Abstract

For graphene nanoribbons with Rashba spin-orbit coupling, the peculiar magnetic response due to the presence of a magnetization and geometric confinement are analyzed within a tight-binding model. We observe a sizable transverse susceptibility that can be considered as a gate voltage-induced magnetoelectric torque without the need of a bias voltage, with different directions for zigzag and armchair ribbons. The local torque generates non-collinear spin polarization between the two edges and/or along the ribbon, and the net torque averages to zero if the magnetization is homogeneous. Nevertheless, a nonzero net torque can appear in partially magnetized nanoribbons or in nanoflakes of irregular shapes. The equilibrium spin current produced by the spin-orbit coupling also appears in nanoribbons, but the component flowing in the direction of confinement is strongly suppressed. Even without the magnetization, an out-of-plane polarized chiral edge spin current is produced, resembling that in the quantum spin Hall effect. Moreover, a magnetization pointing perpendicular to the edge produces a laminar flow of edge charge currents, whose flow direction is symmetric (non chiral) or antisymmetric (chiral) between the two edges depends on whether the magnetization points in-plane or out-of-plane.

Highlights

  • The celebrated Rashba spin-orbit coupling (RSOC) has a strong impact on the physical properties of two-dimensional (2D) metals with parabolic bands [1,2], especially their magnetic response and charge to spin interconversion

  • The patterns are translationally invariant along the ribbon direction y, and are either symmetric or antisymmetric under Pzmigir, such that we only show the left half of a unit cell, with size of the arrows and disks indicating the magnitude of the currents and spin polarization, respectively

  • We demonstrate that graphene nanoribbons due to RSOC and geometric confinement display a peculiar magnetic response, including a bias-voltage-free spin torque, chiral and nonchiral edge currents, and equilibrium spin currents

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Summary

INTRODUCTION

The celebrated Rashba spin-orbit coupling (RSOC) has a strong impact on the physical properties of two-dimensional (2D) metals with parabolic bands [1,2], especially their magnetic response and charge to spin interconversion. In magnetized 2D systems, this effect can be exploited to induce magnetization dynamics known as the spin-orbit torque [4,5,6,7,8,9], whose feasibility has been demonstrated extensively in experiments [10,11,12] In addition to these properties, RSOC modifies the equilibrium properties of 2D metals, most notably causing an in-plane polarized spin current flowing throughout the system [13,14,15]. In-plane spin polarization perpendicular to the edge can induce a persistent charge current decaying and oscillating in sign away from the edge [18] This behavior is very similar to that found in other spin-momentum locking systems in proximity to a magnet, such as for topological.

EXTENDED TIGHT-BINDING MODEL OF GRAPHENE
Two-site toy model
Persistent currents and spin torques in zigzag ribbons
Persistent currents and spin torques in armchair ribbons
Partially magnetized nanoribbons and irregular nanoflakes
CONCLUSIONS
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