Fermionic Symmetry-Protected Topological Phase in a Two-Dimensional Hubbard Model

Abstract

We study the two-dimensional (2D) Hubbard model using exact diagonalization for spin-1/2 fermions on the triangular and honeycomb lattices decorated with a single hexagon per site. In certain parameter ranges, the Hubbard model maps to a quantum compass model on those lattices. On the triangular lattice, the compass model exhibits collinear stripe antiferromagnetism, implying $d$-density wave charge order in the original Hubbard model. On the honeycomb lattice, the compass model has a unique, quantum disordered ground state that transforms nontrivially under lattice reflection. The ground state of the Hubbard model on the decorated honeycomb lattice is thus a 2D fermionic symmetry-protected topological phase. This state -- protected by time-reversal and reflection symmetries -- cannot be connected adiabatically to a free-fermion topological phase.

Original: 5+3 pages, 4+2 figures, including the supplemental material. Revised: updated title, content, and references in version 2

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• Interacting topological quantum chemistry of Mott atomic limits
• Easy-plane anisotropic-exchange magnets on a honeycomb lattice: quantum effects and dealing with them
• Classical many-particle systems with unique disordered ground states
• Transport anisotropy and metal-insulator transition in striped Dirac fermion systems