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arxiv: 2605.14735 · v1 · pith:ASUTPFEOnew · submitted 2026-05-14 · ❄️ cond-mat.mes-hall

Anisotropic Surface Spin Waves as Signature of A-type Altermagnets

Zhoujian Sun , Yiyuan Chen , Tao Yu , Hai-Zhou Lu , X. C. Xie This is my paper

Pith reviewed 2026-06-30 20:27 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall
keywords altermagnetssurface spin wavesanisotropicA-typechiralitysymmetry breakingstray fieldresonance absorption
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The pith

Anisotropic surface spin waves serve as a signature of A-type altermagnets

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

The paper identifies anisotropic surface spin waves that appear specifically in A-type altermagnets and do not occur in ferromagnets or conventional antiferromagnets. These waves result from the altermagnet property that spin-opposite sublattices cannot be connected by translation or inversion, which breaks combined spatial-inversion and time-reversal symmetry. The breaking produces two distinct features: positions of the waves that depend on their chirality at top versus bottom surfaces, and frequency contours at constant frequency that split according to chirality. The top-bottom positions can be read out from the stray field while the split contours appear in resonance absorption spectra, supplying a practical route to experimental identification of these materials.

Core claim

We discover a kind of anisotropic surface spin waves in A-type altermagnets, which is absent in ferromagnets and conventional antiferromagnets. The anisotropic surface spin waves arise directly from the nature of altermagnets, i.e., the spin-opposite sublattices cannot be related by translation or inversion, which breaks the combined spatial-inversion and time-reversal symmetry, leading to the anisotropic surface spin waves with two properties, the chirality-dependent top-bottom positions and chiral split constant frequency contours. We further show that these two properties can be measured experimentally from the stray field and by resonance absorption spectrum, respectively. Our results pr

What carries the argument

Anisotropic surface spin waves generated by altermagnetic symmetry breaking in which spin-opposite sublattices cannot be related by translation or inversion

If this is right

  • Chirality-dependent top-bottom positions of the surface spin waves appear in the stray field.
  • Chiral split constant frequency contours appear in the resonance absorption spectrum.
  • The two properties together supply an experimental signature for identifying A-type altermagnets.
  • The signature can guide development of spin-based logic and information-storage devices.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Device concepts could use the chirality dependence to encode information in the top versus bottom surface response.
  • The same symmetry argument might predict analogous surface-wave features in other altermagnet classes that share the relevant sublattice property.
  • Thin-film or nanostructured samples would be natural platforms for testing because surface effects dominate in reduced dimensions.

Load-bearing premise

The anisotropic surface spin waves with chirality-dependent top-bottom positions and chiral split constant frequency contours arise directly and uniquely from altermagnetic symmetry breaking and are absent in ferromagnets and conventional antiferromagnets.

What would settle it

Observation of the same chirality-dependent top-bottom positions and chiral split constant frequency contours for surface spin waves in a ferromagnet or conventional antiferromagnet would falsify the claim of uniqueness to A-type altermagnets.

Figures

Figures reproduced from arXiv: 2605.14735 by Hai-Zhou Lu, Tao Yu, X. C. Xie, Yiyuan Chen, Zhoujian Sun.

Figure 1
Figure 1. Figure 1: FIG. 1. Schematic illustration of the anisotropy of the sur [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Dispersion of the spin waves in the A-type altermagnet as functions of (a) the [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. (a) Schematic of the experimental setup for measur [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. (a) Schematic of the resonance absorption spec [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
read the original abstract

Altermagnets have attracted intense interest because they have the advantages of both ferromagnets and antiferromagnets. However, their experimental identification remains challenging, in particular for the A-type altermagnets that account for a large group of material candidates. Here, we discover a kind of anisotropic surface spin waves in A-type altermagnets, which is absent in ferromagnets and conventional antiferromagnets. The anisotropic surface spin waves arise directly from the nature of altermagnets, i.e., the spin-opposite sublattices cannot be related by translation or inversion, which breaks the combined spatial-inversion and time-reversal symmetry, leading to the anisotropic surface spin waves with two properties, the chirality-dependent top-bottom positions and chiral split constant frequency contours. We further show that these two properties can be measured experimentally from the stray field and by resonance absorption spectrum, respectively. Our results provide a signature for detecting altermagnets and will inspire spin-based logic and information-storage devices.

