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arxiv: 2604.10231 · v1 · submitted 2026-04-11 · ❄️ cond-mat.mtrl-sci

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Quantifying chirality of phonons

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Pith reviewed 2026-05-10 15:51 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords chiral phononsdynamical chiralityphonon angular momentumlattice vibrationsenantiomersfirst-principles calculations
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The pith

A framework quantifies the dynamical chirality of phonons with measures that distinguish enantiomers.

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

This paper develops a quantitative framework for the chirality of phonons, which are lattice vibrations that carry angular momentum and show handedness. It introduces momentum-resolved dynamical chirality to examine individual modes at specific wave vectors and bulk dynamical chirality to describe the overall effect from thermally excited modes. First-principles calculations on chiral and achiral materials illustrate how these measures reveal handedness, population imbalances, and allow distinction between mirror-image crystals. This advances the field by turning qualitative observations of chiral phonons into measurable quantities.

Core claim

We introduce two quantitative measures: momentum-resolved dynamical chirality, which provides a mode- and wave-vector-resolved picture of phonon chirality, and the bulk dynamical chirality, which characterizes the collective behavior of thermally populated chiral phonons. Using first-principles calculations for both chiral and achiral materials, we demonstrate how these quantities capture the handedness and population imbalance of phonon modes and serve as a means to distinguish the enantiomers of chiral crystals.

What carries the argument

The momentum-resolved dynamical chirality and bulk dynamical chirality measures that quantify phonon handedness in a dynamical way.

If this is right

  • These measures give a detailed view of chirality for each phonon mode and wave vector.
  • The bulk measure accounts for the combined effect of all thermally populated chiral phonons.
  • They reveal both the handedness and any imbalance in mode populations.
  • The framework successfully distinguishes left- and right-handed versions of chiral crystals.

Where Pith is reading between the lines

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

  • Adoption of these measures could standardize comparisons of phonon chirality across different materials and studies.
  • It may lead to better predictions of how chiral phonons interact with light or other excitations.
  • Testing the measures against more experimental data on helicity-dependent effects would strengthen their physical basis.

Load-bearing premise

The proposed measures correctly capture the physical handedness and population imbalance of phonons independent of specific calculation methods.

What would settle it

Finding a chiral material where the calculated dynamical chirality measures do not match the observed handedness in optical experiments or fail to assign opposite values to enantiomers.

Figures

Figures reproduced from arXiv: 2604.10231 by Dominik Maximilian Juraschek, Gakuto Kusuno, Hiroaki Kusunose, Takuya Satoh, Yu-Chi Huang, Yusuke Hashimoto.

Figure 1
Figure 1. Figure 1: FIG. 1. A chiral phonon in a branch [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Momentum-resolved dynamical chirality [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Schematic of chiral phonons for different values of bulk dynamical chirality and momentum-resolved dynamical chirality [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
read the original abstract

Recent years have witnessed growing interest in chiral phonons, lattice vibrations carrying angular momentum and exhibiting handedness, as revealed by helicity-dependent optical phenomena. Despite this progress, a quantitative characterization of phonon chirality as a dynamical property has remained elusive. In this work, we propose a theoretical framework to quantify the dynamical chirality of lattice vibrations. We introduce two quantitative measures: momentum-resolved dynamical chirality, which provides a mode- and wave-vector-resolved picture of phonon chirality, and the bulk dynamical chirality, which characterizes the collective behavior of thermally populated chiral phonons. Using first-principles calculations for both chiral and achiral materials, we demonstrate how these quantities capture the handedness and population imbalance of phonon modes and serve as a means to distinguish the enantiomers of chiral crystals.

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 introduces a theoretical framework to quantify dynamical chirality of phonons. It defines two scalar measures—momentum-resolved dynamical chirality (mode- and wave-vector-resolved) and bulk dynamical chirality (collective thermal population)—and applies them via first-principles calculations to both chiral and achiral crystals, claiming these quantities capture handedness, population imbalance, and enable enantiomer distinction.

Significance. If the definitions prove well-posed and the numerical demonstrations reproducible, the work supplies a practical, quantitative tool for an emerging area of phonon physics tied to angular momentum and helicity-dependent optics. The use of first-principles methods on real materials is a strength that could facilitate adoption.

minor comments (3)
  1. The abstract states the measures but supplies no explicit formulas; the main text should include the precise mathematical definitions (e.g., any integrals or sums over phonon eigenvectors or frequencies) early in the theory section so readers can verify independence from fitting parameters.
  2. Clarify how the bulk dynamical chirality is obtained from the momentum-resolved quantity (thermal averaging procedure, temperature range, Brillouin-zone sampling) and confirm that the reported distinction between enantiomers survives changes in exchange-correlation functional or k-point density.
  3. Figure captions and axis labels should explicitly state the units or normalization of the chirality measures and indicate which panels correspond to chiral versus achiral test cases.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive summary and significance assessment of our work on quantifying dynamical chirality of phonons. The recommendation for minor revision is noted. No specific major comments were raised in the report, so we have no point-by-point responses to provide here. We will address any minor issues identified during the revision process.

