Recognition: 2 theorem links
· Lean TheoremTopology-constrained spin-wave modes of asymmetric antibimerons and their clusters
Pith reviewed 2026-05-10 17:47 UTC · model grok-4.3
The pith
Asymmetric antibimerons support discrete localized spin-wave modes that split into N-fold multiplets when clustered.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
An isolated asymmetric antibimeron supports a discrete spectrum of localized modes reflecting its internal degrees of freedom. When multiple asymmetric antibimerons form a cluster, inter-texture coupling leads to the splitting of these modes into N-fold multiplets. An effective coupled-oscillator model based on meron pairs captures the essential collective dynamics, revealing that the motion of the clusters can be understood in terms of well-defined normal modes governed by topology-constrained particle-like degrees of freedom.
What carries the argument
effective coupled-oscillator model based on meron pairs, which converts the topology-constrained internal structure of each antibimeron into particle-like degrees of freedom and accounts for their inter-texture coupling
If this is right
- The normal-mode spectrum of any cluster is fixed by its size N and can therefore be chosen in advance.
- Asymmetric antibimeron clusters supply a set of low-lying resonances whose frequencies are set by topology rather than by external fields.
- The same effective description shows that the entire cluster behaves as a single object with well-defined normal modes of motion.
- The platform is directly usable for spin-wave nano-oscillators whose resonance set is programmable by assembling different numbers of textures.
Where Pith is reading between the lines
- The same meron-pair oscillator picture may apply to other paired topological textures, allowing the model to be tested on bimerons or skyrmion pairs.
- Changing the distance between antibimerons inside a fixed-size cluster offers an additional tuning knob for the splitting that the paper does not explore.
- If the particle-like normal modes survive in larger assemblies, clusters could serve as movable elements whose internal oscillations are protected by topology.
Load-bearing premise
The simple oscillator model built from meron pairs reproduces the full spin-wave spectrum of the magnetic textures without important missing contributions from damping or from details of the micromagnetic energy.
What would settle it
Micromagnetic simulations of a cluster containing a specific number N of asymmetric antibimerons that produce mode frequencies or degeneracies that deviate from the N-fold splitting predicted by the coupled-oscillator model would falsify the claim.
Figures
read the original abstract
Collective modes are a defining signature of coupled degrees of freedom, forming a bridge between understanding of interactions in condensed-matter systems and emergent functionality. Topological magnetic textures provide a natural platform to realize and control such collective modes at the nanoscale. Here we theoretically identify and characterize low-energy collective spin-wave excitations of isolated asymmetric antibimerons and their clusters in ultrathin ferromagnetic films. We demonstrate that an isolated asymmetric antibimeron supports a discrete spectrum of localized modes, reflecting its internal degrees of freedom. When multiple asymmetric antibimerons form a cluster, inter-texture coupling leads to the splitting of these modes into $N$-fold multiplets, where $N$ denotes the number of asymmetric antibimerons. To rationalize these findings, we introduce an effective coupled-oscillator model based on meron pairs that captures the essential collective dynamics of the system. This emergent classical mechanics description reveals that the motion of asymmetric antibimeron clusters can be understood in terms of well-defined normal modes governed by topology-constrained particle-like degrees of freedom. These results establish coupled asymmetric antibimerons as a tunable platform for spin-wave based nano-oscillators, whose normal-mode spectrum is controllable through cluster size, thus providing a programmable set of low-lying resonances for these nano-oscillators.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript theoretically identifies and characterizes low-energy collective spin-wave excitations of isolated asymmetric antibimerons and their clusters in ultrathin ferromagnetic films. An isolated asymmetric antibimeron is shown to support a discrete spectrum of localized modes reflecting its internal degrees of freedom. In clusters of N such textures, inter-texture coupling splits these modes into N-fold multiplets. These observations are rationalized via an effective coupled-oscillator model based on meron pairs, which maps the collective dynamics to normal modes governed by topology-constrained particle-like degrees of freedom. The work positions such clusters as a tunable platform for spin-wave nano-oscillators with resonances controllable by cluster size.
