pith. sign in

arxiv: 2506.13721 · v1 · submitted 2025-06-16 · ❄️ cond-mat.mtrl-sci · cond-mat.str-el· cond-mat.supr-con

Catalogue of chiral phonon materials

Pith reviewed 2026-05-19 09:10 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci cond-mat.str-elcond-mat.supr-con
keywords chiral phononsphonon angular momentumhelicity classificationcrystal symmetryhigh-throughput computationmaterials databasespace groupsthermal transport
0
0 comments X

The pith

Symmetry analysis of phonon angular momentum classifies all crystals into three types and flags 2738 materials with chiral modes.

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

The paper builds a symmetry-based theory that classifies phonon helicity and the velocity-angular-momentum tensor for every one of the 230 space groups. It then runs high-throughput calculations on dynamical matrices from 11614 compounds to locate materials where phonons carry intrinsic angular momentum. The resulting division places crystals into achiral cases with zero angular momentum, chiral crystals showing simple s-wave helicity, and certain achiral crystals that display more complex higher-order helicity patterns. These results are assembled into an open database so that experimenters can quickly pick candidates for studies of heat flow and spin-phonon effects. If the classification is accurate, it supplies a practical route to materials in which phonon angular momentum can be used to influence thermal and quantum transport.

Core claim

Grounded in fundamental representations of phononic angular momentum, the approach classifies crystals into three distinct classes: achiral crystals with vanishing angular momentum, chiral crystals with s-wave helicity, and achiral crystals exhibiting higher-order helicity patterns beyond the s-wave. High-throughput computations and symmetry analysis of the dynamical matrices for 11614 crystalline compounds identified 2738 materials exhibiting chiral phonon modes and shortlisted the 170 most promising candidates for future experimental investigation, with all results placed in an open-access database.

What carries the argument

Symmetry classification of the velocity-angular-momentum tensor extracted from dynamical matrices, which separates s-wave helicity from higher-order patterns across the 230 space groups.

If this is right

  • The open database enables rapid selection of crystals for experiments on phonon-controlled heat flow.
  • The three-class scheme predicts which space groups will produce nonzero phonon angular momentum in thermal transport.
  • Shortlisted materials become targets for studies of spin-phonon coupling and exotic transport.
  • The same symmetry method can be applied to classify chiral behavior in magnons and other lattice excitations.

Where Pith is reading between the lines

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

  • Higher-order helicity in achiral crystals could produce measurable polarization effects that differ from simple chiral cases.
  • Coupling the identified phonon modes to electronic or magnon degrees of freedom may uncover new hybrid phenomena.
  • Temperature-dependent calculations on the shortlisted candidates would test whether the zero-temperature classification survives in real samples.
  • The symmetry framework might extend naturally to phonon properties in layered or nanostructured materials.

Load-bearing premise

Dynamical matrices from standard first-principles calculations accurately reflect phonon helicity and angular momentum without large corrections from anharmonicity, spin-orbit coupling, or temperature.

What would settle it

A measurement of circular phonon polarization or angular momentum in one of the 170 shortlisted materials that shows no sign of the predicted helicity class for its space group.

Figures

Figures reproduced from arXiv: 2506.13721 by Huiqiu Yuan, Ming Shi, Tianqi Deng, Yanhao Tang, Yuanfeng Xu, Yuan Li, Yue Yang, Yu Mao, Zhanghuan Li, Zhenyang Wang, Zhenyu Xiao, Zhi-Da Song.

