Pith. sign in

REVIEW 2 major objections 2 minor 64 references

Topological Lifshitz transition-induced bipolarity of anomalous Nernst effect in kagome magnet YCo3

T0 review · 2 major / 2 minor · reviewed 2026-06-29 · grok-4.3

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

Pith's one-line read Temperature-driven Lifshitz transition reverses the anomalous Nernst sign in YCo3

desk verdict The paper reports a temperature-driven sign flip in the anomalous Nernst coefficient of YCo3 near 100 K that tracks a slope change in anomalous Hall conductivity, with the link to a Lifshitz transition resting on DFT node placement. read the letter →

arxiv 2605.29297 v1 pith:ROTVF2KV submitted 2026-05-28 cond-mat.mtrl-sci

Sheng Xu , Yue-Yang Wu , Hao-Ran Bai , Zheng Li , Shu-Xiang Li , Jun-Jian Mi , Tian-Hao Li , Ze-Wei Wang
show 5 more authors
Ze-Kai Dong Jiang Ma Xiao-Bo Wu Qian Tao Zhu-An Xu
This is my paper · ORCID
classification cond-mat.mtrl-sci
keywords kagomemagnetanomalousNernsteffecttopologicalLifshitztransitionWeylnodesYCo3Hallconductivitybipolarthermoelectric
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 shows that in the kagome magnet YCo3 the anomalous Nernst coefficient changes sign near 100 K as temperature rises. This reversal arises because the evolving magnetic moments on cobalt atoms shift the Fermi level across Weyl nodes in the band structure, triggering a topological Lifshitz transition. A sympathetic reader would care because sign reversal enables bipolar thermoelectric devices that can be controlled by magnetism rather than external fields. The intrinsic nature of the effect is supported by the piecewise linear dependence of anomalous Hall conductivity on magnetization and by first-principles calculations.

What carries the argument

Topological Lifshitz transition: a change in Fermi-surface topology when temperature-tuned magnetization moves the Fermi level across Weyl nodes.

What would settle it

ARPES data or refined calculations showing the Fermi level does not cross a Weyl node near 100 K while the sign reversal still occurs, or the reversal vanishing when magnetization is held fixed.

Watch

Extended reading notes

Core claim

The central claim is that the bipolarity of the anomalous Nernst effect in YCo3, manifested as the sign reversal of the anomalous Nernst coefficient SAyx around 100 K, results from a temperature-induced topological Lifshitz transition. This transition is enabled by the temperature evolution of Co moments that shift the Fermi level relative to the Weyl nodes. The anomalous Hall and Nernst effects are dominated by the intrinsic mechanism, with the anomalous Hall conductivity showing a piecewise-linear dependence on magnetization consistent with the Karplus-Luttinger mechanism.

Load-bearing premise

The first-principles calculations correctly locate the Weyl nodes and Fermi level so their relative motion with temperature produces the observed sign reversal rather than extrinsic scattering or unrelated band evolution.

Share X Bluesky LinkedIn Reddit HN

Editorial analysis

A structured set of objections, weighed in public.

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

Referee Report

2 major / 2 minor

Summary. The manuscript reports experimental observation of sizable anomalous Hall and Nernst effects below TC ~ 225 K in the kagome magnet YCo3. The anomalous Hall conductivity shows a piecewise-linear dependence on magnetization with an abrupt slope change near 100 K, while the anomalous Nernst coefficient SAyx reverses sign at the same temperature. First-principles calculations are invoked to argue for an intrinsic (Karplus-Luttinger) mechanism, and the anomalies are suggested to arise from a temperature-induced topological Lifshitz transition in which Co-moment evolution shifts the Fermi level relative to Weyl nodes.

