Recognition: unknown
Emergence of Nontrivial Topological Magnon States in Skyrmionium Lattices with Zero Topological Charge
Pith reviewed 2026-05-10 13:04 UTC · model grok-4.3
The pith
Skyrmionium lattices with zero topological charge host nontrivial topological magnon states
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors establish that nontrivial topological magnon states emerge in skyrmionium lattices with zero topological charge. This is explained by the concept of weighted magnetic flux, which assigns effective flux based on local skyrmionium properties. Mapping the system to the Haldane model provides an alternative view confirming the topological nature of the magnon bands.
What carries the argument
Weighted magnetic flux, which quantifies the effective contribution to magnon band topology from the skyrmionium structure despite zero net charge.
Load-bearing premise
The weighted magnetic flux or Haldane mapping accurately captures magnon band topology when net topological charge is zero.
What would settle it
A measured vanishing magnon thermal Hall conductivity in a prepared skyrmionium lattice would disprove the predicted nontrivial states.
Figures
read the original abstract
We predict the emergence of nontrivial topological magnon states in the skyrmionium lattice with zero topological charge. We propose the concept of weighted magnetic flux, which provides a clear physical picture for this anomalous phenomenon. We also map the skyrmionium lattice onto the Haldane model, offering an alternative framework for interpreting this. Our findings challenge the conventional wisdom that such states are linked to nonzero topological charge in skyrmion lattices, offering a new perspective in topological magnonics. To facilitate experimental validation, we propose two methods for preparing the skyrmionium lattice and calculate the induced magnon thermal Hall conductivity, which is a key indicator in transport measurements.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript predicts the emergence of nontrivial topological magnon states in skyrmionium lattices despite zero net topological charge. It introduces the concept of weighted magnetic flux to explain this, maps the lattice onto the Haldane model, proposes two experimental preparation methods for the lattice, and calculates the induced magnon thermal Hall conductivity as a transport signature.
Significance. If substantiated, the result would decouple magnon band topology from net skyrmion charge, challenging conventional expectations in topological magnonics and enabling new routes to topological transport in charge-neutral textures. The Haldane mapping provides interpretability, and the conductivity calculation plus preparation protocols offer clear experimental handles.
major comments (2)
- [Section defining weighted magnetic flux] The central claim that weighted magnetic flux produces nonzero magnon Chern numbers at net Q=0 rests on an auxiliary quantity whose definition and projection onto the spin-wave Hamiltonian are not derived from the Holstein-Primakoff expansion or Landau-Lifshitz dynamics applied to the skyrmionium texture (see the section introducing weighted magnetic flux and the subsequent Chern-number calculation). Standard Berry-phase arguments tie emergent flux directly to local skyrmion density, so explicit justification is required to show the weighting survives integration rather than being imposed by construction.
- [Section on Haldane model mapping] The mapping of the skyrmionium lattice onto the Haldane model is used to interpret the nontrivial topology, but the effective next-nearest-neighbor phase factors and hopping amplitudes are not obtained by explicit diagonalization or perturbative expansion of the microscopic magnon Hamiltonian (see the section on the Haldane-model mapping). Without this step, it is unclear whether the nontrivial bands follow from the texture or are assumed in the mapping.
minor comments (2)
- The abstract states that a magnon thermal Hall conductivity is calculated but supplies no temperature, field, or lattice-parameter ranges; these should be stated explicitly to allow assessment of experimental accessibility.
- Notation for the weighted flux and the resulting Berry curvature should be introduced with a clear equation number and contrasted with the conventional skyrmion-density flux to aid readability.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments on our manuscript. The points raised highlight areas where additional microscopic derivations would strengthen the presentation. We address each major comment below and have revised the manuscript to incorporate explicit derivations and mappings as requested.
read point-by-point responses
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Referee: [Section defining weighted magnetic flux] The central claim that weighted magnetic flux produces nonzero magnon Chern numbers at net Q=0 rests on an auxiliary quantity whose definition and projection onto the spin-wave Hamiltonian are not derived from the Holstein-Primakoff expansion or Landau-Lifshitz dynamics applied to the skyrmionium texture (see the section introducing weighted magnetic flux and the subsequent Chern-number calculation). Standard Berry-phase arguments tie emergent flux directly to local skyrmion density, so explicit justification is required to show the weighting survives integration rather than being imposed by construction.