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

0 major / 3 minor

Summary. The manuscript claims that A-type altermagnets host anisotropic surface spin waves absent in ferromagnets and conventional antiferromagnets. These waves arise from the breaking of combined PT symmetry because opposite-spin sublattices cannot be related by translation or inversion. The waves exhibit two properties: chirality-dependent top-bottom positions and chiral split constant-frequency contours. The authors propose these can be measured via stray-field imaging and resonance absorption spectra, respectively, providing an experimental signature for A-type altermagnets.

Significance. If the symmetry-based derivation holds, the result supplies a concrete, falsifiable experimental signature for a large class of altermagnetic candidates whose identification remains difficult. The absence of free parameters or fitted quantities in the central symmetry argument is a strength. The work could stimulate both fundamental studies of altermagnetic surface states and applications in spin-based logic.

minor comments (3)
  1. The abstract and introduction would benefit from a one-sentence definition of 'A-type altermagnet' for readers outside the immediate subfield.
  2. Figure captions should explicitly state the material parameters (exchange constants, anisotropy, etc.) used to generate the plotted dispersions and stray-field maps.
  3. A brief comparison table or paragraph contrasting the predicted surface-wave features with those of a conventional antiferromagnet (e.g., MnF2 or NiO) under identical boundary conditions would strengthen the uniqueness claim.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive assessment of our work, the accurate summary of our claims, and the recommendation for minor revision. The referee's evaluation highlights the potential value of the proposed signature for A-type altermagnets. No specific major comments were provided in the report.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper's central derivation rests on a symmetry argument: A-type altermagnets are defined by spin-opposite sublattices that cannot be related by translation or inversion, which breaks combined PT symmetry and produces the stated anisotropic surface spin-wave properties (chirality-dependent positions and split constant-frequency contours). These features are shown to be absent by construction in ferromagnets and conventional antiferromagnets due to their differing symmetries. No equations, parameters, or predictions are shown to reduce to fitted inputs or self-citations; the experimental signatures follow directly from the symmetry-derived properties without self-referential loops. The derivation is therefore self-contained against external symmetry benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the symmetry properties that define A-type altermagnets; no free parameters, new entities, or additional axioms are mentioned in the abstract.

axioms (1)
  • domain assumption Spin-opposite sublattices in A-type altermagnets cannot be related by translation or inversion, breaking combined spatial-inversion and time-reversal symmetry.
    Stated directly in the abstract as the origin of the anisotropic surface spin waves.

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Forward citations

Cited by 1 Pith paper

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Reference graph

Works this paper leans on

120 extracted references · 4 canonical work pages · cited by 1 Pith paper · 1 internal anchor

  1. [1]

    Emerging research landscape of altermagnetism

    L. Šmejkal, J. Sinova, and T. Jungwirth, “Emerging research landscape of altermagnetism”, Phys. Rev. X 12, 040501 (2022)

    2022

  2. [2]

    Beyond con- ventional ferromagnetism and antiferromagnetism: A phasewithnonrelativisticspinandcrystalrotationsym- metry

    L. Šmejkal, J. Sinova, and T. Jungwirth, “Beyond con- ventional ferromagnetism and antiferromagnetism: A phasewithnonrelativisticspinandcrystalrotationsym- metry”, Phys. Rev. X12, 031042 (2022)

    2022

  3. [3]

    Observation of time- reversal symmetry breaking in the band structure of altermagnetic RuO2

    O. Fedchenko, J. Minár, A. Akashdeep, S. W. D’Souza, D. Vasilyev, O. Tkach,et al., “Observation of time- reversal symmetry breaking in the band structure of altermagnetic RuO2”, Sci. Adv.10, eadj4883 (2024)

    2024

  4. [4]

    Unconventional magnons in collinear mag- nets dictated by spin space groups

    X. Chen, Y. Liu, P. Liu, Y. Yu, J. Ren, J. Li, A. Zhang, and Q. Liu, “Unconventional magnons in collinear mag- nets dictated by spin space groups”, Nature640, 349 (2025)

    2025

  5. [5]

    Chiral magnons in altermagnetic RuO2

    L. Šmejkal, A. Marmodoro, K.-H. Ahn, R. González- Hernández, I. Turek, S. Mankovsky,et al., “Chiral magnons in altermagnetic RuO2”, Phys. Rev. Lett.131, 256703 (2023)

    2023

  6. [6]

