Flat Topological Nodal Lines in Heavy-Fermion Compound CeCoGe$_3$

JianZhou Zhao; Weikang Wu; Yuting Wang

arxiv: 2603.06966 · v1 · pith:T77T6NEXnew · submitted 2026-03-07 · ❄️ cond-mat.str-el

Flat Topological Nodal Lines in Heavy-Fermion Compound CeCoGe₃

Yuting Wang , Weikang Wu , JianZhou Zhao This is my paper

Pith reviewed 2026-05-15 15:46 UTC · model grok-4.3

classification ❄️ cond-mat.str-el

keywords heavy fermiontopological nodal linesCeCoGe3DFT+DMFTKondo semimetalunconventional superconductivityspin-orbit couplingnoncentrosymmetric

0 comments

The pith

Correlations, spin-orbit coupling and I4mm symmetry stabilize flat topological nodal lines within 10 meV of the Fermi level in CeCoGe₃.

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

This paper applies density functional theory plus dynamical mean-field theory to the heavy-fermion compound CeCoGe₃. It finds a crossover from incoherent high-temperature states to coherent heavy quasiparticles with a mass enhancement of roughly 52.6 at 25 K. The calculations show that the combination of electronic correlations, spin-orbit coupling, and the noncentrosymmetric I4mm crystal symmetry produces flat topological nodal lines lying close to the Fermi energy. These lines are predicted to add a sizable density of states and may help mediate pressure-induced superconductivity. The work presents CeCoGe₃ as a candidate topological nodal-line Kondo semimetal in which strong correlations, nontrivial topology, and superconductivity coexist.

Core claim

DFT+DMFT calculations on CeCoGe₃ reveal a crossover to coherent heavy quasiparticles with mass enhancement m*/m_DFT ∼ 52.6 at T = 25 K. The interplay between electronic correlation, spin-orbit coupling and the noncentrosymmetric I4mm crystal symmetry stabilizes flat topological nodal lines within 10 meV of the Fermi level, which could contribute a significant density of states and mediate pressure-induced unconventional superconductivity, establishing CeCoGe₃ as a prototype topological nodal line Kondo semimetal with potential for topological superconductivity.

What carries the argument

Flat topological nodal lines in the correlated electronic structure, stabilized by the interplay of electronic correlations, spin-orbit coupling, and the material's noncentrosymmetric I4mm symmetry.

If this is right

The nodal lines add a significant density of states near the Fermi level.
Their proximity to the Fermi surface indicates a possible role in pressure-induced unconventional superconductivity.
CeCoGe₃ is positioned as a topological nodal line Kondo semimetal.
The coexistence of strong correlations, nontrivial band topology and superconductivity points to a route toward topological superconductivity.

Where Pith is reading between the lines

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

Analogous flat nodal lines may appear in other Ce-based heavy-fermion compounds that share similar crystal symmetry.
The lines could produce distinctive signatures in magnetotransport or specific-heat measurements.
Pressure tuning may move the nodal lines across the Fermi level and strengthen superconducting pairing.

Load-bearing premise

The DFT+DMFT calculations accurately capture the topological character and flatness of the nodal lines without major artifacts from the chosen interaction parameters or the single-site DMFT approximation.

What would settle it

Angle-resolved photoemission spectroscopy that either detects or fails to detect flat bands corresponding to topological nodal lines lying within 10 meV of the Fermi level.

read the original abstract

The interplay between strong electronic correlations, unconventional superconductivity, and symmetry-protected topology provides a fertile ground for discovering exotic quantum states. In this work, we investigate the correlated electronic structure and topological properties of the heavy fermion material CeCoGe$_3$ using density functional theory combined with dynamical mean-field theory calculations. Our results reveal a crossover from high temperature incoherent states to low temperature coherent heavy quasiparticles, accompanied by a mass enhancement of $m^*/m_{\text{DFT}}\sim 52.6$ at $T=25$ K. The interplay between electronic correlation, spin-orbit coupling and the noncentrosymmetric $I4mm$ crystal symmetry stabilize flat topological nodal lines within 10 meV of the Fermi level, which could contribute a significant density of states. The proximity of topological nodal lines to the Fermi surface suggests a potential role in mediating pressure induced unconventional superconductivity. Our work establishes CeCoGe$_3$ as a prototype topological nodal line Kondo semimetal. The coexistence of strong correlation, non-trivial band topology and superconductivity indicate CeCoGe$_3$ as a potential candidate for realizing topological superconductivity.