Significance. If validated, the identification of topology-constrained modes and their N-fold splitting would provide a concrete example of how topological magnetic textures can host programmable collective excitations at the nanoscale, bridging spin-wave physics with emergent particle-like behavior. The effective model offers an intuitive classical-mechanics description that could guide device design, though its predictive power hinges on quantitative agreement with full micromagnetic dynamics.
major comments (2)
- [Effective coupled-oscillator model] The central claim that the effective coupled-oscillator model (based on meron pairs) captures the essential collective dynamics and reproduces the N-fold multiplet splitting rests on an unverified assumption. No explicit derivation of the model from the micromagnetic energy functional or Landau-Lifshitz-Gilbert equation is shown, nor is there quantitative comparison (e.g., eigenvalue matching or mode-profile overlap) between model predictions and simulated spectra to confirm that damping or higher-order interactions remain negligible.
- [Cluster dynamics and mode splitting] For the cluster results, the manuscript reports splitting into N-fold multiplets but does not provide tabulated frequencies, damping rates, or error estimates from the full simulations versus the model. This leaves the load-bearing assertion that topology-constrained degrees of freedom dominate untested against possible deviations.
minor comments (2)
- [Abstract] The abstract states that the model 'captures the essential collective dynamics' without defining the criterion for 'essential' or listing the free parameters (inter-texture coupling strengths). Clarify this in the main text.
- [Results] Notation for the localized modes and multiplets should be introduced consistently (e.g., labeling the discrete spectrum indices) to aid readability when comparing isolated and clustered cases.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and the constructive comments, which help clarify the presentation of the effective model and the quantitative validation of the cluster results. We address each major comment below.
read point-by-point responses
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Referee: [Effective coupled-oscillator model] The central claim that the effective coupled-oscillator model (based on meron pairs) captures the essential collective dynamics and reproduces the N-fold multiplet splitting rests on an unverified assumption. No explicit derivation of the model from the micromagnetic energy functional or Landau-Lifshitz-Gilbert equation is shown, nor is there quantitative comparison (e.g., eigenvalue matching or mode-profile overlap) between model predictions and simulated spectra to confirm that damping or higher-order interactions remain negligible.
Authors: We acknowledge that the effective model is introduced on the basis of the observed mode structure and the meron-pair representation of each antibimeron, without a full microscopic derivation from the LLG equation. The model is constructed to incorporate the topological constraints and the symmetry-allowed couplings between the internal degrees of freedom. To strengthen the manuscript we will add an expanded section that details the symmetry arguments underlying the oscillator Hamiltonian and the fitting procedure for the parameters. We will also include direct quantitative comparisons of eigenfrequencies and mode profiles between the model and micromagnetic simulations, together with an assessment of the influence of damping. revision: partial
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Referee: [Cluster dynamics and mode splitting] For the cluster results, the manuscript reports splitting into N-fold multiplets but does not provide tabulated frequencies, damping rates, or error estimates from the full simulations versus the model. This leaves the load-bearing assertion that topology-constrained degrees of freedom dominate untested against possible deviations.
Authors: We agree that tabulated comparisons would make the agreement more transparent. In the revised version we will insert tables that list the simulated eigenfrequencies and damping rates for clusters of size N = 2 to 5, together with the corresponding predictions of the effective model and the relative deviations. This will allow a direct evaluation of how well the topology-constrained degrees of freedom account for the observed spectra. revision: yes
Circularity Check
No significant circularity; effective model provides independent topological rationalization
full rationale
The derivation begins with micromagnetic identification of discrete localized modes for isolated asymmetric antibimerons and N-fold splitting in clusters. The effective coupled-oscillator model based on meron pairs is introduced afterward to rationalize the observed spectra and normal modes. No quoted equations or steps reduce the model eigenvalues or frequencies to parameters fitted from the same simulation data by construction, nor do self-citations load-bear the central claims. The topology-constrained particle-like degrees of freedom supply an independent interpretive layer rather than a tautological restatement of inputs.