    Electrical switching of an anti- ferromagnet

    P. Wadley, B. Howells, J. Železn` y, C. Andrews, V. Hills, R. P. Campion,et al., “Electrical switching of an anti- ferromagnet”, Science351, 587 (2016)

    2016

  7. [7]

    Subtera- hertzspinpumpingfromaninsulatingantiferromagnet

    P. Vaidya, S. A. Morley, J. van Tol, Y. Liu, R. Cheng, A. Brataas, D. Lederman, and E. Del Barco, “Subtera- hertzspinpumpingfromaninsulatingantiferromagnet”, Science368, 160 (2020)

    2020

  8. [8]

    A spin-valve-like mag- netoresistance of an antiferromagnet-based tunnel junc- tion

    B. G. Park, J. Wunderlich, X. Martí, V. Hol` y, Y. Kurosaki, M. Yamada,et al., “A spin-valve-like mag- netoresistance of an antiferromagnet-based tunnel junc- tion”, Nat. Mater.10, 347 (2011)

    2011

  9. [9]

    Room-temperature perpendicular exchange couplingandtunnelinganisotropicmagnetoresistancein an antiferromagnet-based tunnel junction

    Y. Y. Wang, C. Song, B. Cui, G. Y. Wang, F. Zeng, and F. Pan, “Room-temperature perpendicular exchange couplingandtunnelinganisotropicmagnetoresistancein an antiferromagnet-based tunnel junction”, Phys. Rev. Lett.109, 137201 (2012)

    2012

  10. [10]

    Room-temperature antiferromagnetic memory resistor

    X. Marti, I. Fina, C. Frontera, J. Liu, P. Wadley, Q. He, et al., “Room-temperature antiferromagnetic memory resistor”, Nat. Mater.13, 367 (2014)

    2014

  11. [11]

    Electrical switching of altermagnetism

    Y. Chen, X. Liu, H.-Z. Lu, and X. Xie, “Electrical switching of altermagnetism”, Phys. Rev. Lett.135, 016701 (2025)

    2025

  12. [12]

    Antiferroelectric altermagnets: An- tiferroelectricity alters magnets

    X. Duan, J. Zhang, Z. Zhu, Y. Liu, Z. Zhang, I. Žu- tić, and T. Zhou, “Antiferroelectric altermagnets: An- tiferroelectricity alters magnets”, Phys. Rev. Lett.134, 106801 (2025)

    2025

  13. [13]

    Ferroelectric switchable alter- magnetism

    M. Gu, Y. Liu, H. Zhu, K. Yananose, X. Chen, Y. Hu, A. Stroppa, and Q. Liu, “Ferroelectric switchable alter- magnetism”, Phys. Rev. Lett.134, 106802 (2025)

    2025

  14. [14]

    Spin-group symmetry in magnetic materials with negligible spin- orbit coupling

    P. Liu, J. Li, J. Han, X. Wan, and Q. Liu, “Spin-group symmetry in magnetic materials with negligible spin- orbit coupling”, Phys. Rev. X12, 021016 (2022)

    2022

  15. [15]

    Spin current generation in organic antiferromagnets

    M. Naka, S. Hayami, H. Kusunose, Y. Yanagi, Y. Mo- tome, and H. Seo, “Spin current generation in organic antiferromagnets”, Nat. Commun.10, 4305 (2019)

    2019

  16. [16]

    anomalous Hall effect inκ-type organic antiferromagnets

    M. Naka, S. Hayami, H. Kusunose, Y. Yanagi, Y. Mo- tome, and H. Seo, “anomalous Hall effect inκ-type organic antiferromagnets”, Phys. Rev. B102, 075112 (2020)

    2020

  17. [17]

    Altermagnetism: Exploring new frontiers in magnetism and spintronics

    L. Bai, W. Feng, S. Liu, L. Šmejkal, Y. Mokrousov, and Y. Yao, “Altermagnetism: Exploring new frontiers in magnetism and spintronics”, Adv. Funct. Mater.34, 2409327 (2024)

    2024

  18. [18]

    Altermagnets as a new class of functional materials

    C. Song, H. Bai, Z. Zhou, L. Han, H. Reichlova, J. H. Dil, J. Liu, X. Chen, and F. Pan, “Altermagnets as a new class of functional materials”, Nat. Rev. Mater.10, 473 (2025)

    2025

  19. [19]

