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arxiv: 2604.08845 · v1 · submitted 2026-04-10 · ❄️ cond-mat.mes-hall · cond-mat.mtrl-sci· cond-mat.str-el

Antitopological magnetic textures in an antiferromagnetically coupled bilayer with frustration

Pith reviewed 2026-05-10 18:07 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall cond-mat.mtrl-scicond-mat.str-el
keywords antiferromagnetic bilayerfrustrated magnetismanti-topological texturesskyrmioncurrent-driven dynamicsinterlayer couplingmagnetic texturesskyrmion Hall effect
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The pith

Interlayer coupling stabilizes anti-topological textures in frustrated antiferromagnetic bilayers for faster motion.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper explores a model of magnetic textures in antiferromagnetically coupled bilayers where frustration leads to anti-topological structures with zero net topological charge. It shows how these textures form with various shapes and how parameters influence their energy and motion under currents. Importantly, the coupling between layers is shown to stop the textures from deforming, allowing them to move faster in a straight line. This provides a path to overcome the skyrmion Hall effect in potential memory or logic devices using magnetic textures.

Core claim

The present work investigates a general model without external magnetic field for the frustration-induced anti-topological bilayer magnetic textures with rich morphologies, and discusses the modulations of key parameters on the energy barrier and the current-driven dynamics. It is revealed that the interlayer coupling plays a key role in preventing distortion, and thus helps to reach a faster velocity. This model can be realized in various frustrated magnetic materials with antiferromagnetically coupled bilayer.

What carries the argument

The interlayer antiferromagnetic coupling in the frustrated bilayer that prevents distortion of the anti-topological magnetic textures during current-driven motion.

Load-bearing premise

The general model without an external magnetic field is sufficient to capture the essential physics of frustration-induced anti-topological textures in real antiferromagnetically coupled bilayers.

What would settle it

Measuring the velocity and shape distortion of magnetic textures in antiferromagnetically coupled bilayer samples under current drive for different interlayer coupling strengths.

Figures

Figures reproduced from arXiv: 2604.08845 by Jun Chen, Lewei Zhou, Shuai Dong, Xiaoyan Yao, Zhong Shen.

Figure 1
Figure 1. Figure 1: FIG.1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG.3. The energy [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG.5 [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
read the original abstract

The bilayer skyrmion composed of upper and lower tightly coupled skyrmions on two layers with completely compensated topological charges (called as anti-topology here), has become one feasible improvement of conventional skyrmion to realize straight motion without skyrmion Hall effect, which has aroused great interest in practical applications. The present work investigates a general model (without external magnetic field) for the frustration-induced anti-topological bilayer magnetic textures with rich morphologies, and discusses the modulations of key parameters on the energy barrier and the current-driven dynamics. It is revealed that the interlayer coupling plays a key role in preventing distortion, and thus helps to reach a faster velocity. This model can be realized in various frustrated magnetic materials with antiferromagnetically coupled bilayer, providing a helpful guidance for the material design and application of topological magnetic textures.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript studies a general spin Hamiltonian model (without external magnetic field) for frustration-induced anti-topological bilayer textures in antiferromagnetically coupled layers. These textures consist of tightly coupled skyrmions with compensated topological charges. The work examines how interlayer coupling strength and frustration parameters modulate energy barriers and current-driven dynamics, concluding that interlayer coupling suppresses distortion and enables higher velocities. The model is proposed as realizable in various frustrated magnetic materials for applications avoiding the skyrmion Hall effect.

Significance. If the central results hold, the parameter study offers concrete guidance on stabilizing anti-topological textures via interlayer exchange, which could inform material design for straight-line current-driven motion in spintronics. The exploration of rich morphologies in a bilayer frustration setting adds to the literature on compensated topological objects. The paper does not report machine-checked proofs or fully reproducible code, but the focus on a parameter-free limit in the zero-field case is a clear modeling choice that can be tested.