Axiom & Free-Parameter Ledger
free parameters (1)
- inter-texture coupling strengths
axioms (2)
- domain assumption Asymmetric antibimerons exist as stable topological textures in ultrathin ferromagnetic films
- domain assumption Meron pairs provide an accurate reduced description of antibimeron internal degrees of freedom
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
localized AAB modes... split into N-fold multiplets... topology-constrained particle-like degrees of freedom
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
Goldstein,Classical Mechanics, 2nd ed
H. Goldstein,Classical Mechanics, 2nd ed. (Addison-Wesley, Reading, Mass., 1980)
1980
-
[2]
A. V . Chumak, V . I. Vasyuchka, A. A. Serga, and B. Hille- brands, Magnon spintronics, Nat. Phys.11, 453 (2015)
2015
-
[3]
Flebuset al., The 2024 magnonics roadmap, J
B. Flebuset al., The 2024 magnonics roadmap, J. Phys. Con- dens. Matter36, 363501 (2024)
2024
-
[4]
Kosevich, B
A. Kosevich, B. Ivanov, and A. Kovalev, Magnetic solitons, Phys. Rep.194, 117 (1990)
1990
-
[5]
A. Fert, N. Reyren, and V . Cros, Magnetic skyrmions: advances in physics and potential applications, Nat. Rev. Mater.2, 17031 (2017)
2017
-
[6]
G ¨obel, I
B. G ¨obel, I. Mertig, and O. A. Tretiakov, Beyond skyrmions: Review and perspectives of alternative magnetic quasiparticles, Phys. Rep.895, 1 (2021)
2021
-
[7]
Y . Zhou, S. Li, X. Liang, and Y . Zhou, Topological spin tex- tures: Basic physics and devices, Adv. Mater.37, 2312935 (2025)
2025
-
[8]
S. S. P. Parkin, M. Hayashi, and L. Thomas, Magnetic domain- wall racetrack memory, Science320, 190 (2008)
2008
-
[9]
A. Fert, V . Cros, and J. Sampaio, Skyrmions on the track, Nat. Nanotechnol.8, 152 (2013)
2013
-
[10]
Grollier, D
J. Grollier, D. Querlioz, K. Y . Camsari, K. Everschor-Sitte, S. Fukami, and M. D. Stiles, Neuromorphic spintronics, Nat. Electron.3, 360 (2020)
2020
-
[11]
Pirro, V
P. Pirro, V . I. Vasyuchka, A. A. Serga, and B. Hillebrands, Ad- vances in coherent magnonics, Nat. Rev. Mater.6, 1114 (2021)
2021
-
[12]
A. V . Chumaket al., Advances in magnetics roadmap on spin- wave computing, IEEE Trans. Magn.58, 1 (2022)
2022
-
[13]
Y . Sun, T. Lin, N. Lei, X. Chen, W. Kang, Z. Zhao, D. Wei, C. Chen, S. Pang, L. Hu, L. Yang, E. Dong, L. Zhao, L. Liu, Z. Yuan, A. Ullrich, C. H. Back, J. Zhang, D. Pan, J. Zhao, M. Feng, A. Fert, and W. Zhao, Experimental demonstration of a skyrmion-enhanced strain-mediated physical reservoir com- puting system, Nat. Commun.14, 3434 (2023)
2023
-
[14]
Everschor-Sitte, A
K. Everschor-Sitte, A. Majumdar, K. Wolk, and D. Meier, Topological magnetic and ferroelectric systems for reservoir computing, Nat. Rev. Phys.6, 455 (2024)
2024
-
[15]
T. H. R. Skyrme, A unified field theory of mesons and baryons, Nucl. Phys.31, 556 (1962)
1962
-
[16]
A. A. Belavin and A. M. Polyakov, Metastable states of two- dimensional isotropic ferromagnets, JETP Lett.22, 503 (1975)
1975
-
[17]
M ¨uhlbauer, B
S. M ¨uhlbauer, B. Binz, F. Jonietz, C. Pfleiderer, A. Rosch, A. Neubauer, R. Georgii, and P. Boni, Skyrmion lattice in a chiral magnet, Science323, 915 (2009)
2009
-
[18]
U. K. R ¨oßler, A. N. Bogdanov, and C. Pfleiderer, Spontaneous skyrmion ground states in magnetic metals, Nature442, 797 (2006)
2006
-
[19]
Nagaosa and Y
