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The landscape of the Hubbard model

Subir Sachdev

TL;DR

The article provides a comprehensive, gauge-theoretic survey of the Hubbard model across lattices and densities, focusing on Dirac-like low-energy physics on the honeycomb lattice and the emergence of symmetry-broken and topologically ordered phases. It develops and interconnects multiple theoretical frameworks—Gross-Neveu–Yukawa criticality, U(1) and SU(2) gauge theories, and rotor/ spinon decompositions—to describe semi-metals, Néel and VBS insulators, spin liquids, and fractionalized Fermi liquids, and extends these insights to nonzero temperature with AdS/CFT-inspired transport predictions. A central thrust is the unification of conventional and exotic phases via emergent gauge fields and deconfined criticality, including a deconfined QCD-like fixed point and a lattice-symmetry–driven VBS order. The work further links condensed-mmatter gauge theories to holographic metal constructions, illustrating how holography can capture universal quantum-critical transport and the short relaxation times characteristic of these strongly interacting 2+1D systems.

Abstract

I present a pedagogical survey of a variety of quantum phases of the Hubbard model. The honeycomb lattice model has a conformal field theory connecting the semi-metal to the insulator with Neel order. States with fractionalized excitations are linked to the deconfined phases of gauge theories. I also consider the confining phases of such gauge theories, and show how Berry phases of monopoles induce valence bond solid order. The triangular lattice model can display a metal-insulator transition from a Fermi liquid to a deconfined spin liquid, and I describe the theory of this transition. The bilayer triangular lattice is used to illustrate another compressible metallic phase, the `fractionalized Fermi liquid'. I make numerous connections of these phases and critical points to the AdS/CFT correspondence. In particular, I argue that two recent holographic constructions connect respectively to the Fermi liquid and fractionalized Fermi liquid phases.

The landscape of the Hubbard model

TL;DR

The article provides a comprehensive, gauge-theoretic survey of the Hubbard model across lattices and densities, focusing on Dirac-like low-energy physics on the honeycomb lattice and the emergence of symmetry-broken and topologically ordered phases. It develops and interconnects multiple theoretical frameworks—Gross-Neveu–Yukawa criticality, U(1) and SU(2) gauge theories, and rotor/ spinon decompositions—to describe semi-metals, Néel and VBS insulators, spin liquids, and fractionalized Fermi liquids, and extends these insights to nonzero temperature with AdS/CFT-inspired transport predictions. A central thrust is the unification of conventional and exotic phases via emergent gauge fields and deconfined criticality, including a deconfined QCD-like fixed point and a lattice-symmetry–driven VBS order. The work further links condensed-mmatter gauge theories to holographic metal constructions, illustrating how holography can capture universal quantum-critical transport and the short relaxation times characteristic of these strongly interacting 2+1D systems.

Abstract

I present a pedagogical survey of a variety of quantum phases of the Hubbard model. The honeycomb lattice model has a conformal field theory connecting the semi-metal to the insulator with Neel order. States with fractionalized excitations are linked to the deconfined phases of gauge theories. I also consider the confining phases of such gauge theories, and show how Berry phases of monopoles induce valence bond solid order. The triangular lattice model can display a metal-insulator transition from a Fermi liquid to a deconfined spin liquid, and I describe the theory of this transition. The bilayer triangular lattice is used to illustrate another compressible metallic phase, the `fractionalized Fermi liquid'. I make numerous connections of these phases and critical points to the AdS/CFT correspondence. In particular, I argue that two recent holographic constructions connect respectively to the Fermi liquid and fractionalized Fermi liquid phases.

Paper Structure

This paper contains 17 sections, 122 equations, 16 figures.

Figures (16)

  • Figure 1: The honeycomb lattice with its A (green) and B (red) sublattices
  • Figure 2: The first Brillouin zone of the honeycomb lattice.
  • Figure 3: The lower band of the dispersion in Eq. (\ref{['spec']}) for $\mu=0$
  • Figure 4: The large $U$ state with antiferromagnetic (Néel) order.
  • Figure 5: The honeycomb lattice with a vacancy.
  • ...and 11 more figures