Stripes, Pseudogaps, and Van Hove Nesting in the Three-band tJ Model

TL;DR

This paper uses slave boson calculations in the three-band tJ model, including phonon coupling, to explain pseudogap phenomena and Fermi surface evolution in underdoped cuprates, highlighting phase separation and Van Hove nesting effects.

Contribution

It introduces a detailed theoretical framework incorporating phonons and strong correlations to explain pseudogap features and Fermi surface changes in high-T_c cuprates.

Findings

Van Hove nesting induces phase separation limited by Coulomb forces.

Dispersions differ significantly between uniform, phase-separated, and striped regimes.

Doping dependence explains photoemission and thermodynamic pseudogap experiments.

Abstract

Slave boson calculations have been carried out in the three-band tJ model for the high-T_c cuprates, with the inclusion of coupling to oxygen breathing mode phonons. Phonon-induced Van Hove nesting leads to a phase separation between a hole-doped domain and a (magnetic) domain near half filling, with long-range Coulomb forces limiting the separation to a nanoscopic scale. Strong correlation effects pin the Fermi level close to, but not precisely at the Van Hove singularity (VHS), which can enhance the tendency to phase separation. The resulting dispersions have been calculated, both in the uniform phases and in the phase separated regime. In the latter case, distinctly different dispersions are found for large, random domains and for regular (static) striped arrays, and a hypothetical form is presented for dynamic striped arrays. The doping dependence of the latter is found to provide an excellent description of photoemission and thermodynamic experiments on pseudogap formation in underdoped cuprates. In particular, the multiplicity of observed gaps is explained as a combination of flux phase plus charge density wave (CDW) gaps along with a superconducting gap. The largest gap is associated with VHS nesting. The apparent smooth evolution of this gap with doping masks a crossover from CDW-like effects near optimal doping to magnetic effects (flux phase) near half filling. A crossover from large Fermi surface to hole pockets with increased underdoping is found. In the weakly overdoped regime, the CDW undergoes a quantum phase transition ($T_{CDW}\to 0$), which could be obscured by phase separation.