Pith. sign in

REVIEW 2 major objections 5 minor 36 references

Lattice-induced spin dynamics in Dirac magnet CoTiO3

T0 review · 2 major / 5 minor · reviewed 2026-08-15 · deepseek-v4-flash

Challenge this review Re-run · record.json Download PDF Read on arXiv ↗ Review JSON

Pith's one-line read Resonant THz excitation of phonons in the antiferromagnet CoTiO3 produces coherent magnon dynamics and a slow, surface-driven magneto-optic response tied to magnetic order.

desk verdict A credible new THz pump-probe result on CoTiO3 with a plausible magnon assignment that is not fully pinned down; the slow magnetic-order-dependent rotation is the more robust finding. read the letter →

arxiv 2508.20354 v1 pith:22ZBFBQU submitted 2025-08-28 cond-mat.mtrl-sci cond-mat.otherphysics.optics

Andrey Baydin , Jiaming Luo , Zhiren He , Jacques Doumani , Tong Lin , Fuyang Tay , Jiaming He , Jianshi Zhou
show 3 more authors
Guru Khalsa Junichiro Kono Hanyu Zhu
This is my paper · ORCID
classification cond-mat.mtrl-scicond-mat.otherphysics.optics
keywords light-drivenphononsmagnonsspin-latticecouplingtime-resolvedmagneto-opticspectroscopyCoTiO3antiferromagnetTHzpump-probe
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper reports that THz pulses tuned to lattice vibrations in the antiferromagnet CoTiO3 drive coherent spin dynamics: resonantly excited phonons and phonon-polaritons excite the 1.3 THz antiferromagnetic magnon, and a slow polarization rotation of an optical probe grows over hundreds of picoseconds, well beyond the pulse duration and the coherent phonon and magnon lifetimes. The slow rotation appears only below the Néel temperature, grows linearly with pump fluence, and is nearly independent of pump polarization, so the authors take it to be magnetic in origin. Because bulk CoTiO3 has no net out-of-plane magnetic moment, they argue that the response requires symmetry breaking extrinsic to the bulk magnetic space group, most plausibly a surface spin Seebeck effect in which THz heating creates a thermal gradient that drives a magnon spin current into the bulk. If this picture is right, light can control magnetic order through the lattice, and surface degrees of freedom can dominate nominally bulk light-driven spin phenomena in complex oxides.

What carries the argument

The central objects are THz-driven phonon-polaritons and the surface spin Seebeck mechanism. Phonon-polaritons couple the pump field to lattice displacement through infrared-active $E_u$ modes; near a transverse-optical phonon the dielectric response diverges, maximizing atomic displacement, which in turn modifies exchange interactions and excites the 1.3 THz magnon. The slow signal is modeled as a spin current $\mathbf{J}_s = \kappa \nabla T$ generated by the thermal gradient at the symmetry-reduced surface; the heat-kernel solution of the 1D diffusion equation gives an accumulated magnetization proportional to $\sqrt{t}$, matching the observed slow rise and the linear fluence dependence.

What would settle it

Measure the slow component in a CoTiO3 thin film, or with a pump geometry that removes the surface thermal gradient by heating uniformly through the thickness; the 1D spin Seebeck model predicts the sqrt(t) accumulation should vanish or change sign when the surface gradient is removed, while a nonmagnetic birefringence origin would persist.

Watch

Extended reading notes

Core claim

The central claim is that resonant THz excitation of infrared-active phonons in CoTiO3 sets off a chain: phonon-polariton excitation produces coherent antiferromagnetic magnon oscillations at 1.3 THz, together with a slow, magnetic-order-dependent magneto-optic rotation whose amplitude follows a $\sqrt{t}$ law matching a one-dimensional heat-diffusion model of spin accumulation driven by a surface thermal gradient. This is surprising because the easy-plane antiferromagnet's bulk magnetic space group forbids a net out-of-plane magnetization, which normal-incidence Faraday rotation would require. The authors therefore propose that the surface, where the magnetic space group is reduced, upholds a weak out-of-plane moment; the THz-induced temperature gradient generates a magnon spin current whose accumulated flux produces the observed long-lived rotation. They also find that the coherent magnon is strongest when the pump is near the transverse-optical phonon frequencies, and that the high-frequency response tracks Raman-active phonon modes, indicating phonon-mediated excitation pathways.