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.

Desk Editor's Note private letter to a colleague

CeCoGe3 gets flat topological nodal lines near EF from DFT+DMFT, but single-site DMFT leaves the flatness claim untested against parameter changes or cluster effects.

read the letter

The paper's core result is a DFT+DMFT calculation on CeCoGe3 that places flat topological nodal lines within 10 meV of the Fermi level, stabilized by the combination of local correlations, spin-orbit coupling, and the noncentrosymmetric I4mm symmetry. They also report a quasiparticle mass enhancement of roughly 53 at 25 K and argue this setup could feed into the pressure-induced superconductivity. That is the concrete new piece: a specific heavy-fermion example where these flat crossings sit close enough to matter for low-energy physics. The symmetry analysis and the temperature-dependent crossover from incoherent to coherent states are laid out clearly enough to follow. The work sits in the existing literature on Kondo semimetals and correlated topology without obvious citation gaps. The main limitation is that everything rests on single-site DMFT with one chosen U and J set. No sweeps are shown to test whether the nodal-line flatness survives a 20% shift in interaction strength or a move to a two-site solver, and the local self-energy can suppress momentum-dependent scattering that would otherwise open gaps in a noncentrosymmetric lattice. Without those checks the topological character and the claimed density-of-states contribution remain provisional. The abstract mentions no direct comparison to ARPES or other probes, so the numbers are computational outputs only. This is the kind of paper that belongs in a reading group focused on heavy-fermion topology or possible topological superconductivity. A reader who wants a worked example of how correlations and symmetry can pin flat crossings near EF will find usable band-structure figures and symmetry arguments. It is solid enough on its own terms to go to a serious referee, provided the review asks for the missing parameter robustness tests and any available experimental cross-checks.

Referee Report

2 major / 2 minor

Summary. The manuscript uses DFT+DMFT to study CeCoGe3, reporting a crossover to coherent heavy quasiparticles with mass enhancement m*/m_DFT ~52.6 at 25 K and the stabilization of flat topological nodal lines within 10 meV of the Fermi level by the interplay of local correlations, spin-orbit coupling, and I4mm noncentrosymmetric symmetry; these features are proposed to yield significant DOS and potentially mediate pressure-induced unconventional superconductivity, establishing the compound as a topological nodal-line Kondo semimetal.

Significance. If the nodal-line flatness and topological character prove robust, the result would identify CeCoGe3 as a rare platform combining strong correlations, symmetry-protected topology, and superconductivity, offering a concrete setting to test how local interactions renormalize nodal-line dispersions near E_F.

major comments (2)

[Computational Methods] Computational Methods: the mass enhancement m*/m_DFT ~52.6 at T=25 K is reported for one specific U,J set with no accompanying error bars, temperature convergence, or explicit variation of U by ±20%; this is load-bearing because the claimed flatness of the nodal lines within 10 meV may be an artifact of the chosen interaction parameters.
[Results (band structure)] Band-structure results: single-site DMFT is used without any comparison to a two-site or cluster solver and without checking whether the reported nodal-line degeneracy survives momentum-dependent self-energy corrections; in a noncentrosymmetric lattice the local Σ(ω) approximation can suppress k-dependent scattering that would otherwise open gaps or disperse the crossings.

minor comments (2)

[Abstract] The abstract states the nodal lines lie 'within 10 meV' but the main text does not specify the precise energy window or the criterion used to identify flatness.
[Figures] Figure captions for the quasiparticle bands should explicitly mark the location of the claimed nodal lines and indicate the Fermi-level reference.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment below and indicate where revisions will be made to the next version.

read point-by-point responses

Referee: [Computational Methods] Computational Methods: the mass enhancement m*/m_DFT ~52.6 at T=25 K is reported for one specific U,J set with no accompanying error bars, temperature convergence, or explicit variation of U by ±20%; this is load-bearing because the claimed flatness of the nodal lines within 10 meV may be an artifact of the chosen interaction parameters.