    Altermagnetism: An unconventional spin-ordered phase of matter

    T. Jungwirth, R. M. Fernandes, E. Fradkin, A. H. Mac- Donald, J. Sinova, and L. Šmejkal, “Altermagnetism: An unconventional spin-ordered phase of matter”, New- ton1, 100162 (2025)

    2025

  20. [20]

    Predictable gate-field control of spin in altermagnets with spin-layer coupling

    R.-W. Zhang, C. Cui, R. Li, J. Duan, L. Li, Z.-M. Yu, and Y. Yao, “Predictable gate-field control of spin in altermagnets with spin-layer coupling”, Phys. Rev. Lett. 133, 056401 (2024)

    2024

  21. [21]

    Realizing al- termagnetism in Fermi-Hubbard models with ultracold atoms

    P. Das, V. Leeb, J. Knolle, and M. Knap, “Realizing al- termagnetism in Fermi-Hubbard models with ultracold atoms”, Phys. Rev. Lett.132, 263402 (2024)

    2024

  22. [22]

    Discovery of a metallic room-temperature d-wave al- termagnet KV2Se2O

    B. Jiang, M. Hu, J. Bai, Z. Song, C. Mu, G. Qu,et al., “Discovery of a metallic room-temperature d-wave al- termagnet KV2Se2O”, arXiv:2408.00320 (2024)

    work page arXiv 2024

  23. [23]

    Topologi- cal superconductivity in two-dimensional altermagnetic metals

    D. Zhu, Z.-Y. Zhuang, Z. Wu, and Z. Yan, “Topologi- cal superconductivity in two-dimensional altermagnetic metals”, Phys. Rev. B108, 184505 (2023)

    2023

  24. [24]

    Crystal thermal transport in altermagnetic RuO2

    X. Zhou, W. Feng, R.-W. Zhang, L. Šmejkal, J. Sinova, Y. Mokrousov, and Y. Yao, “Crystal thermal transport in altermagnetic RuO2”, Phys. Rev. Lett.132, 056701 (2024)

    2024

  25. [25]

    Gapless superconducting state and mirage gap in altermagnets

    M. Wei, L. Xiang, F. Xu, L. Zhang, G. Tang, and J. Wang, “Gapless superconducting state and mirage gap in altermagnets”, Phys. Rev. B109, L201404 (2024)

    2024

  26. [26]

    dcJosephson effect in altermagnets

    J.A.Ouassou, A.Brataas, andJ.Linder,“dcJosephson effect in altermagnets”, Phys. Rev. Lett.131, 076003 (2023)

    2023

  27. [27]

    RKKY in- teraction in Rashba altermagnets

    M. Amundsen, A. Brataas, and J. Linder, “RKKY in- teraction in Rashba altermagnets”, Phys. Rev. B110, 054427 (2024)

    2024

  28. [28]

    Spin pumping from a ferromag- netic insulator into an altermagnet

    C. Sun and J. Linder, “Spin pumping from a ferromag- netic insulator into an altermagnet”, Phys. Rev. B108, L140408 (2023)

    2023

  29. [29]

    Skyrmion Hall 6 effect in altermagnets

    Z. Jin, Z. Zeng, Y. Cao, and P. Yan, “Skyrmion Hall 6 effect in altermagnets”, Phys. Rev. Lett.133, 196701 (2024)

    2024

  30. [30]

    Tunable second harmonic in altermagnetic Josephson junctions

    H.-P. Sun, S.-B. Zhang, C.-A. Li, and B. Trauzettel, “Tunable second harmonic in altermagnetic Josephson junctions”, Phys. Rev. B111, 165406 (2025)

    2025

  31. [31]

    Diagnos- ing altermagnetic phases through quantum oscillations

    Z.-X. Li, H. Zhou, X. Wan, and W. Chen, “Diagnos- ing altermagnetic phases through quantum oscillations”, Phys. Rev. B111, 125119 (2025)

    2025

  32. [32]

    Anoma- lous Hall effects in magnetic weak topological insulator films

    R. Chen, X.-X. Yi, B. Zhou, and D.-H. Xu, “Anoma- lous Hall effects in magnetic weak topological insulator films”, Phys. Rev. B111, 045409 (2025)

    2025

  33. [33]

    Distin- guishing between topological Majorana and trivial zero modes via transport and shot noise study in an alter- magnet heterostructure

