An exactly solvable BCS-Hubbard Model in arbitrary dimensions
arXiv:1709.08411 · doi:10.1103/PhysRevLett.120.046401
Abstract
We introduce in this paper an exact solvable BCS-Hubbard model in arbitrary dimensions. The model describes a p-wave BCS superconductor with equal spin pairing moving on a bipartite (cubic, square etc.) lattice with on site Hubbard interaction . We show that the model becomes exactly solvable for arbitrary when the BCS pairing amplitude equals the hopping amplitude . The nature of the solution is described in detail in this paper. The construction of the exact solution is parallel to the exactly solvable Kitaev honeycomb model for quantum spins and can be viewed as a generalization of Kitaev's construction to interacting lattice fermions. The BCS-Hubbard model discussed in this paper is just an example of a large class of exactly solvable lattice fermion models that can be constructed similarly.
5 pages, 3 figures
References in corpus (7)
- Exact results for spin dynamics and fractionization in the Kitaev Model
- An exact chiral spin liquid with non-Abelian anyons
- Topological characterization of quantum phase transitions in a S=1/2 spin model
- Exact results on the Kitaev model on a hexagonal lattice: spin states, string and brane correlators, and anyonic excitations
- Weyl spin liquids
- A -matrix generalization of the Kitaev model
- Entanglement of a 3D generalization of the Kitaev model on the diamond lattice