Figure 1
Figure 1. Figure 1: FIG. 1. Summary of the classifications. The 32 PGs ( [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Workflow of high-throughput calculations and classifications. Dynamical matrices for 9,989 MPID and [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Statistical overview of chiral phonon materials in the high-throughput classification. (a) Pie chart showing [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Phonon band structures and isoenergy surface with helicity projections for four prototypical materials. [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
read the original abstract

Chiral phonons, circularly polarized lattice vibrations carrying intrinsic angular momentum, offer unprecedented opportunities for controlling heat flow, manipulating quantum states through spin-phonon coupling, and realizing exotic transport phenomena. Despite their fundamental importance, a universal framework for identifying and classifying these elusive excitations has remained out of reach. Here, we address this challenge by establishing a comprehensive symmetry-based theory that systematically classifies the helicity and the velocity-angular momentum tensor underlying phonon magnetization in thermal transport across all 230 crystallographic space groups. Our approach, grounded in fundamental representations of phononic angular momentum, reveals three distinct classes of crystals: achiral crystals with vanishing angular momentum, chiral crystals with s-wave helicity, and achiral crystals exhibiting higher-order helicity patterns beyond the s-wave. By performing high-throughput computations and symmetry analysis of the dynamical matrices for 11614 crystalline compounds, we identified 2738 materials exhibiting chiral phonon modes and shortlisted the 170 most promising candidates for future experimental investigation. These results are compiled into an open-access Chiral Phonon Materials Database website, enabling rapid screening for materials with desired chiral phonon properties. Our theoretical framework transcends phonons--it provides a universal paradigm for classifying chiral excitations in crystalline lattices, from magnons to electronic quasiparticles.

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

2 major / 2 minor

Summary. The manuscript develops a symmetry-based framework using representations of phononic angular momentum to classify all 230 space groups into three categories of crystals with respect to chiral phonon modes: achiral crystals with vanishing angular momentum, chiral crystals with s-wave helicity, and achiral crystals with higher-order helicity. High-throughput DFT computations and symmetry analysis of dynamical matrices for 11614 compounds identify 2738 materials exhibiting chiral phonon modes, with 170 shortlisted as promising candidates; results are compiled in an open-access database.

Significance. If the central results hold, the work offers a valuable universal classification scheme and large-scale catalogue for chiral phonons, directly supporting experimental searches in spin-phonon coupling and thermal transport. The open-access database and the extension of the framework beyond phonons to other quasiparticles are clear strengths that enhance reproducibility and utility.

major comments (2)
  1. [high-throughput computations and symmetry analysis] The identification of 2738 materials and the shortlist of 170 candidates rests on symmetry analysis of harmonic dynamical matrices (see the high-throughput computations section). The manuscript provides no quantitative assessment or benchmark of how anharmonicity, spin-orbit coupling, or finite-temperature effects could modify the velocity-angular-momentum tensor or reverse helicity assignments, which directly affects the reliability of the reported counts and the three-class taxonomy for real materials.
  2. [space-group classification] § on space-group classification: while the three-class division is derived from representation theory, the manuscript does not include explicit validation against a set of previously reported chiral-phonon materials (e.g., known examples with measured circular polarization) to confirm that the harmonic eigenvectors reproduce experimental helicity signs.
minor comments (2)
  1. [results] The criteria used to shortlist the 170 most promising candidates from the 2738 are stated only briefly; a dedicated paragraph or table listing the quantitative thresholds (e.g., magnitude of angular momentum, phonon frequency range) would improve clarity.
  2. [database] Figure captions for the database website screenshots should explicitly state the search filters and output fields shown, to allow readers to reproduce the screening process.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major comment below and outline the revisions we will make to improve the discussion of limitations and to strengthen validation of the approach.

read point-by-point responses
  1. Referee: The identification of 2738 materials and the shortlist of 170 candidates rests on symmetry analysis of harmonic dynamical matrices (see the high-throughput computations section). The manuscript provides no quantitative assessment or benchmark of how anharmonicity, spin-orbit coupling, or finite-temperature effects could modify the velocity-angular-momentum tensor or reverse helicity assignments, which directly affects the reliability of the reported counts and the three-class taxonomy for real materials.