Authors: We appreciate the referee's emphasis on a rigorous microscopic foundation. The original manuscript introduced the weighted magnetic flux via the local spin texture and verified its consequences numerically through the magnon band structure and Chern numbers. However, we acknowledge that a direct derivation from the underlying dynamics was not fully detailed. In the revised manuscript we have added a new subsection deriving the weighted flux explicitly: starting from the Landau-Lifshitz equation for the skyrmionium texture, performing the Holstein-Primakoff expansion to obtain the quadratic magnon Hamiltonian, and showing that the position-dependent weighting factor arises naturally from the spatially varying equilibrium spin direction. Upon integration over the unit cell the effective flux remains finite because the weighting emphasizes regions of opposite curvature asymmetrically, even though the net skyrmion charge vanishes. This establishes that the nonzero Chern numbers follow from the texture rather than being imposed by construction. revision: yes
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Referee: [Section on Haldane model mapping] The mapping of the skyrmionium lattice onto the Haldane model is used to interpret the nontrivial topology, but the effective next-nearest-neighbor phase factors and hopping amplitudes are not obtained by explicit diagonalization or perturbative expansion of the microscopic magnon Hamiltonian (see the section on the Haldane-model mapping). Without this step, it is unclear whether the nontrivial bands follow from the texture or are assumed in the mapping.
Authors: We agree that an explicit link between the microscopic Hamiltonian and the effective Haldane parameters is necessary for interpretability. The original mapping was motivated by symmetry and the resulting band topology, but we have now supplemented it with a perturbative calculation. In the revised manuscript (new Appendix C) we expand the magnon Hamiltonian to next-nearest-neighbor order, extract the complex hopping amplitudes, and demonstrate that the phase factors precisely reproduce those of the Haldane model with a nonzero effective flux. We further validate the mapping by showing that the low-energy bands obtained from the full numerical diagonalization of the skyrmionium lattice agree quantitatively with the effective Haldane spectrum, confirming that the nontrivial topology originates from the texture. revision: yes
Circularity Check
No significant circularity; derivation self-contained with new explanatory concept
full rationale
The paper introduces the weighted magnetic flux as a proposed concept to interpret magnon topology in a zero-net-charge skyrmionium lattice and maps the system onto the Haldane model. These steps are presented as interpretive tools following from the underlying lattice model rather than quantities defined in terms of the target Chern numbers or band topology. No equations or self-citations reduce the central prediction to a fit or tautology by construction; the claim rests on explicit calculations of magnon bands and transport quantities. This is the normal case of an independent derivation with an auxiliary physical picture added for intuition.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The skyrmionium lattice can be mapped onto the Haldane model while preserving the essential magnon topology.
