Nagaoka states in the SU() Hubbard model
arXiv:1210.4774 · doi:10.1103/PhysRevA.87.013617
Abstract
We present an extension of Nagaoka's theorem in the SU() generalization of the infinite- Hubbard model. It is shown that, when there is exactly one hole, the fully polarized states analogous to the ferromagnetic states in the SU(2) Hubbard model are ground states. For a restricted class of models satisfying the connectivity condition, these fully polarized states are the unique ground states up to the trivial degeneracy due to the SU() symmetry. We also give examples of lattices in which the connectivity condition can be verified explicitly. The examples include the triangular, kagome, and hypercubic lattices in dimensions, among which the cases of and 3 are experimentally realizable in ultracold atomic gases loaded into optical lattices.
9 pages, 7 figures
References in corpus (6)
- An SU(N) Mott insulator of an atomic Fermi gas realized by large-spin Pomeranchuk cooling
- Ultracold fermions and the SU(N) Hubbard model
- Ultracold Gases of Ytterbium: Ferromagnetism and Mott States in an SU(6) Fermi System
- Mott Insulators of Ultracold Fermionic Alkaline Earth Atoms: Underconstrained Magnetism and Chiral Spin Liquid
- BCS pairing in Fermi systems with several flavors
- Ground state phase diagram of the repulsive SU(3) Hubbard model in Gutzwiller approximation