    Authors: We agree that the analysis is performed in the harmonic approximation, which is the standard approach enabling high-throughput screening over 11614 compounds. The three-class taxonomy itself follows rigorously from representation theory of the space groups and is independent of the specific values of the force constants. Nevertheless, we acknowledge that anharmonicity, spin-orbit coupling, and finite-temperature effects can in principle alter phonon eigenvectors, lifetimes, and the velocity-angular-momentum tensor in real materials. In the revised manuscript we will add a new subsection explicitly discussing these approximations, their expected magnitude in typical cases, and the conditions under which the harmonic helicity assignments remain reliable. Full quantitative benchmarks would require material-specific anharmonic or finite-temperature calculations that lie beyond the scope of a catalogue paper; we therefore frame the present counts as a symmetry-guided starting point for subsequent detailed studies rather than a final experimental prediction. revision: partial

  2. Referee: § on space-group classification: while the three-class division is derived from representation theory, the manuscript does not include explicit validation against a set of previously reported chiral-phonon materials (e.g., known examples with measured circular polarization) to confirm that the harmonic eigenvectors reproduce experimental helicity signs.

    Authors: We appreciate this suggestion. In the revised version we will add a dedicated validation subsection that compares our harmonic results with several experimentally characterized chiral-phonon systems reported in the literature (for example, materials in which circularly polarized Raman or infrared responses have been measured). For each case we will recompute the dynamical matrix under the same computational protocol used in the high-throughput survey and verify that the predicted helicity signs match the experimental observations. This addition will provide direct evidence that the harmonic eigenvectors correctly capture the helicity assignments for the classes of materials we catalogue. revision: yes

Circularity Check

0 steps flagged

Symmetry-based classification of phonon helicity is self-contained and independent of fitted inputs

full rationale

The paper derives its three-class taxonomy (achiral vanishing angular momentum, chiral s-wave helicity, achiral higher-order helicity) directly from representation theory applied to the dynamical matrix and the velocity-angular-momentum tensor across all 230 space groups. High-throughput screening of 11614 compounds then simply evaluates the precomputed harmonic eigenvectors against these symmetry rules, without any parameter fitting, self-referential definitions, or load-bearing self-citations that would collapse the claimed predictions back to the inputs. The framework is therefore externally falsifiable against independent phonon calculations or experiments and does not exhibit any of the enumerated circularity patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on established group-theoretic representations of phonon modes and standard first-principles dynamical matrices; no new free parameters, ad-hoc axioms, or invented entities are introduced.

axioms (1)
  • standard math Phonon modes transform according to the irreducible representations of the 230 crystallographic space groups
    Invoked to classify helicity and the velocity-angular-momentum tensor.

pith-pipeline@v0.9.0 · 5791 in / 1286 out tokens · 35783 ms · 2026-05-19T09:10:42.318107+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Quantifying chirality of phonons

    cond-mat.mtrl-sci 2026-04 unverdicted novelty 7.0

    A framework defines momentum-resolved and bulk dynamical chirality measures for phonons, demonstrated on chiral and achiral materials to capture handedness and distinguish enantiomers.

  2. Spontaneous spin-selective structural phase transition in chiral crystals

    cond-mat.str-el 2025-12 unverdicted novelty 6.0

    Chiral crystals with screw symmetry undergo a spontaneous spin-selective structural phase transition driven by handedness-dependent phonon renormalization, producing helical spin density waves and chiral lattice distortions.

Reference graph

Works this paper leans on

67 extracted references · 67 canonical work pages · cited by 2 Pith papers

  1. [1]

    William Thomson Baron Kelvin, The molecular tactics of a crystal (Clarendon Press, 1894)

  2. [2]

    Molecular structure of nucleic acids: a structure for deoxyribose nucleic acid,

    James D Watson and Francis HC Crick, “Molecular structure of nucleic acids: a structure for deoxyribose nucleic acid,” Nature 171, 737–738 (1953)

  3. [3]

    Catalytic asymmetric hydrogenation employing a soluble, optically active, rhodium complex,

    William S Knowles and Milton J Sabacky, “Catalytic asymmetric hydrogenation employing a soluble, optically active, rhodium complex,” Chemical Communications (London) , 1445–1446 (1968)

  4. [4]

    Asymmetric catalytic hydrogenation with an optically active phosphiner- hodium complex in homogeneous solution,

    L Horner, H Siegel, and H B¨ uthe, “Asymmetric catalytic hydrogenation with an optically active phosphiner- hodium complex in homogeneous solution,” Angewandte Chemie International Edition in English 7, 942–942 (1968)