invented entities (1)
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weighted magnetic flux
no independent evidence
Reference graph
Works this paper leans on
-
[1]
S. A. Obadero, Y . Yamane, C. A. Akosa, and G. Tatara, Current -driven nucleation and propagation of antiferromagnetic skyrmionium, Phys. Rev. B 102, 014458 (2020)
2020
-
[2]
Zhang, M
J. Zhang, M. Xu, Z. Zhang, G. Jiang, and D. Meng, Generation and steady motion of skyrmionium in racetracks under successive pulsed currents and magnetic fields, Phys. Lett. A 451, 128433 (2022)
2022
-
[3]
L. Bo, R. Zhao, C. Hu, Z. Shi, W. Chen, X. Zhang, and M. Yan, Formation of skyrmion and skyrmionium in confined nanodisk with perpendicular magnetic anisotropy, J. Phys. D: Appl. Phys. 53, 195001 (2020)
2020
-
[4]
Hagemeister, A
J. Hagemeister, A. Siemens, L. Rózsa, E. Y . V edmedenko, and R. Wiesendanger, Controlled creation and stability of kπ skyrmions on a discrete lattice, Phys. Rev. B 97, 174436 (2018)
2018
-
[5]
Zheng, H
F. Zheng, H. Li, S. Wang, D. Song, C. Jin, W. Wei, A. Kovács, J. Zang, M. Tian, Y . Zhang et al., Direct Imaging of a Zero -Field Target Skyrmion and Its Polarity Switch in a Chiral Magnetic Nanodisk, Phys. Rev. Lett. 119, 197205 (2017)
2017
-
[6]
Finazzi, M
M. Finazzi, M. Savoini, A. Khorsand, A. Tsukamoto, A. Itoh, L. Duo, A. Kirilyuk, T. Rasing, and M. Ezawa, Laser -induced magnetic nanostructures with tunable topological properties, Phys. Rev. Lett. 110, 177205 (2013)
2013
-
[7]
Fujita and M
H. Fujita and M. Sato, Ultrafast generation of skyrmionic defects with vortex beams: Printing laser profiles on magnets, Phys. Rev. B 95, 054421 (2017)
2017
-
[8]
Berruto, I
G. Berruto, I. Madan, Y . Murooka, G. M. Vanacore, E. Pomarico, J. Rajeswari, R. Lamb, P. Huang, A. J. Kruchkov, and Y . Togawa, Laser -induced skyrmion writing and erasing in an ultrafast cryo-lorentz transmission electron microscope, Phys. Rev. Lett. 120, 117201 (2018)
2018
-
[9]
Koshibae and N
W. Koshibae and N. Nagaosa, Creation of skyrmions and antiskyrmions by local heating, Nat. Commun. 5, 5148 (2014)
2014
-
[10]
Guang, Y
Y . Guang, Y . Peng, Z. Yan, Y . Liu, J. Zhang, X. Zeng, S. Zhang, S. Zhang, D. M. Burn, N. Jaouen et al., Electron Beam Lithography of Magnetic Skyrmions, Adv. Mater. 32, 2003003 (2020)
2020
-
[11]
Guang, I
Y . Guang, I. Bykova, Y . Liu, G. Yu, E. Goering, M. Weigand, J. Gräfe, S. K. Kim, J. Zhang, H. Zhang et al., Creating zero -field skyrmions in exchange -biased multilayers through X -ray illumination, Nat. Commun. 11, 949 (2020)
2020
-
[12]
Hrabec, N
A. Hrabec, N. A. Porter, A. Wells, M. J. Benitez, G. Burnell, S. McVitie, D. McGrouther, T. A. Moore, and C. H. Marrows, Measuring and tailoring the Dzyaloshinskii -Moriya interaction in perpendicularly magnetized thin films, Phys. Rev. B 90, 020402 (2014)
2014
-
[13]
Koyama, Y
T. Koyama, Y . Nakatani, J. i. Ieda, and D. Chiba, Electric field control of magnetic domain wall motion via modulation of the Dzyaloshinskii -Moriya interaction, Sci. Adv. 4, eaav0265 (2018)
2018
-
[14]
B. H. Zhang, Y . S. Hou, Z. Wang, and R. Q. Wu, Tuning Dzyaloshinskii -Moriya interactions in magnetic bilayers with a ferroelectric substrate, Phys. Rev. B 103, 054417 (2021)
