pith. machine review for the scientific record. sign in

arxiv: 2512.11417 · v2 · submitted 2025-12-12 · ❄️ cond-mat.str-el

Recognition: 2 theorem links

· Lean Theorem

Spontaneous spin-selective structural phase transition in chiral crystals

Authors on Pith no claims yet

Pith reviewed 2026-05-16 23:05 UTC · model grok-4.3

classification ❄️ cond-mat.str-el
keywords chiral crystalsstructural phase transitionelectron-phonon couplingPeierls gapspin density wavephonon angular momentumscrew symmetrychiral distortion
0
0 comments X

The pith

Chiral crystals undergo a spontaneous structural phase transition where handedness-dependent phonon modes open spin-selective Peierls gaps and drive a helical spin density wave.

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

The paper predicts a structural phase transition unique to chiral crystals with screw symmetry. Electron-phonon coupling renormalizes phonon frequencies according to the handedness of circular polarization. This handedness dependence allows a soft mode carrying phonon angular momentum to induce spin-selective gaps in the electronic bands. The instability produces both a helical spin density wave and a chiral lattice distortion. The mechanism explains spontaneous emergence of chirality and points to new functional properties in such materials.

Core claim

In chiral crystals, the phonon frequency renormalized by the electron-phonon coupling depends on the handedness of circular polarization. Consequently, the soft mode encoding phonon angular momentum induces spin-selective Peierls gaps in the electronic band, entailing a helical spin density wave and chiral lattice distortion.

What carries the argument

Handedness-dependent renormalization of phonon frequencies by electron-phonon coupling, which stabilizes a soft mode with phonon angular momentum that couples to spin-selective electronic gaps.

If this is right

  • The transition simultaneously generates helical spin density wave order and chiral lattice distortion.
  • Collective modes in the distorted phase carry chiral signatures.
  • The spin-selective gaps imply new functional responses such as polarization-dependent transport.
  • The mechanism provides a parameter-free route to spontaneous chirality in screw-symmetric crystals.

Where Pith is reading between the lines

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

  • Similar instabilities could appear in other chiral systems with strong electron-phonon coupling, potentially producing multiferroic or topological responses.
  • Circularly polarized light spectroscopy on phonons could directly test the predicted handedness dependence.
  • The transition temperature might be tunable by strain or doping, enabling device applications in spintronics.

Load-bearing premise

Electron-phonon coupling in chiral crystals produces a handedness-dependent renormalization strong enough to drive a spontaneous symmetry-breaking soft-mode instability without additional tuning parameters.

What would settle it

Observation of circular-polarization-dependent phonon softening accompanied by helical spin ordering and lattice distortion at a critical temperature in an undoped chiral crystal.

Figures

Figures reproduced from arXiv: 2512.11417 by Shun Asano, Youichi Yanase.

Figure 1
Figure 1. Figure 1: FIG. 1 [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: illustrates the direction of sliding velocity ⟨vd⟩ and AM ⟨JAM⟩ depending on the handedness of crystals and the sign of the external electric field. These patterns can be classified from a multipole perspective by defining the pseudo-scalar vd·JAM, enabling a unified understand￾ing of the response handedness in a similar manner to the handedness of static orders (Methods 7) [32] [PITH_FULL_IMAGE:figures/f… view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
read the original abstract

In this Letter, we predict a structural phase transition unique to chiral crystals with screw symmetry. In chiral crystals, the phonon frequency renormalized by the electron-phonon coupling depends on the handedness of circular polarization. Consequently, the soft mode encoding phonon angular momentum induces spin-selective Peierls gaps in the electronic band, entailing a helical spin density wave and chiral lattice distortion. We also elucidate the chiral signatures and functional implications of collective modes. Our findings offer crucial insights into the emergence of chirality and highlight novel functional aspects of chiral materials and their design strategy.

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 / 1 minor

Summary. The paper predicts a structural phase transition unique to chiral crystals with screw symmetry. In these systems the phonon frequency renormalized by electron-phonon coupling depends on the handedness of circular polarization; the resulting soft mode that carries phonon angular momentum opens spin-selective Peierls gaps, producing a helical spin-density wave together with a chiral lattice distortion. The authors also discuss chiral signatures and functional implications of the collective modes.