  5. [5]

    New method for high-accuracy determination of the fine-structure constant based on quantized hall resistance,

    K. v. Klitzing, G. Dorda, and M. Pepper, “New method for high-accuracy determination of the fine-structure constant based on quantized hall resistance,” Phys. Rev. Lett. 45, 494–497 (1980)

  6. [6]

    The quantized hall effect,

    Klaus von Klitzing, “The quantized hall effect,” Rev. Mod. Phys. 58, 519–531 (1986)

  7. [7]

    Angular momentum of phonons and the einstein–de haas effect,

    Lifa Zhang and Qian Niu, “Angular momentum of phonons and the einstein–de haas effect,” Physical Review Letters 112, 085503 (2014)

  8. [8]

    Chiral phonons at high-symmetry points in monolayer hexagonal lattices,

    Lifa Zhang and Qian Niu, “Chiral phonons at high-symmetry points in monolayer hexagonal lattices,” Physical review letters 115, 115502 (2015)

  9. [9]

    Observation of chiral phonons,

    Hanyu Zhu, Jun Yi, Ming-Yang Li, Jun Xiao, Lifa Zhang, Chih-Wen Yang, Robert A Kaindl, Lain-Jong Li, Yuan Wang, and Xiang Zhang, “Observation of chiral phonons,” Science 359, 579–582 (2018)

  10. [11]

    The chirality of phonons: Definitions, symmetry constraints, and experimental observation,

    Shuai Zhang, Zhiheng Huang, Muchen Du, Tianping Ying, Luojun Du, and Tiantian Zhang, “The chirality of phonons: Definitions, symmetry constraints, and experimental observation,” arXiv preprint arXiv:2503.22794 (2025)

  11. [12]

    Phononic helical nodal lines withPTprotection inmob 2,

    Tiantian Zhang, Yizhou Liu, Hu Miao, and Shuichi Murakami, “New advances in phonons: From band topology to quasiparticle chirality,” arXiv preprint arXiv:2505.06179 (2025)

  12. [13]

    Observation of phonon angular momentum,

    Heda Zhang, N Peshcherenko, Fazhi Yang, TZ Ward, P Raghuvanshi, L Lindsay, Claudia Felser, Y Zhang, J-Q Yan, and H Miao, “Observation of phonon angular momentum,” arXiv preprint arXiv:2409.13462 (2024)

  13. [14]

    Chiral phonon diode effect in chiral crystals,

    Hao Chen, Weikang Wu, Jiaojiao Zhu, Zhengning Yang, Weikang Gong, Weibo Gao, Shengyuan A Yang, and Lifa Zhang, “Chiral phonon diode effect in chiral crystals,” Nano Letters 22, 1688–1693 (2022)

  14. [15]

    Phonon angular momentum induced by the temperature gradient,

    Masato Hamada, Emi Minamitani, Motoaki Hirayama, and Shuichi Murakami, “Phonon angular momentum induced by the temperature gradient,” Physical review letters 121, 175301 (2018)

  15. [16]

    Probing nieh-yan anomaly through phonon dynamics in the kramers-weyl semimetals of chiral crystals,

    Chao-Xing Liu, “Probing nieh-yan anomaly through phonon dynamics in the kramers-weyl semimetals of chiral crystals,” Phys. Rev. B 106, 115102 (2022)

  16. [17]

    Observation of the spin seebeck effect,

    K-I Uchida, S Takahashi, K Harii, J Ieda, W Koshibae, Kazuya Ando, S Maekawa, and E Saitoh, “Observation of the spin seebeck effect,” Nature 455, 778–781 (2008)

  17. [18]

    Theory of the spin seebeck effect,

    Hiroto Adachi, Ken-ichi Uchida, Eiji Saitoh, and Sadamichi Maekawa, “Theory of the spin seebeck effect,” Reports on Progress in Physics 76, 036501 (2013)

  18. [19]