    D. Mondal, A. Pal, A. Saha, and T. Nag, “Distin- guishing between topological Majorana and trivial zero modes via transport and shot noise study in an alter- magnet heterostructure”, Phys. Rev. B111, L121401 (2025)

    2025

  34. [34]

    Giant and tunneling magnetoresistance in unconventional collinear antiferro- magnets with nonrelativistic spin-momentum coupling

    L. Šmejkal, A. B. Hellenes, R. González-Hernández, J. Sinova, and T. Jungwirth, “Giant and tunneling magnetoresistance in unconventional collinear antiferro- magnets with nonrelativistic spin-momentum coupling”, Phys. Rev. X12, 011028 (2022)

    2022

  35. [35]

    Spin-neutral currents for spintronics

    D.-F. Shao, S.-H. Zhang, M. Li, C.-B. Eom, and E. Y. Tsymbal, “Spin-neutral currents for spintronics”, Nat. Commun.12, 7061 (2021)

    2021

  36. [36]

    Multifunctional antiferromagnetic mate- rials with giant piezomagnetism and noncollinear spin current

    H.-Y. Ma, M. Hu, N. Li, J. Liu, W. Yao, J.-F. Jia, and J. Liu, “Multifunctional antiferromagnetic mate- rials with giant piezomagnetism and noncollinear spin current”, Nat. Commun.12, 2846 (2021)

    2021

  37. [37]

    Efficient electrical spin splitter based on nonrelativis- tic collinear antiferromagnetism

    R.González-Hernández, L.Šmejkal, K.Výborný, Y.Ya- hagi, J. Sinova, T. c. v. Jungwirth, and J. Železný, “Efficient electrical spin splitter based on nonrelativis- tic collinear antiferromagnetism”, Phys. Rev. Lett.126, 127701 (2021)

    2021

  38. [38]

    Tilted spin current generated by the collinear antiferromagnet ruthenium dioxide

    A. Bose, N. J. Schreiber, R. Jain, D.-F. Shao, H. P. Nair, J. Sun,et al., “Tilted spin current generated by the collinear antiferromagnet ruthenium dioxide”, Nat. Electron.5, 267 (2022)

    2022

  39. [39]

    Finite- momentum Cooper pairing in proximitized altermag- nets

    S.-B. Zhang, L.-H. Hu, and T. Neupert, “Finite- momentum Cooper pairing in proximitized altermag- nets”, Nat. Commun.15, 1801 (2024)

    2024

  40. [40]

    Fulde-ferrell-larkin- ovchinnikov state induced by antiferromagnetic order in κ-type organic conductors

    S. Sumita, M. Naka, and H. Seo, “Fulde-ferrell-larkin- ovchinnikov state induced by antiferromagnetic order in κ-type organic conductors”, Phys. Rev. Res.5, 043171 (2023)

    2023

  41. [41]

    Zero-field finite-momentum and field-induced superconductivity in altermagnets

    D. Chakraborty and A. M. Black-Schaffer, “Zero-field finite-momentum and field-induced superconductivity in altermagnets”, Phys. Rev. B110, L060508 (2024)

    2024

  42. [42]

    Unconventional p-waveandfinite-momentumsuperconductivityinduced by altermagnetism through the formation of Bogoliubov Fermi surface

    S. Hong, M. J. Park, and K.-M. Kim, “Unconventional p-waveandfinite-momentumsuperconductivityinduced by altermagnetism through the formation of Bogoliubov Fermi surface”, Phys. Rev. B111, 054501 (2025)

    2025

  43. [43]

    Pair density waves and super- current diode effect in altermagnets

    G. Sim and J. Knolle, “Pair density waves and super- current diode effect in altermagnets”, Phys. Rev. B112, L020502 (2025)

    2025

  44. [44]

    Coulomb drag in altermagnets

    H.-J. Lin, S.-B. Zhang, H.-Z. Lu, and X. C. Xie, “Coulomb drag in altermagnets”, Phys. Rev. Lett.134, 136301 (2025)

    2025

  45. [45]

    Altermagnetic lifting of Kramers spin degeneracy

    J. Krempask` y, L. Šmejkal, S. D’souza, M. Hajlaoui, G. Springholz, K. Uhlířová,et al., “Altermagnetic lifting of Kramers spin degeneracy”, Nature626, 517 (2024)

    2024

  46. [46]