Circularity Check

0 steps flagged

No significant circularity in proposed chirality measures

full rationale

The paper introduces momentum-resolved dynamical chirality and bulk dynamical chirality as new quantitative definitions applied to first-principles phonon calculations on both chiral and achiral crystals. These measures are presented as a theoretical framework to capture handedness and thermal population imbalance, with numerical demonstrations serving as validation rather than derivation. No load-bearing step reduces by construction to self-definition, fitted inputs renamed as predictions, or self-citation chains; the central claims remain independent of the inputs and rest on the explicit definitions and external computational benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no free parameters, axioms, or invented entities are identifiable from the provided text.

pith-pipeline@v0.9.0 · 5447 in / 1043 out tokens · 29100 ms · 2026-05-10T15:51:04.313858+00:00 · methodology

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Reference graph

Works this paper leans on

48 extracted references · 5 canonical work pages · 1 internal anchor

  1. [1]

    D. M. Juraschek, R. M. Geilhufe, H. Zhu, M. Basini, P. Baum, A. Baydin, S. Chaudhary, M. Fechner, B. Fle- bus, G. Grissonnanche, A. I. Kirilyuk, M. Lemeshko, S. F. Maehrlein, M. Mignolet, S. Murakami, Q. Niu, U. Nowak, C. P. Romao, H. Rostami, T. Satoh, N. A. Spaldin, H. Ueda, and L. Zhang, Chiral phonons, Nat. Phys.21, 1532 (2025)

  2. [2]

    Ishito, H

    K. Ishito, H. Mao, Y. Kousaka, Y. Togawa, S. Iwasaki, T. Zhang, S. Murakami, J. Kishine, and T. Satoh, Truly chiral phonons inα-HgS, Nat. Phys.19, 35 (2023)

  3. [3]

    H. Ueda, M. Garc´ ıa-Fern´ andez, S. Agrestini, C. P. Ro- mao, J. van den Brink, N. A. Spaldin, K.-J. Zhou, and U. Staub, Chiral phonons in quartz probed by X-rays, Nature618, 946 (2023)

  4. [4]

    Zhang and Q

    L. Zhang and Q. Niu, Chiral phonons at high-symmetry points in monolayer hexagonal lattices, Phys. Rev. Lett. 115, 115502 (2015)

  5. [5]

    Zhuet al., Observation of chiral phonons, Science359, 579 (2018)

    H. Zhuet al., Observation of chiral phonons, Science359, 579 (2018)

  6. [6]

    H. Chen, W. Wu, J. Zhu, S. A. Yang, and L. Zhang, Propagating chiral phonons in three-dimensional materi- als, Nano Lett.21, 3060 (2021)

  7. [7]

    Ishito, H

    K. Ishito, H. Mao, K. Kobayashi, Y. Kousaka, Y. Togawa, H. Kusunose, J. Kishine, and T. Satoh, Chiral phonons: circularly polarized raman spectroscopy and ab initio cal- culations in a chiral crystal tellurium, Chirality35, 338 (2023)

  8. [8]

    Oishi, Y

    E. Oishi, Y. Fujii, and A. Koreeda, Selective observation of enantiomeric chiral phonons inα-quartz, Phys. Rev. B109, 104306 (2024)

  9. [9]

    Dornes, Y

    C. Dornes, Y. Acremann, M. Savoini, M. Kubli, M. J. Neugebauer, E. Abreu, L. Huber, G. Lantz, C. A. F. Vaz, H. Lemke, E. M. Bothschafter, M. Porer, V. Es- posito, L. Rettig, M. Buzzi, A. Alberca, Y. W. Windsor, P. Beaud, U. Staub, D. Zhu, S. Song, J. M. Glownia, and S. L. Johnson, The ultrafast Einstein–de Haas effect, Na- ture565, 209 (2019)

  10. [10]

    S. R. Tauchert, M. Volkov, D. Ehberger, D. Kazenwadel, M. Evers, H. Lange, A. Donges, A. Book, W. Kreuz- paintner, U. Nowak, and P. Baum, Polarized phonons carry angular momentum in ultrafast demagnetization, Nature602, 73 (2022)

  11. [11]