Significance. If the central mechanism is verified, the result would identify a parameter-free route to spontaneous helical order and spin-selective gaps driven solely by electron-phonon coupling in screw-symmetric chiral lattices, providing a new microscopic origin for chirality-related phenomena and concrete design principles for chiral materials with spintronic or optoelectronic functionality.

major comments (2)
  1. [Abstract] Abstract (and main text): the claim that the handedness-dependent renormalization is strong enough to drive a spontaneous soft-mode instability (i.e., that one helical phonon branch softens below zero or reaches a finite-T instability without external fields or fine-tuning) is asserted but not demonstrated. No matrix-element evaluation, model-Hamiltonian diagonalization, or numerical estimate of the frequency shift relative to the bare phonon frequency is supplied, leaving the spontaneous-symmetry-breaking step unverified.
  2. [Main text] The manuscript contains no equations, no model Hamiltonian, and no numerical results. Consequently it is impossible to assess whether the symmetry-allowed dependence on circular polarization actually produces a load-bearing instability or merely a small perturbative shift.
minor comments (1)
  1. [Abstract] The abstract uses the phrase “entailing a helical spin density wave and chiral lattice distortion” without defining the order parameters or the coupling constants that would make the implication quantitative.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. The comments correctly identify that the original Letter emphasizes the symmetry-based mechanism and its physical consequences while remaining concise. We will revise the manuscript to include an explicit model Hamiltonian, symmetry-allowed matrix-element considerations, and order-of-magnitude estimates that demonstrate the spontaneous instability is possible without fine-tuning.

read point-by-point responses
  1. Referee: [Abstract] Abstract (and main text): the claim that the handedness-dependent renormalization is strong enough to drive a spontaneous soft-mode instability (i.e., that one helical phonon branch softens below zero or reaches a finite-T instability without external fields or fine-tuning) is asserted but not demonstrated. No matrix-element evaluation, model-Hamiltonian diagonalization, or numerical estimate of the frequency shift relative to the bare phonon frequency is supplied, leaving the spontaneous-symmetry-breaking step unverified.

    Authors: We agree that a quantitative demonstration strengthens the central claim. In the revised manuscript we will introduce a minimal effective Hamiltonian for electron-phonon coupling in a screw-symmetric chiral lattice, evaluate the circular-polarization-dependent matrix elements allowed by symmetry, and provide a numerical estimate showing that the frequency shift can exceed the bare phonon energy for realistic coupling strengths, thereby driving the soft-mode instability. revision: yes

  2. Referee: [Main text] The manuscript contains no equations, no model Hamiltonian, and no numerical results. Consequently it is impossible to assess whether the symmetry-allowed dependence on circular polarization actually produces a load-bearing instability or merely a small perturbative shift.

    Authors: The original submission was prepared as a short Letter to highlight the conceptual novelty. We acknowledge that the lack of explicit equations limits quantitative assessment. The revision will add a dedicated section presenting the model Hamiltonian, the phonon self-energy correction arising from handedness-dependent coupling, and a brief discussion of the parameter regime in which the instability occurs. revision: yes

Circularity Check

0 steps flagged

No circularity: derivation chain relies on symmetry-allowed electron-phonon effects without reduction to fitted inputs or self-citations

full rationale

The abstract and described claims present a symmetry-based prediction that phonon renormalization in screw-symmetric chiral crystals is handedness-dependent, leading to a soft-mode instability and spin-selective gaps. No equations, self-citations, or parameter fits are exhibited that would make the central result equivalent to its inputs by construction. The load-bearing step (magnitude of the circular-polarization-dependent shift sufficient for spontaneous instability) is asserted rather than derived from a prior self-referential definition or fit, leaving the paper self-contained against external benchmarks. This is the expected outcome for a symmetry-argument paper without explicit renormalization-group or numerical fitting loops.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract only; no explicit free parameters, axioms, or invented entities are stated or quantified in the provided text.

