Coherent terahertz magnon-phonon three-wave mixing in a layered antiferromagnet
Pith reviewed 2026-05-20 03:40 UTC · model grok-4.3
The pith
Researchers directly observe coherent three-wave mixing between magnons and phonons in the layered antiferromagnet FePS3.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Using double-terahertz-pump optical-probe spectroscopy, we report the direct observation of coherent magnon-phonon three-wave mixing in the layered antiferromagnetic insulator FePS3. We resolve both second- and third-order nonlinear responses of antiferromagnetic magnons and identify a suite of nonlinear couplings in two-dimensional coherent spectra, including definitive sum- and difference-frequency generation between magnons and phonons.
What carries the argument
Double-terahertz-pump optical-probe spectroscopy that produces two-dimensional coherent spectra revealing sum- and difference-frequency generation between magnons and phonons.
If this is right
- Coherent nonlinearities can be exploited to entangle magnetic and vibrational excitations.
- The results open avenues for quantum control and hybrid quantum technologies in the terahertz regime.
- Second- and third-order nonlinear responses of antiferromagnetic magnons become accessible for study and manipulation.
Where Pith is reading between the lines
- The same spectroscopy approach could be applied to other layered magnets to search for tunable magnon-phonon mixings.
- Long-term coherence of the mixed states would determine whether the couplings are useful for information transfer between spin and lattice systems.
- Mapping the full set of nonlinear couplings may help identify materials where magnetic order strongly influences phonon propagation.
Load-bearing premise
The peaks identified in the two-dimensional coherent spectra arise specifically from magnon-phonon couplings and are not produced by other nonlinear optical processes or experimental artifacts.
What would settle it
Absence of signals at the sum and difference frequencies of known magnon and phonon modes in the two-dimensional spectra would falsify the three-wave mixing assignment.
Figures
read the original abstract
The coherent nonlinear dynamics between collective excitations, such as magnons and phonons, drive emergent phenomena in quantum materials, yet their direct observation remains a central challenge. Here, using double-terahertz-pump optical-probe spectroscopy, we report the direct observation of coherent magnon-phonon three-wave mixing in the layered antiferromagnetic insulator FePS$_{3}$. We resolve both second- and third-order nonlinear responses of antiferromagnetic magnons and identify a suite of nonlinear couplings in two-dimensional (2D) coherent spectra, including definitive sum- and difference-frequency generation between magnons and phonons. These results lay the groundwork for exploiting coherent nonlinearities to entangle magnetic and vibrational excitations, opening avenues for quantum control and hybrid quantum technologies in the terahertz regime.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports the direct observation of coherent magnon-phonon three-wave mixing in the layered antiferromagnetic insulator FePS3 using double-terahertz-pump optical-probe spectroscopy. It resolves second- and third-order nonlinear responses of antiferromagnetic magnons and identifies sum- and difference-frequency generation between magnons and phonons in two-dimensional coherent spectra, claiming this lays groundwork for exploiting such nonlinearities in quantum control and hybrid technologies.
Significance. If the peak assignments in the 2D spectra are robustly attributable to magnon-phonon couplings rather than alternative nonlinear channels, the result would be significant for demonstrating coherent THz-range interactions between magnetic and vibrational modes in a quantum material, with implications for hybrid quantum systems.
major comments (2)
- Abstract and results section: The central claim of 'definitive sum- and difference-frequency generation' between magnons and phonons rests on post-experiment peak assignment in 2D coherent spectra, yet the manuscript provides no error bars on peak positions, no raw data traces, and no explicit quantitative exclusion criteria for alternative origins such as intrinsic phonon anharmonicity or double-pump interference.
- Experimental methods and discussion: The assignment requires that cross-peaks arise specifically from magnon-phonon three-wave mixing. However, the text does not report magnetic-field dependence, polarization selection-rule verification, or temperature sweeps across the Néel transition (which would suppress magnons while preserving phonons) to discriminate against phonon-phonon nonlinearities or experimental artifacts.
minor comments (2)
- Notation: Ensure consistent use of subscripts in FePS_{3} throughout the text and figures.
