Coherent high-velocity chiral magnons in the metallic altermagnet CrSb
Pith reviewed 2026-05-17 21:14 UTC · model grok-4.3
The pith
Metallic altermagnet CrSb displays chiral spin splitting in its magnon spectrum along the Γ-L direction.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
CrSb is a perfectly compensated Ising altermagnet below 733 K. Polarized neutron diffraction confirms the magnetic structure, while inelastic scattering maps out coherent, highly dispersive magnons with velocities of 61 km/s in-plane and 58 km/s out-of-plane. The dispersions along high-symmetry lines are reproduced by a minimal model with J1 = 23 meV (AFM), J2 = -5.4 meV (FM), J3 = 5.2 meV (AFM), and D = 0.15 meV. Along the Γ-L line, distinct signatures of chiral spin splitting appear, arising from higher-order altermagnetic exchange and constituting the first such report in a metallic altermagnet.
What carries the argument
higher-order altermagnetic exchange interactions producing chiral spin splitting in the magnon dispersion along the Γ-L direction
If this is right
- Coherent magnons with large velocities exist well above room temperature in this metallic altermagnet.
- The material provides a platform for spintronic applications based on spin-split magnons.
- The minimal Heisenberg model with third-neighbor alternating interactions describes the observed dispersions along high-symmetry directions.
- Chiral splitting is a direct consequence of the altermagnetic order in this system.
Where Pith is reading between the lines
- The high magnon velocities could support fast information transfer in magnonic devices without requiring external fields due to the compensated nature.
- Similar chiral effects may appear in other metallic altermagnets once low-symmetry paths are probed with inelastic scattering.
Load-bearing premise
That the magnon dispersions are fully and accurately described by the minimal third-nearest-neighbor Heisenberg model with alternating signs and small Ising anisotropy without needing itinerant electron effects or higher-order terms.
What would settle it
A calculation or measurement that shows the observed splitting along Γ-L can be reproduced without invoking higher-order altermagnetic exchange, or that the high-symmetry dispersions require additional interaction terms beyond the proposed minimal model.
Figures
read the original abstract
We report the collective magnetism of the metallic altermagnet CrSb. Magnetic susceptibility and polarized neutron diffraction measurements show that CrSb is a perfectly compensated Ising altermagnet below a N\'eel temperature of $T_N = 733(4)$ K. Inelastic neutron scattering experiments reveal coherent and highly-dispersive antiferromagnetic spin waves with large group velocities of 61(2) km s$^{-1}$ and 58(2) km s$^{-1}$ along the in-plane and out-of-plane directions, respectively. The observed magnon dispersions along high-symmetry directions of the Brillouin zone are well described by a minimal Heisenberg model up to third nearest neighbors of alternating antiferromagnetic and ferromagnetic character, $J_1 = 23(4)$ meV, $J_2 = -5.4(8)$ meV, $J_3 = 5.2(8)$ meV, and an Ising single-ion anisotropy term $D = 0.15(4)$ meV. We observe clear momentum space signatures of chiral spin splitting along the low-symmetry $\Gamma$-$L$ direction, characteristic of higher-order altermagnetic exchange interactions, the first such observation in a metallic altermagnet. These findings identify CrSb as a singular material: a metallic altermagnet in which coherent spin-split magnons persist well above room temperature, providing a compelling platform for spintronic applications.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports that CrSb is a perfectly compensated Ising altermagnet with TN = 733(4) K, confirmed via magnetic susceptibility and polarized neutron diffraction. Inelastic neutron scattering shows coherent, highly dispersive antiferromagnetic magnons with group velocities of 61(2) km s^{-1} (in-plane) and 58(2) km s^{-1} (out-of-plane). These dispersions along high-symmetry Brillouin zone directions are fitted to a minimal Heisenberg model limited to third-nearest-neighbor interactions of alternating sign (J1 = 23(4) meV, J2 = -5.4(8) meV, J3 = 5.2(8) meV) plus a small Ising anisotropy D = 0.15(4) meV. Clear momentum-space signatures of chiral spin splitting are observed along the low-symmetry Γ-L direction and attributed to higher-order altermagnetic exchange interactions, presented as the first such observation in a metallic altermagnet.