Significance. If the topological assignment holds, the result would demonstrate direct magnetic control over the sign of the anomalous Nernst effect via a Lifshitz transition in a kagome system, offering a route to bipolar thermoelectric response. The combination of transport data with DFT band-structure input is a standard approach in the field, but the strength of the conclusion rests entirely on the accuracy of the calculated node positions and moment-induced shifts.

major comments (2)
  1. [Discussion / first-principles section] The central claim that the observed ~100 K anomalies constitute a Lifshitz transition at Weyl nodes is load-bearing for the title and abstract interpretation. The manuscript must supply the calculated energies of the relevant Weyl nodes relative to EF together with the magnitude of the EF shift induced by the measured change in Co moment between 50 K and 150 K; without these numbers it is impossible to verify that a node crossing or van-Hove feature occurs on the experimental temperature scale.
  2. [Discussion] Typical DFT errors in absolute band positions are 0.1–0.5 eV. The paper should therefore test the robustness of the Lifshitz assignment by shifting the calculated Fermi level or node energies within this window and showing that the sign reversal and slope change remain consistent with the data only for the reported node placement.
minor comments (2)
  1. [Abstract] The abstract uses the cautious phrasing “could be interpreted”; the main text should maintain the same level of qualification when stating the Lifshitz scenario.
  2. [Figures] Figure captions and axis labels for the temperature-dependent SAyx and σxy data should explicitly state the measurement geometry and the definition of the anomalous Nernst coefficient to avoid ambiguity with the ordinary Nernst term.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the detailed and constructive report. The two major comments correctly identify that the manuscript currently lacks explicit numerical values for the Weyl-node energies and the moment-induced Fermi-level shift, as well as a robustness test against typical DFT uncertainties. We address both points below and will revise the manuscript accordingly.

read point-by-point responses

  1. Referee: [Discussion / first-principles section] The central claim that the observed ~100 K anomalies constitute a Lifshitz transition at Weyl nodes is load-bearing for the title and abstract interpretation. The manuscript must supply the calculated energies of the relevant Weyl nodes relative to EF together with the magnitude of the EF shift induced by the measured change in Co moment between 50 K and 150 K; without these numbers it is impossible to verify that a node crossing or van-Hove feature occurs on the experimental temperature scale.

    Authors: We agree that the absence of these explicit numbers weakens the quantitative support for the Lifshitz-transition interpretation. In the revised manuscript we will report the DFT-computed energies of the relevant Weyl nodes relative to EF together with the calculated Fermi-level shift arising from the measured change in Co moment between 50 K and 150 K, thereby allowing direct verification that the crossing occurs on the experimental temperature scale. revision: yes

  2. Referee: [Discussion] Typical DFT errors in absolute band positions are 0.1–0.5 eV. The paper should therefore test the robustness of the Lifshitz assignment by shifting the calculated Fermi level or node energies within this window and showing that the sign reversal and slope change remain consistent with the data only for the reported node placement.

    Authors: We acknowledge that typical DFT errors must be addressed. In the revision we will add a robustness analysis in which the Fermi level (or node energies) is shifted by ±0.1–0.5 eV; we will demonstrate that the qualitative features of the anomalous-Hall slope change and Nernst sign reversal remain consistent with experiment only when the nodes are placed near the reported position. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No circularity; experimental transport data and external DFT support tentative Lifshitz interpretation without internal reduction.

full rationale

The paper reports measured sign reversal of the anomalous Nernst coefficient SAyx near 100 K together with a piecewise-linear change in anomalous Hall conductivity, both below TC ~225 K. It states that these features 'could be interpreted as a topological Lifshitz transition' enabled by Co-moment evolution shifting EF relative to Weyl nodes, with the intrinsic mechanism 'suggested' by first-principles calculations. No equation or claim reduces a derived quantity to a fitted parameter by construction, nor does any load-bearing premise rest on a self-citation chain; the Lifshitz reading is offered as one possible reading of independent experimental and cited computational results rather than a self-contained prediction.