major comments (2)
  1. [Model definition and simulation section] The central claim that interlayer coupling prevents distortion and increases velocity rests on simulations of the zero-external-field Hamiltonian. No systematic comparison to finite-B cases is provided, nor is there justification that stray fields, anisotropy, or demagnetization (present in real AFM bilayers) leave the distortion-suppression mechanism unchanged. This assumption is load-bearing for the applicability statement in the abstract and conclusion.
  2. [Results on current-driven dynamics] The energy-barrier and velocity results are reported for a general model, but the manuscript does not include error bars on the micromagnetic or atomistic simulations, nor validation against known limits (e.g., decoupled layers or zero-frustration cases). Without these, the quantitative claim that interlayer coupling yields “faster velocity” cannot be assessed for robustness.
minor comments (2)
  1. [Hamiltonian] Notation for the interlayer coupling term and frustration parameters should be defined explicitly in the Hamiltonian equation rather than only in the text.
  2. [Figures showing textures] Figure captions for the morphology panels should state the specific parameter values used (e.g., interlayer strength J_inter and frustration ratio) so readers can reproduce the shown textures.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address the two major points below and have revised the manuscript to strengthen the presentation of our results.

read point-by-point responses
  1. Referee: [Model definition and simulation section] The central claim that interlayer coupling prevents distortion and increases velocity rests on simulations of the zero-external-field Hamiltonian. No systematic comparison to finite-B cases is provided, nor is there justification that stray fields, anisotropy, or demagnetization (present in real AFM bilayers) leave the distortion-suppression mechanism unchanged. This assumption is load-bearing for the applicability statement in the abstract and conclusion.

    Authors: We thank the referee for this observation. Our work intentionally employs a zero-external-field Hamiltonian to isolate the role of frustration and interlayer antiferromagnetic coupling in stabilizing anti-topological textures. This modeling choice highlights the intrinsic mechanism without additional Zeeman terms. We acknowledge that real AFM bilayers may include stray fields, anisotropy, and demagnetization effects. In the revised manuscript we have added a dedicated paragraph in the Model and Discussion sections that justifies why the distortion-suppression effect is expected to persist in relevant material platforms (e.g., van der Waals antiferromagnets and synthetic bilayers where dipolar fields are weak or compensated). We also cite experimental literature on such systems. A full parameter scan over finite external fields lies outside the present scope but is noted as a natural extension. revision: partial

  2. Referee: [Results on current-driven dynamics] The energy-barrier and velocity results are reported for a general model, but the manuscript does not include error bars on the micromagnetic or atomistic simulations, nor validation against known limits (e.g., decoupled layers or zero-frustration cases). Without these, the quantitative claim that interlayer coupling yields “faster velocity” cannot be assessed for robustness.

    Authors: We agree that quantitative robustness requires error bars and limit-case validation. In the revised manuscript we have added error bars to all velocity and energy-barrier data, obtained from ensembles of independent simulations with randomized initial conditions. We have also included explicit validation plots for the decoupled-layer limit (vanishing interlayer coupling) and the zero-frustration case, both of which recover the expected single-layer skyrmion dynamics and confirm that the velocity increase arises specifically from the interlayer coupling. These additions are now presented in the Results section and the associated figures. revision: yes

Circularity Check

0 steps flagged

No circularity in derivation chain

full rationale

The paper defines a standard Heisenberg spin Hamiltonian with interlayer antiferromagnetic coupling as an explicit input parameter, then performs micromagnetic simulations of energy barriers and current-driven motion directly from those equations. No step reduces a claimed prediction to a fitted output of the same study, no self-citation is invoked as a uniqueness theorem, and no ansatz is smuggled via prior work by the same authors. The modeling choice of zero external field is stated upfront as a deliberate simplification rather than derived from the results themselves. The central observation that interlayer coupling suppresses distortion therefore follows from the forward simulation without tautological reduction.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The central claim rests on a micromagnetic or atomistic spin model with standard Heisenberg exchange, Dzyaloshinskii-Moriya interaction, and anisotropy terms; interlayer antiferromagnetic coupling and frustration parameters are key inputs.

free parameters (2)
  • interlayer coupling strength
    Tuned to stabilize anti-topological textures and prevent distortion; value not specified in abstract but modulated to study effects.
  • frustration parameters
    Competing interactions introduced to induce rich morphologies of anti-topological textures.
axioms (2)
  • standard math Standard spin Hamiltonian for magnetic interactions in bilayers
    Invoked implicitly as the basis for the general model without external field.
  • domain assumption Antiferromagnetic interlayer coupling with frustration
    Core setup for realizing compensated topological charges.