Significance. If the experimental observations and model interpretation hold, the work identifies CrSb as a metallic altermagnet supporting coherent, high-velocity spin-split magnons well above room temperature, which would provide a compelling platform for spintronic applications. Credit is due for the use of complementary techniques (susceptibility, polarized neutron diffraction, and inelastic scattering) that together support the compensated altermagnetic order and the reported magnon dispersions. The direct experimental identification of chiral splitting along Γ-L is a notable result.
major comments (2)
- [Abstract and inelastic neutron scattering results] Abstract and the inelastic neutron scattering section: The claim that high-symmetry dispersions are 'well described' by the minimal local-moment Heisenberg model with the listed J1, J2, J3, and D values is load-bearing for attributing the observed Γ-L chiral splitting solely to higher-order altermagnetic exchange. In a metallic system such as CrSb, the manuscript does not discuss or rule out possible itinerant-electron renormalization, Stoner excitations, or Landau damping that could modify effective exchanges or broaden modes, potentially affecting both the velocity values and the assignment of the splitting.
- [Abstract] Abstract: The fitted parameters are reported with uncertainties (e.g., J1 = 23(4) meV), but no details are provided on the fitting procedure, χ² values, number of data points, or tests of alternative models that include longer-range or conduction-electron-mediated terms. This omission weakens the justification for the minimal model as uniquely appropriate.
minor comments (2)
- [Abstract] The abstract states velocities with errors but does not specify how these uncertainties were propagated from the dispersion fits or from the instrument resolution.
- [Introduction] A brief comparison in the introduction or discussion to prior chiral magnon observations in insulating altermagnets would help contextualize the novelty of the metallic case.
Simulated Author's Rebuttal
We thank the referee for their careful reading of our manuscript and for the constructive comments, which highlight important considerations for metallic altermagnets. We address each major comment in turn below, providing the strongest honest defense of our results while committing to revisions where appropriate to strengthen the presentation.
read point-by-point responses
-
Referee: [Abstract and inelastic neutron scattering results] Abstract and the inelastic neutron scattering section: The claim that high-symmetry dispersions are 'well described' by the minimal local-moment Heisenberg model with the listed J1, J2, J3, and D values is load-bearing for attributing the observed Γ-L chiral splitting solely to higher-order altermagnetic exchange. In a metallic system such as CrSb, the manuscript does not discuss or rule out possible itinerant-electron renormalization, Stoner excitations, or Landau damping that could modify effective exchanges or broaden modes, potentially affecting both the velocity values and the assignment of the splitting.
Authors: The referee correctly notes that itinerant effects merit discussion in a metallic system. However, the inelastic neutron scattering data show sharp, coherent magnon branches with large group velocities (61 and 58 km/s) that remain well-defined over a wide energy range and up to high temperatures, with no evidence of significant broadening that would signal strong Landau damping or Stoner continuum overlap. This coherence, together with the perfectly compensated order confirmed by polarized neutron diffraction and the high TN = 733 K, supports the applicability of a local-moment Heisenberg description as a leading-order model for the high-symmetry dispersions. The chiral splitting along Γ-L is an experimental observation tied to the altermagnetic symmetry breaking and is not derived from the minimal model itself. In the revised manuscript we will add a concise discussion paragraph in the inelastic neutron scattering section explicitly addressing why itinerant renormalization is expected to be weak in CrSb, citing the mode sharpness and the success of the minimal fit. revision: yes
-
Referee: [Abstract] Abstract: The fitted parameters are reported with uncertainties (e.g., J1 = 23(4) meV), but no details are provided on the fitting procedure, χ² values, number of data points, or tests of alternative models that include longer-range or conduction-electron-mediated terms. This omission weakens the justification for the minimal model as uniquely appropriate.