Load-bearing premise

The slow rotation is assumed to be a Faraday rotation caused by a net out-of-plane magnetization accumulated at the surface, rather than a pump-induced birefringence, reflectivity change, or another nonmagnetic optical effect.

Editorial extensions

If this is right

  • In CoTiO3, lattice excitation by THz light is an effective handle on antiferromagnetic spin dynamics: resonant phonon-polariton driving produces coherent magnon oscillations and a long-lived magnetic response.
  • The slow magneto-optic response below the Néel temperature implies that light-driven spin phenomena in nominally bulk complex oxides can carry a strong extrinsic surface contribution, complicating interpretations based on bulk symmetry alone.
  • The observed $\sqrt{t}$ accumulation and linear fluence dependence are consistent with a magnon spin Seebeck current driven by a surface thermal gradient, so the surface acts as a spin-current source under THz illumination.
  • Distinguishing chiral-phonon from spin-Seebeck mechanisms calls for thin-film samples that remove the thermal gradient; the model predicts the slow component should disappear or change character there.
  • The pump-polarization dependence of the slow signal points to an additional strain-gradient or birefringence contribution with the same polar-vector symmetry as the thermal gradient, leaving an experimental route to separate the two.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Beyond the paper: if the surface spin Seebeck picture holds, the same THz protocol should generate a detectable spin-current signal in other easy-plane antiferromagnets with surface-allowed weak moments, and the sign of the accumulated rotation should track the pump penetration depth and surface termination.
  • Beyond the paper: the linear-polarization anisotropy in the slow signal could be tested directly by shaping the pump spot to create a controlled asymmetric thermal gradient and checking whether the slow rotation direction follows the gradient direction.
  • Beyond the paper: applying a small out-of-plane magnetic field near the surface would settle the magnetic origin of the slow component, since a Faraday rotation from accumulated out-of-plane magnetization should respond to the field once local anisotropy pinning is overcome, whereas a birefringence artifact would not.
Share X Bluesky LinkedIn Reddit HN

Signed reviews

No signed human review yet.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

2 major / 5 minor

Summary. The manuscript reports time-resolved THz pump–optical probe measurements on bulk CoTiO3. Below the Néel temperature, the pump produces (i) a coherent 1.3 THz oscillation attributed to the Γ-point antiferromagnetic magnon, (ii) high-frequency oscillations near 7.2, 8.1, and 10.2 THz attributed to Raman-active phonons excited through phonon-polariton coupling, and (iii) a slow, long-lived increase in the probe polarization rotation that scales linearly with fluence and appears only in the antiferromagnetic phase. The authors propose that the slow signal arises from a surface-driven spin Seebeck effect and describe it with a 1D heat-diffusion model, while explicitly acknowledging other possible mechanisms. Supporting density-functional-theory phonon calculations and SpinW magnon calculations are presented in the appendix.

Significance. If the mode assignments are correct, the work provides time-domain evidence for phonon-polariton-driven spin dynamics in a Dirac magnet and shows that extrinsic symmetry breaking (surface or penetration-depth effects) can dominate the magneto-optic response of a nominally compensated antiferromagnet. The paper is careful in several places to label the slow-signal mechanism as a suggestion rather than a proof, and it includes explicit calculations of phonon and magnon spectra. The main significance, however, hinges on the unambiguous identification of the 1.3 THz coherent mode as a magnon and on the exclusion of nonmagnetic contributions to the slow polarization rotation.