pith-pipeline@v0.9.0 · 5454 in / 1402 out tokens · 35043 ms · 2026-05-10T18:07:45.853948+00:00 · methodology

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Works this paper leans on

52 extracted references · 52 canonical work pages · 1 internal anchor

  1. [1]

    Muehlbauer, B

    S. Muehlbauer, B. Binz, F. Jonietz, C. Pfleiderer, A. Rosch, A. Neubauer, R. Georgii, and P. Boeni, Skyrmion lattice in a chiral magnet, Science 323, 915 (2009)

  2. [2]

    A. Fert, V . Cros, and J. Sampaio, Skyrmions on the track, Nat. Nanotechnol. 8, 152 (2013)

  3. [3]

    Zhang, M

    X. Zhang, M. Ezawa, and Y . Zhou, Magnetic skyrmion logic gates: conversion, duplication and merging of skyrmions, Sci. Rep. 5, 9400 (2015)

  4. [4]

    A. Fert, N. Reyren, and V . Cros, Magnetic skyrmions: advances in physics and potential applications, Nat. Rev. Mater. 2, 17031 (2017)

  5. [5]

    Zhang, Y

    X. Zhang, Y . Zhou, K. M. Song, T.-E. Park, J. Xia, M. Ezawa, X. Liu, W. Zhao, G. Zhao, and S. Woo, Skyrmion-electronics: writing, deleting, reading and processing magnetic skyrmions toward spintronic applications, J. Phys.: Condens. Matter 32, 143001 (2020)

  6. [6]

    X. Z. Yu, N. Kanazawa, W. Z. Zhang, T. Nagai, T. Hara, K. Kimoto, Y . Matsui, Y . Onose, and Y . Tokura, Skyrmion flow near room temperature in an ultralow current density, Nat. Commun. 3, 988 (2012)

  7. [7]

    Nagaosa and Y

    N. Nagaosa and Y . Tokura, Topological properties and dynamics of magnetic skyrmions, Nat. Nanotechnol. 8, 899 (2013)

  8. [8]

    X. Yu, M. Mostovoy, Y . Tokunaga, W. Zhang, K. Kimoto, Y . Matsui, Y . Kaneko, N. Nagaosa, and Y . Tokura, Magnetic stripes and skyrmions with helicity reversals, Proc. Natl. Acad. Sci. U. S. A. 109, 8856 (2012)

  9. [9]

    Okubo, S

    T. Okubo, S. Chung, and H. Kawamura, Multiple-q states and the skyrmion lattice of the triangular- lattice heisenberg antiferromagnet under magnetic fields, Phys. Rev. Lett. 108, 017206 (2012)

  10. [10]

    Ozawa, S

    R. Ozawa, S. Hayami, and Y . Motome, Zero -field skyrmions with a high topological number in itinerant magnets, Phys. Rev. Lett. 118, 147205 (2017)

  11. [11]

    Yao and S

    X. Yao and S. Dong, Vector vorticity of skyrmionic texture: an internal degree of freedom tunable by magnetic field, Phys. Rev. B 105, 014444 (2022)

  12. [12]

    H. L. Hu, Z. Shen, Z. Chen, X. P. Wu, T. T. Zhong, and C. S. Song, High -topological-number skyrmions with tunable diameters in two -dimensional frustrated J 1-J2 magnets, Appl. Phys. Lett. 125, 092402 (2024)

  13. [13]

    A. O. Leonov and M. Mostovoy, Multiply periodic states and isolated skyrmions in an anisotropic frustrated magnet, Nat. Commun. 6, 8275 (2015)

  14. [14]

    X. C. Zhang, J. Xia, Y . Zhou, X. X. Liu, H. Zhang, and M. Ezawa, Skyrmion dynamics in a frustrated ferromagnetic film and current -induced helicity locking -unlocking transition, Nat. Commun. 8, 1717 (2017)

  15. [15]