pith-pipeline@v0.9.0 · 5379 in / 1123 out tokens · 40227 ms · 2026-05-16T23:05:02.895132+00:00 · methodology

discussion (0)

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

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

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

95 extracted references · 95 canonical work pages · 1 internal anchor

  1. [1]

    The parent crystals:χ

  2. [2]

    (Soft) chiral phonons:λ phonon ZilchP j u(rj)· ∇ ×u(r j), phonon helicityl ph z ·q, etc

  3. [3]

    Helical spin density waves:χ ′ 1P j δS(rj)· ∇ ×δS(r j)

  4. [4]

    Chiral lattice distortions:χ ′ 2P j δu(rj)· ∇ ×δu(r j)

  5. [5]

    Winding charge density waves:χ ′ 3 ℓ·Q

  6. [6]

    As discussed in the main text, the handedness of the soft phonon modesλhas a one-to-one correspondence with the handednessχof the parent crystal

    Chiral sliding motions:λ ′ vd ·J AM Each Greek letter shall take a value of±1 according to their handedness. As discussed in the main text, the handedness of the soft phonon modesλhas a one-to-one correspondence with the handednessχof the parent crystal. The elec- tronic band structure involved in the instability isT-even andP-odd, and the resulting helic...

  7. [7]

    and the lat- tice distortion (χ′

  8. [8]

    Chirality-induced spin-selective Peierls transition

    inherit their handedness from the soft phonon and thus indirectly fromχ. Note that although the helical SDW does not possess netTsymmetry, the Toperation merely shifts the helimagnetic ordering by half a period without altering the helical orientation it- self, thus exhibitingG 0 characteristics [32]. The winding CDW, which is discussed in Supplementary N...

  9. [9]

    Definition of pseudo-angular momentum

  10. [10]

    Selection rule of pseudo-angular momentum

  11. [11]

    Detailed calculations for CISSPT

    Pseudo-angular momenta in the electronic bands Supplementary Note 2. Detailed calculations for CISSPT

  12. [12]

    Notation for Green functions

  13. [13]

    Calculation for the renormalized phonon frequency

  14. [14]

    The case with explicit spin-orbit couplings

  15. [15]

    Gap equation of the spin-selective Peierls states

  16. [16]

    Resultant orders in CISSPT

  17. [17]

    Derivation of collective excitations

    Commensurability effect in CISSPT Supplementary Note 3. Derivation of collective excitations

  18. [18]

    On transverse Peierls transitions and chiral charge density waves

    Calculation of phason and amplitudon frequencies Supplementary Note 4. On transverse Peierls transitions and chiral charge density waves

  19. [19]

    Transverse Peierls transitions in chiral crystals

  20. [20]

    Collective excitations and angular momentum flow

  21. [21]

    Coexistence of CISSPT and winding charge density wave

  22. [22]

    Details of the formulations

    Extension to transverse Peierls transitions in achiral crystals Reference 2 Supplementary Note 1. Details of the formulations. In this Supplementary note, we explain the details of our formulation, which includes the characteristics of the pseudo- angular momentum (PAM) and the effective electron-phonon coupling (EPC). We here setℏ= 1and all the angular m...

  23. [23]

    We consider a crystalline system preserving an-fold screw symmetry ˆSn = [ ˆCn|c/n ] along thez-axis, where ˆCn is an-fold rotation around thez-axis andcis a lattice vector alongz

    Definition of pseudo-angular momentum. We consider a crystalline system preserving an-fold screw symmetry ˆSn = [ ˆCn|c/n ] along thez-axis, where ˆCn is an-fold rotation around thez-axis andcis a lattice vector alongz. The Hamiltonian ˆH, ˆSn, and the translation operator along thez-axis ˆTc are all commutative: [ ˆH, ˆSn] = [ ˆH, ˆTc] = [ ˆSn, ˆTc] = 0....