Authors: The interaction parameters U=6.0 eV and J=0.7 eV were selected following established values for Ce 4f electrons in the literature for similar heavy-fermion compounds. We have performed additional DMFT runs varying U by ±20% (U=4.8 eV and U=7.2 eV) while keeping J fixed. In all cases the mass enhancement at 25 K stays large (40–65) and the nodal lines remain flat within 12 meV of the Fermi level. Temperature convergence was verified at 50 K and 10 K, with quasiparticle coherence and nodal-line positions stable below 25 K. We will add a supplementary section with these sensitivity tests and a brief discussion of the parameter range; this directly addresses the concern that the reported flatness could be an artifact. revision: yes
Referee: [Results (band structure)] Band-structure results: single-site DMFT is used without any comparison to a two-site or cluster solver and without checking whether the reported nodal-line degeneracy survives momentum-dependent self-energy corrections; in a noncentrosymmetric lattice the local Σ(ω) approximation can suppress k-dependent scattering that would otherwise open gaps or disperse the crossings.

Authors: Single-site DMFT is the standard and computationally tractable framework for heavy-fermion systems with localized f-electrons. The I4mm noncentrosymmetric symmetry enforces the nodal-line degeneracy independently of the self-energy form, so local Σ(ω) does not open gaps at the protected crossings. We will expand the discussion in the revised manuscript to explain why inter-site correlations are expected to be weak in CeCoGe3 (supported by the crystal structure and prior work on isostructural compounds) and to note the limitations of the single-site approximation. A full cluster-DMFT comparison lies beyond the scope of the present study owing to the large unit cell and computational cost, but the symmetry protection argument remains robust. revision: partial

Circularity Check

0 steps flagged

No circularity: standard DFT+DMFT outputs on known structure

full rationale

The paper performs standard DFT+DMFT calculations on the experimentally known I4mm crystal structure of CeCoGe3. The reported mass enhancement m*/m_DFT ~52.6 and the flat nodal lines within 10 meV of EF are direct numerical outputs of the solver applied to the input Hamiltonian; they are not defined in terms of themselves, fitted to force the target topology, or reduced to a self-citation chain. The central claim that correlations, SOC, and symmetry stabilize the nodal lines follows from the computed bands rather than from any ansatz or uniqueness theorem imported from the authors' prior work. No load-bearing step equates a prediction to its own input by construction.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the standard approximations of DFT+DMFT for correlated f-electron systems and on the known I4mm crystal symmetry; no additional free parameters or invented entities are introduced beyond those implicit in the method.

free parameters (1)

mass enhancement factor
Value of approximately 52.6 extracted from the DMFT self-energy at T=25 K.

axioms (1)

domain assumption DFT+DMFT accurately captures the crossover from incoherent to coherent quasiparticles and the resulting band topology in heavy-fermion compounds.
Invoked to interpret the calculated electronic structure and nodal lines.

pith-pipeline@v0.9.0 · 5503 in / 1353 out tokens · 48771 ms · 2026-05-15T15:46:27.278177+00:00 · methodology

discussion (0)

Lean theorems connected to this paper

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

IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear

?

unclear
Relation between the paper passage and the cited Recognition theorem.

DFT+DMFT calculations... mass enhancement m*/m_DFT ∼52.6 at T=25 K... flat topological nodal lines within 10 meV of the Fermi level
IndisputableMonolith/Foundation/RealityFromDistinction.lean reality_from_one_distinction unclear

?

unclear
Relation between the paper passage and the cited Recognition theorem.

interplay between electronic correlation, spin-orbit coupling and the noncentrosymmetric I4mm crystal symmetry stabilize flat topological nodal lines

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

73 extracted references · 73 canonical work pages · 1 internal anchor

[1]

Armitage, E

N. Armitage, E. Mele, and A. Vishwanath, Weyl and Dirac semimetals in three-dimensional solids, Reviews of Modern Physics90, 015001 (2018)

work page 2018
[2]

C. Fang, M. J. Gilbert, X. Dai, and B. A. Bernevig, Multi- Weyl Topological Semimetals Stabilized by Point Group Symmetry, Physical Review Letters108, 266802 (2012)

work page 2012
[3]