Assumptions & free parameters 0 free parameters · 1 assumptions · 0 invented entities

The central claim rests on the accuracy of first-principles calculations for the band structure of YCo3 and on the assumption that the observed transport anomalies arise from the proposed Lifshitz transition; no explicit free parameters or new entities are introduced in the abstract.

assumptions (1)
  • domain assumption First-principles calculations correctly locate the Weyl nodes and describe the temperature evolution of the Fermi level relative to them in YCo3.
    Invoked to interpret the sign reversal and slope change as a Lifshitz transition.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Topological Lifshitz transition-induced bipolarity of anomalous Nernst effect in kagome magnet YCo3." pith.science (2026). https://pith.science/paper/ROTVF2KV

@misc{pith2026260529297,
  author       = {Pith},
  title        = {Pith review of: Topological Lifshitz transition-induced bipolarity of anomalous Nernst effect in kagome magnet YCo3},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/ROTVF2KV}},
  note         = {Machine review of arXiv:2605.29297}
}
read the original abstract

The kagome lattice, renowned for hosting topological band structures and rich magnetic behaviors, offers an exceptional setting to investigate unconventional transport in magnetic topological systems. Controlling the polarity of the anomalous Nernst effect (ANE) is crucial for designing flexible thermoelectric devices, such as thermopiles, where the ability to switch the thermoelectric voltage sign can dramatically enhance energy conversion efficiency and output. Here, we demonstrate such a bipolar ANE in the kagome magnet YCo3, driven by a temperature-induced topological Lifshitz transition. With a Curie temperature TC~225 K, sizable anomalous Hall and Nernst effects emerge below TC. Supported by the first-principles calculations, the AHE and ANE are suggested to be dominated by the intrinsic mechanism. Furthermore, the intrinsic anomalous Hall conductivity exhibits a piecewise-linear dependence on magnetization, with an abrupt slope change near 100 K, consistent with the Karplus-Luttinger mechanism. Concurrently, the anomalous Nernst coefficient SAyx reverses its sign around the same temperature, realizing the crucial bipolarity. These anomalies could be interpreted as a topological Lifshitz transition, enabled by the evolution of Co moments that could shift the Fermi level relative to Weyl nodes. Our work reveals YCo3 as a prototypical kagome magnet where temperature and magnetism directly govern both Weyl node topology and the bipolar ANE, opening a pathway to magnetically control thermoelectric output in topological quantum materials.

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

64 extracted references · 1 canonical work pages

  1. [1]

    Complex Thermoelectric Materials,

    G. J. Snyder and E. S. Toberer, “Complex Thermoelectric Materials,” Nature Materials 7 (2008): 105–114

    2008

  2. [2]

    Potential of Thermoelectric Power Generation Using Anomalous Nernst Effect in Magnetic Materials,

    Y. Sakuraba, “Potential of Thermoelectric Power Generation Using Anomalous Nernst Effect in Magnetic Materials,” Scripta Materialia 111 (2016): 29–32

    2016

  3. [3]

    Topological Thermoelectrics,

    C. Fu, Y. Sun, and C. Felser, “Topological Thermoelectrics,” APL Materials 8 (2020): 040913

    2020

  4. [4]

    Thermoelectrics: From Longitudinal to Transverse,

    K. Uchida and J. P. Heremans, “Thermoelectrics: From Longitudinal to Transverse,” Joule 6 (2022): 2240–2245

    2022

  5. [5]

    Bipolarity of Large Anomalous Nernst Effect in Weyl Magnet-Based Alloy Films,

    S. Noguchi, K. Fujiwara, Y. Yanagi, et al., “Bipolarity of Large Anomalous Nernst Effect in Weyl Magnet-Based Alloy Films,” Nature Physics 20 (2024): 254–260

    2024

  6. [6]

    Topological Insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a Single Dirac Cone on the Surface,

    H. Zhang, C.-X. Liu, X.-L. Qi, X. Dai, Z. Fang, and S.-C. Zhang, “Topological Insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a Single Dirac Cone on the Surface,” Nature Physics 5 (2009): 438

    2009

  7. [7]