    Observation of a giant band splitting in altermagnetic MnTe

    T. Osumi, S. Souma, T. Aoyama, K. Yamauchi, A. Honma, K. Nakayama, T. Takahashi, K. Ohgushi, and T. Sato, “Observation of a giant band splitting in altermagnetic MnTe”, Phys. Rev. B109, 115102 (2024)

    2024

  47. [47]

    Broken Kramers degeneracy in altermagnetic MnTe

    S. Lee, S. Lee, S. Jung, J. Jung, D. Kim, Y. Lee,et al., “Broken Kramers degeneracy in altermagnetic MnTe”, Phys. Rev. Lett.132, 036702 (2024)

    2024

  48. [48]

    Observation of plaid-like spin splitting in a non- coplanar antiferromagnet

    Y.-P. Zhu, X. Chen, X.-R. Liu, Y. Liu, P. Liu, H. Zha, et al., “Observation of plaid-like spin splitting in a non- coplanar antiferromagnet”, Nature626, 523 (2024)

    2024

  49. [49]

    Observation of spin splitting in room- temperature metallic antiferromagnet CrSb

    M. Zeng, M.-Y. Zhu, Y.-P. Zhu, X.-R. Liu, X.-M. Ma, Y.-J. Hao,et al., “Observation of spin splitting in room- temperature metallic antiferromagnet CrSb”, Adv. Sci. 11, 2406529 (2024)

    2024

  50. [50]

    Three-dimensional mapping of the altermagnetic spin splitting in CrSb

    G. Yang, Z. Li, S. Yang, J. Li, H. Zheng, W. Zhu,et al., “Three-dimensional mapping of the altermagnetic spin splitting in CrSb”, Nat. Commun.16, 1442 (2025)

    2025

  51. [51]

    Large band splitting ing-wave altermagnet CrSb

    J. Ding, Z. Jiang, X. Chen, Z. Tao, Z. Liu, T. Li,et al., “Large band splitting ing-wave altermagnet CrSb”, Phys. Rev. Lett.133, 206401 (2024)

    2024

  52. [52]

    Topological weyl altermagnetism in CrSb

    C. Li, M. Hu, Z. Li, Y. Wang, W. Chen, B. Thiagara- jan,et al., “Topological weyl altermagnetism in CrSb”, Commun. Phys.8, 311 (2025)

    2025

  53. [53]

    Crystal-symmetry-paired spin–valley locking in a layered room-temperature metallic altermagnet can- didate

    F. Zhang, X. Cheng, Z. Yin, C. Liu, L. Deng, Y. Qiao, et al., “Crystal-symmetry-paired spin–valley locking in a layered room-temperature metallic altermagnet can- didate”, Nat. Phys.21, 760 (2025)

    2025

  54. [54]

    A metallic room-temperature d-wave altermag- net

    B. Jiang, M. Hu, J. Bai, Z. Song, C. Mu, G. Qu, et al., “A metallic room-temperature d-wave altermag- net”, Nat. Phys.21, 754 (2025)

    2025

  55. [55]

    Nanoscale imaging and control of altermagnetism in MnTe

    O. Amin, A. Dal Din, E. Golias, Y. Niu, A. Zakharov, S. Fromage,et al., “Nanoscale imaging and control of altermagnetism in MnTe”, Nature636, 348 (2024)

    2024

  56. [56]

    X-ray magnetic circular dichroism in altermagneticα-MnTe

    A. Hariki, A. Dal Din, O. Amin, T. Yamaguchi, A. Badura, D. Kriegner,et al., “X-ray magnetic circular dichroism in altermagneticα-MnTe”, Phys. Rev. Lett. 132, 176701 (2024)

    2024

  57. [57]

    Revealing the altermagnetism in hematite via XMCD imaging and anomalous Hall electrical transport

    E. Galindez-Ruales, R. Gonzalez-Hernandez, C. Schmitt, S. Das, F. Fuhrmann, A. Ross,et al., “Revealing the altermagnetism in hematite via XMCD imaging and anomalous Hall electrical transport”, Adv. Mater.37, e05019 (2025)

    2025

  58. [58]

    Large anisotropic x-ray magnetic circular dichroism in altermagnetic CrSb with collinear antiferromagnetic structure at room tempera- ture