    I. H. Choi, S. G. Jeong, S. Song, S. Park, D. B. Shin, W. S. Choi, and J. S. Lee, Real-time dynamics of an- gular momentum transfer from spin to acoustic chiral phonon in oxide heterostructures, Nature Nanotechnol- ogy19, 1277 (2024)

  12. [12]

    Minakova, C

    O. Minakova, C. Paiva, M. Frenzel, M. S. Spencer, J. M. Urban, C. Ringkamp, M. Wolf, G. Mussler, D. M. Juraschek, and S. F. Maehrlein, Direct observation of an- gular momentum transfer among crystal lattice modes, arXiv:2503.11626 (2025)

  13. [13]

    Nabei, C

    Y. Nabei, C. Yang, H. Sun, H. Jones, T. Mai, T. Wang, R. Bodin, B. Pandey, Z. Wang, Y. Xiong, A. H. Comstock, B. Ewing, J. Bingen, R. Sun, D. Smirnov, W. Zhang, A. Hoffmann, R. Rao, M. Hu, Z. V. Vardeny, B. Yan, X. Li, J. Zhou, J. Liu, and D. Sun, Orbital see- beck effect induced by chiral phonons, Nature Physics 22, 245 (2026)

  14. [14]

    K. Ohe, H. Shishido, M. Kato, S. Utsumi, H. Matsuura, and Y. Togawa, Chirality-induced selectivity of phonon angular momenta in chiral quartz crystals, Phys. Rev. Lett.132, 056302 (2024)

  15. [15]

    Das Gupta, S

    D. Das Gupta, S. K. Maiti, and L. M. P´ erez, Electri- cally driven spin currents in dna, Science China Physics, Mechanics & Astronomy67, — (2024)

  16. [16]

    Hamada, E

    M. Hamada, E. Minamitani, M. Hirayama, and S. Mu- rakami, Phonon angular momentum induced by the tem- perature gradient, Phys. Rev. Lett.121, 175301 (2018)

  17. [17]

    Zhang and S

    T. Zhang and S. Murakami, Chiral phonons and pseu- doangular momentum in nonsymmorphic systems, Phys. Rev. Research4, L012024 (2022)

  18. [18]

    Abraham and A

    E. Abraham and A. Nitzan, Quantifying the chirality of vibrational modes in helical structures, Phys. Rev. Lett. 133, 268001 (2024)

  19. [19]

    J. Feng, E. D. Abraham, J. E. Subotnik, and A. Nitzan, Rectification of vibrational energy transfer in driven chi- ral molecules, J. Chem. Phys.163, 234110 (2025)

  20. [20]

    H. Wang, D. Fan, H. C. Po, X. Wan, and F. Tang, Cat- alog of phonon emergent particles and chiral phonons: Symmetry-based classification and materials database in- vestigation, arXiv:2601.17353 (2026), arXiv:2601.17353 6 [cond-mat.mtrl-sci]

  21. [21]

    Y. Yang, Z. Xiao, Y. Mao, Z. Li, Z. Wang, T. Deng, Y. Tang, Z.-D. Song, Y. Li, H. Yuan, M. Shi, and Y. Xu, Catalogue of chiral phonon materials, arXiv:2506.13721 (2025), arXiv:2506.13721 [cond-mat.mtrl-sci]

  22. [22]

    Tsunetsugu and H

    H. Tsunetsugu and H. Kusunose, Theory of energy dis- persion of chiral phonons, J. Phys. Soc. Jpn.92, 023601 (2023)

  23. [23]

    Tsunetsugu and H

    H. Tsunetsugu and H. Kusunose, Chiral phonons in a cubic lattice, J. Phys. Soc. Jpn.95, 013601 (2026)

  24. [24]

    Baroni, S

    S. Baroni, S. de Gironcoli, A. Dal Corso, and P. Gi- annozzi, Phonons and related crystal properties from density-functional perturbation theory, Rev. Mod. Phys. 73, 515 (2001)

  25. [25]

    Gonzeet al., Recent developments in the abinit soft- ware package, Comput

    X. Gonzeet al., Recent developments in the abinit soft- ware package, Comput. Phys. Commun.248, 107042 (2020)

  26. [26]

    [24? ? ?, 25]

    See Supplemental Material, which includes Refs. [24? ? ?, 25]

  27. [27]

    L. D. Barron, True and false chirality and absolute asym- metric synthesis, J. Am. Chem. Soc.108, 5539 (1986)

  28. [28]

    L. D. Barron, Symmetry and molecular chirality, Chem. Soc. Rev.15, 189 (1986)

  29. [29]

    Zhang and Q

    L. Zhang and Q. Niu, Angular momentum of phonons and the Einstein–de Haas effect, Phys. Rev. Lett.112, 085503 (2014)

  30. [30]

