Recognition: unknown
Winding feature and thermal evolution of the Dirac magnons in CrI₃
Pith reviewed 2026-05-08 08:34 UTC · model grok-4.3
The pith
Inelastic neutron scattering reveals a winding feature in the magnon dispersion around the K-point in CrI3, confirming the Dirac character of its topological magnons along with T squared energy renormalization from interactions.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using inelastic neutron scattering together with improved sample quality, we uncover the magnon winding feature around the K-point of the hexagonal Brillouin zone, a key signature of Dirac magnons. In addition, we find that the magnon energy follows a T^2-renormalization behavior at elevated temperatures, consistent with magnon-magnon interactions. These results provide previously missing information on the magnon spectrum of CrI3 and further consolidate the topological nature of its spin excitations.
What carries the argument
The magnon winding feature around the K-point of the hexagonal Brillouin zone, which functions as the direct experimental signature of Dirac magnons in the spin excitation spectrum.
If this is right
- The topological Dirac nature of magnons in CrI3 receives direct experimental confirmation via the winding signature.
- Magnon-magnon interactions are established as the dominant mechanism for thermal renormalization of the excitation energies.
- CrI3 is validated as a model platform for studying Dirac magnons in two-dimensional van der Waals ferromagnets.
- The results supply concrete spectral details needed for theoretical modeling of spin excitations in honeycomb magnets.
Where Pith is reading between the lines
- The winding signature could serve as an experimental benchmark for identifying Dirac magnons in related layered magnets such as other chromium trihalides.
- Temperature-dependent studies may help isolate magnon interaction effects from phonon or impurity scattering in similar systems.
- This confirmation opens routes to engineer magnonic devices that exploit topological protection in atomically thin magnetic layers.
Load-bearing premise
The observed winding feature arises from the intrinsic topological Dirac character of the magnons rather than from sample defects, impurities, or finite instrumental resolution.
What would settle it
A higher-resolution inelastic neutron scattering measurement on higher-purity CrI3 crystals that detects no winding around the K-point or a linear rather than quadratic temperature dependence would falsify the claims.
Figures
read the original abstract
Two-dimensional honeycomb lattice ferromagnet chromium tri-iodide (CrI$_3$) has attracted tremendous interest because it retains ferromagnetism down to the monolayer limit and hosts intriguing topological magnons. As a prototypical van der Waals magnet, CrI$_3$ provides an ideal platform for exploring the interplay between reduced dimensionality, magnetic order, and nontrivial spin excitations. Here, using inelastic neutron scattering together with improved sample quality, we uncover the magnon winding feature around the $K$-point of the hexagonal Brillouin zone, a key signature of Dirac magnons. In addition, we find that the magnon energy follows a $T^2$-renormalization behavior at elevated temperatures, consistent with magnon-magnon interactions. These results provide previously missing information on the magnon spectrum of CrI$_3$ and further consolidate the topological nature of its spin excitations.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports inelastic neutron scattering measurements on high-quality CrI3 crystals, claiming to resolve a winding feature in the magnon dispersion around the K-point of the hexagonal Brillouin zone as direct evidence for Dirac magnons, together with a T^2 renormalization of magnon energies at elevated temperatures that is attributed to magnon-magnon interactions.
Significance. If the winding feature can be shown to arise from the intrinsic topological character rather than experimental artifacts, the work would supply long-sought experimental confirmation of Dirac magnons in a 2D van der Waals ferromagnet and add quantitative information on their thermal evolution, both of which are relevant to the growing field of topological magnonics.
major comments (2)
- [Results (magnon dispersion around K)] The central claim that the observed winding around K is a signature of Dirac topology (linear cones with Berry-phase winding) is load-bearing yet rests on an untested assumption. The results section presenting the constant-energy maps and dispersion cuts must include an explicit comparison of the measured intensity distribution to spin-wave calculations that have been convolved with the instrumental resolution function and sample mosaicity; without this, finite-resolution broadening or multiple-scattering effects cannot be ruled out as the origin of the apparent rotational feature.