    W. Li, W. Li, M. Zou, Y. Yin, H. Li, G. Qu, Y. Huang, R. Yu, H. Yang, and B. Wang, “Large anisotropic x-ray magnetic circular dichroism in altermagnetic CrSb with collinear antiferromagnetic structure at room tempera- ture”, Phys. Rev. B111, 224417 (2025)

    2025

  59. [59]

    Altermagnetic nanotextures revealed in bulk MnTe

    R. Yamamoto, L. A. Turnbull, M. Schmidt, J. C. Cor- saletti Filho, H. J. Binger, M. Di Pietro Martínez,et al., “Altermagnetic nanotextures revealed in bulk MnTe”, Phys. Rev. Appl.24, 034037 (2025)

    2025

  60. [60]

    An anomalous Hall effect in altermagnetic ruthe- nium dioxide

    Z. Feng, X. Zhou, L. Šmejkal, L. Wu, Z. Zhu, H. Guo, et al., “An anomalous Hall effect in altermagnetic ruthe- nium dioxide”, Nat. Electron.5, 735 (2022)

    2022

  61. [61]

    Spontaneous anomalous Hall effect arising from an unconventional compensated magnetic phase in a semiconductor

    R. D. Gonzalez Betancourt, J. Zubáč, R. Gonzalez- Hernandez, K. Geishendorf, Z. Šobáň, G. Springholz, et al., “Spontaneous anomalous Hall effect arising from an unconventional compensated magnetic phase in a semiconductor”, Phys. Rev. Lett.130, 036702 (2023)

    2023

  62. [62]

    Quantum geometry induced nonlinear transport in altermagnets

    Y. Fang, J. Cano, and S. A. A. Ghorashi, “Quantum geometry induced nonlinear transport in altermagnets”, Phys. Rev. Lett.133, 106701 (2024)

    2024

  63. [63]

    Intrinsic anomalous Hall effect in altermagnets

    L. Attias, A. Levchenko, and M. Khodas, “Intrinsic anomalous Hall effect in altermagnets”, Phys. Rev. B 110, 094425 (2024)

    2024

  64. [64]

    Saturation of the anomalous Hall effect at high magnetic fields in 7 altermagnetic RuO2

    T. Tschirner, P. Keßler, R. D. Gonzalez Betancourt, T. Kotte, D. Kriegner, B. Büchner,et al., “Saturation of the anomalous Hall effect at high magnetic fields in 7 altermagnetic RuO2”, APL Mater.11, 101103 (2023)

    2023

  65. [65]

    Coexistence of anomalousHalleffectandweakmagnetizationinanom- inally collinear antiferromagnet MnTe

    K. P. Kluczyk, K. Gas, M. J. Grzybowski, P. Skupiński, M. A. Borysiewicz, T. Fąs,et al., “Coexistence of anomalousHalleffectandweakmagnetizationinanom- inally collinear antiferromagnet MnTe”, Phys. Rev. B 110, 155201 (2024)

    2024

  66. [66]

    Observation ofa spontaneousanomalous Hall response inthe Mn5Si3 d-wave altermagnet candidate

    H. Reichlova, R. Lopes Seeger, R. González-Hernández, I. Kounta, R. Schlitz, D. Kriegner,et al., “Observation ofa spontaneousanomalous Hall response inthe Mn5Si3 d-wave altermagnet candidate”, Nat. Commun.15, 4961 (2024)

    2024

  67. [67]

    Anisotropic magnetoresistance in altermagnetic MnTe

    R. D. Gonzalez Betancourt, J. Zubáč, K. Geishendorf, P.Ritzinger, B.Růžičková, T.Kotte,et al.,“Anisotropic magnetoresistance in altermagnetic MnTe”, npj Spin- tronics2, 45 (2024)

    2024

  68. [68]

    Observation of the anoma- lous Nernst effect in altermagnetic candidate Mn5Si3

    A.Badura, W.H.Campos, V.K.Bharadwaj, I.Kounta, L. Michez, M. Petit,et al., “Observation of the anoma- lous Nernst effect in altermagnetic candidate Mn5Si3”, Nat. Commun.16, 7111 (2025)

    2025

  69. [69]

    Third-order nonlinear Hall effect in alter- magnet RuO2

    R. Y. Chu, L. Han, Z. H. Gong, X. Z. Fu, H. Bai, S. X. Liang,et al., “Third-order nonlinear Hall effect in alter- magnet RuO2”, Phys. Rev. Lett.135, 216703 (2025)