major comments (2)
  1. [Appendix IV A, Fig. 5] The assignment of the 1.3 THz coherent mode to the Γ-point magnon is not unique. The authors' own phonon calculation (Fig. 5) shows that zone-folding of acoustic branches brings modes near 1.3–1.5 THz to the zone center; such a folded acoustic phonon would also appear only below TN and could be excited via anharmonic coupling to the resonantly driven IR phonons. The Appendix dismisses this alternative with the statement that the folded phonon's Raman activity 'should be very weak' compared to the magnons, but no calculation, symmetry estimate, or measurement is provided. Because the central conclusion that phonon-polariton excitation drives antiferromagnetic magnon dynamics rests on this identification, the manuscript needs either a quantitative estimate of the folded-phonon Raman/magneto-optic response or a magnetic-field-dependent measurement that tracks the known magnon frequency. Without one of these, the evidence is not uniquely supportive of the magnon assignment.
  2. [Section II, after Fig. 4] The slow polarization rotation is interpreted as a Faraday rotation from a net out-of-plane magnetization, but nonmagnetic contributions have not been experimentally excluded. The text itself states that Faraday rotation is 'one possible source' and later acknowledges strain-gradient birefringence as an alternative, yet the abstract and conclusion present the slow signal as a magneto-optic response with a spin origin. A polarization-resolved measurement that separates Faraday rotation from pump-induced linear birefringence, or a magnetic-field test, is needed to support the surface spin Seebeck interpretation. As written, the slow-signal feature is consistent with the proposed mechanism but does not uniquely establish it.
minor comments (5)
  1. [Section II, Eq. (1)] The fit parameters τ_rise and τ_decay are not reported, and the slow-component subtraction is not shown; please provide these values so the FFT decomposition can be reproduced.
  2. [Fig. 3(a) caption] The caption 'Polarization rotation for different center frequencies of the THz pump maximized when the reflectivity of the crystal is the lowest' is incomplete; it should state the plotted quantity and normalization. Also, the √t fits with amplitudes a = 36.4, 15.7, 2.7 are mentioned in the text but are not visible in the figure.
  3. [Section II, heat-diffusion model] The x0→0 limit is used to obtain the √t scaling without discussing whether the finite THz penetration depth is indeed negligible on the measured picosecond-to-hundreds-of-picosecond time window; please either justify this limit or show the finite-x0 solution for the relevant parameters.
  4. [Figs. 3(c) and 4(b)] No error bars or repeated-measurement statistics are provided for the fluence dependence, the angular dependence, or the relative amplitudes of the √t fits; given that several conclusions rely on quantitative comparisons, please add at least representative uncertainty estimates.
  5. [Appendix Table I] The DFT phonon frequencies in Table I are not directly compared with the experimental IR frequencies (8.6 THz and 12.5 THz) cited in the text; a side-by-side comparison would clarify the level of agreement.

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity: magnon identification and slow dynamics rest on external data and an analytic model, not on fitted inputs.

full rationale

The paper's central claims do not reduce to their inputs. The 1.3 THz feature is assigned to the antiferromagnetic magnon by frequency matching to externally measured THz-TDS data (Ref. 16) and to magnon dispersions computed from exchange parameters of Yuan et al. (Ref. 10); no magnon frequency is fit in this work. The high-frequency oscillations are assigned to Raman phonons by comparison with published phonon frequencies (Ref. 15). The slow polarization rotation is modeled with a 1D heat-diffusion equation whose sqrt(t) time dependence is derived analytically, and only the overall amplitude is fitted per pump frequency; the linear fluence dependence is also derived and compared with data. Self-citations (Refs. 16, 13, 7, 19) are prior measurements, calculations, or methods, not the present result, and they serve as independent empirical evidence outside the paper's fitted values. The Appendix does acknowledge the alternative that zone-folded acoustic phonons could appear near 1.3 THz, and its dismissal relies on the prior field-dependent magnon response of Ref. 16; this is a limitation in evidence strength or a correctness risk, not a circular reduction, because the cited field dependence is an external observable not defined by the present paper. No equation is equivalent to its input by construction, and no fitted parameter is renamed as a prediction. Therefore the derivation is self-contained with respect to circularity.

Assumptions & free parameters 3 free parameters · 5 assumptions · 0 invented entities

The paper introduces no new particles, fields, or conserved quantities. Its central claim rests on standard model parameters, prior characterization of CoTiO3, and a proposed surface spin Seebeck mechanism that is explicitly tentative.