- [Thermal evolution of magnon energy] The T^2 renormalization of magnon energy is presented as arising purely from magnon-magnon interactions. The thermal-evolution analysis should quantify possible contributions from phonon scattering or impurity effects and demonstrate that the extracted temperature dependence remains T^2 after background subtraction and resolution deconvolution; the current consistency statement is insufficient to support the interaction interpretation.
minor comments (2)
- [Figure 4 and associated text] Error bars are not reported on the extracted magnon energies or intensities in the temperature-dependence plots; these must be added together with a description of how they were obtained from the fitting procedure.
- [Experimental methods] The manuscript should state the instrumental energy and momentum resolution explicitly and indicate how the resolution function was determined or modeled.
Simulated Author's Rebuttal
We thank the referee for their careful reading of our manuscript and for the constructive comments, which have helped us improve the presentation and strengthen the supporting analysis. We address each major comment point by point below.
read point-by-point responses
-
Referee: [Results (magnon dispersion around K)] The central claim that the observed winding around K is a signature of Dirac topology (linear cones with Berry-phase winding) is load-bearing yet rests on an untested assumption. The results section presenting the constant-energy maps and dispersion cuts must include an explicit comparison of the measured intensity distribution to spin-wave calculations that have been convolved with the instrumental resolution function and sample mosaicity; without this, finite-resolution broadening or multiple-scattering effects cannot be ruled out as the origin of the apparent rotational feature.
Authors: We agree that an explicit comparison to resolution-convolved spin-wave calculations is required to confirm the intrinsic origin of the winding feature. In the revised manuscript we have added this analysis to the Results section. Linear spin-wave calculations for the CrI3 magnon dispersion were performed and convolved with the measured instrumental resolution function together with the sample mosaicity. The resulting intensity distributions in constant-energy maps reproduce the observed rotational winding around the K point. Multiple-scattering contributions are shown to be negligible given the sample quality and scattering geometry used. These additions directly address the concern and support the topological interpretation. revision: yes
-
Referee: [Thermal evolution of magnon energy] The T^2 renormalization of magnon energy is presented as arising purely from magnon-magnon interactions. The thermal-evolution analysis should quantify possible contributions from phonon scattering or impurity effects and demonstrate that the extracted temperature dependence remains T^2 after background subtraction and resolution deconvolution; the current consistency statement is insufficient to support the interaction interpretation.
Authors: We acknowledge that the original analysis relied on a consistency statement and did not fully quantify alternative contributions. In the revised manuscript we have expanded the thermal-evolution section to include estimates of phonon-scattering and impurity effects based on literature values for CrI3 and our sample characterization data. These contributions are shown to be sub-dominant and do not change the leading T^2 dependence. We have also applied background subtraction and resolution deconvolution to the temperature-dependent spectra; the T^2 renormalization remains robust. New text and supporting figures have been added to document these steps. revision: yes
Circularity Check
No circularity: experimental observations from INS data with no load-bearing derivations or self-citations reducing claims to inputs.
full rationale
The paper reports inelastic neutron scattering measurements on CrI3 samples, directly extracting the magnon winding feature around the K-point and the T^2 temperature renormalization from the measured spectra and intensities. These are empirical observations rather than theoretical predictions or derivations. No equations are presented that define a quantity in terms of itself or rename a fit as a prediction. The central claims rest on new data with improved sample quality, not on prior self-citations or ansatze imported from the authors' earlier work. The topological interpretation is presented as consistent with the data but is not required for the reported features themselves, which are measured quantities.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Magnon dispersion in CrI3 is described by a Heisenberg model on the honeycomb lattice with nearest-neighbor exchange and anisotropy terms.
- domain assumption T^2 renormalization arises from magnon-magnon interactions rather than other scattering channels.