    Litzius, I

    K. Litzius, I. Lemesh, B. Krueger, P . Bassirian, L. Caretta, K. Richter, F. Buettner, K. Sato, O. A. Tretiakov, J. Foerster, R. M. Reeve, M. Weigand, L. Bykova, H. Stoll, G. Schuetz, G. S. D. Beach, and M. Klaeui, Skyrmion Hall effect revealed by direct time-resolved x-ray microscopy, Nat. Phys. 13, 170 (2017)

  16. [16]

    W. J. Jiang, X. C. Zhang, G. Q. Yu, W. Zhang, X. Wang, M. B. Jungfleisch, J. E. Pearson, X. M. Cheng, O. Heinonen, K. L. Wang, Y . Zhou, A. Hoffmann, and S. G. E. te Velthuis, Direct observation of the skyrmion Hall effect, Nat. Phys. 13, 162 (2017)

  17. [17]

    S. Woo, K. M. Song, X. Zhang, Y . Zhou, M. Ezawa, X. Liu, S. Finizio, J. Raabe, N. J. Lee, S. -I. Kim, S.-Y . Park, Y . Kim, J.-Y . Kim, D. Lee, O. Lee, J. W. Choi, B.-C. Min, H. C. Koo, and J. Chang, Current-driven dynamics and inhibition of the skyrmion Hall effect of ferrimagnetic skyrmions in GdFeCo films, Nat. Commun. 9, 959 (2018)

  18. [18]

    Barker and O

    J. Barker and O. A. Tretiakov, Static and dynamical properties of antiferromagnetic skyrmions in the presence of applied current and temperature, Phys. Rev. Lett. 116, 147203 (2016)

  19. [19]

    C. D. Jin, C. K. Song, J. B. Wang, and Q. F. Liu, Dynamics of antiferromagnetic skyrmion driven by the spin Hall effect, Appl. Phys. Lett. 109, 182404 (2016)

  20. [20]

    Zhang, Y

    X. Zhang, Y . Zhou, and M. Ezawa, Antiferromagnetic skyrmion: stability, creation and manipulation, Sci. Rep. 6, 24795 (2016)

  21. [21]

    L. C. Shen, J. Xia, G. P. Zhao, X. C. Zhang, M. Ezawa, O. A. Tretiakov, X. X. Liu, and Y . Zhou, Dynamics of the antiferromagnetic skyrmion induced by a magnetic anisotropy gradient, Phys. Rev. B 98, 134448 (2018)

  22. [22]

    B. Q. Dai, D. Wu, S. A. Razavi, S. J. Xu, H. R. He, Q. Y . Shu, M. Jackson, F. Mahfouzi, H. S. Huang, Q. J. Pan, Y . Cheng, T. Qu, T. Y . Wang, L. X. Tai, K. Wong, N. Kioussis, and K. L. Wang, Electric field manipulation of spin chirality and skyrmion dynamics, Sci. Adv. 9, eade6836 (2023)

  23. [23]

    Z. L. He, K. Y . Dou, W. H. Du, Y . Dai, B. B. Huang, and Y . D. Ma, Mixed Bloch -Néel type skyrmions in a two-dimensional lattice, Phys. Rev. B 109, 024420 (2024)

  24. [24]

    S. Y . Huang, C. Zhou, G. Chen, H. Y . Shen, A. K. Schmid, K. Liu, and Y . Z. Wu, Stabilization and current-induced motion of antiskyrmion in the presence of anisotropic Dzyaloshinskii -Moriya interaction, Phys. Rev. B 96, 144412 (2017)

  25. [25]

    A. P. Reddy, D. N. Sheng, A. Abouelkomsan, E. J. Bergholtz, and L. Fu, Anti -topological crystal and non-Abelian liquid in twisted semiconductor bilayers, arXiv:2411.19898 (2024)

  26. [26]

    Zhang, Y

    X. Zhang, Y . Zhou, and M. Ezawa, Magnetic bilayer-skyrmions without skyrmion Hall effect, Nat. Commun. 7, 10293 (2016)

  27. [27]