free parameters (3)
  • Hubbard U for Co 3d = 3.5 eV
    Chosen in DFT to reproduce the experimental ~2.4 eV bandgap; it affects the calculated phonon frequencies used to assign the 7.2, 8.1, and 10.2 THz features.
  • A, tau_rise, tau_decay from Eq. (1) = not reported
    Equation (1) is fit to each trace to remove the slow component before Fourier analysis; the values and uncertainties are not tabulated, so the magnon peak position in the FFT depends on an unreported background subtraction.
  • Relative amplitudes of sqrt(t) fits = 36.4, 15.7, 2.7 (arbitrary units)
    Amplitude scale factors for the slow-rise curves at 11, 13, and 8 THz pump frequencies; these are fitted to data and are not physically constrained.
assumptions (5)
  • domain assumption Surface symmetry reduction to P1 permits a net ferromagnetic component and a weak out-of-plane moment.
    Location: Section II, "At the surface, the symmetry is reduced to P1 from Pbar{1}.1'c in the bulk... A weak out-of-plane moment is still expected to appear due to out-of-plane symmetry breaking." This is a postulate about the surface magnetic structure, not a measured property.
  • domain assumption The linear spin Seebeck relation J_s = kappa * grad(T) operates in this antiferromagnet, and the resulting spin current accumulates as a detectable magnetization.
    Location: Section II, "The imbalance of opposite spins at the surface will then lead to a net spin current induced by a thermal gradient, i.e. J_s = kappa * grad(T), and carried by the magnon." This relies on Ref. 22 theory without direct confirmation in CoTiO3.
  • domain assumption Bulk CoTiO3 has no net out-of-plane magnetic moment in its magnetic space group, so any out-of-plane Faraday rotation requires additional symmetry breaking.
    Location: Section II, "The net spin is expected to be in-plane... the observation of polarization rotation of a normal-incident probe pulse requires additional symmetry breaking." This follows from the known magnetic structure and symmetry analysis, not from an in-situ measurement of the moment.
  • standard math The 1D heat equation solution with a Dirichlet boundary and an exponential initial temperature profile describes the surface temperature evolution.
    Location: Section II and Appendix-model paragraph; the solution is taken from Carslaw and Jaeger, Ref. 23, and is a standard application of the heat kernel.
  • domain assumption SpinW linear spin wave theory with exchange parameters from Yuan et al. (Ref. 10) correctly represents the 1.3 THz magnon mode.
    Location: Appendix A; the identification of the 1.3 THz oscillation as a magnon relies on this prior model and on THz-TDS data from Ref. 16.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Lattice-induced spin dynamics in Dirac magnet CoTiO3." pith.science (2026). https://pith.science/paper/22ZBFBQU

@misc{pith2026250820354,
  author       = {Pith},
  title        = {Pith review of: Lattice-induced spin dynamics in Dirac magnet CoTiO3},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/22ZBFBQU}},
  note         = {Machine review of arXiv:2508.20354}
}
read the original abstract

Spin-lattice coupling is crucial for understanding the spin transport and dynamics for spintronics and magnonics applications. Recently, cobalt titanate (CoTiO3), an easy-plane antiferromagnet, has been found to host axial phonons with a large magnetic moment, which may originate from spin-lattice coupling. Here, we investigate the effect of light-driven lattice dynamics on the magnetic properties of CoTiO3 using time-resolved spectroscopy with a THz pump and a magneto-optic probe. We found resonantly driven Raman active phonons, phonon-polariton-induced excitation of the antiferromagnetic magnons, and a slow increase in the polarization rotation of the probe, all indicating symmetry breaking that is not intrinsic to the magnetic space group. The temperature dependence confirmed that the observed spin dynamics is related to the magnetic order, and we suggest surface effects as a possible mechanism. Our results of THz-induced spin-lattice dynamics signify that extrinsic symmetry breaking may contribute strongly and unexpectedly to light-driven phenomena in bulk complex oxides.

Figures

Figures reproduced from arXiv: 2508.20354 by the authors.

Figure 2
Figure 2. FIG. 2. (a) Polarization rotation signal in the frequency do [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 4
Figure 4. FIG. 4. (a) The polarization rotation signal for different po [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 3
Figure 3. FIG. 3. Polarization rotation for different center frequencies [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figures from the paper (1 more)
Figure 5
Figure 5. Figure 5: FIG. 5. Calculated phonon and magnon dispersion along high [PITH_FULL_IMAGE:figures/full_fig_p006_5.png]

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

36 extracted references · 16 canonical work pages

  1. [1]

    author author L. J. \ Cornelissen , author K. Oyanagi , author T. Kikkawa , author Z. Qiu , author T. Kuschel , author G. E. W. \ Bauer , author B. J. \ van Wees ,\ and\ author E. Saitoh ,\ title title Nonlocal magnon-polaron transport in yttrium iron garnet , \ https://doi.org/10.1103/PhysRevB.96.104441 journal journal Phys. Rev. B \ volume 96 ,\ pages 1...

    doi:10.1103/physrevb.96.104441

  2. [2]

    Zhang , author Y

    author author X. Zhang , author Y. Zhang , author S. Okamoto ,\ and\ author D. Xiao ,\ title title Thermal Hall Effect Induced by Magnon - Phonon Interactions , \ https://doi.org/10.1103/PhysRevLett.123.167202 journal journal Phys. Rev. Lett. \ volume 123 ( year 2019 ),\ 10.1103/PhysRevLett.123.167202 NoStop

    work page doi:10.1103/physrevlett.123.167202

  3. [3]

