Abstract

Strongly-interacting nanomagnetic arrays are crucial across an ever-growing suite of technologies. Spanning neuromorphic computing, control over superconducting vortices and reconfigurable magnonics, the utility and appeal of these arrays lies in their vast range of distinct, stable magnetization states. Different states exhibit different functional behaviours, making precise, reconfigurable state control an essential cornerstone of such systems. However, few existing methodologies may reverse an arbitrary array element, and even fewer may do so under electrical control, vital for device integration. We demonstrate selective, reconfigurable magnetic reversal of ferromagnetic nanoislands via current-driven motion of a transverse domain wall in an adjacent nanowire. The reversal technique operates under all-electrical control with no reliance on external magnetic fields, rendering it highly suitable for device integration across a host of magnonic, spintronic and neuromorphic logic architectures. Here, the reversal technique is leveraged to realize two fully solid-state reconfigurable magnonic crystals, offering magnonic gating, filtering, transistor-like switching and peak-shifting without reliance on global magnetic fields.

Highlights

  • Strongly-interacting nanomagnetic arrays are crucial across an ever-growing suite of technologies

  • Alongside mature technologies such as data storage, nanomagnetic arrays support a host of more recent applications including neuromorphic computation[1,2,3,4,5], superconducting vortex control[6,7,8,9] and reconfigurable magnonic crystals[10,11,12,13,14] (RMCs)

  • The versatility and utility of the technique are demonstrated via two active magnonic system designs: a reconfigurably gateable one-dimensional (1D) transmissionline reconfigurable magnonic crystals10–14 (RMCs) optimized for travelling-wave magnons supporting multiple gate types and on/off ratios up to 35 and a twodimensional (2D) RMC optimized for standing-wave magnons with single-frequency on/off ratios of up to 9 × 103 and mode shifting of Δf = 0.96 GHz

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Summary

Introduction

Strongly-interacting nanomagnetic arrays are crucial across an ever-growing suite of technologies. The tightly localized stray field of a current-driven 180° transverse domain wall (DW) in a nanowire is used to induce dynamic topological defects in adjacent ferromagnetic (FM) nanoislands, driving magnetic reversal.

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