Abstract

We consider analytically current-driven dynamics of magnetic Néel walls in heavy metal/ferromagnetic metal/oxide trilayers where strong spin–orbit coupling and interfacial Dzyaloshinskii–Moriya interaction (i-DMI) coexist. We show that field-like spin–orbit torque (FL-SOT) with effective field along (n being the interface normal and being the charge current direction) and i-DMI induced torque can both lead to Walker breakdown suppression meanwhile leaving the wall mobility (velocity versus current density) unchanged. However, i-DMI itself can not induce the ‘universal absence of Walker breakdown’ (UAWB) while FL-SOT exceeding a certain threshold can. Finitely-enlarged Walker limits before UAWB are theoretically calculated and well explain existing data. In addition, change in wall mobility and even its sign-inversion can be understood only if the anti-damping-like SOT is appended. For Néel walls in ferromagnetic-metal layer with both perpendicular and in-plane anisotropies, we have calculated the respective modifications of wall mobility under the coexistence of spin-transfer torque, SOTs and i-DMI. Analytics shows that in trilayers with perpendicular anisotropy strong enough spin Hall angle and appropriate sign of i-DMI parameter can lead to sign-inversion in wall mobility even under small enough current density, while in those with in-plane anisotropy this only occurs for current density in a specific range.

Highlights

  • Pure current-induced domain wall propagation in magnetic nanostructures has attracted intensive attention for decades starting from academic interests in understanding the interplay between itinerant spinful electrons and localized magnetic moments[1, 2, 3, 4]

  • In this work we focus on domain wall dynamics rather than physical sources of spin-orbit torques (SOTs), TSOT can be written as TSOT = −γHFLm × n × J − γHADLm × m × n × J

  • We analytically investigate the current-induced domain wall dynamics in HM/FMM/Oxide trilayers with strong spin-orbit coupling (SOC) and interfacial Dzyaloshinskii-Moriya interaction (i-DMI)

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Summary

Introduction

Pure current-induced domain wall propagation in magnetic nanostructures has attracted intensive attention for decades starting from academic interests in understanding the interplay between itinerant spinful electrons and localized magnetic moments[1, 2, 3, 4]. Analytics with Lagrangian functional[68, 69, 70] and simulations[71, 72, 73, 74, 75, 76, 77] based on Landau-Lifshitz-Gilbert (LLG) dynamical equation[78] have been performed to explain Neel wall dynamics in HM/FMM/Oxide trilayers in the framework of one-dimensional collective coordinate model (1D-CCM) All these works focus on two novel features in experiments: (i) Walker breakdown suppression high wall velocity and (ii) wall motion opposed to electron flow and the corresponding “polarity sensitivity”.

Modeling and preparations
Dynamical equation
Static wall configuration
General scalar LLG equations
Brief review of wall dynamics under pure STT
Coexistence of STT and FL-SOT
Coexistence of STT and i-DMI
Mobility change by ADL-SOT
Mobility change in PMA systems
Mobility change in IPMA systems
Discussions
Summary
Full Text
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