Phase separation in the particle-hole asymmetric Hubbard model
arXiv:cond-mat/0610803 · doi:10.1103/PhysRevB.75.125103
Abstract
The paramagnetic phase diagram of the Hubbard model with nearest-neighbor (NN) and next-nearest-neighbor (NNN) hopping on the Bethe lattice is computed at half-filling and in the weakly doped regime using the self-energy functional approach for dynamical mean-field theory. NNN hopping breaks the particle-hole symmetry and leads to a strong asymmetry of the electron-doped and hole-doped regimes. Phase separation occurs at and near half-filling, and the critical temperature of the Mott transition is strongly suppressed.
8 pages, 8 figures
References in corpus (7)
- Variational cluster approach to correlated electron systems in low dimensions
- Self-energy-functional approach: Analytical results and the Mott-Hubbard transition
- Mott transition in Kagomé lattice Hubbard model
- Phase separation in the Hubbard model
- Hopping on the Bethe lattice: Exact results for densities of states and dynamical mean-field theory
- Dynamical mean field study of the Mott transition in the half-filled Hubbard model on a triangular lattice
- Green functions for nearest- and next-nearest-neighbor hopping on the Bethe lattice
Cited by in corpus (5)
- Phase separation and competition of superconductivity and magnetism in the two-dimensional Hubbard model: From strong to weak coupling
- Half-filled Hubbard Model on a Bethe lattice with next-nearest neighbor hopping
- Doping-driven Mott transition in La_{1-x}Sr_xTiO_3 via simultaneous electron and hole doping of t2g subbands
- Non-perturbative conserving approximations and Luttinger's sum rule
- Anderson localization on Falicov-Kimball model with next-nearest-neighbor hopping and long-range correlated disorder