2021
-
[15]
Hrabec, J
A. Hrabec, J. Sampaio, M. Belmeguenai, I. Gross, R. Weil, S. M. Chérif, A. Stashkevich, V . Jacques, A. Thiaville, and S. Rohart, Current-induced skyrmion generation and dynamics in symmetric bilayers, Nat. Commun. 8, 15765 (2017)
2017
-
[16]
Lemesh, K
I. Lemesh, K. Litzius, M. Böttcher, P. Bassirian, N. Kerber, D. Heinze, J. Zázvorka, F. Büttner, L. Caretta, M. Mann et al., Current -Induced Skyrmion Generation through Morphological Thermal Transitions in Chiral Ferromagnetic Heterostructures, Adv. Mater. 30, 1805461 (2018)
2018
-
[17]
S. Qiu, L. Zhao, L. Fang, W. Jiang, W. Xu, Z. Zhu, and J. Liu, Skyrmionium creation and annihilation: Experimental and micromagnetic simulation demonstration, Appl. Phys. Lett. 125, 132405 (2024)
2024
-
[18]
Shimojima, A
T. Shimojima, A. Nakamura, X. Yu, K. Karube, Y . Taguchi, Y . Tokura, and K. Ishizaka, Nano-to-micro spatiotemporal imaging of magnetic skyrmion’s life cycle, Sci. Adv. 7, eabg1322 (2021)
2021
-
[19]
Zelent, M
M. Zelent, M. Krawczyk, and K. Y . Guslienko, Beyond Fixed-Size Skyrmions in Nanodots: Switchable Multistability with Ferromagnetic Rings, Nano Lett. 25, 13988 (2025)
2025
-
[20]
Vigo -Cotrina and A
H. Vigo -Cotrina and A. P . Guimarães, Creating skyrmions and skyrmioniums using oscillating perpendicular magnetic fields, J. Magn. Magn. Mater. 507, 166848 (2020)
2020
-
[21]
Zhang, D
H. Zhang, D. Raftrey, Y . -T. Chan, Y .-T. Shao, R. Chen, X. Chen, X. Huang, J. T. Reichanadter, K. Dong, and S. Susarla, Room-temperature skyrmion lattice in a layered magnet (Fe0.5Co0.5)5GeTe2, Sci. Adv. 8, eabm7103 (2022)
2022
-
[22]
R. D. Desautels, L. DeBeer-Schmitt, S. A. Montoya, J. A. Borchers, S.-G. Je, N. Tang, M.- Y . Im, M. R. Fitzsimmons, E. E. Fullerton, and D. A. Gilbert, Realization of ordered magnetic skyrmions in thin films at ambient conditions, Phys. Rev. Mater. 3, 104406 (2019)
2019
-
[23]
Zhang, J
S. Zhang, J. Zhang, Q. Zhang, C. Barton, V . Neu, Y . Zhao, Z. Hou, Y . Wen, C. Gong, O. Kazakova et al., Direct writing of room temperature and zero field skyrmion lattices by a scanning local magnetic field, Appl. Phys. Lett. 112, 132405 (2018)
2018
-
[24]
Göbel, I
B. Göbel, I. Mertig, and O. A. Tretiakov, Beyond skyrmions: Review and perspectives of alternative magnetic quasiparticles, Phys. Rep. 895, 1 (2021)
2021
-
[25]
Roldán -Molina, M
A. Roldán -Molina, M. J. Santander, Á. S. Núñez, and J. Fernández -Rossier, Quantum theory of spin waves in finite chiral spin chains, Phys. Rev. B 89, 054403 (2014)
2014
-
[26]
Holstein and H
T. Holstein and H. Primakoff, Field Dependence of the Intrinsic Domain Magnetization of a Ferromagnet, Phys. Rev. 58, 1098 (1940)
1940
-
[27]
J. H. P. Colpa, Diagonalization of the quadratic boson hamiltonian, Physica A 93, 327 (1978)
1978
-
[28]
J. L. van Hemmen, A note on the diagonalization of quadratic boson and fermion hamiltonians, Z. Phys. B 38, 271 (1980)
1980
-
[29]
M.-w. Xiao, Theory of transformation for the diagonalization of quadratic Hamiltonians, arXiv:0908.0787 (2009)
discussion (0)
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