    Topological Semimetal and Fermi-arc Surface States in the Electronic Structure of Pyrochlore Iridates,

    X. Wan, A. M. Turner, A. Vishwanath, and S. Y. Savrasov, “Topological Semimetal and Fermi-arc Surface States in the Electronic Structure of Pyrochlore Iridates,” Physical Review B 83 (2011): 205101

    2011

  8. [8]

    Topological Nodal Semimetals,

    A. A. Burkov, M. D. Hook, and L. Balents, “Topological Nodal Semimetals,” Physical Review B 84 (2011): 235126

    2011

Show all 64 references
  1. [9]

    Dirac Semimetal and Topological Phase Transitions in A3Bi (A=Na, K, Rb),

    Z. Wang, Y. Sun, X.-Q. Chen, et al., “Dirac Semimetal and Topological Phase Transitions in A3Bi (A=Na, K, Rb),” Physical Review B 85 (2012): 195320

    2012

  2. [10]

    Large Intrinsic Anomalous Hall Effect in Half-Metallic Ferromagnet Co3Sn2S2 with Magnetic Weyl Fermions,

    Q. Wang, Y. Xu, R. Lou, et al., “Large Intrinsic Anomalous Hall Effect in Half-Metallic Ferromagnet Co3Sn2S2 with Magnetic Weyl Fermions,” Nature Communications 9 (2018): 3681

    2018

  3. [11]

    Giant Anomalous Hall Effect in a Ferromagnetic Kagome-Lattice Semimetal,

    E. Liu, Y. Sun, N. Kumar, et al., “Giant Anomalous Hall Effect in a Ferromagnetic Kagome-Lattice Semimetal,” Nature Physics 14 (2018): 1125

    2018

  4. [12]

    Zero-Field Nernst Effect in a Ferromagnetic Kagome-Lattice Weyl-Semimetal Co3Sn2S2,

    S. N. Guin, P. Vir, Y. Zhang, et al., “Zero-Field Nernst Effect in a Ferromagnetic Kagome-Lattice Weyl-Semimetal Co3Sn2S2,” Advanced Materials 31 (2019): 1806622

    2019

  5. [13]

    Large Anomalous Nernst Effect at Room Temperature in a Chiral Antiferromagnet,

    M. Ikhlas, T. Tomita, T. Koretsune, et al., “Large Anomalous Nernst Effect at Room Temperature in a Chiral Antiferromagnet,” Nature Physics 13 (2017): 1085

    2017

  6. [14]

    Intrinsic Anomalous Nernst Effect Amplified by Disorder in a Half-Metallic Semimetal,

    L. Ding, J. Koo, L. Xu, et al., “Intrinsic Anomalous Nernst Effect Amplified by Disorder in a Half-Metallic Semimetal,” Physical Review X 9 (2019): 041061

    2019

  7. [15]

    High-Performance Bulk Thermoelectrics with All-Scale Hierarchical Architectures,

    K. Biswas, J. He, I. D. Blum, et al., “High-Performance Bulk Thermoelectrics with All-Scale Hierarchical Architectures,” Nature 489 (2012): 414

    2012

  8. [16]

    Ultralow Thermal Conductivity and High Thermoelectric Figure of Merit in SnSe Crystals,

    L.-D. Zhao, S.-H. Lo, Y. Zhang, et al., “Ultralow Thermal Conductivity and High Thermoelectric Figure of Merit in SnSe Crystals,” Nature 508 (2014): 373

    2014

  9. [17]

    Tetradymites as Thermoelectrics and Topological Insulators,

    J. P. Heremans, R. J. Cava, and N. Samarth, “Tetradymites as Thermoelectrics and Topological Insulators,” Nature Reviews Materials 2 (2017): 17049

    2017

  10. [18]

    Advancesin Thermoelectric Materials Research: Looking Back and Moving Forward,

    J. He and T. M. Tritt, “Advancesin Thermoelectric Materials Research: Looking Back and Moving Forward,” Science 357 (2017): eaak9997

