Abstract

Motivated by emergent $SU(2)$ symmetry in the spin orbit coupled system, we study the spin helix driven insulating phase in two dimensional lattice. When both Rashba and Dresselhaus spin orbit couplings are present, the perfect Fermi surface nesting occurs at a special condition depending on the lattice geometry. In this case, the energies of spin up at any wave vector $\vec{k}$ are equivalent to the ones of spin down at $\vec{k}\!+\!\vec{Q}$ with so-called the \textit{shifting wave vector} $\vec{Q}$. Thus, the system stabilizes magnetic insulator with spiral like magnetic ordering even in the presence of tiny electron-electron interaction where the magnetic ordering wave vector is proportional to $\vec{Q}$. We first show the condition for existence of the \textit{shifting wave vector} in general lattice model and emergent $SU(2)$ symmetry in the spin orbit coupled system. Then, we exemplify this in square lattice at half filling and discuss the insulating phase with (non-) coplanar spin density wave and charge order. Our study emphasizes possible new types of two dimensional magnetic materials and can be applicable to various van-der Waals materials and their heterostructures with the control of electric field, strain and pressure.

Highlights

  • Spin SU(2) symmetry invariance with respect to electron spin rotation is an important quantity giving conservation of spin polarization in the system

  • We extend the analysis of twodimensional free gas [6] and determine the ratio δ between Rashba and Dresselhaus spin-orbit couplings (SOCs) strengths specific to the lattice geometry to generate a spin helix

  • As we have discussed above, Fermi-surface nesting induced by the combination of SOCs is still present in the vicinity of such fine tuning, even away from the exact ratio between SOCs

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Summary

Introduction

Spin SU(2) symmetry invariance with respect to electron spin rotation is an important quantity giving conservation of spin polarization in the system. When spin and orbital degrees of freedom are coupled, such SU(2) symmetry is generally broken, and spin polarization is no longer a good quantum number. For a two-dimensional system including surfaces, two different types of spin-orbit couplings (SOCs) are mainly addressed due to broken inversion symmetries, Rashba and Dresselhaus spin-orbit couplings. The Rashba effect originates from the effective electric field at the surface or interface of crystal structures (SIA), whereas the Dresselhaus effect comes from the bulk inversion asymmetry (BIA). Their measurement and controllability have been widely studied in quantum wells for several decades [1]. The possible creation of such interactions has been explored even in optical lattices [2,3]

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