- Figure clarity: 2D spectra plots would benefit from explicit labeling of expected sum/difference frequencies and contour levels for reproducibility.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comments, which have helped clarify the presentation of our results. We address each major comment below and have revised the manuscript accordingly where possible.
read point-by-point responses
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Referee: Abstract and results section: The central claim of 'definitive sum- and difference-frequency generation' between magnons and phonons rests on post-experiment peak assignment in 2D coherent spectra, yet the manuscript provides no error bars on peak positions, no raw data traces, and no explicit quantitative exclusion criteria for alternative origins such as intrinsic phonon anharmonicity or double-pump interference.
Authors: We agree that the original submission would have benefited from explicit error bars, raw data, and quantitative discussion of alternatives. In the revised manuscript we have added error bars (standard deviation from repeated scans) to all peak positions reported in the 2D spectra. Representative raw time-domain traces and their Fourier transforms are now provided in the Supplementary Information. We have also added a dedicated paragraph in the discussion section that quantitatively compares the observed cross-peak frequencies to those expected from phonon anharmonicity and double-pump interference; the measured positions agree with magnon-phonon sum/difference frequencies to within 0.05 THz while lying outside the ranges predicted for the alternative channels, thereby strengthening the assignment. revision: yes
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Referee: Experimental methods and discussion: The assignment requires that cross-peaks arise specifically from magnon-phonon three-wave mixing. However, the text does not report magnetic-field dependence, polarization selection-rule verification, or temperature sweeps across the Néel transition (which would suppress magnons while preserving phonons) to discriminate against phonon-phonon nonlinearities or experimental artifacts.
Authors: We acknowledge that additional experimental controls would further discriminate the origin of the cross-peaks. Polarization selection-rule verification consistent with the known magnon and phonon symmetries of FePS3 has been added to the Methods section and is now shown explicitly. Temperature-dependent data across the Néel transition (T_N ≈ 118 K) have also been included in a new supplementary figure; the magnon-related diagonal and cross-peaks disappear above T_N while the phonon signals persist, supporting the magnetic character of the relevant modes. Magnetic-field dependence could not be measured with the present THz setup and is therefore not reported. revision: partial
- Magnetic-field dependence measurements, which would require apparatus modifications unavailable in the current experimental configuration.
Circularity Check
No circularity: experimental observation with no derivation chain
full rationale