Authors: We agree that additional information on the fitting procedure would improve transparency. The quoted parameters and uncertainties were obtained via least-squares fitting of the minimal Heisenberg model (J1, J2, J3, D) to the measured magnon dispersion points along multiple high-symmetry lines. In the revised manuscript we will include a brief description of the fitting protocol, the number of independent data points used, the resulting χ² per degree of freedom, and a short comparison demonstrating that extending the model with fourth-neighbor or conduction-electron-mediated terms yields no statistically significant improvement. These details will be placed in the main text or a supplementary note so that readers can assess the justification for the minimal model. revision: yes
Circularity Check
No significant circularity; results grounded in direct experimental data
full rationale
The paper reports experimental observations from magnetic susceptibility, polarized neutron diffraction, and inelastic neutron scattering. High-symmetry magnon dispersions are characterized by fitting a minimal Heisenberg model (J1, J2, J3, D), but this is a standard post-measurement parameterization rather than a derivation that reduces any claimed result to the fit by construction. The chiral spin splitting along the low-symmetry Γ-L direction is presented as a separate experimental signature attributed to higher-order altermagnetic interactions, without equations that define the splitting in terms of the fitted parameters or prior self-citations. No self-definitional loops, fitted inputs renamed as predictions, or load-bearing self-citations appear in the provided text. The derivation chain remains self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
free parameters (4)
- J1 =
23(4) meV
- J2 =
-5.4(8) meV
- J3 =
5.2(8) meV
- D =
0.15(4) meV
axioms (1)
- domain assumption Magnon dispersions in CrSb are described by a minimal Heisenberg model with interactions up to third nearest neighbors plus single-ion anisotropy
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The observed magnon dispersions along high-symmetry directions of the Brillouin zone are well described by a minimal Heisenberg model up to third nearest neighbors of alternating antiferromagnetic and ferromagnetic character, J1 = 23(4) meV, J2 = −5.4(8) meV, J3 = 5.2(8) meV, and an Ising single-ion anisotropy term D = 0.15(4) meV.
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.
Forward citations
Cited by 1 Pith paper
-
Band splitting in altermagnet CrSb
Magnetic groups formalism applied to CrSb reveals additional momentum-dependent spin splitting in electron bands beyond the exchange approximation of spin groups theory.
Reference graph
Works this paper leans on
-
[1]
2.Determination of the spin Hamiltonian of CrSb from inelastic neutron scattering
or Pz ∥(1-10) depending on the scattering plane, and 3 FIG. 2.Determination of the spin Hamiltonian of CrSb from inelastic neutron scattering. (a)Brillouin zone of CrSb with indicated high-symmetry directions.(b)INS spectrum of CrSb measured at 5 K around the (101) Bragg position with an incident neutron energyEi = 50 meV, revealing a magnon gap of 13(2) ...
-
[2]
L. Šmejkal, J. Sinova, and T. Jungwirth, Beyond conven- tional ferromagnetism and antiferromagnetism: A phase with nonrelativistic spin and crystal rotation symmetry, Phys. Rev. X12, 031042 (2022)
work page 2022
-
[3]
K.-H. Ahn, A. Hariki, K.-W. Lee, and J. Kuneš, Antifer- romagnetism in RuO2 as d-wave Pomeranchuk instability, Phys. Rev. B99, 184432 (2019)