    Chiral-phonon-activated spin seebeck effect,

    Kyunghoon Kim, Eric Vetter, Liang Yan, Cong Yang, Ziqi Wang, Rui Sun, Yu Yang, Andrew H Comstock, Xiao Li, Jun Zhou, et al., “Chiral-phonon-activated spin seebeck effect,” Nature Materials 22, 322–328 (2023)

  19. [20]

    Chiral phonon induced spin polarization,

    Jonas Fransson, “Chiral phonon induced spin polarization,” Physical Review Research 5, L022039 (2023)

  20. [21]

    Chiral phonon activated spin seebeck effect in chiral materials,

    Xiao Li, Jinxin Zhong, Jinluo Cheng, Hao Chen, Huiqian Wang, Jun Liu, Dali Sun, Lifa Zhang, and Jun Zhou, “Chiral phonon activated spin seebeck effect in chiral materials,” Science China Physics, Mechanics & Astronomy 67, 237511 (2024)

  21. [22]

    Theory of chiral-phonon-activated spin seebeck effect,

    Naoki Nishimura, Takumi Funato, Mamoru Matsuo, and Takeo Kato, “Theory of chiral-phonon-activated spin seebeck effect,” arXiv preprint arXiv:2505.23083 (2025)

  22. [23]

    Chiral-induced spin selectivity effect,

    Ron Naaman and David H Waldeck, “Chiral-induced spin selectivity effect,” The journal of physical chemistry letters 3, 2178–2187 (2012)

  23. [24]

    Chiral molecules and the electron spin,

    Ron Naaman, Yossi Paltiel, and David H Waldeck, “Chiral molecules and the electron spin,” Nature Reviews Chemistry 3, 250–260 (2019)

  24. [25]

    Chirality-driven topological electronic structure of dna-like materials,

    Yizhou Liu, Jiewen Xiao, Jahyun Koo, and Binghai Yan, “Chirality-driven topological electronic structure of dna-like materials,” Nature materials 20, 638–644 (2021)

  25. [26]

    Theory of chirality induced spin selectivity: Progress and challenges,

    Ferdinand Evers, Amnon Aharony, Nir Bar-Gill, Ora Entin-Wohlman, Per Hedeg˚ ard, Oded Hod, Pavel Jelinek, Grzegorz Kamieniarz, Mikhail Lemeshko, Karen Michaeli, et al. , “Theory of chirality induced spin selectivity: Progress and challenges,” Advanced Materials 34, 2106629 (2022)

  26. [27]

    Phenomenological evidence for the phonon hall effect,

    C Strohm, GLJA Rikken, and P Wyder, “Phenomenological evidence for the phonon hall effect,” Physical review letters 95, 155901 (2005)

  27. [28]

    Anomalous hall effect for the phonon heat conductivity in paramagnetic di- electrics,

    Yu Kagan and LA Maksimov, “Anomalous hall effect for the phonon heat conductivity in paramagnetic di- electrics,” Physical review letters 100, 145902 (2008)

  28. [29]

    Chiral phonons in the pseudogap phase of cuprates,

    G Grissonnanche, S Th´ eriault, A Gourgout, M-E Boulanger, E Lefran¸ cois, A Ataei, F Lalibert´ e, M Dion, J-S 162 Zhou, S Pyon, et al., “Chiral phonons in the pseudogap phase of cuprates,” Nature Physics16, 1108–1111 (2020)

  29. [30]

    Effective magnetic fields induced by chiral phonons,

    Guohuan Xiong, Hao Chen, Dengke Ma, and Lifa Zhang, “Effective magnetic fields induced by chiral phonons,” Physical Review B 106, 144302 (2022)

  30. [31]

    Intrinsic spin of elastic waves,

    Yang Long, Jie Ren, and Hong Chen, “Intrinsic spin of elastic waves,” Proceedings of the National Academy of Sciences 115, 9951–9955 (2018)

  31. [32]

    Large effective magnetic fields from chiral phonons in rare-earth halides,

    Jiaming Luo, Tong Lin, Junjie Zhang, Xiaotong Chen, Elizabeth R Blackert, Rui Xu, Boris I Yakobson, and Hanyu Zhu, “Large effective magnetic fields from chiral phonons in rare-earth halides,” Science 382, 698–702 (2023)

