Abstract

The current-induced spin–orbit torque in single-layer ferromagnetic CoFeB thin films is quantitatively investigated by using in-plane harmonic Hall measurements. After the subtraction of thermal contributions such as the anomalous and ordinary Nernst effects, the obtained overall spin–orbit torque is successfully decomposed into damping-like (DL) and field-like (FL) terms. The DL and FL torques exhibit opposite trends of ferromagnetic layer thickness dependence before saturation, giving rise to distinctively different spin torque efficiencies: the DL torque efficiency shows a strong thickness dependence, while the FL torque efficiency is almost independent of the thickness. Such a result shows strong evidence that the DL torque originates from a spin-Hall-like charge-spin conversion in the ferromagnet, while the FL torque stems from interfacial effects such as the Rashba–Edelstein effect. With both DL and FL torques quantified in the single-layer CoFeB, our results exhibit an important step toward the understanding of nontrivial spin–orbit torques in single-layer ferromagnetic thin films.

Highlights

  • While the FM-layer-induced spin–orbit torque (SOT) was confirmed in FM trilayers, its mechanism appears to be complicated because of the existence of two FM layers and multiple interfaces

  • SOT studies focused on the experimental determination of torques in FM single layers

  • The decomposed DL and FL torques are on the same order of magnitude but show opposite trends of thickness dependence before saturation

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Summary

Introduction

While the FM-layer-induced SOT was confirmed in FM trilayers, its mechanism appears to be complicated because of the existence of two FM layers and multiple interfaces. We quantitatively determine and disentangle the current-induced SOT in CoFeB single-layer thin films via in-plane harmonic Hall measurements.

Results
Conclusion
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