Stability of superfluid phases in the 2D Spin-Polarized Attractive Hubbard Model
arXiv:1309.6668 · doi:10.1209/0295-5075/95/37003
Abstract
We study the evolution from the weak coupling (BCS-like limit) to the strong coupling limit of tightly bound local pairs (LP's) with increasing attraction, in the presence of the Zeeman magnetic field () for , within the spin-polarized attractive Hubbard model. The broken symmetry Hartree approximation {as well as the} strong coupling expansion are used. We also apply the Kosterlitz-Thouless (KT) scenario to determine the phase coherence temperatures. For spin independent hopping integrals (), we find no stable homogeneous polarized superfluid (SC) state in the ground state for the strong attraction and obtain that for a two-component Fermi system on a 2D lattice with population imbalance, phase separation (PS) is favoured for a fixed particle concentration, even on the LP (BEC) side. We also examine the influence of spin dependent hopping integrals (mass imbalance) on the stability of the SC phase. We find a topological quantum phase transition (Lifshitz type) from the unpolarized superfluid phase (SC) to SC and tricritical points in the () and () ground state phase diagrams. We also construct the finite temperature phase diagrams for both and and analyze the possibility of occurrence of a spin polarized KT superfluid.
7 pages, 4 figures
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- Reentrant Fulde-Ferrell-Larkin-Ovchinnikov superfluidity in the honeycomb lattice
- Effective potential and quantum criticality for imbalanced Fermi mixtures
- Feasibility of a Fulde-Ferrell-Larkin-Ovchinnikov superfluid Fermi atomic gas
- Spin-polarized superconducting phase in semiconducting system with next-nearest-neighbor hopping on the honeycomb lattice
- Connection between the semiconductor--superconductor transition and the spin-polarized superconducting phase in the honeycomb lattice