    2017

  11. [19]

    High Thermoelectric Cooling Performance of n-type Mg3Bi2-Based Materials,

    J. Mao, H. Zhu, Z. Ding, et al., “High Thermoelectric Cooling Performance of n-type Mg3Bi2-Based Materials,” Science 365 (2019): 495

    2019

  12. [20]

    Pressure-Tunable Large Anomalous Hall Effect of the Ferromagnetic Kagome-Lattice Weyl Semimetal Co3Sn2S2,

    X. L. Chen, M. Y. Wang, C. C. Gu, et al., “Pressure-Tunable Large Anomalous Hall Effect of the Ferromagnetic Kagome-Lattice Weyl Semimetal Co3Sn2S2,” Physical Review B 100 (2019): 165145

    2019

  13. [21]

    Experimental Observation of the Quantum Anomalous Hall Effect in a Magnetic Topological,

    C.-Z. Chang, J. Zhang, X. Feng, et al., “Experimental Observation of the Quantum Anomalous Hall Effect in a Magnetic Topological,” Science 340 (2013): 167–170

    2013

  14. [22]

    Trajectory of the Anomalous Hall Effect Towards the Quantized State in a Ferromagnetic Topological Insulator,

    J. G. Checkelsky, R. Yoshimi, A. Tsukazaki, K. S. Takahashi,Y. Kozuka, J. Falson, M. Kawasaki, and Y. Tokura, “Trajectory of the Anomalous Hall Effect Towards the Quantized State in a Ferromagnetic Topological Insulator,” Nature Physics 10 (2014): 731–736

    2014

  15. [23]

    Large Anomalous Hall Effect in a Non-Collinear Antiferromagnet at Room Temperature,

    S. Nakatsuji, N. Kiyohara, and T. Higo, “Large Anomalous Hall Effect in a Non-Collinear Antiferromagnet at Room Temperature,” Nature 527 (2015): 212

    2015

  16. [24]

    Evidence for Magnetic Weyl Fermions in a Correlated Metal,

    K. Kuroda, T. Tomita, M. T. Suzuki, et al., “Evidence for Magnetic Weyl Fermions in a Correlated Metal,” Nature Materials 16 (2017): 1090

    2017

  17. [25]

    Quantum-Limit Chern Topological Magnetism in TbMn6Sn6,

    J.-X. Yin, W. Ma, T. A. Cochran, et al., “Quantum-Limit Chern Topological Magnetism in TbMn6Sn6,” Nature 583 (2020): 533

    2020

  18. [26]

    Anomalous Nernst and Righi-Leduc Effects in Mn3Sn: Berry Curvature and Entropy Flow,

    X. Li, L. Xu, L. Ding, et al., “Anomalous Nernst and Righi-Leduc Effects in Mn3Sn: Berry Curvature and Entropy Flow,” Physical Review Letters 119 (2017): 056601

    2017

  19. [27]

    Anomalous Transport Due to Weyl Fermionsin the Chiral Antiferromagnets Mn3X, X=Sn, Ge,

    T. Chen, T. Tomita, S. Minami, et al., “Anomalous Transport Due to Weyl Fermionsin the Chiral Antiferromagnets Mn3X, X=Sn, Ge,” Nature Communications 12 (2021): 572

    2021

  20. [28]

    Large Room Temperature Anomalous Transverse Thermoelectric Effect in Kagome Antiferromagnet YMn6Sn6,

    S. Roychowdhury, A. M. Ochs, S. N. Guin, et al., “Large Room Temperature Anomalous Transverse Thermoelectric Effect in Kagome Antiferromagnet YMn6Sn6,” Advanced Materials 34 (2022): 2201350

    2022

  21. [29]

    Berry Curvature Unravelled by the Anomalous Nernst effect in Mn3Ge,

    C. Wuttke, F. Caglieris, S. Sykora, et al., “Berry Curvature Unravelled by the Anomalous Nernst effect in Mn3Ge,” Physical Review B 100 (2019): 085111