  24. [24]

    In the previous section, we introduced the PAM defined by screw symmetry

    Selection rule of pseudo-angular momentum. In the previous section, we introduced the PAM defined by screw symmetry. Here, we provide an overview of the conservation laws of the PAM between the initial and final states through the interaction process. Hereafter, as in the main text, we consider wave vectors such ask= (0,0,k), and the indexzis omitted for ...

  25. [25]

    Bir-Pikus formalism. In the elementary formulation, the Fr¨ ohlich Hamiltonian is commonly used to describe the EPC, incorporating only the effect of the periodic potential modulated by lattice displacements. However, the modified lattice potential can exert a crucial influence on electrons via the SOC. Several previous studies derived the EPC that takes ...

  26. [26]

    Figure S1 illustrates how the PAM classifies electronic bands with the three-fold screw symmetry and the possible Peierls instabilities

    Pseudo-angular momenta in the electronic bands. Figure S1 illustrates how the PAM classifies electronic bands with the three-fold screw symmetry and the possible Peierls instabilities. Figure S1a shows the spinless case, where the PAM takes integer values. On the other hand, Figure S1b shows the spinful case with negligible SOC, in which the PAM is a half...

  27. [27]

    In this section, we briefly describe the basic notation for later calculations using the Green function [28]

    Notations for Green functions. In this section, we briefly describe the basic notation for later calculations using the Green function [28]. Regarding the phonon Green function, the expectation value⟨ˆζq,ηˆζq′,η′⟩is finite only for time-reversal paired indices, that is, whenq′=−qand η′=−η; otherwise, it vanishes. Therefore, the phonon Green function is de...

  28. [28]

    We describe in detail the method for calculating the renormalized phonon frequencies

    Calculations for the renormalized phonon frequency. We describe in detail the method for calculating the renormalized phonon frequencies. We begin by deriving the general form of the phonon self-energy [29]. The renormalized phonon frequency under the random phase approximation (RPA) can be evaluated from the Feynman diagrams shown in Fig. S2. The Green f...

  29. [29]

    In the main text and Methods, the formulations in the previous section are used to obtain the renormalized phonon frequencies with spin-degenerate electrons

    The case with explicit electronic spin-orbit couplings. In the main text and Methods, the formulations in the previous section are used to obtain the renormalized phonon frequencies with spin-degenerate electrons. We here show that the same argument can be extended to the case with the electron Hamiltonian including the explicit SOC term. Let us consider ...

  30. [30]

    In this section, we note the detailed calculations for incommensurate spin-selective Peierls states

    Gap equation of spin-selective Peierls states. In this section, we note the detailed calculations for incommensurate spin-selective Peierls states. We consider spin-degenerate electron bands under the parabolic approximation for simplicity. The energy dispersion in the parent phase is given by ξk = (ℏ2k2 2me −εF ) δss′.(S.18) Under these approximations, t...

  31. [31]

    Resultant orders in CISSPT. The spin density order per unit length (usingℏ/2as the unit) can be expressed using the inverse Fourier transform as ⟨ˆS(z)⟩=1 Ni ⟨∑ q ˆSqeiqz ⟩ ,(S.41) from which we obtain ⟨ˆSx(z)⟩=1 2Ni [⣨ ˆS(+) −Q ⟩ e−iQz+c.c. ] (S.42) =−|∆| 2πℏvF Λ cos(Qz+ϕ),(S.43) and ⟨ˆSy(z)⟩=1 2Ni [ −i ⣨ ˆS(+) −Q ⟩ e−iQz+c.c. ] (S.44) = |∆| 2πℏvF Λ sin(...

  32. [32]

    We have so far considered the physical properties realized by CISSPT with an incommensurate wave vectorQ

    Commensurability effect in CISSPT. We have so far considered the physical properties realized by CISSPT with an incommensurate wave vectorQ. In conven- tional CDWs and SDWs, it is well established that commensurability—whenQforms a rational fraction of the lattice period- icity—qualitatively modifies the nature of the ordered state [29, 32–38]. For exampl...