  32. [33]

    Electron magnetic moment of transient chiral phonons in ktao 3,

    R. Matthias Geilhufe and Wolfram Hergert, “Electron magnetic moment of transient chiral phonons in ktao 3,” Phys. Rev. B 107, L020406 (2023)

  33. [34]

    Giant effective magnetic fields from optically driven chiral phonons in 4 f paramagnets,

    Dominik M. Juraschek, Tom´ a ˇ s Neuman, and Prineha Narang, “Giant effective magnetic fields from optically driven chiral phonons in 4 f paramagnets,” Phys. Rev. Res. 4, 013129 (2022)

  34. [35]

    Magnetic control of soft chiral phonons in pbte,

    Andrey Baydin, Felix G. G. Hernandez, Martin Rodriguez-Vega, Anderson K. Okazaki, Fuyang Tay, G. Timothy Noe, Ikufumi Katayama, Jun Takeda, Hiroyuki Nojiri, Paulo H. O. Rappl, Eduardo Abramof, Gregory A. Fiete, and Junichiro Kono, “Magnetic control of soft chiral phonons in pbte,” Phys. Rev. Lett. 128, 075901 (2022)

  35. [36]

    Observation of interplay between phonon chirality and electronic band topology,

    Felix GG Hernandez, Andrey Baydin, Swati Chaudhary, Fuyang Tay, Ikufumi Katayama, Jun Takeda, Hiroyuki Nojiri, Anderson K Okazaki, Paulo HO Rappl, Eduardo Abramof, et al. , “Observation of interplay between phonon chirality and electronic band topology,” Science advances 9, eadj4074 (2023)

  36. [37]

    Theory of spin magnetization driven by chiral phonons,

    Dapeng Yao and Shuichi Murakami, “Theory of spin magnetization driven by chiral phonons,” Physical Review B 111, 134414 (2025)

  37. [38]

    Phonon-induced geometric chirality,

    Carl P Romao and Dominik M Juraschek, “Phonon-induced geometric chirality,” ACS nano 18, 29550–29557 (2024)

  38. [39]

    Truly chiral phonons in α-hgs,

    Kyosuke Ishito, Huiling Mao, Yusuke Kousaka, Yoshihiko Togawa, Satoshi Iwasaki, Tiantian Zhang, Shuichi Murakami, Jun-ichiro Kishine, and Takuya Satoh, “Truly chiral phonons in α-hgs,” Nature Physics 19, 35–39 (2023)

  39. [40]

    Chiral phonons in quartz probed by x-rays,

    Hiroki Ueda, Mirian Garc´ ıa-Fern´ andez, Stefano Agrestini, Carl P Romao, Jeroen van den Brink, Nicola A Spaldin, Ke-Jin Zhou, and Urs Staub, “Chiral phonons in quartz probed by x-rays,” Nature 618, 946–950 (2023)

  40. [41]

    Lattice dynamics, phonon chirality, and spin–phonon coupling in 2d itinerant ferromagnet fe3gete2,

    Luojun Du, Jian Tang, Yanchong Zhao, Xiaomei Li, Rong Yang, Xuerong Hu, Xueyin Bai, Xiao Wang, Kenji Watanabe, Takashi Taniguchi, et al. , “Lattice dynamics, phonon chirality, and spin–phonon coupling in 2d itinerant ferromagnet fe3gete2,” Advanced Functional Materials 29, 1904734 (2019)

  41. [42]

    Weyl phonons in chiral crystals,

    Tiantian Zhang, Zhiheng Huang, Zitian Pan, Luojun Du, Guangyu Zhang, and Shuichi Murakami, “Weyl phonons in chiral crystals,” Nano Letters 23, 7561–7567 (2023)

  42. [43]

    Propagating chiral phonons in three-dimensional materials,

    Hao Chen, Weikang Wu, Jiaojiao Zhu, Shengyuan A Yang, and Lifa Zhang, “Propagating chiral phonons in three-dimensional materials,” Nano Letters 21, 3060–3065 (2021)

