivity.
Contribution
It demonstrates that correlation effects significantly alter mean-field superconductivity predictions, identifying a hidden singularity signaling the pseudogap phase in the Hubbard model.
Findings
Hidden singularity appears near the mean-field critical temperature.
The singularity indicates the onset of the pseudogap phase.
Density of states exhibits a V-shape near zero energy.
Abstract
The hidden Bose-Einstein singularities of correlated electron systems, whose possible existence has been pointed out in a previous paper based on quantum field theory of ordered phases [T. Kita, J. Phys. Soc. Jpn. {\bf 93}, 124704 (2024)], are studied in more detail in terms of the attractive Hubbard model, for which the mean-field theory predicts that spin-singlet superconductivity is realized at low enough temperatures for any band structure and interaction strength. It is shown that incorporating correlation effects should change the mean-field superconducting solution substantially and qualitatively even in the weak coupling, implying that the system lies in the strong-coupling region perturbatively. The hidden singularity is found to be present around the mean-field superconducting temperature , below which the standard self-consistent treatment by quantum field…
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