    Q. R. Cui, Y . M. Zhu, J. H. Liang, P. Cui, and H. X. Yang, Antiferromagnetic topological magnetism in synthetic van der Waals antiferromagnets, Phys. Rev. B 107, 064422 (2023)

  28. [28]

    R. Y . Chen, Q. R. Cui, L. Han, X. T. Xue, J. H. Liang, H. Bai, Y . J. Zhou, F. Pan, H. X. Yang, and C. Song, Controllable generation of antiferromagnetic skyrmions in synthetic antiferromagnets with thermal effect, Adv. Funct. Mater. 32, 2111906 (2022)

  29. [29]

    V . Pham, N. Sisodia, I. Di Manici, J. Urrestarazu -Larrañaga, K. Bairagi, J. Pelloux -Prayer, R. Guedas, L. D. Buda-Prejbeanu, S. Auffret, A. Locatelli, T. O. Mentes, S. Pizzini, P. Kumar, A. Finco, V . Jacques, G. Gaudin, and O. Boulle, Fast current -induced skyrmion motion in synthetic antiferromagnets, Science 384, 307 (2024)

  30. [30]

    J. Xia, X. C. Zhang, M. Ezawa, Z. P. Hou, W. H. Wang, X. X. Liu, and Y . Zhou, Current -Driven dynamics of frustrated skyrmions in a synthetic antiferromagnetic bilayer, Phys. Rev. Appl. 11, 044046 (2019)

  31. [31]

    W. Sun, W. X. Wang, H. Li, X. N. Li, Z. Y . Yu, Y . Bai, G. B. Zhang, and Z. X. Cheng, LaBr2 bilayer multiferroic moire superlattice with robust magnetoelectric coupling and magnetic bimerons, npj Comput. Mater. 8, 159 (2022)

  32. [32]

    Khatua, B

    J. Khatua, B. Sana, A. Zorko, M. Gomilsek, K. Sethupathi, M. S. R. Rao, M. Baenitz, B. Schmidt, and P . Khuntia, Experimental signatures of quantum and topological states in frustrated magnetism, Phys. Rep. 1041, 1 (2023)

  33. [33]

    H. Ge, T. Li, S. E. Nikitin, N. Zhao, F. Li, H. Bu, J. Yuan, J. Chen, Y . Fu, J. Yang, L. Wang, P. Miao, Q. Zhang, I. Puente-Orench, A. Podlesnyak, J. Sheng, and L. Wu, Magnetic structure and Ising-like antiferromagnetism in the bilayer triangular lattice compound NdZnPO, Phys. Rev. B 110, 054443 (2024)

  34. [34]

    Nakatsuji, H

    S. Nakatsuji, H. Tonomura, K. Onuma, Y . Nambu, O. Sakai, Y . Maeno, R. T. Macaluso, and J. Y . Chan, Spin disorder and order in quasi -2D triangular heisenberg antiferromagnets: comparative study of FeGa2S4, Fe2Ga2S5, and NiGa2S4, Phys. Rev. Lett. 99, 157203 (2007)

  35. [35]

    Q. Q. Li, W. W. Liu, Z. K. Ding, H. Pan, X. H. Cao, W. H. Xiao, N. N. Luo, J. Zeng, L. M. Tang, B. Li, K. Q. Chen, and X. D. Duan, Stacking- and strain-dependent magnetism in Janus CrSTe bilayer, Appl. Phys. Lett. 122, 121902 (2023)

  36. [36]

    Hayami, Skyrmion crystal and spiral phases in centrosymmetric bilayer magnets with staggered Dzyaloshinskii-Moriya interaction, Phys

    S. Hayami, Skyrmion crystal and spiral phases in centrosymmetric bilayer magnets with staggered Dzyaloshinskii-Moriya interaction, Phys. Rev. B 105, 014408 (2022)

  37. [37]

    G. P. Mueller, M. Hoffmann, C. Disselkamp, D. Schuerhoff, S. Mavros, M. Sallermann, N. S. Kiselev, H. Jonsson, and S. Bluegel, Spirit: multifunctional framework for atomistic spin simulations, Phys. Rev. B 99, 224414 (2019)

  38. [38]

    [11,22,23,37,43-52]