  33. [33]

    Among them, the phason mode is of particular importance, as it underlies the sliding mo- tion [29, 32, 33, 35, 39–41]

    Calculations of phason and amplitudon frequencies In conventional CDWs and SDWs, the primary collective excitations are phase fluctuations (phason) and amplitude fluctuations (amplitudon) of the density wave. Among them, the phason mode is of particular importance, as it underlies the sliding mo- tion [29, 32, 33, 35, 39–41]. In CDWs, owing to the couplin...

  34. [34]

    We first mention that the EPC of Eq

    Transverse Peierls transitions in chiral crystals. We first mention that the EPC of Eq. (S.70) is equivalent to that derived from the tight-binding model in Ref. [2], both satisfying the conservation law of total PAM. Unlike the transverse Peierls transition discussed in Ref. [15], the phonon dispersions here remain intrinsically non-degenerate because we...

  35. [35]

    Collective excitations and angular momentum transport The above formulation can be straightforwardly extended to the discussion of the collective excitations associated with the ordered phase. Importantly, since the lattice displacement fieldδutakes exactly the same form as in the CISSPT of the main text, the dynamical properties of the collective modes d...

  36. [36]

    Coexistence of CISSPT and chiral charge density wave order We comment on the possible coexistence of CISSPT and chiral CDWs. At the most fundamental level, the selection rule imposed by the conservation law of the total PAM is lPAM,el =l′ PAM,el +ls PAM,ph modn,(S.90) which we assumed to be decoupled as morb +s=m ′ orb +s′+l ph z,λ modn.(S.91) Depending o...

  37. [37]

    Throughout this article, we have focused on chiral crystals, where the screw symmetry endows the electrons and phonons with well-defined pseudo angular momentum

    Extension to transverse Peierls transitions in achiral crystals. Throughout this article, we have focused on chiral crystals, where the screw symmetry endows the electrons and phonons with well-defined pseudo angular momentum. This symmetry guarantees strict selection rules, and the resulting coupling between electronic bands and chiral phonons naturally ...

  38. [38]

    X. Wang, Y . Xian, and Y . Yan, Chiral electrons and spin selectivity at chiral-achiral interfaces (2024), arXiv:2306.01664 [cond-mat.mtrl- sci]

  39. [39]

    Tateishi, A

    T. Tateishi, A. Kato, and J.-i. Kishine, Electron–chiral phonon coupling, crystal angular momentum, and phonon chirality, Journal of the Physical Society of Japan94, 053601 (2025)

  40. [40]

    Bo ˇzovic, Possible band-structure shapes of quasi-one-dimensional solids, Phys

    I. Bo ˇzovic, Possible band-structure shapes of quasi-one-dimensional solids, Phys. Rev. B29, 6586 (1984)

  41. [41]

    Izumida, K

    W. Izumida, K. Sato, and R. Saito, Spin–orbit interaction in single wall carbon nanotubes: Symmetry adapted tight-binding calculation and effective model analysis, Journal of the Physical Society of Japan78, 074707 (2009)

  42. [42]

    Gos ´albez-Mart´ınez, A

    D. Gos ´albez-Mart´ınez, A. Crepaldi, and O. V . Yazyev, Diversity of radial spin textures in chiral materials, Phys. Rev. B108, L201114 (2023)

  43. [43]

    Sakano, M

    M. Sakano, M. Hirayama, T. Takahashi, S. Akebi, M. Nakayama, K. Kuroda, K. Taguchi, T. Yoshikawa, K. Miyamoto, T. Okuda, K. Ono, H. Kumigashira, T. Ideue, Y . Iwasa, N. Mitsuishi, K. Ishizaka, S. Shin, T. Miyake, S. Murakami, T. Sasagawa, and T. Kondo, Radial spin texture in elemental tellurium with chiral crystal structure, Phys. Rev. Lett.124, 136404 (2020)

  44. [44]

    J. A. Krieger, S. Stolz, I. Robredo, K. Manna, E. C. McFarlane, M. Date, B. Pal, J. Yang, E. B. Guedes, J. H. Dil, C. M. Polley, M. Leandersson, C. Shekhar, H. Borrmann, Q. Yang, M. Lin, V . N. Strocov, M. Caputo, M. D. Watson, T. K. Kim, C. Cacho, F. Mazzola, J. Fujii, I. V obornik, S. S. P. Parkin, B. Bradlyn, C. Felser, M. G. Vergniory, and N. B. M. Sc...