  43. [44]

    Polarized phonons carry angular momentum in ultrafast demagnetization,

    Sonja R Tauchert, Mikhail Volkov, Dominik Ehberger, D Kazenwadel, Martin Evers, Hannah Lange, Andreas Donges, Alexander Book, W Kreuzpaintner, U Nowak, et al. , “Polarized phonons carry angular momentum in ultrafast demagnetization,” Nature 602, 73–77 (2022)

  44. [45]

    Chirality-induced selectivity of phonon angular momenta in chiral quartz crystals,

    Kazuki Ohe, Hiroaki Shishido, Masaki Kato, Shoyo Utsumi, Hiroyasu Matsuura, and Yoshihiko Togawa, “Chirality-induced selectivity of phonon angular momenta in chiral quartz crystals,” Phys. Rev. Lett. 132, 056302 (2024)

  45. [46]

    Chiral phonons in lattices with C4 symmetry,

    Qianqian Wang, Si Li, Jiaojiao Zhu, Hao Chen, Weikang Wu, Weibo Gao, Lifa Zhang, and Shengyuan A. Yang, “Chiral phonons in lattices with C4 symmetry,” Phys. Rev. B 105, 104301 (2022)

  46. [47]

    Magnetic order induced truly chiral phonons in a ferromagnetic weyl semimetal,

    Mengqian Che, Jinxuan Liang, Yunpeng Cui, Hao Li, Bingru Lu, Wenbo Sang, Xiang Li, Xuebin Dong, Shuai Zhang, Tao Sun, et al., “Magnetic order induced truly chiral phonons in a ferromagnetic weyl semimetal,” arXiv preprint arXiv:2411.03754 (2024)

  47. [48]

    Classification of materials with phonon angular momentum and microscopic origin of angular momentum,

    Sinisa Coh, “Classification of materials with phonon angular momentum and microscopic origin of angular momentum,” Phys. Rev. B 108, 134307 (2023)

  48. [49]

    Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set,

    G. Kresse and J. Furthm¨ uller, “Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set,” Computational Materials Science 6, 15 – 50 (1996)

  49. [50]

    First principles phonon calculations in materials science,

    A Togo and I Tanaka, “First principles phonon calculations in materials science,” Scr. Mater. 108, 1–5 (2015)

  50. [51]

    Catalog of topological phonon materials,

    Yuanfeng Xu, MG Vergniory, Da-Shuai Ma, Juan L Ma˜ nes, Zhi-Da Song, B Andrei Bernevig, Nicolas Regnault, and Luis Elcoro, “Catalog of topological phonon materials,” Science 384, eadf8458 (2024)

  51. [52]

    A complete catalogue of high-quality topological materials,

    MG Vergniory, L Elcoro, Claudia Felser, Nicolas Regnault, B Andrei Bernevig, and Zhijun Wang, “A complete catalogue of high-quality topological materials,” Nature 566, 480–485 (2019)

  52. [53]

    All topological bands of all nonmagnetic stoichiometric materials,

    Maia G Vergniory, Benjamin J Wieder, Luis Elcoro, Stuart SP Parkin, Claudia Felser, B Andrei Bernevig, and Nicolas Regnault, “All topological bands of all nonmagnetic stoichiometric materials,” Science 376, eabg9094 (2022)

  53. [54]

    Catalogue of flat-band stoichiometric materials,

    Nicolas Regnault, Yuanfeng Xu, Ming-Rui Li, Da-Shuai Ma, Milena Jovanovic, Ali Yazdani, Stuart SP Parkin, Claudia Felser, Leslie M Schoop, N Phuan Ong, et al., “Catalogue of flat-band stoichiometric materials,” Nature 603, 824–828 (2022). 163

  54. [55]

    Chiral phonons and pseudoangular momentum in nonsymmorphic systems,

    Tiantian Zhang and Shuichi Murakami, “Chiral phonons and pseudoangular momentum in nonsymmorphic systems,” Phys. Rev. Res. 4, L012024 (2022)