N. Nagaosa and Y . Tokura, Topological properties and dynam- ics of magnetic skyrmions, Nat. Nanotechnol.8, 899 (2013)
2013
-
[20]
Koshibae and N
W. Koshibae and N. Nagaosa, Creation of skyrmions and anti- skyrmions by local heating, Nat. Commun.5, 5148 (2014)
2014
-
[21]
S.-G. Je, P. Vallobra, T. Srivastava, J.-C. Rojas-S ´anchez, T. H. Pham, M. Hehn, G. Malinowski, C. Baraduc, S. Auffret, G. Gaudin, S. Mangin, H. B ´ea, and O. Boulle, Creation of magnetic skyrmion bubble lattices by ultrafast laser in ultrathin films, Nano Lett.18, 7362 (2018). 8
2018
-
[22]
Ohara, X
K. Ohara, X. Zhang, Y . Chen, S. Kato, J. Xia, M. Ezawa, O. A. Tretiakov, Z. Hou, Y . Zhou, G. Zhao, J. Yang, and X. Liu, Reversible transformation between isolated skyrmions and bimerons, Nano Lett.22, 8559 (2022)
2022
-
[23]
Neubauer, C
A. Neubauer, C. Pfleiderer, B. Binz, A. Rosch, R. Ritz, P. G. Niklowitz, and P. B¨oni, Topological Hall effect in theAphase of MnSi, Phys. Rev. Lett.102, 186602 (2009)
2009
-
[24]
Heinze, K
S. Heinze, K. von Bergmann, M. Menzel, J. Brede, A. Kubet- zka, R. Wiesendanger, G. Bihlmayer, and S. Bl ¨ugel, Sponta- neous atomic-scale magnetic skyrmion lattice in two dimen- sions, Nat. Phys.7, 713 (2011)
2011
-
[25]
Hirschberger, T
M. Hirschberger, T. Nakajima, S. Gao, L. Peng, A. Kikkawa, T. Kurumaji, M. Kriener, Y . Yamasaki, H. Sagayama, H. Nakao, K. Ohishi, K. Kakurai, Y . Taguchi, X. Yu, T.-h. Arima, and Y . Tokura, Skyrmion phase and competing magnetic orders on a breathing kagom´e lattice, Nat. Commun.10, 5831 (2019)
2019
-
[26]
X. Z. Yu, N. Kanazawa, W. Z. Zhang, T. Nagai, T. Hara, K. Ki- moto, Y . Matsui, Y . Onose, and Y . Tokura, Skyrmion flow near room temperature in an ultralow current density, Nat. Commun. 3, 988 (2012)
2012
-
[27]
Zhang, Y
X. Zhang, Y . Zhou, and M. Ezawa, Antiferromagnetic skyrmion: Stability, creation and manipulation, Sci. Rep.6, 24795 (2016)
2016
-
[28]
Barker and O
J. Barker and O. A. Tretiakov, Static and dynamical properties of antiferromagnetic skyrmions in the presence of applied cur- rent and temperature, Phys. Rev. Lett.116, 147203 (2016)
2016
-
[29]
O. J. Amin, S. F. Poole, S. Reimers, L. X. Barton, A. Dal Din, F. Maccherozzi, S. S. Dhesi, V . Nov´ak, F. Krizek, J. S. Chauhan, R. P. Campion, A. W. Rushforth, T. Jungwirth, O. A. Treti- akov, K. W. Edmonds, and P. Wadley, Antiferromagnetic half- skyrmions electrically generated and controlled at room tem- perature, Nat. Nanotechnol.18, 849 (2023)
2023
-
[30]
X. Z. Yu, Y . Onose, N. Kanazawa, J. H. Park, J. H. Han, Y . Mat- sui, N. Nagaosa, and Y . Tokura, Real-space observation of a two-dimensional skyrmion crystal, Nature465, 901 (2010)
2010
-
[31]
S. Seki, X. Z. Yu, S. Ishiwata, and Y . Tokura, Observation of skyrmions in a multiferroic material, Science336, 198 (2012)
2012
-
[32]
Tokunaga, X
Y . Tokunaga, X. Z. Yu, J. S. White, H. M. Rønnow, D. Morikawa, Y . Taguchi, and Y . Tokura, A new class of chiral materials hosting magnetic skyrmions beyond room tempera- ture, Nat. Commun.6, 7638 (2015)
2015
-
[33]
Legrand, D
W. Legrand, D. Maccariello, F. Ajejas, S. Collin, A. Vecchi- ola, K. Bouzehouane, N. Reyren, V . Cros, and A. Fert, Room- temperature stabilization of antiferromagnetic skyrmions in synthetic antiferromagnets, Nat. Mater.19, 34 (2020)