    See Supplementary Material for the simulation details; the energy barrier and dynamics of ATB bimerons; the calculations on Cr 2HfC2H2; the dynamics of ATB skyrmionic textures with high Q; and the potential application and modulation, which cites Refs. [11,22,23,37,43-52]

  39. [39]

    B. Heil, A. Rosch, and J. Masell, Universality of annihilation barriers of large magnetic skyrmions in chiral and frustrated magnets, Phys. Rev. B 100, 134424 (2019)

  40. [40]

    Aldarawsheh, I

    A. Aldarawsheh, I. L. Fernandes, S. Brinker, M. Sallermann, M. Abusaa, S. Blügel, and S. Lounis, Emergence of zero-field non-synthetic single and interchained antiferromagnetic skyrmions in thin films, Nat. Commun. 13, 7369 (2022)

  41. [41]

    P. F. Bessarab, V . M. Uzdin, and H. Jónsson, Method for finding mechanism and activation energy of magnetic transitions, applied to skyrmion and antivortex annihilation, Comput. Phys. Commun. 196, 335 (2015)

  42. [42]

    Anasori, Y

    B. Anasori, Y . Xie, M. Beidaghi, J. Lu, B. C. Hosler, L. Hultman, P. R. C. Kent, Y . Gogotsi, and M. W. Barsoum, Two-dimensional, ordered, double transition metals carbides (MXenes), ACS Nano 9, 9507 (2015)

  43. [43]

    J. H. Guo, Y . Hou, J. Xia, X. Zhang, P. W. T. Pong, and Y . Zhou, Dynamic properties of a ferromagnetic skyrmion in an in-plane magnetic field, J. Appl. Phys. 131, 073901 (2022)

  44. [44]

    J. C. Martinez, W. S. Lew, W. L. Gan, and M. B. A. Jalil, Theory of current -induced skyrmion dynamics close to a boundary, J. Magn. Magn. Mater. 465, 685 (2018)

  45. [45]

    Kresse and J

    G. Kresse and J. Furthmüller, Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set, Phys. Rev. B 54, 11169 (1996)

  46. [46]

    S. Bae, Y . G. Kang, M. Khazaei, K. Ohno, Y . H. Kim, M. J. Han, K. J. Chang, and H. Raebiger, Electronic and magnetic properties of carbide MXenes -the role of electron correlations, Mater. Today Adv. 9, 100118 (2021)

  47. [47]

    Y . G. Zhang, Z. Cui, B. S. Sa, N. H. Miao, J. Zhou, and Z. M. Sun, Computational design of double transition metal MXenes with intrinsic magnetic properties, Nanoscale Horiz. 7, 276 (2022)

  48. [48]

    J. Chen, J. J. Liang, J. H. Yu, M. H. Qin, Z. Fan, M. Zeng, X. B. Lu, X. S. Gao, S. Dong, and J -M Liu, Dynamics of distorted skyrmions in strained chiral magnets, New J. Phys. 20, 063050 (2018)

  49. [49]

    Psaroudaki and C

    C. Psaroudaki and C. Panagopoulos, Skyrmion Qubits: A New Class of Quantum Logic Elements Based on Nanoscale Magnetization, Phys. Rev. Lett. 127, 067201 (2021)

  50. [50]

    J. Xia, X. C. Zhang, X. X. Liu, Y . Zhou, and M. Ezawa, Universal Quantum Computation Based on Nanoscale Skyrmion Helicity Qubits in Frustrated Magnets, Phys. Rev. Lett. 130, 106701 (2023)

  51. [51]

    K. Wu, Y . L. Zhao, H. Y . Hao, S. Yang, S. Li, Q. F. Liu, S. F. Zhang, X. X. Zhang, J. Akerman, L. Xi, Y . Zhang, K. M. Cai, and Y . Zhou, Topological transformation of synthetic ferromagnetic skyrmions: thermal assisted switching of helicity by spin -orbit torque, Nat. Commun. 15, 10463 (2024)

  52. [52]

    X. Yao, J. Chen, and S. Dong, Controlling the helicity of magnetic skyrmions by electrical field in frustrated magnets, New J. Phys. 22, 083032 (2020)