work page 2019
- [4]
-
[5]
L. Šmejkal, R. González-Hernández, T. Jungwirth, and J. Sinova, Crystal time-reversal symmetry breaking and spontaneous Hall effect in collinear antiferromagnets, Sci. Adv.6, eaaz8809 (2020)
work page 2020
- [6]
-
[7]
H.-Y. Ma, M. Hu, N. Li, J. Liu, W. Yao, J.-F. Jia, and J. Liu, Multifunctional antiferromagnetic materials with giant piezomagnetism and noncollinear spin current, Nat. Commun.12, 2846 (2021)
work page 2021
-
[8]
M. Naka, Y. Motome, and H. Seo, Perovskite as a spin current generator, Phys. Rev. B103, 125114 (2021)
work page 2021
-
[9]
L. Šmejkal, J. Sinova, and T. Jungwirth, Emerging re- search landscape of altermagnetism, Phys. Rev. X12, 040501 (2022)
work page 2022
-
[10]
J. R. Hortensius, D. Afanasiev, M. Matthiesen, R. Leen- ders, R. Citro, A. V. Kimel, R. V. Mikhaylovskiy, B. A. Ivanov, and A. D. Caviglia, Coherent spin-wave transport in an antiferromagnet, Nat. Phys.17, 1001 (2021)
work page 2021
-
[11]
L. Šmejkal, A. B. Hellenes, R. González-Hernández, J. Sinova, and T. Jungwirth, Giant and tunneling magne- toresistance in unconventional collinear antiferromagnets with nonrelativistic spin-momentum coupling, Phys. Rev. X12, 011028 (2022)
work page 2022
-
[12]
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)
work page 2019
-
[13]
D.-F. Shao, S.-H. Zhang, M. Li, C.-B. Eom, and E. Y. Tsymbal, Spin-neutral currents for spintronics, Nat. Com- mun.12, 7061 (2021)
work page 2021
-
[14]
K. Sourounis and A. Manchon, Efficient generation of spin currents in altermagnets via magnon drag, Phys. Rev. B 111, 134448 (2025)
work page 2025
- [15]
-
[16]
K. Monkman, J. Weng, N. Heinsdorf, A. Nocera, and M. Franz, Persistent spin currents in superconducting altermagnets, arXiv:2507.22139 (2025)
-
[17]
Proximitizing altermagnets with conventional superconductors,
N. Heinsdorf and M. Franz, Proximitizing altermag- nets with conventional superconductors, arXiv:2509.03774 (2025)
-
[18]
Y. Fang, J. Cano, and S. A. A. Ghorashi, Quantum geom- etry induced nonlinear transport in altermagnets, Phys. Rev. Lett.133, 106701 (2024)
work page 2024
-
[19]
M. Ezawa, Intrinsic nonlinear conductivity induced by quantum geometry in altermagnets and measurement of the in-plane néel vector, Phys. Rev. B110, L241405 (2024)
work page 2024
-
[20]
P. A. McClarty and J. G. Rau, Landau theory of alter- magnetism, Phys. Rev. Lett.132, 176702 (2024)
work page 2024
-
[21]
Heinsdorf, Altermagnetic instabilities from quantum geometry, Phys
N. Heinsdorf, Altermagnetic instabilities from quantum geometry, Phys. Rev. B111, 174407 (2025)
work page 2025
-
[22]
H. Yu, J. Xiao, and H. Schultheiss, Magnetic texture based magnonics, Phys. Rep.905, 1 (2021)
work page 2021
- [23]
-
[24]
O. Gomonay, V. Kravchuk, R. Jaeschke-Ubiergo, K. Yer- shov, T. Jungwirth, L. Šmejkal, J. van den Brink, and J. Sinova, Structure, control, and dynamics of altermag- netic textures, npj Spintronics2, 35 (2024)
work page 2024
- [25]
-
[26]
S. Lee, S. Lee, S. Jung, J. Jung, D. Kim, Y. Lee, B. Seok, J. Kim, B. G. Park, L. Šmejkal,et al., Broken Kramers degeneracy in altermagnetic MnTe, Phys. Rev. Lett.132, 036702 (2024)
work page 2024
-
[27]
J. Krempask` y, L. Šmejkal, S. D’souza, M. Hajlaoui, G. Springholz, K. Uhlířová, F. Alarab, P. Constantinou, V. Strocov, D. Usanov,et al., Altermagnetic lifting of Kramers spin degeneracy, Nature626, 517 (2024)
work page 2024
- [28]
-
[29]
S. Reimers, L. Odenbreit, L. Šmejkal, V. N. Strocov, P. Constantinou, A. B. Hellenes, R. Jaeschke Ubiergo, W. H. Campos, V. K. Bharadwaj, A. Chakraborty,et al., Direct observation of altermagnetic band splitting in CrSb thin films, Nat. Commun.15, 2116 (2024)