2020
-
[34]
Tokura and N
Y . Tokura and N. Kanazawa, Magnetic skyrmion materials, Chem. Rev.121, 2857 (2021)
2021
-
[35]
Meisenheimer, H
P. Meisenheimer, H. Zhang, D. Raftrey, X. Chen, Y .-T. Shao, Y .-T. Chan, R. Yalisove, R. Chen, J. Yao, M. C. Scott, W. Wu, D. A. Muller, P. Fischer, R. J. Birgeneau, and R. Ramesh, Or- dering of room-temperature magnetic skyrmions in a polar van der Waals magnet, Nat. Commun.14, 3744 (2023)
2023
-
[36]
Petrova and O
O. Petrova and O. Tchernyshyov, Spin waves in a skyrmion crystal, Phys. Rev. B84, 214433 (2011)
2011
-
[37]
Mochizuki, Spin-wave modes and their intense excitation effects in skyrmion crystals, Phys
M. Mochizuki, Spin-wave modes and their intense excitation effects in skyrmion crystals, Phys. Rev. Lett.108, 017601 (2012)
2012
-
[38]
Schwarze, J
T. Schwarze, J. Waizner, M. Garst, A. Bauer, I. Stasinopou- los, H. Berger, C. Pfleiderer, and D. Grundler, Universal heli- magnon and skyrmion excitations in metallic, semiconducting and insulating chiral magnets, Nat. Mater.14, 478 (2015)
2015
-
[39]
Mruczkiewicz, P
M. Mruczkiewicz, P. Gruszecki, M. Zelent, and M. Krawczyk, Collective dynamical skyrmion excitations in a magnonic crys- tal, Phys. Rev. B93, 174429 (2016)
2016
-
[40]
V . P. Kravchuk, O. Gomonay, D. D. Sheka, D. R. Rodrigues, K. Everschor-Sitte, J. Sinova, J. van den Brink, and Y . Gaididei, Spin eigenexcitations of an antiferromagnetic skyrmion, Phys. Rev. B99, 184429 (2019)
2019
-
[41]
S. Seki, M. Garst, J. Waizner, R. Takagi, N. D. Khanh, Y . Oka- mura, K. Kondou, F. Kagawa, Y . Otani, and Y . Tokura, Propaga- tion dynamics of spin excitations along skyrmion strings, Nat. Commun.11, 256 (2020)
2020
-
[42]
L. Shen, X. Li, J. Xia, L. Qiu, X. Zhang, O. A. Tretiakov, M. Ezawa, and Y . Zhou, Dynamics of ferromagnetic bimerons driven by spin currents and magnetic fields, Phys. Rev. B102, 104427 (2020)
2020
-
[43]
L. Shen, J. Xia, Z. Chen, X. Li, X. Zhang, O. A. Tretiakov, Q. Shao, G. Zhao, X. Liu, M. Ezawa, and Y . Zhou, Nonrecip- rocal dynamics of ferrimagnetic bimerons, Phys. Rev. B105, 014422 (2022)
2022
-
[44]
X. Yu, N. Kanazawa, X. Zhang, Y . Takahashi, K. V . Iak- oubovskii, K. Nakajima, T. Tanigaki, M. Mochizuki, and Y . Tokura, Spontaneous vortex-antivortex pairs and their topo- logical transitions in a chiral-lattice magnet, Adv. Mater.36, 2306441 (2024)
2024
- [45]
-
[46]
Y . A. Kharkov, O. P. Sushkov, and M. Mostovoy, Bound states of skyrmions and merons near the Lifshitz point, Phys. Rev. Lett.119, 207201 (2017)
2017
-
[47]
G ¨obel, A
B. G ¨obel, A. Mook, J. Henk, I. Mertig, and O. A. Tretiakov, Magnetic bimerons as skyrmion analogues in in-plane magnets, Phys. Rev. B99, 060407(R) (2019)
2019
-
[48]
Gao, S.-G
N. Gao, S.-G. Je, M.-Y . Im, J. W. Choi, M. Yang, Q. Li, T. Y . Wang, S. Lee, H.-S. Han, K.-S. Lee, W. Chao, C. Hwang, J. Li, and Z. Q. Qiu, Creation and annihilation of topological meron pairs in in-plane magnetized films, Nat. Commun.10, 5603 (2019)
2019
-
[49]
J. Chen, X. Li, L. Shen, Z. Wang, H. Zhang, A. Litvinenko, J. Åkerman, X. Xu, O. A. Tretiakov, and Y . Zhou, Current- induced dynamics of bloch domain-wall bimerons, Phys. Rev. B112, 224420 (2025)
2025
-
[50]
