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Robust edge states in magnetic soliton racetrack

Z.-X. Li, Zhenyu Wang, Yunshan Cao, H. W. Zhang, and Peng Yan
Phys. Rev. B 103, 054438 – Published 25 February 2021

Abstract

Precise positioning of magnetic solitons requires controllable artificial pinning, while the accurate determination of the pinning profile remains a challenge. Here, we propose a topological solution to this problem. Taking the domain wall (DW) as a representative example, we study the collective dynamics of interacting DWs in a magnetic racetrack with pinning sites of alternate distances. By mapping the governing equations of DW motion to the Su-Schrieffer-Heeger model and evaluating the quantized Zak phase, we predict two topologically distinct phases in the racetrack. A robust edge state emerges at either one or both ends depending on the parity of the DW number and the ratio of alternating intersite lengths. We show that the in-gap DW oscillation frequency has a fixed value which depends only on the geometrical shape of the pinning notch, and is insensitive to device imperfections and inhomogeneities. The spring coefficient of the pinning potential can be quantified as the square of the robust DW frequency multiplied by its constant mass. Our findings pave the way to determining the pinning potential with high accuracy for generic magnetic solitons and suggest as well that the magnetic soliton-based racetrack is a unique playground to study topological phase transitions.

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  • Received 4 October 2020
  • Revised 25 January 2021
  • Accepted 17 February 2021

DOI:https://doi.org/10.1103/PhysRevB.103.054438

©2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Z.-X. Li, Zhenyu Wang, Yunshan Cao, H. W. Zhang, and Peng Yan*

  • School of Electronic Science and Engineering and State Key Laboratory of Electronic Thin Films and Integrated Devices, University of Electronic Science and Technology of China, Chengdu 610054, China

  • *Corresponding author: yan@uestc.edu.cn

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Vol. 103, Iss. 5 — 1 February 2021

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Images

  • Figure 1
    Figure 1

    (a) Illustration of the vortex, skyrmion, and DW racetrack with periodic pinnings. The micromagnetic structure of Néel-type DWs pinned by cuboid notches with lx=20 nm, ly=9 nm, and lz=5 nm is plotted, with the unit cell containing two DWs at sites A and B. d1 and d2 are the intracellular and intercellular distances between notches, respectively. (b) The components of normalized magnetization along the center of DW racetrack with d1=160 nm and d2=140 nm.

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  • Figure 2
    Figure 2

    (a) Dependence of the coupling strength I on d. Black circles denote simulation results and red solid line represents the analytical formula. (b) The two eigenfrequencies of a DW-DW pair varying with d.

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  • Figure 3
    Figure 3

    (a) Band structure of an infinite DW racetrack for different intracellular lengths: d1=120, 140, and 160 nm, with d2 being fixed to 140 nm. (b) Dependence of the Zak phase on the ratio d1/d2.

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  • Figure 4
    Figure 4

    (a) Spectrum of a finite DW racetrack for different d1/d2. The dotted blue line denotes the boundary separating two topologically distinct phases; the red segment represents the in-gap mode. (b) Eigenfrequencies of the DW lattice with d1/d2=8/7. The spatial distribution of DW-oscillation amplitude for the edge (c) and bulk (d) states. Inset: Comparison between analytical and numerical results. (e) Spectrum of disordered DW racetracks. (f) Spectrum with (red dots) and without (black dots) defects.

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  • Figure 5
    Figure 5

    (a) Schematic plot of a finite racetrack containing 39 DWs, with d1=160 nm and d2=140 nm. (b) The temporal Fourier spectra of the DW oscillations at edge (1st DW) and bulk (20th DW) positions. The spatial distribution of amplitude of DW oscillations for edge (c) and bulk (d) states.

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  • Figure 6
    Figure 6

    Schematic plot of a single DW (a) and a DW-DW pair (b). The Fourier spectra of the DW oscillation for a single DW (c) and a DW-DW pair (d). (e) The DW position as a function of time for different modes.

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  • Figure 7
    Figure 7

    (a) Spectrum of a finite racetrack containing 40 DWs for different d1/d2. The red segment represents the in-gap mode. (b) Eigenfrequencies of the DW lattice with d1/d2=8/7. The spatial distribution of DW-oscillation amplitude for the edge (c) and bulk (d) states. (e) Spectrum of disordered DW racetracks. (f) Spectrum with (red dots) and without (black dots) defects.

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  • Figure 8
    Figure 8

    (a) Schematic plot of a finite racetrack containing 40 DWs, with d1=160 nm and d2=140 nm. (b) The temporal Fourier spectra of the DW oscillation at edge (1st DW) and bulk (20th DW) positions. The spatial distribution of the DW oscillation amplitude for edge (c) and bulk (d) states.

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  • Figure 9
    Figure 9

    Proposed scheme to determine the STT non-adiabaticity β by experimentally measuring the slope of XbJ curve.

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