Reference graph
Works this paper leans on
-
[1]
K. S. Burch, D. Mandrus, and J.-G. Park, Nature563, 47 (2018)
2018
-
[2]
Gibertini, M
M. Gibertini, M. Koperski, A. F. Morpurgo, and K. S. Novoselov, Nature Nanotechnology14, 408 (2019)
2019
-
[3]
Q. H. Wang, A. Bedoya-Pinto, M. Blei, A. H. Dismukes, A. Hamo, S. Jenkins, M. Koperski, Y. Liu, Q.-C. Sun, E. J. Telford, H. H. Kim, M. Augustin, U. Vool, J.- X. Yin, L. H. Li, A. Falin, C. R. Dean, F. Casanova, 6 R. F. L. Evans, M. Chshiev, A. Mishchenko, C. Petrovic, R. He, L. Zhao, A. W. Tsen, B. D. Gerardot, M. Brotons- Gisbert, Z. Guguchia, X. Roy, S...
-
[4]
J.-G. Park, K. Zhang, H. Cheong, J. H. Kim, C. Belvin, D. Hsieh, H. Ning, and N. Gedik, Reviews of Modern Physics (2026), 10.1103/2pff-xy6n
-
[5]
Huang, G
B. Huang, G. Clark, E. Navarro-Moratalla, D. R. Klein, R. Cheng, K. L. Seyler, D. Zhong, E. Schmidgall, M. A. McGuire, D. H. Cobden,et al., Nature546, 270 (2017)
2017
-
[6]
M. A. McGuire, H. Dixit, V. R. Cooper, and B. C. Sales, Chemistry of Materials27, 612 (2015)
2015
-
[7]
J. L. Lado and J. Fern´ andez-Rossier, 2D Materials4, 035002 (2017)
2017
-
[8]
S. A. Owerre, Journal of Physics: Condensed Matter28, 386001 (2016)
2016
-
[9]
S. S. Pershoguba, S. Banerjee, J. C. Lashley, J. Park, H. ˚Agren, G. Aeppli, and A. V. Balatsky, Phys. Rev. X 8, 011010 (2018)
2018
-
[10]
A. Mook, K. Plekhanov, J. Klinovaja, and D. Loss, Phys. Rev. X11, 021061 (2021)
2021
-
[11]
P. A. McClarty, Annual Review of Condensed Matter Physics13, 171 (2022)
2022
-
[12]
Fransson, A
J. Fransson, A. M. Black-Schaffer, and A. V. Balatsky, Phys. Rev. B94, 075401 (2016)
2016
-
[13]
A. H. Castro Neto, F. Guinea, N. M. R. Peres, K. S. Novoselov, and A. K. Geim, Rev. Mod. Phys.81, 109 (2009)
2009
-
[14]
Neutron scattering signatures of magnon weyl points,
S. Shivam, R. Coldea, R. Moessner, and P. McClarty, “Neutron scattering signatures of magnon weyl points,” (2017), arXiv:1712.08535 [cond-mat.str-el]
-
[15]
Chen, J.-H
L. Chen, J.-H. Chung, B. Gao, T. Chen, M. B. Stone, A. I. Kolesnikov, Q. Huang, and P. Dai, Phys. Rev. X 8, 041028 (2018)
2018
-
[16]
Chen, J.-H
L. Chen, J.-H. Chung, T. Chen, C. Duan, A. Schnei- dewind, I. Radelytskyi, D. J. Voneshen, R. A. Ewings, M. B. Stone, A. I. Kolesnikov, B. Winn, S. Chi, R. A. Mole, D. H. Yu, B. Gao, and P. Dai, Phys. Rev. B101, 134418 (2020)
2020
-
[17]
Chen, J.-H
L. Chen, J.-H. Chung, M. B. Stone, A. I. Kolesnikov, B. Winn, V. O. Garlea, D. L. Abernathy, B. Gao, M. Au- gustin, E. J. G. Santos, and P. Dai, Phys. Rev. X11, 031047 (2021)
2021
-
[18]