    2019

  22. [30]

    ExchangeBiased Topological Transverse Thermoelectric Effects in a Kagome ferrimagnet,

    H. Zhang, J. Koo, C. Xu, M. Sretenovic, B. Yan, and X. Ke, “ExchangeBiased Topological Transverse Thermoelectric Effects in a Kagome ferrimagnet,” Nature Communications 13 (2022): 1091

    2022

  23. [31]

    Massive Dirac Fermions in a Ferromagnetic Kagome Metal,

    L. Ye, M. Kang, J. Liu, et al., “Massive Dirac Fermions in a Ferromagnetic Kagome Metal,” Nature 555 (2018): 638

    2018

  24. [32]

    Topological Nernst Effect, Anomalous Nernst Effect, and Anomalous Thermal Hall Effect in the Dirac Semimetal Fe3Sn2,

    H. Zhang, C. Q. Xu, and X. Ke, “Topological Nernst Effect, Anomalous Nernst Effect, and Anomalous Thermal Hall Effect in the Dirac Semimetal Fe3Sn2,” Physical Review B 103 (2021): L201101

    2021

  25. [33]

    Iron-Based Binary Ferromagnets for Transverse Thermoelectric Conversion,

    A. Sakai, S. Minami, T. Koretsune, et al., “Iron-Based Binary Ferromagnets for Transverse Thermoelectric Conversion,” Nature 581 (2020): 53

    2020

  26. [34]

    Angle-Dependent Magnetoresistance and itsImplicationsfor Lifshitz Transition in W2As3,

    J. Wang, H. Yang, L. Ding, et al., “Angle-Dependent Magnetoresistance and itsImplicationsfor Lifshitz Transition in W2As3,” npj Quantum Materials 4 (2019): 58

    2019

  27. [35]

    Large Nernst Effect and Possible Temperature-Induced Lifshitz Transition in Topological Semimetal YbMnSb2,

    S. Xu, C. Jiang, S.-X. Li, J.-J. Mi, et al., “Large Nernst Effect and Possible Temperature-Induced Lifshitz Transition in Topological Semimetal YbMnSb2,” Physical Review B 107 (2023): 245138

    2023

  28. [36]

    Itinerant Electron Metamagnetism and Magnetic Anisotropy in the Y(Co1−xFex)3 System,

    M. I. Bartashevich, T. Goto, and K. Koui, “Itinerant Electron Metamagnetism and Magnetic Anisotropy in the Y(Co1−xFex)3 System,” Physica B: Condensed Matter 292 (2000): 9

    2000

  29. [37]

    Magnetic Phase Relations of RCo,

    Q. He and Y. Guo, “Magnetic Phase Relations of RCo,” IEEE Transactions on Magnetics 51 (2015): 1

    2015

  30. [38]

    Polarized-Neutron-Diffraction Study of Magnetic Moments in Yttrium-Cobalt Alloys,

    E. Kren, J. Schweizer, and F. Tasset, “Polarized-Neutron-Diffraction Study of Magnetic Moments in Yttrium-Cobalt Alloys,” Physical Review 186 (1969): 479

    1969

  31. [39]

    Thermal Expansion and High Field Magnetization of a Single Crystal γ-Phase HydrideYCo3H3.9,

    M. I. Bartashevich, T. Goto, M. Yamaguchi, I. Yamamoto, and A. V. Andreev, “Thermal Expansion and High Field Magnetization of a Single Crystal γ-Phase HydrideYCo3H3.9,” Solid State Communications 82 (1992): 201

    1992

  32. [40]

    Magnetic Anisotropy in RCo3 (R = Lu and Y) Single Crystals,

    D. S. Neznakhin, A. M. Bartashevich, A. S. Volegov, M. I. Bartashevich, and A. V. Andreev, “Magnetic Anisotropy in RCo3 (R = Lu and Y) Single Crystals,” Journal of Magnetism and Magnetic Materials 539 (2021): 168367