O. A. Tretiakov and O. Tchernyshyov, V ortices in thin ferro- magnetic films and the skyrmion number, Phys. Rev. B75, 012408 (2007)
2007
-
[51]
Castro, D
M. Castro, D. G ´alvez-Poblete, S. Castillo-Sep ´ulveda, V . L. Carvalho-Santos, A. S. Nunez, and S. Allende, Bimerons as edge states in thin magnetic strips, Nano Lett.25, 7249 (2025)
2025
-
[52]
X. Li, L. Shen, Y . Bai, J. Wang, X. Zhang, M. E. J. Xia, O. A. Tretiakov, X. Xu, M. Mruczkiewicz, M. Krawczyk, Y . Xu, R. F. L. Evans, R. W. Chantrell, and Y . Zhou, Bimeron clusters in chiral antiferromagnets, npj Comput. Mater.6, 169 (2020)
2020
-
[53]
F. G. Aliev, J. F. Sierra, A. A. Awad, G. N. Kakazei, D.-S. Han, S.-K. Kim, V . Metlushko, B. Ilic, and K. Y . Guslienko, Spin waves in circular soft magnetic dots at the crossover between vortex and single domain state, Phys. Rev. B79, 174433 (2009)
2009
-
[54]
V ogt, O
K. V ogt, O. Sukhostavets, H. Schultheiss, B. Obry, P. Pirro, A. A. Serga, T. Sebastian, J. Gonzalez, K. Y . Guslienko, and B. Hillebrands, Optical detection of vortex spin-wave eigen- modes in microstructured ferromagnetic disks, Phys. Rev. B84, 174401 (2011)
2011
-
[55]
Sch ¨utte and M
C. Sch ¨utte and M. Garst, Magnon-skyrmion scattering in chiral magnets, Phys. Rev. B90, 094423 (2014)
2014
-
[56]
J. C. Loudon, A. O. Leonov, A. N. Bogdanov, M. C. Hatnean, and G. Balakrishnan, Direct observation of attractive skyrmions and skyrmion clusters in the cubic helimagnet Cu2OSeO3, Phys. Rev. B97, 134403 (2018). 9
2018
-
[57]
C. Naya, D. Schubring, M. Shifman, and Z. Wang, Skyrmions and hopfions in three-dimensional frustrated magnets, Phys. Rev. B106, 094434 (2022)
2022
-
[58]
H. R. O. Sohn, S. M. Vlasov, V . M. Uzdin, A. O. Leonov, and I. I. Smalyukh, Real-space observation of skyrmion clusters with mutually orthogonal skyrmion tubes, Phys. Rev. B100, 104401 (2019)
2019
-
[59]
Such an extended descrip- tion would be consistent with the gyration of the merons ob- served in the micromagnetic simulations, but lies beyond the scope of this work
A gyrotropic term is not included explicitly, as its incorporation would require at least a two-dimensional collective-coordinate description of the meron dynamics. Such an extended descrip- tion would be consistent with the gyration of the merons ob- served in the micromagnetic simulations, but lies beyond the scope of this work
-
[60]
Garcia-Sanchez, J
F. Garcia-Sanchez, J. Sampaio, N. Reyren, V . Cros, and J.- V . Kim, A skyrmion-based spin-torque nano-oscillator, New J. Phys.18, 075011 (2016)
2016
-
[61]
L. Shen, J. Xia, G. Zhao, X. Zhang, M. Ezawa, O. A. Treti- akov, X. Liu, and Y . Zhou, Spin torque nano-oscillators based on antiferromagnetic skyrmions, Appl. Phys. Lett.114, 042402 (2019)
2019
-
[62]
L. Shen, Q. Shao, J. Åkerman, and Y . Zhou, Terahertz spin torque nano-oscillator based on a ferrimagnetic skyrmion lat- tice, npj Spintron.4, 5 (2026)
2026
-
[63]
C. H. Marrows, J. Barker, T. A. Moore, and T. Moorsom, Neuromorphic computing with spintronics, npj Spintron.2, 12 (2024). SUPPLEMENTARY INFORMATION S1. MAGNON DISPERSION A. In-plane field We begin by considering the micromagnetic Hamiltonian given by Eq. (1) in the main text to derive the magnon dispersion. This dispersion relation characterizes the magn...
2024
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