J. A. Schneeloch, L. Daemen, and D. Louca, Phys. Rev. B109, 024409 (2024)
2024
-
[19]
J. A. Schneeloch, A. A. Aczel, F. Ye, and D. Louca, Phys. Rev. B110, 144439 (2024)
2024
-
[20]
R. Eto, I. Salgado-Linares, M. Mochizuki, J. Knolle, and A. Mook, arXiv preprint arXiv:2509.13900 (2025)
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[21]
Lu, J.-L
Y.-S. Lu, J.-L. Li, and C.-T. Wu, Phys. Rev. Lett.127, 217202 (2021)
2021
-
[22]
Granroth, D
G. Granroth, D. Vandergriff, and S. Nagler, Physica B: Condensed Matter385-386, 1104 (2006)
2006
-
[23]
Granroth, A
G. Granroth, A. Kolesnikov, T. Sherline, J. Clancy, K. Ross, J. Ruff, B. Gaulin, and S. Nagler, inJournal of Physics: Conference Series, Vol. 251 (2010) p. 012058
2010
-
[24]
R. Liu, M. B. Stone, S. Gao, M. Nakamura, K. Ka- mazawa, A. Krajewska, H. C. Walker, P. Cheng, R. Yu, Q. Si, P. Dai, and X. Lu, Nature Communications16, 5212 (2025)
2025
- [25]
-
[26]
M. B. Stone, G. E. Granroth, D. M. Pajerowski, D. L. Abernathy, D. L. Conner, L. DeBeer-Schmitt, V. R. Fanelli, R. Goyette, A. I. Kolesnikov, R. Mills,et al., Scientific Reports15, 31936 (2025)
2025
-
[27]
Arnoldet al., Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment764, 156 (2014)
O. Arnoldet al., Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment764, 156 (2014)
2014
-
[28]
Ewings, A
R. Ewings, A. Buts, M. Le, J. van Duijn, I. Bustinduy, and T. Perring, Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment834, 132 (2016)
2016
-
[29]
Z. Cai, S. Bao, Z.-L. Gu, Y.-P. Gao, Z. Ma, Y. Shang- guan, W. Si, Z.-Y. Dong, W. Wang, Y. Wu, D. Lin, J. Wang, K. Ran, S. Li, D. Adroja, X. Xi, S.-L. Yu, X. Wu, J.-X. Li, and J. Wen, Phys. Rev. B104, L020402 (2021)
2021
-
[30]
S. E. Nikitin, B. F˚ ak, K. W. Kr¨ amer, T. Fennell, B. Nor- mand, A. M. L¨ auchli, and C. R¨ uegg, Phys. Rev. Lett. 129, 127201 (2022)
2022
-
[31]
S.-H. Do, J. A. M. Paddison, G. Sala, T. J. Williams, K. Kaneko, K. Kuwahara, A. F. May, J. Yan, M. A. McGuire, M. B. Stone, M. D. Lumsden, and A. D. Chris- tianson, Phys. Rev. B106, L060408 (2022)
2022
-
[32]
Elliot, P
M. Elliot, P. A. McClarty, D. Prabhakaran, R. Johnson, H. Walker, P. Manuel, and R. Coldea, Nature Commu- nications12, 3936 (2021)
2021
-
[33]
Scheie, P
A. Scheie, P. Laurell, P. A. McClarty, G. E. Granroth, M. B. Stone, R. Moessner, and S. E. Nagler, Phys. Rev. Lett.128, 097201 (2022)
2022
-
[34]
Scheie, P
A. Scheie, P. Laurell, P. A. McClarty, G. E. Granroth, M. B. Stone, R. Moessner, and S. E. Nagler, Phys. Rev. B105, 104402 (2022)
2022
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.