    Streib , author N

    author author S. Streib , author N. Vidal-Silva , author K. Shen ,\ and\ author G. E. W. \ Bauer ,\ title title Magnon-phonon interactions in magnetic insulators , \ https://doi.org/10.1103/PhysRevB.99.184442 journal journal Phys. Rev. B \ volume 99 ,\ pages 184442 ( year 2019 ) NoStop

    doi:10.1103/physrevb.99.184442

  4. [4]

    Sivarajah , author A

    author author P. Sivarajah , author A. Steinbacher , author B. Dastrup , author J. Lu , author M. Xiang , author W. Ren , author S. Kamba , author S. Cao ,\ and\ author K. A. \ Nelson ,\ title title THz -frequency magnon-phonon-polaritons in the collective strong-coupling regime , \ https://doi.org/10.1063/1.5083849 journal journal J. Appl. Phys. \ volume...

    work page doi:10.1063/1.5083849

  5. [5]

    author author D. A. \ Bozhko , author V. I. \ Vasyuchka , author A. V. \ Chumak ,\ and\ author A. A. \ Serga ,\ title title Magnon-phonon interactions in magnon spintronics , \ https://doi.org/10.1063/10.0000872 journal journal Low Temp. Phys. \ volume 46 ,\ pages 383--399 ( year 2020 ) NoStop

    doi:10.1063/10.0000872

  6. [6]

    Hioki , author Y

    author author T. Hioki , author Y. Hashimoto ,\ and\ author E. Saitoh ,\ title title Coherent oscillation between phonons and magnons , \ https://doi.org/10.1038/s42005-022-00888-1 journal journal Commun. Phys. \ volume 5 ,\ pages 1--8 ( year 2022 ) NoStop

    doi:10.1038/s42005-022-00888-1

  7. [7]

    Luo , author S

    author author J. Luo , author S. Li , author Z. Ye , author R. Xu , author H. Yan , author J. Zhang , author G. Ye , author L. Chen , author D. Hu , author X. Teng , author W. A. \ Smith , author B. I. \ Yakobson , author P. Dai , author A. H. \ Nevidomskyy , author R. He ,\ and\ author H. Zhu ,\ title title Evidence for Topological Magnon – Phonon Hybrid...

    work page doi:10.1021/acs.nanolett.3c00351

  8. [8]

    Liao , author J

    author author L. Liao , author J. Liu , author J. Puebla , author Q. Shao ,\ and\ author Y. Otani ,\ title title Hybrid magnon-phonon crystals , \ https://doi.org/10.1038/s44306-024-00052-1 journal journal npj Spintronics \ volume 2 ,\ pages 1--6 ( year 2024 ) NoStop

    work page doi:10.1038/s44306-024-00052-1

Show all 36 references
  1. [9]

    author author T. F. \ Nova , author A. Cartella , author A. Cantaluppi , author M. Först , author D. Bossini , author R. V. \ Mikhaylovskiy , author A. V. \ Kimel , author R. Merlin ,\ and\ author A. Cavalleri ,\ title title An effective magnetic field from optically driven ph...

    doi

  2. [10]

    Yuan , author I

    author author B. Yuan , author I. Khait , author G.-J. \ Shu , author F. C. \ Chou , author M. B. \ Stone , author J. P. \ Clancy , author A. Paramekanti ,\ and\ author Y.-J. \ Kim ,\ title title Dirac magnons in a honeycomb lattice quantum xy magnet CoTiO3 , \ https://doi.org...

    doi

  3. [11]

    Elliot , author P

    author author M. Elliot , author P. A. \ McClarty , author D. Prabhakaran , author R. D. \ Johnson , author H. C. \ Walker , author P. Manuel ,\ and\ author R. Coldea ,\ title title Order-by-disorder from bond-dependent exchange and intensity signature of nodal quasiparticles ...