work page 2024
-
[30]
G. Yang, Z. Li, S. Yang, J. Li, H. Zheng, W. Zhu, Z. Pan, Y. Xu, S. Cao, W. Zhao,et al., Three-dimensional map- ping of the altermagnetic spin splitting in CrSb, Nat. Commun.16, 1442 (2025)
work page 2025
- [31]
- [32]
-
[33]
Z. Liu, M. Ozeki, S. Asai, S. Itoh, and T. Masuda, Chiral split magnon in altermagnetic MnTe, Phys. Rev. Lett. 133, 156702 (2024)
work page 2024
-
[34]
Q. Sun, J. Guo, D. Wang, D. L. Abernathy, W. Tian, and C. Li, Observation of chiral magnon band splitting in altermagnetic hematite, Phys. Rev. Lett.135, 186703 (2025)
work page 2025
-
[35]
W. Szuszkiewicz, E. Dynowska, B. Witkowska, and B. Hennion, Spin-wave measurements on hexagonal MnTe of NiAs-type structure by inelastic neutron scattering, Phys. Rev. B73, 104403 (2006)
work page 2006
-
[36]
V. C. Morano, Z. Maesen, S. E. Nikitin, J. Lass, D. G. Mazzone, and O. Zaharko, Absence of altermagnetic 7 magnon band splitting in MnF2, Phys. Rev. Lett.134, 226702 (2025)
work page 2025
- [37]
-
[38]
G. Poelchen, J. Hellwig, M. Peters, D. Y. Usachov, K. Kliemt, C. Laubschat, P. M. Echenique, E. V. Chulkov, C. Krellner, S. S. P. Parkin, D. V. Vyalikh, A. Ernst, and K. Kummer, Long-lived spin waves in a metallic antifer- romagnet, Nat. Commun.14, 5422 (2023)
work page 2023
-
[39]
B. Rai, K. Patra, S. Bera, S. Kalimuddin, K. Deb, M. Mon- dal, P. Mahadevan, and N. Kumar, Direction-dependent conduction polarity in altermagnetic CrSb, Advanced Sci- ence , 2502226 (2025)
work page 2025
-
[40]
W. J. Takei, D. E. Cox, and G. Shirane, Magnetic struc- tures in CrTe-CrSb solid solutions, J. App. Phys.37, 973 (1966)
work page 1966
-
[41]
J. Yuan, Y. Song, X. Xing, and J. Chen, Magnetic struc- ture and uniaxial negative thermal expansion in antifer- romagnetic CrSb, Dalton Trans.49, 17605 (2020)
work page 2020
-
[42]
A. I. Snow, Neutron diffraction investigation of the atomic magnetic moment orientation in the antiferromagnetic compound CrSb, Phys. Rev.85, 365 (1952)
work page 1952
-
[43]
G. E. Granroth, A. I. Kolesnikov, T. E. Sherline, J. P. Clancy, K. A. Ross, J. P. C. Ruff, B. D. Gaulin, and S. E. Nagler, SEQUOIA: A newly operating chopper spectrometer at the SNS, J. Phys. Conf. Ser251, 012058 (2010)
work page 2010
-
[44]
P. Radhakrishna and J. W. Cable, Inelastic-neutron- scattering studies of spin-wave excitations in the pnictides MnSb and CrSb, Phys. Rev. B54, 11940 (1996)
work page 1996
-
[45]
Fawcett, Spin-density-wave antiferromagnetism in chromium, Rev
E. Fawcett, Spin-density-wave antiferromagnetism in chromium, Rev. Mod. Phys.60, 209 (1988)
work page 1988
-
[46]
H. Wang, R. Yuan, Y. Zhou, Y. Zhang, J. Chen, S. Liu, H. Jia, D. Yu, J.-P. Ansermet, C. Song, and H. Yu, Long- distance coherent propagation of high-velocity antiferro- magnetic spin waves, Phys. Rev. Lett.130, 096701 (2023)
work page 2023
-
[47]
S. Toth and B. Lake, Linear spin wave theory for single-q incommensurate magnetic structures, J. Phys: Condens Matter27, 166002 (2015)
work page 2015
-
[48]
Y.-F. Zhang, X.-S. Ni, K. Chen, and K. Cao, Chiral magnon splitting in altermagnetic CrSb from first princi- ples, Phys. Rev. B111, 174451 (2025)
work page 2025
-
[49]
V. P. Kravchuk, K. V. Yershov, J. I. Facio, Y. Guo, O. Janson, O. Gomonay, J. Sinova, and J. van den Brink, Chiral magnetic excitations and domain textures ofg- wave altermagnets, Phys. Rev. B112, 144421 (2025)
work page 2025
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.