    2021

  33. [41]

    Hall Effect in Ferromagnetics,

    R. Karplus and J. M. Luttinger, “Hall Effect in Ferromagnetics,” Physical Review 95 (1954): 1154–1160

    1954

  34. [42]

    Efficiency of Ab-Initio Total Energy Calculations for Metals and Semiconductors Using a Plane-Wave Basis Set,

    G. Kresse and J. Furthmüller, “Efficiency of Ab-Initio Total Energy Calculations for Metals and Semiconductors Using a Plane-Wave Basis Set,” Journal of Computational Materials Science 6 (1996): 15

    1996

  35. [43]

    EfficientIterative Schemesfor Ab Initio Total-Energy Calculations Using a Plane-Wave Basis Set,

    G. Kresse and J. Furthmüller, “EfficientIterative Schemesfor Ab Initio Total-Energy Calculations Using a Plane-Wave Basis Set,” Physical Review B 54 (1996): 11169

    1996

  36. [44]

    Inhomogeneous Electron Gas,

    P. Hohenberg and W. Kohn, “Inhomogeneous Electron Gas,” Physical Review 136 (1964): B864

    1964

  37. [45]

    Self-Consistent Equations Including Exchange and Correlation,

    W. Kohn and L. J. Sham, “Self-Consistent Equations Including Exchange and Correlation,” Physical Review 140 (1965): A1133

    1965

  38. [46]

    Generalized Gradient Approximation Made Simple,

    J. P. Perdew, K. Burke, and M. Ernzerhof, “Generalized Gradient Approximation Made Simple,” Physical Review Letters 77 (1996): 3865

    1996

  39. [47]

    Villars, PAULINGFILE in: Inorganic Solid Phases, SpringerMaterials (2016)

    P. Villars, PAULINGFILE in: Inorganic Solid Phases, SpringerMaterials (2016)

    2016

  40. [48]

    Evolution of the Magnetic Behavior of the Co Subsystem in YCo3 Caused by Small Variations in Stoichiometry and Al Substitution,

    I. Dubenko, I. Y. Gaidukova, A. S. Markosyan, et al., “Evolution of the Magnetic Behavior of the Co Subsystem in YCo3 Caused by Small Variations in Stoichiometry and Al Substitution,” Journal of Alloys and Compounds 303 (2000): 285

    2000

  41. [49]

    Crystal Structure and Magnetic Properties of V-doped YCo2 and YCo3 and Their Hydrides,

    H. Michor, G. Hilscher, O. Myakush, et al., “Crystal Structure and Magnetic Properties of V-doped YCo2 and YCo3 and Their Hydrides,” Journal of Alloys and Compounds 509 (2011): 5200

    2011

  42. [50]

    Co Metamagnetism in Y1−xNdxCo3 Under Ultra-High Magnetic Field,

    K. Koui, M. I. Bartashevich, T. Goto, H. Aruga Katori, and M. Yamaguchi, “Co Metamagnetism in Y1−xNdxCo3 Under Ultra-High Magnetic Field,” Physica B: Condensed Matter 201 (1994): 143

    1994

  43. [51]

    Temperature Induced Itinerant Electron Metamagnetism in ErCo3 and HoCo3: Influence of an External Field and Pressure,

    E. Gratz, A. S. Markosyan, I. Yu. Gaidukova, et al., “Temperature Induced Itinerant Electron Metamagnetism in ErCo3 and HoCo3: Influence of an External Field and Pressure,” Solid State Communications 120 (2001): 191

    2001

  44. [52]

    Itinerant Metamagnetic Transition in the Ferromagnet LuCo3 Induced by High Field: Instability of the 3-Electron Subsystem,

    D. S. Neznakhin, D. I. Radzivonchik, D. I. Gorbunov, et al., “Itinerant Metamagnetic Transition in the Ferromagnet LuCo3 Induced by High Field: Instability of the 3-Electron Subsystem,” Physical Review B 101 (2020): 224432