    2021

  4. [12]

    Chaudhary , author D

    author author S. Chaudhary , author D. M. \ Juraschek , author M. Rodriguez-Vega ,\ and\ author G. A. \ Fiete ,\ title title Giant effective magnetic moments of chiral phonons from orbit-lattice coupling , \ https://doi.org/10.1103/PhysRevB.110.094401 journal journal Phys. Rev...

    doi

  5. [13]

    Lujan , author J

    author author D. Lujan , author J. Choe , author S. Chaudhary , author G. Ye , author C. Nnokwe , author M. Rodriguez-Vega , author J. He , author F. Y. \ Gao , author T. N. \ Nunley , author E. Baldini , author J. Zhou , author G. A. \ Fiete , author R. He ,\ and\ author X. L...

    doi

  6. [14]

    author author T. T. \ Mai , author Y. Li , author K. F. \ Garrity , author D. Shaw , author T. DeLazzer , author R. L. \ Dally , author T. Adel , author M. F. \ Mu\ noz , author A. Giovannone , author C. Lyon , author A. Pawbake , author C. Faugeras , author F. Le Mardele , au...

  7. [15]

    Dubrovin , author N

    author author R. Dubrovin , author N. Siverin , author M. Prosnikov , author V. Chernyshev , author N. Novikova , author P. Christianen , author A. Balbashov ,\ and\ author R. Pisarev ,\ title title Lattice dynamics and spontaneous magnetodielectric effect in ilmenite CoTiO3 ,...

  8. [16]

    Choe , author A

    author author J. Choe , author A. Baydin , author G. Ye , author B. Ma , author C. Nnokwe , author M. Rodriguez-Vega , author D. Lujan , author S. Chaudhary , author F. Tay , author J. He , author H. Nojiri , author J. Zhou , author G. A. \ Fiete , author J. Kono , author R. H...

    doi

  9. [17]

    Liu , author H

    author author B. Liu , author H. Bromberger , author A. Cartella , author T. Gebert , author M. Först ,\ and\ author A. Cavalleri ,\ title title Generation of narrowband, high-intensity, carrier-envelope phase-stable pulses tunable between 4 and 18 THz , \ https://doi.org/10.1...

    doi

  10. [18]

    Lin , author R

    author author T. Lin , author R. Xu , author X. Chen , author Y. Guan , author M. Yao , author J. Zhang , author X. Li ,\ and\ author H. Zhu ,\ title title Subwavelength, Phase - Sensitive Microscopy of Third - Order Nonlinearity in Terahertz Frequencies , \ https://doi.org/10...

    doi

  11. [19]

    Luo , author T

    author author J. Luo , author T. Lin , author J. Zhang , author X. Chen , author E. R. \ Blackert , author R. Xu , author B. I. \ Yakobson ,\ and\ author H. Zhu ,\ title title Large effective magnetic fields from chiral phonons in rare-earth halides , \ https://doi.org/10.1126...

    doi

  12. [20]

    Hoffmann , author K

    author author M. Hoffmann , author K. Dey , author J. Werner , author R. Bag , author J. Kaiser , author H. Wadepohl , author Y. Skourski , author M. Abdel-Hafiez , author S. Singh ,\ and\ author R. Klingeler ,\ title title Magnetic phase diagram, magnetoelastic coupling, and ...

    doi

  13. [21]

    author author D. M. \ Juraschek , author T. Neuman ,\ and\ author P. Narang ,\ title title Giant effective magnetic fields from optically driven chiral phonons in 4f paramagnets , \ https://doi.org/10.1103/PhysRevResearch.4.013129 journal journal Physical Review Research \ vol...

    doi

  14. [22]

    Adachi , author K.-i

    author author H. Adachi , author K.-i. \ Uchida , author E. Saitoh ,\ and\ author S. Maekawa ,\ title title Theory of the spin seebeck effect , \ https://doi.org/10.1088/0034-4885/76/3/036501 journal journal Rep. Prog. Phys. \ volume 76 ,\ pages 036501 ( year 2013 ) NoStop

    doi

  15. [23]

    author author H. S. \ Carslaw \ and\ author J. C. \ Jaeger ,\ title Conduction of heat in solids , \ \ ( publisher Oxford University Press ,\ year 1959 )\ Chap.\ chapter 2.4 , pp.\ pages 58--62 NoStop

    1959

  16. [24]

    Schoofs , author M

    author author F. Schoofs , author M. Egilmez , author T. Fix , author J. L. \ MacManus-Driscoll ,\ and\ author M. G. \ Blamire ,\ title title Structural and magnetic properties of CoTiO3 thin films on SrTiO3 (001) , \ https://doi.org/10.1016/j.jmmm.2012.12.017 journal journal ...