    Coh, Classification of materials with phonon angular momentum and microscopic origin of angular momen- tum, Phys

    S. Coh, Classification of materials with phonon angular momentum and microscopic origin of angular momen- tum, Phys. Rev. B108, 134307 (2023)

  31. [31]

    Kusunose, J

    H. Kusunose, J. Kishine, and H. M. Yamamoto, Emer- gence of chirality from electron spins, physical fields, and material–field composites, Appl. Phys. Lett.124, 260501 (2024)

  32. [32]

    Kishine, H

    J. Kishine, H. Kusunose, and H. M. Yamamoto, On the definition of chirality and enantioselective fields, Isr. J. Chem.62, e202200049 (2022)

  33. [33]

    A. Inda, R. Oiwa, S. Hayami, H. M. Yamamoto, and H. Kusunose, Quantification of chirality based on electric toroidal monopole, J. Chem. Phys.160, 184117 (2024)

  34. [34]

    Oiwa and H

    R. Oiwa and H. Kusunose, Rotation, electric-field re- sponses, and absolute enantioselection in chiral crystals, Phys. Rev. Lett.129, 116401 (2022)

  35. [35]

    Hayami and H

    S. Hayami and H. Kusunose, Unified description of elec- tronic orderings and cross correlations by complete multi- pole representation, J. Phys. Soc. Jpn.93, 072001 (2024)

  36. [36]

    H. Ueda, A. Nag, C. P. Romao, M. Garc´ ıa-Fern´ andez, K.- J. Zhou, and U. Staub, Chiral phonons in polar LiNbO 3, Nature Communications17, 212 (2025)

  37. [37]

    Bousquet, M

    E. Bousquet, M. Fava, Z. Romestan, F. G´ omez-Ortiz, E. E. McCabe, and A. H. Romero, Structural chirality and related properties in periodic inorganic solids: review and perspectives, J. Phys.: Condens. Matter37, 163004 (2025)

  38. [38]

    M. Fava, A. H. Romero, and E. Bousquet, Handedness selection and hysteresis of chiral orders in crystals, Phys. Rev. Lett.135, 146102 (2025)

  39. [39]

    N. A. Spaldin, Towards a modern theory of chiralization, arXiv:2601.16042 10.48550/arXiv.2601.16042 (2026)

  40. [40]

    G´ omez-Ortiz, S

    F. G´ omez-Ortiz, S. M. Taganga, E. E. McCabe, A. H. Romero, and E. Bousquet, Chirality cannot be fer- roic in enantiomorphic space-groups, arXiv:2603.22501 10.48550/arXiv.2603.22501 (2026)

  41. [41]

    L. D. Landau and E. M. Lifshitz,Statistical Physics, Part 1, 3rd ed., Course of Theoretical Physics, Vol. 5 (Butterworth-Heinemann, Oxford, 1980)

  42. [42]

    P. M. Chaikin and T. C. Lubensky,Principles of Con- densed Matter Physics(Cambridge University Press, Cambridge, UK and New York, NY, USA, 1995)

  43. [43]

    Goldenfeld,Lectures on Phase Transitions and the Renormalization Group, Frontiers in Physics, Vol

    N. Goldenfeld,Lectures on Phase Transitions and the Renormalization Group, Frontiers in Physics, Vol. 85 (Westview Press, Boulder, CO, 1992). Supplemental Material: Quantifying chirality of phonons Yu-Chi Huang, 1, 2 Gakuto Kusuno, 1 Yusuke Hashimoto,3 Dominik M. Juraschek, 2 Hiroaki Kusunose, 4 and Takuya Satoh 1, 5 1Department of Physics, Institute of S...

  44. [44]

    Phonons and related crystal properties from density-functional perturbation theory,

    S. Baroni, S. de Gironcoli, A. Dal Corso, and P. Giannozzi, “Phonons and related crystal properties from density-functional perturbation theory,” Rev. Mod. Phys.73, 515 (2001)

  45. [45]

    The Abinit project: Impact, environment and recent developments,

    X. Gonzeet al., “The Abinit project: Impact, environment and recent developments,” Comput. Phys. Commun.248, 107042 (2020). 10

  46. [46]

    Generalized gradient approximation made simple,

    J. P. Perdew, K. Burke, and M. Ernzerhof, “Generalized gradient approximation made simple,” Phys. Rev. Lett.77, 3865 (1996)

  47. [47]

    First principles phonon calculations in materials science,

    A. Togo and I. Tanaka, “First principles phonon calculations in materials science,” Scr. Mater.108, 1 (2015)

  48. [48]

    Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set,

    G. Kresse and J. Furthm¨ uller, “Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set,” Phys. Rev. B54, 11169 (1996)