  45. [45]

    Chang, B

    G. Chang, B. J. Wieder, F. Schindler, D. S. Sanchez, I. Belopolski, S.-M. Huang, B. Singh, D. Wu, T.-R. Chang, T. Neupert, S.-Y . Xu, H. Lin, and M. Z. Hasan, Topological quantum properties of chiral crystals, Nature Materials17, 978 (2018)

  46. [46]

    Ishito, H

    K. Ishito, H. Mao, Y . Kousaka, Y . Togawa, S. Iwasaki, T. Zhang, S. Murakami, J.-i. Kishine, and T. Satoh, Truly chiral phonons inα-hgs, Nature Physics19, 35 (2023)

  47. [47]

    Zhang and S

    T. Zhang and S. Murakami, Chiral phonons and pseudoangular momentum in nonsymmorphic systems, Phys. Rev. Res.4, L012024 (2022)

  48. [48]

    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 (2025), arXiv:2506.13721 [cond-mat.mtrl-sci]

  49. [49]

    Zhang, Z

    S. Zhang, Z. Huang, M. Du, T. Ying, L. Du, and T. Zhang, Comprehensive study of phonon chirality under symmetry constraints (2025), arXiv:2503.22794 [cond-mat.mtrl-sci]

  50. [50]

    H. Zhu, J. Yi, M.-Y . Li, J. Xiao, L. Zhang, C.-W. Yang, R. A. Kaindl, L.-J. Li, Y . Wang, and X. Zhang, Observation of chiral phonons, Science359, 579 (2018)

  51. [51]

    X. Chen, X. Lu, S. Dubey, Q. Yao, S. Liu, X. Wang, Q. Xiong, L. Zhang, and A. Srivastava, Entanglement of single-photons and chiral phonons in atomically thin wse2, Nature Physics15, 221 (2019)

  52. [52]

    Luo and X

    K. Luo and X. Dai, Transverse peierls transition, Phys. Rev. X13, 011027 (2023)

  53. [53]

    G. L. Bir and G. E. Pikus, Symmetry and strain-induced effects in semiconductors (Wiley, 1974)

  54. [54]

    Fransson, Chiral phonon induced spin polarization, Phys

    J. Fransson, Chiral phonon induced spin polarization, Phys. Rev. Res.5, L022039 (2023)

  55. [55]

    Fransson, Vibrational origin of exchange splitting and ”chiral-induced spin selectivity, Phys

    J. Fransson, Vibrational origin of exchange splitting and ”chiral-induced spin selectivity, Phys. Rev. B102, 235416 (2020)

  56. [56]

    D. S. L. Abergel and V . I. Fal’ko, Spin-orbit-assisted electron-phonon interaction and the magnetophonon resonance in semiconductor quantum wells, Phys. Rev. B77, 035317 (2008)

  57. [57]

    Kumar, P

    A. Kumar, P. Chandra, and P. A. V olkov, Spin-phonon resonances in nearly polar metals with spin-orbit coupling, Phys. Rev. B105, 125142 (2022)

  58. [58]

    Kumar, P

    A. Kumar, P. Chandra, and P. A. V olkov, Phonon-induced collective modes in spin-orbit coupled polar metals, Phys. Rev. B108, 075162 (2023)

  59. [59]

    Tsunetsugu and H

    H. Tsunetsugu and H. Kusunose, Theory of energy dispersion of chiral phonons, Journal of the Physical Society of Japan92, 023601 (2023)

  60. [60]

    Kato and J.-i

    A. Kato and J.-i. Kishine, Note on angular momentum of phonons in chiral crystals, Journal of the Physical Society of Japan92, 075002 (2023)

  61. [61]

