Spin-orbit coupled repulsive Fermi atoms in a one-dimensional optical lattice

Abstract

Motivated by recent experimental development, we investigate spin–orbit coupled repulsive Fermi atoms in a one-dimensional optical lattice. Using the density-matrix renormalization group method, we calculate the momentum distribution function, gap, and spin-correlation function to reveal rich ground-state properties. We find that spin–orbit coupling (SOC) can generate unconventional momentum distribution, which depends crucially on the filling. We call the corresponding phase with zero gap the SOC-induced metallic phase. We also show that SOC can drive the system from the antiferromagnetic to ferromagnetic Mott insulators with spin rotating. As a result, a second-order quantum phase transition between the spin-rotating ferromagnetic Mott insulator and the SOC-induced metallic phase is predicted at the strong SOC. Here spin rotating means the spin orientations of the nearest-neighbor sites are not parallel or antiparallel, i.e., they have an intersection angle $\theta \in (0,\pi ).$ Finally, we show that the momentum k _peak , at which the peak of the spin-structure factor appears, can also be affected dramatically by SOC. The analytical expression of this momentum with respect to the SOC strength is also derived, which suggests that the predicted spin-rotating ferromagnetic ( k _peak < π /2 ) and antiferromagnetic ( π /2 < k _peak < π ) correlations can be detected experimentally by measuring the SOC-dependent spin-structure factor via time-of-flight imaging.

Keywords

• repulsive Fermi atoms
• spin-orbit coupling
• optical lattice
• 03.75.Ss
• 67.85.Lm