Abstract

Current-induced magnetic domain wall (DW) motion is an important operating principle of spintronic devices. Injected current generates spin torques (STs) on the DWs in two ways. One is the spin transfer from magnetic domains to the walls by the current flowing in the magnet. Current flow in attached heavy metals also generates another ST because of the spin-Hall effect. Both phenomena explain the wall motions well; therefore, their respective contribution is an important issue. Here, we show the simultaneous measurement of both torques by using magnetic facet domains that form mountain-shaped domains with straight walls. When the STs and the external magnetic field push the walls in opposite directions, the walls should have equilibrium angles to create balanced states. Such angles can be modulated by an additional in-plane magnetic field. Angle measurements distinguish the STs because each torque has a distinct mechanism related to the DW structure.

Highlights

  • Current-induced magnetic domain wall (DW) motion is an important operating principle of spintronic devices

  • The electric current flowing in the magnet has a polarized spin direction caused by the magnetization

  • We turned on I flowing in the +y direction and applied Hz to fully saturate the magnetization in the –z direction

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Summary

Introduction

Current-induced magnetic domain wall (DW) motion is an important operating principle of spintronic devices. One of the most representative methods is the alternate current (AC) harmonic technique[35,36,37], which detects the magnetization tilting of a magnetic domain induced by the SOT effect generated by an in-plane current flowing in heavy metal layers. Another measurement method, STferromagnetic resonance (FMR)[38,39], detects the SOT. Most of these experiments are performed on patterned wire structures to simplify the DW position

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