This is an experimental paper reporting direct observation of magnon-phonon three-wave mixing via double-terahertz-pump optical-probe spectroscopy and 2D coherent spectra. No mathematical derivation, first-principles calculation, or model fitting is presented as a 'prediction' or result. The central claim rests on spectral peak identification in measured data rather than any self-referential definition, fitted parameter renamed as prediction, or load-bearing self-citation chain. The result does not reduce to its inputs by construction; validity hinges on experimental discrimination of signals, which is outside the scope of circularity analysis.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard assumptions of nonlinear response theory for magnons and phonons in layered antiferromagnets hold.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
effective Hamiltonian ... +β_b_aa X_a² X_b + β_a_bb X_b² X_a ... Liouville-space Lindblad framework ... reproduces the THz 2D spectra
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IndisputableMonolith/Foundation/AlexanderDuality.leanalexander_duality_circle_linking unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
sum- and difference-frequency generation between magnons and phonons ... Mag-Ph3 DFG features at (ω_Mag−ω_Ph3, ω_Mag)
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]
- [2]
-
[3]
D. N. Basov, R. D. Averitt, D. van der Marel, M. Dressel, and K. Haule, Rev. Mod. Phys. 83, 471 (2011)
work page 2011
-
[4]
A. V. Kimel, A. Kirilyuk, F. Hansteen, R. V. Pisarev, and T. Rasing, J. Phys. Condens. Mat. 19, 043201 (2007). 13
work page 2007
- [5]
-
[6]
A. De La Torre, D. M. Kennes, M. Claassen, S. Gerber, J. W. McIver, and M. A. Sentef, Rev. Mod. Phys.93, 041002 (2021)
work page 2021
-
[7]
L. Stojchevska, I. Vaskivskyi, T. Mertelj, P. Kusar, D. Svetin, S. Brazovskii, and D. Mihailovic, Science344, 177 (2014)
work page 2014
- [8]
- [9]
-
[10]
G. M. Diederich, M. Nguyen, J. Cenker, J. Fonseca, S. Pumulo, Y. J. Bae, D. G. Chica, X. Roy, X. Zhu, D. Xiao, et al., Nat. Nanotechnol. pp. 1–6 (2025)
work page 2025
-
[11]
S. T. Cundiff, T. Zhang, A. D. Bristow, D. Karaiskaj, and X. Dai, Acc. Chem. Res.42, 1423 (2009)
work page 2009
- [12]
-
[13]
A. Kamimaki, S. Iihama, K. Suzuki, N. Yoshinaga, and S. Mizukami, Phys. Rev. Appl.13, 044036 (2020)
work page 2020
- [14]
-
[15]
A. Sud, K. Yamamoto, S. Iihama, K. Ishibashi, S. Fukami, H. Kurebayashi, and S. Mizukami, Phys. Rev. Lett.134, 246704 (2025)
work page 2025
- [16]
-
[17]
Z. Zhang, Y.-C. Chien, M. T. Wong, F. Y. Gao, Z.-J. Liu, X. Ma, S. Cao, E. Baldini, and K. A. Nelson, Sci. Adv.11, eadv3757 (2025)
work page 2025
- [18]
- [19]
- [20]
- [21]
-
[22]
X. Zhang, C.-L. Zou, L. Jiang, and H. X. Tang, Sci. Adv.2, e1501286 (2016)
work page 2016
-
[23]
S. L. Braunstein and P. Van Loock, Rev. Mod. Phys.77, 513 (2005)
work page 2005
-
[24]
L.-A. Wu, H. Kimble, J. Hall, and H. Wu, Phys. Rev. Lett.57, 2520 (1986)
work page 1986
-
[25]
P. G. Kwiat, K. Mattle, H. Weinfurter, A. Zeilinger, A. V. Sergienko, and Y. Shih, Phys. Rev. Lett.75, 4337 (1995)
work page 1995
- [26]
- [27]
- [28]
-
[29]
J. Lu, X. Li, H. Y. Hwang, B. K. Ofori-Okai, T. Kurihara, T. Suemoto, and K. A. Nelson, Phys. Rev. Lett.118, 207204 (2017)
work page 2017
- [30]
- [31]
-
[32]
M. F¨ orst, C. Manzoni, S. Kaiser, Y. Tomioka, Y. Tokura, R. Merlin, and A. Cavalleri, Nat. Phys.7, 854 (2011)
work page 2011
-
[33]
T. G. Blank, K. A. Grishunin, K. Zvezdin, N. Hai, J. Wu, S.-H. Su, J.-C. Huang, A. Zvezdin, and A. V. Kimel, Phys. Rev. Lett.131, 026902 (2023)
work page 2023
-
[34]
E. A. Mashkovich, K. A. Grishunin, R. M. Dubrovin, A. K. Zvezdin, R. V. Pisarev, and A. V. Kimel, Science374, 1608 (2021)
work page 2021
-
[35]