    2025

  70. [70]

    Separation of inverse altermagnetic spin- splitting effect from inverse spin Hall effect in RuO2

    C.-T. Liao, Y.-C. Wang, Y.-C. Tien, S.-Y. Huang, and D. Qu, “Separation of inverse altermagnetic spin- splitting effect from inverse spin Hall effect in RuO2”, Phys. Rev. Lett.133, 056701 (2024)

    2024

  71. [71]

    Efficient spin-to-charge conversion via altermagnetic spin splitting effect in antiferromagnet RuO2

    H. Bai, Y. C. Zhang, Y. J. Zhou, P. Chen, C. H. Wan, L. Han,et al., “Efficient spin-to-charge conversion via altermagnetic spin splitting effect in antiferromagnet RuO2”, Phys. Rev. Lett.130, 216701 (2023)

    2023

  72. [72]

    Altermagnet-driven magnon spin split- ting Nernst effect

    Y. Yang, D. Wang, B. Yang, P. Wang, Y. Mu, Y. Tian,et al., “Altermagnet-driven magnon spin split- ting Nernst effect”, Phys. Rev. Lett.136, 026701 (2026)

    2026

  73. [73]

    Chi- ral split magnon in altermagnetic MnTe

    Z. Liu, M. Ozeki, S. Asai, S. Itoh, and T. Masuda, “Chi- ral split magnon in altermagnetic MnTe”, Phys. Rev. Lett.133, 156702 (2024)

    2024

  74. [74]

    Observation of chiral magnon band split- ting in altermagnetic Hematite

    Q. Sun, J. Guo, D. Wang, D. L. Abernathy, W. Tian, and C. Li, “Observation of chiral magnon band split- ting in altermagnetic Hematite”, Phys. Rev. Lett.135, 186703 (2025)

    2025

  75. [75]

    Coherent high-velocity chiral magnons in the metallic altermagnet CrSb

    A. K. Singh, N. Heinsdorf, A. A. Mancilla, J. Ban- nies, A. Maity, A. I. Kolesnikov,et al., “Chiral spin-split magnons in the metallic altermagnet CrSb”, arXiv:2511.16086 (2025)

    work page internal anchor Pith review Pith/arXiv arXiv 2025

  76. [76]

    Systematic mapping of altermagnetic magnons by resonant inelas- tic x-ray circular dichroism

    N. Biniskos, M. dos Santos Dias, S. Agrestini, D. Sviták, K.-J. Zhou, J. Pospíšil, and P. Čermák, “Systematic mapping of altermagnetic magnons by resonant inelas- tic x-ray circular dichroism”, Nat. Commun.16, 9311 (2025)

    2025

  77. [77]

    Circular dichroism inresonantinelasticx-rayscattering: Probingaltermag- netic domains in MnTe

    D. Takegami, T. Aoyama, T. Okauchi, T. Yamaguchi, S. Tippireddy, S. Agrestini,et al., “Circular dichroism inresonantinelasticx-rayscattering: Probingaltermag- netic domains in MnTe”, Phys. Rev. Lett.135, 196502 (2025)

    2025

  78. [78]

    General stacking theory for altermagnetism in bilayer systems

    B. Pan, P. Zhou, P. Lyu, H. Xiao, X. Yang, and L. Sun, “General stacking theory for altermagnetism in bilayer systems”, Phys. Rev. Lett.133, 166701 (2024)

    2024

  79. [79]

    Non-relativistic spin splitting above and below the Fermi level in a g-wave altermagnet

    N. Dale, O. A. Ashour, M. Vila, R. B. Regmi, J. Fox, C. W. Johnson, A. Fedorov, A. Stibor, N. J. Ghimire, and S. M. Griffin, “Non-relativistic spin splitting above and below the Fermi level in a g-wave altermagnet”, arXiv:2411.18761 (2024)

    work page arXiv 2024

  80. [80]

    Electronic structure of a layered altermagnetic compound CoNb4Se8

    A. P. Sakhya, M. I. Mondal, M. Sprague, R. B. Regmi, A. K. Kumay, H. Sheokand, I. Mazin, N. J. Ghimire, M. Neupane,et al., “Electronic structure of a layered altermagnetic compound CoNb4Se8”, arXiv:2503.16670 (2025)

    work page arXiv 2025

Showing first 80 references.