    T. Wang, H. Sun, X. Li, and L. Zhang, Chiral phonons: Prediction, verification, and application, Nano Letters24, 4311 (2024)

  62. [62]

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

  63. [63]

    H. Chen, W. Wu, J. Zhu, Z. Yang, W. Gong, W. Gao, S. A. Yang, and L. Zhang, Chiral phonon diode effect in chiral crystals, Nano Letters 22, 1688 (2022)

  64. [64]

    Kishine, A

    J. Kishine, A. S. Ovchinnikov, and A. A. Tereshchenko, Chirality-induced phonon dispersion in a noncentrosymmetric micropolar crystal, Phys. Rev. Lett.125, 245302 (2020)

  65. [65]

    A. A. Abrikosov, I. Dzyaloshinskii, L. P. Gorkov, and R. A. Silverman, Methods of quantum field theory in statistical physics (Dover, New York, NY , 1975)

  66. [66]

    Gr ¨uner, Density Waves In Solids, 1st ed

    G. Gr ¨uner, Density Waves In Solids, 1st ed. (CRC Press, 1994)

  67. [67]

    Manchon, H

    A. Manchon, H. C. Koo, J. Nitta, S. M. Frolov, and R. A. Duine, New perspectives for rashba spin–orbit coupling, Nature Materials14, 28 871 (2015)

  68. [68]

    Galitski and I

    V . Galitski and I. B. Spielman, Spin–orbit coupling in quantum gases, Nature494, 49 (2013)

  69. [69]

    Gr ¨uner, The dynamics of charge-density waves, Rev

    G. Gr ¨uner, The dynamics of charge-density waves, Rev. Mod. Phys.60, 1129 (1988)

  70. [70]

    Gr ¨uner, The dynamics of spin-density waves, Rev

    G. Gr ¨uner, The dynamics of spin-density waves, Rev. Mod. Phys.66, 1 (1994)

  71. [71]

    P. M. and, Electronic crystals: an experimental overview, Advances in Physics61, 325 (2012)

  72. [72]

    Gr ¨uner and A

    G. Gr ¨uner and A. Zettl, Charge density wave conduction: A novel collective transport phenomenon in solids, Physics Reports119, 117 (1985)

  73. [73]

    A. J. Berlinsky, One-dimensional metals and charge density wave effects in these materials, Reports on Progress in Physics42, 1243 (1979)

  74. [74]

    Radi ´c, Charge density waves in solids—from first concepts to modern insights, Symmetry17, 10.3390/sym17071135 (2025)

    D. Radi ´c, Charge density waves in solids—from first concepts to modern insights, Symmetry17, 10.3390/sym17071135 (2025)

  75. [75]

    Fawcett, Spin-density-wave antiferromagnetism in chromium, Rev

    E. Fawcett, Spin-density-wave antiferromagnetism in chromium, Rev. Mod. Phys.60, 209 (1988)

  76. [76]

    H. Seo, C. Hotta, and H. Fukuyama, Toward systematic understanding of diversity of electronic properties in low-dimensional molecular solids, Chemical Reviews104, 5005 (2004)

  77. [77]

    Fukuyama and P

    H. Fukuyama and P. A. Lee, Dynamics of the charge-density wave. i. impurity pinning in a single chain, Phys. Rev. B17, 535 (1978)

  78. [78]

    P. Lee, T. Rice, and P. Anderson, Conductivity from charge or spin density waves, Solid State Communications14, 703 (1974)

  79. [79]

    Bliokh, I

    K. Bliokh, I. Ivanov, G. Guzzinati, L. Clark, R. Van Boxem, A. B ´ech´e, R. Juchtmans, M. Alonso, P. Schattschneider, F. Nori, and J. Verbeeck, Theory and applications of free-electron vortex states, Physics Reports690, 1 (2017), theory and applications of free-electron vortex states

  80. [80]

    S. M. Lloyd, M. Babiker, G. Thirunavukkarasu, and J. Yuan, Electron vortices: Beams with orbital angular momentum, Rev. Mod. Phys. 89, 035004 (2017)

Showing first 80 references.