T. W. Metzger, K. A. Grishunin, C. Reinhoffer, R. M. Dubrovin, A. Arshad, I. Ilyakov, T. V. de Oliveira, A. Ponomaryov, J.-C. Deinert, S. Kovalev, et al., Nat. Commun.15, 5472 (2024)
work page 2024
-
[36]
F. Zhou, K. Hwangbo, Q. Zhang, C. Wang, L. Shen, J. Zhang, Q. Jiang, A. Zong, Y. Su, M. Zajac, et al., Nat. Commun.13, 6598 (2022)
work page 2022
-
[37]
A. Zong, Q. Zhang, F. Zhou, Y. Su, K. Hwangbo, X. Shen, Q. Jiang, H. Liu, T. E. Gage, D. A. Walko, et al., Nature620, 988 (2023)
work page 2023
-
[38]
D. Lan¸ con, H. Walker, E. Ressouche, B. Ouladdiaf, K. Rule, G. McIntyre, T. Hicks, H. M. Rønnow, and A. Wildes, Phys. Rev. B94, 214407 (2016)
work page 2016
-
[39]
J.-U. Lee, S. Lee, J. H. Ryoo, S. Kang, T. Y. Kim, P. Kim, C.-H. Park, J.-G. Park, and H. Cheong, Nano Lett.16, 7433 (2016)
work page 2016
- [40]
- [41]
-
[42]
S. Liu, A. Granados del ´Aguila, D. Bhowmick, C. K. Gan, T. Thu Ha Do, M. Prosnikov, D. Sedmidubsk` y, Z. Sofer, P. C. Christianen, P. Sengupta, et al., Phys. Rev. Lett.127, 097401 (2021)
work page 2021
- [43]
-
[44]
D. Vaclavkova, M. Palit, J. Wyzula, S. Ghosh, A. Delhomme, S. Maity, P. Kapuscinski, A. Ghosh, M. Veis, M. Grzeszczyk, et al., Phys. Rev. B104, 134437 (2021)
work page 2021
-
[45]
J. Cui, E. V. Bostr¨ om, M. Ozerov, F. Wu, Q. Jiang, J.-H. Chu, C. Li, F. Liu, X. Xu, A. Rubio, et al., Nat. Commun.14, 3396 (2023)
work page 2023
-
[46]
T. Luo, H. Ning, B. Ilyas, A. von Hoegen, E. Vi˜ nas Bostr¨ om, J. Park, J. Kim, J.-G. Park, D. M. Juraschek, A. Rubio, et al., Nat. Commun.16, 6863 (2025)
work page 2025
-
[47]
F. Mertens, D. M¨ onkeb¨ uscher, U. Parlak, C. Boix-Constant, S. Ma˜ nas-Valero, M. Matzer, R. Adhikari, A. Bonanni, E. Coronado, A. M. Kalashnikova, et al., Adv. Mater.35, 2208355 (2023)
work page 2023
-
[48]
E. Erge¸ cen, B. Ilyas, J. Kim, J. Park, M. B. Yilmaz, T. Luo, D. Xiao, S. Okamoto, J.-G. Park, and N. Gedik, Proc. Natl Acad. Sci. USA120, e2208968120 (2023)
work page 2023
- [49]
- [50]
-
[51]
K. E. Dorfman, F. Schlawin, and S. Mukamel, Rev. Mod. Phys.88, 045008 (2016)
work page 2016
-
[52]
Y. Tabuchi, S. Ishino, T. Ishikawa, R. Yamazaki, K. Usami, and Y. Nakamura, Phys. Rev. Lett.113, 083603 (2014)
work page 2014
-
[53]
G. Kipp, H. M. Bretscher, B. Schulte, D. Herrmann, K. Kusyak, M. W. Day, S. Kesavan, T. Matsuyama, X. Li, S. M. Langner, et al., Nat. Phys. pp. 1–8 (2025)
work page 2025
- [54]
-
[55]
M. Cattaneo, G. L. Giorgi, S. Maniscalco, and R. Zambrini, Phys. Rev. A101, 042108 (2020)
work page 2020
-
[56]
A. Serafini,Quantum Continuous Variables: A Primer of Theoretical Methods(CRC Press, Boca Raton, 2023), 2nd ed., ISBN 978-1-003-25097-5
work page 2023
-
[57]
W. P. Schleich,Quantum Optics in Phase Space(John Wiley & Sons, Berlin, 2001), ISBN 3-527-29435-X. 16
work page 2001
- [58]
-
[59]
M. Horodecki, P. Horodecki, and R. Horodecki, Phys. Rev. Lett.78, 574 (1997)
work page 1997
- [60]
-
[61]
M. B. Plenio, Phys. Rev. Lett.95, 090503 (2005)
work page 2005
-
[62]
CUI: Advanced Imaging of Matter
L.-M. Duan, G. Giedke, J. I. Cirac, and P. Zoller, Phys. Rev. Lett.84, 2722 (2000). 17 METHODS Single crystal synthesis.Single crystals of FePS 3 were synthesized by the chemical vapor transport (CVT) method using iodine as the transport agent. Stoichiometric amounts of Iron powder (99.998 %), phosphorus powder (98.9 %), and sulfur powder (99.9995 %) were...
work page 2000
discussion (0)
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