Exact solution of a two-species quantum dimer model for pseudogap metals
arXiv:1712.01854 · doi:10.1103/PhysRevLett.120.187001
Abstract
We present an exact ground state solution of a quantum dimer model introduced in Ref.[1], which features ordinary bosonic spin-singlet dimers as well as fermionic dimers that can be viewed as bound states of spinons and holons in a hole-doped resonating valence bond liquid. Interestingly, this model captures several essential properties of the metallic pseudogap phase in high- cuprate superconductors. We identify a line in parameter space where the exact ground state wave functions can be constructed at an arbitrary density of fermionic dimers. At this exactly solvable line the ground state has a huge degeneracy, which can be interpreted as a flat band of fermionic excitations. Perturbing around the exactly solvable line, this degeneracy is lifted and the ground state is a fractionalized Fermi liquid with a small pocket Fermi surface in the low doping limit.
Revised version, 8 pages
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Cited by in corpus (12)
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- Small to large Fermi surface transition in a single band model, using randomly coupled ancillas
- Fermi arcs and pseudogap in a lattice model of a doped orthogonal metal
- A slave boson description of pseudogap metals in t-J models
- Bond particle theory for the pseudogap phase of underdoped cuprates
- Fractional Fermi liquid in a generalized model
- Fractionalized Fermi liquids and the cuprate phase diagram
- Signatures of correlated magnetic phases in the local two-particle density matrix
- Solvable lattice models for metals with Z2 topological order
- Quantum oscillations and criticality in a fermionic and bosonic dimer model for the cuprates