    2020

  45. [53]

    Influence of Hydrogen on the Magnetic Properties of Y Co Compounds,

    M. Yamaguchi, H. Ikeda, T. Ohta, et al., “Influence of Hydrogen on the Magnetic Properties of Y Co Compounds,” Journal of the Less Common Metals 106 (1985): 165

    1985

  46. [54]

    Linear Magnetization Dependence of the Intrinsic Anomalous Hall Effect,

    C. Zeng, Y. Yao, Q. Niu, and H. H. Weitering, “Linear Magnetization Dependence of the Intrinsic Anomalous Hall Effect,” Physical Review Letters 96 (2006): 037204

    2006

  47. [55]

    A Simple Theory of the Anomalous Hall Effect in Semiconductors,

    P. Nozières and C. Lewiner, “A Simple Theory of the Anomalous Hall Effect in Semiconductors,” Journal de Physique 34 (1973): 901–915

    1973

  48. [56]

    Intrinsic Versus Extrinsic Anomalous Hall Effect in Ferromagnets,

    S. Onoda, N. Sugimoto, and N. Nagaosa, “Intrinsic Versus Extrinsic Anomalous Hall Effect in Ferromagnets,” Physical Review Letters 97 (2006): 126602

    2006

  49. [57]

    Giant Anomalous Nernst Effect and Quantum-Critical Scaling in a Ferromagnetic Semimetal,

    A. Sakai, Y. P. Mizuta, A. A. Nugroho, et al., “Giant Anomalous Nernst Effect and Quantum-Critical Scaling in a Ferromagnetic Semimetal,” Nature Physics 14 (2018): 1119

    2018

  50. [58]

    Anomalous Nernst Effect in Honeycomb and Kagome Magnet LaCo5 at Room Temperature,

    S. Xu, L. Zhou, S.-X. Li, X.-Y. Zeng, et al., “Anomalous Nernst Effect in Honeycomb and Kagome Magnet LaCo5 at Room Temperature,” Materials Today Physics 38 (2023): 101269

    2023

  51. [59]

    Giant Anomalous Nernst Signal in the Antiferromagnet YbMnBi2,

    Y. Pan, C. Le, B. He, et al., “Giant Anomalous Nernst Signal in the Antiferromagnet YbMnBi2,” Nature Materials 21 (2022): 203–209

    2022

  52. [60]

    Anomalous Nernst Effect Beyond the Magnetization Scaling Relation in the Ferromagnetic Heusler Compound Co2MnGa,

    S. N. Guin, K. Manna, J. Noky, et al., “Anomalous Nernst Effect Beyond the Magnetization Scaling Relation in the Ferromagnetic Heusler Compound Co2MnGa,” NPG Asia Materials 11 (2019): 16

    2019

  53. [61]

    Topological Quantum ,

    B. Bradlyn, L. Elcoro, J. Cano, et al., “Topological Quantum ,” Nature 547 (2017): 298–305

    2017

  54. [62]

    High-Throughput Calculations of Magnetic Topological Materials,

    Y. Xu, L. Elcoro, Z.-D. Song, et al., “High-Throughput Calculations of Magnetic Topological Materials,” Nature 586 (2020): 702–707

    2020

  55. [63]

    Magnetic Topological Quantum Chemistry,

    L. Elcoro, B. J. Wieder, Z. Song, et al., “Magnetic Topological Quantum Chemistry,” Nature Communications 12 (2021): 5965

    2021

  56. [64]

    New Magnetic Topological Materials from High-Throughput Search,

    I. Robredo, Y. Xu, Y. Jiang, et al., “New Magnetic Topological Materials from High-Throughput Search,” arXiv:2408.16851 (2024). FIGURE 1 (a) and (b) Schematic diagrams of anomalous Nernst effect thermopiles. The bipolar design in (b) increases the thermopile density and transv...

    2024

Pith tools

Reviewed June 29, 2026 · model on record in the stance chip above.