    doi

  17. [25]

    Kresse \ and\ author J

    author author G. Kresse \ and\ author J. Hafner ,\ title title Ab initio molecular dynamics for liquid metals , \ https://doi.org/10.1103/PhysRevB.47.558 journal journal Physical Review B \ volume 47 ,\ pages 558--561 ( year 1993 ) NoStop

    doi

  18. [26]

    Kresse \ and\ author J

    author author G. Kresse \ and\ author J. Hafner ,\ title title Ab initio molecular-dynamics simulation of the liquid-metal--amorphous-semiconductor transition in germanium , \ https://doi.org/10.1103/PhysRevB.49.14251 journal journal Phys. Rev. B \ volume 49 ,\ pages 14251--14...

    doi

  19. [27]

    Kresse \ and\ author J

    author author G. Kresse \ and\ author J. Furthmüller ,\ title title Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set , \ https://doi.org/10.1016/0927-0256(96)00008-0 journal journal Computational Materials Science \ v...

    doi

  20. [28]

    Kresse \ and\ author J

    author author G. Kresse \ and\ author J. Furthm\"uller ,\ title title Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set , \ https://doi.org/10.1103/PhysRevB.54.11169 journal journal Phys. Rev. B \ volume 54 ,\ pages 11169--11186 (...

    doi

  21. [29]

    author author P. E. \ Bl\"ochl ,\ title title Projector augmented-wave method , \ https://doi.org/10.1103/PhysRevB.50.17953 journal journal Phys. Rev. B \ volume 50 ,\ pages 17953--17979 ( year 1994 ) NoStop

    1994 doi

  22. [30]

    author author J. P. \ Perdew , author A. Ruzsinszky , author G. I. \ Csonka , author O. A. \ Vydrov , author G. E. \ Scuseria , author L. A. \ Constantin , author X. Zhou ,\ and\ author K. Burke ,\ title title Restoring the density-gradient expansion for exchange in solids and...

    doi

  23. [31]

    author author S. L. \ Dudarev , author G. A. \ Botton , author S. Y. \ Savrasov , author C. J. \ Humphreys ,\ and\ author A. P. \ Sutton ,\ title title Electron-energy-loss spectra and the structural stability of nickel oxide: An LSDA+U study , \ https://doi.org/10.1103/PhysRe...

    doi

  24. [32]

    Agui \ and\ author M

    author author A. Agui \ and\ author M. Mizumaki ,\ title title Intermetallic charge transfer and band gap of MTiO3 ( M=Mn, Fe, Co, and Ni ) studied by o 1s-edge X -ray emission spectroscopy , \ https://doi.org/10.1016/j.elspec.2011.06.001 journal journal J. Electron Spectrosc....

    doi

  25. [33]

    author author R. E. \ Newnham , author J. H. \ Fang ,\ and\ author R. P. \ Santoro ,\ title title Crystal structure and magnetic properties of CoTiO3 , \ https://doi.org/10.1107/S0365110X64000615 journal journal Acta Crystallogr. \ volume 17 ,\ pages 240--242 ( year 1964 ) NoStop

    doi

  26. [34]

    Togo , author L

    author author A. Togo , author L. Chaput , author T. Tadano ,\ and\ author I. Tanaka ,\ title title Implementation strategies in phonopy and phono3py , \ https://doi.org/10.1088/1361-648X/acd831 journal journal J. Phys. Condens. Matter \ volume 35 ,\ pages 353001 ( year 2023 ) NoStop

    doi

  27. [35]

    Togo ,\ title title First-principles phonon calculations with phonopy and phono3py , \ https://doi.org/10.7566/JPSJ.92.012001 journal journal J

    author author A. Togo ,\ title title First-principles phonon calculations with phonopy and phono3py , \ https://doi.org/10.7566/JPSJ.92.012001 journal journal J. Phys. Soc. Jpn. \ volume 92 ,\ pages 012001 ( year 2023 ) NoStop

    2023 doi

  28. [36]

    Toth \ and\ author B

    author author S. Toth \ and\ author B. Lake ,\ title title Linear spin wave theory for single-q incommensurate magnetic structures , \ https://doi.org/10.1088/0953-8984/27/16/166002 journal journal J. Phys.: Condens. Matter \ volume 27 ,\ pages 166002 ( year 2015 ) NoStop

    doi

Pith tools

Reviewed August 15, 2026 · model on record in the stance chip above.