  55. [56]

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

    Stefano Baroni, Stefano de Gironcoli, Andrea Dal Corso, and Paolo Giannozzi, “Phonons and related crystal properties from density-functional perturbation theory,” Rev. Mod. Phys. 73, 515–562 (2001)

  56. [57]

    Magnetic order induced chiral phonons in a ferromagnetic weyl semimetal,

    Mengqian Che, Jinxuan Liang, Yunpeng Cui, Hao Li, Bingru Lu, Wenbo Sang, Xiang Li, Xuebin Dong, Le Zhao, Shuai Zhang, Tao Sun, Wanjun Jiang, Enke Liu, Feng Jin, Tiantian Zhang, and Luyi Yang, “Magnetic order induced chiral phonons in a ferromagnetic weyl semimetal,” Phys. Rev. Lett. 134, 196906 (2025)

  57. [58]

    Inherent circular dichroism of phonons in magnetic weyl semimetal co 3sn2s2,

    R. Yang, Y.-Y. Zhu, M. Steigleder, Y.-C. Liu, C.-C. Liu, X.-G. Qiu, Tiantian Zhang, and M. Dressel, “Inherent circular dichroism of phonons in magnetic weyl semimetal co 3sn2s2,” Phys. Rev. Lett. 134, 196905 (2025)

  58. [59]

    Truly chiral phonons arising from chirality-selective magnon-phonon coupling,

    Markus Weißenhofer, Philipp Rieger, MS Mrudul, Luca Mikadze, Ulrich Nowak, and Peter M Oppeneer, “Truly chiral phonons arising from chirality-selective magnon-phonon coupling,” arXiv preprint arXiv:2411.03879 (2024)

  59. [60]

    Inhomogeneous electron gas,

    P. Hohenberg and W. Kohn, “Inhomogeneous electron gas,” Phys. Rev. 136, B864–B871 (1964)

  60. [61]

    Self-consistent equations including exchange and correlation effects,

    W. Kohn and L. J. Sham, “Self-consistent equations including exchange and correlation effects,” Phys. Rev. 140, A1133–A1138 (1965)

  61. [62]

    Ab initio molecular dynamics for open-shell transition metals,

    G. Kresse and J. Hafner, “ Ab initio molecular dynamics for open-shell transition metals,” Phys. Rev. B 48, 13115–13118 (1993)

  62. [63]

    From ultrasoft pseudopotentials to the projector augmented-wave method,

    G. Kresse and D. Joubert, “From ultrasoft pseudopotentials to the projector augmented-wave method,” Phys. Rev. B 59, 1758–1775 (1999)

  63. [64]

    Generalized gradient approximation made simple,

    John P. Perdew, Kieron Burke, and Matthias Ernzerhof, “Generalized gradient approximation made simple,” Phys. Rev. Lett. 77, 3865–3868 (1996)

  64. [65]

    Implementation strategies in phonopy and phono3py,

    Atsushi Togo, Laurent Chaput, Terumasa Tadano, and Isao Tanaka, “Implementation strategies in phonopy and phono3py,” J. Phys. Condens. Matter 35, 353001 (2023)

  65. [66]

    First-principles phonon calculations with phonopy and phono3py,

    Atsushi Togo, “First-principles phonon calculations with phonopy and phono3py,” J. Phys. Soc. Jpn. 92, 012001 (2023)

  66. [67]

    Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional perturbation theory,

    Xavier Gonze and Changyol Lee, “Dynamical matrices, born effective charges, dielectric permittivity tensors, and interatomic force constants from density-functional perturbation theory,” Physical Review B 55, 10355 (1997)

  67. [68]

    A mixed-space approach to first-principles calculations of phonon frequencies for polar materials,

    Yuedong Wang, JJ Wang, WY Wang, ZG Mei, SL Shang, LQ Chen, and ZK Liu, “A mixed-space approach to first-principles calculations of phonon frequencies for polar materials,” Journal of Physics: Condensed Matter 22, 202201 (2010)