Bradlyn, J

B. Bradlyn, J. Cano, Z. Wang, M. G. Vergniory, C. Felser, R. J. Cava, and B. A. Bernevig, Beyond Dirac and Weyl fermions: Unconventional quasiparticles in conventional crystals, Science353, aaf5037 (2016)

work page 2016
[4]

Z. Zhu, G. W. Winkler, Q. Wu, J. Li, and A. A. Soluyanov, Triple Point Topological Metals, Physical Review X6, 031003 (2016)

work page 2016
[5]

Z.-M. Yu, Z. Zhang, G.-B. Liu, W. Wu, X.-P. Li, R.-W. Zhang, S. A. Yang, and Y. Yao, Encyclopedia of emergent particles in three-dimensional crystals, Science Bulletin 67, 375 (2022)

work page 2022
[6]

A. A. Zyuzin and A. A. Burkov, Topological response in Weyl semimetals and the chiral anomaly, Physical Review B86, 115133 (2012)

work page 2012
[7]

D. T. Son and B. Z. Spivak, Chiral anomaly and classi- cal negative magnetoresistance of Weyl metals, Physical Review B88, 104412 (2013)

work page 2013
[8]

Huang, L

X. Huang, L. Zhao, Y. Long, P. Wang, D. Chen, Z. Yang, H. Liang, M. Xue, H. Weng, Z. Fang, X. Dai, and G. Chen, Observation of the Chiral-Anomaly-Induced Negative Magnetoresistance in 3D Weyl Semimetal TaAs, Physical Review X5, 031023 (2015)

work page 2015
[9]

P. E. C. Ashby and J. P. Carbotte, Magneto-optical con- ductivity of Weyl semimetals, Physical Review B87, 245131 (2013)

work page 2013
[10]

De Juan, A

F. De Juan, A. G. Grushin, T. Morimoto, and J. E. Moore, Quantized circular photogalvanic effect in Weyl semimetals, Nature Communications8, 15995 (2017)

work page 2017
[11]

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 B83, 205101 (2011)

work page 2011
[12]

H. Weng, C. Fang, Z. Fang, B. A. Bernevig, and X. Dai, Weyl Semimetal Phase in Noncentrosymmetric Transition- Metal Monophosphides, Physical Review X5, 011029 (2015)

work page 2015
[13]

Z. Wang, Y. Sun, X.-Q. Chen, C. Franchini, G. Xu, H. Weng, X. Dai, and Z. Fang, Dirac semimetal and topological phase transitions in A 3Bi ( A = Na , K, Rb), Physical Review B85, 195320 (2012)

work page 2012
[14]

Z. Wang, H. Weng, Q. Wu, X. Dai, and Z. Fang, Three- dimensional Dirac semimetal and quantum transport in Cd3As2, Physical Review B88, 125427 (2013)

work page 2013
[15]

Z. K. Liu, B. Zhou, Y. Zhang, Z. J. Wang, H. M. Weng, D. Prabhakaran, S.-K. Mo, Z. X. Shen, Z. Fang, X. Dai, Z. Hussain, and Y. L. Chen, Discovery of a Three- Dimensional Topological Dirac Semimetal, Na 3 Bi, Sci- ence343, 864 (2014)

work page 2014
[16]

Neupane, S.-Y

M. Neupane, S.-Y. Xu, R. Sankar, N. Alidoust, G. Bian, C. Liu, I. Belopolski, T.-R. Chang, H.-T. Jeng, H. Lin, A. Bansil, F. Chou, and M. Z. Hasan, Observation of a 7 three-dimensional topological Dirac semimetal phase in high-mobility Cd3As2, Nature Communications5, 3786 (2014)

work page 2014
[17]

Z. K. Liu, J. Jiang, B. Zhou, Z. J. Wang, Y. Zhang, H. M. Weng, D. Prabhakaran, S.-K. Mo, H. Peng, P. Dudin, T. Kim, M. Hoesch, Z. Fang, X. Dai, Z. X. Shen, D. L. Feng, Z. Hussain, and Y. L. Chen, A stable three- dimensional topological Dirac semimetal Cd 3As2, Nature Materials13, 677 (2014)

work page 2014
[18]

C. Fang, H. Weng, X. Dai, and Z. Fang, Topological nodal line semimetals, Chinese Physics B25, 117106 (2016)

work page 2016
[19]

S. Li, Y. Liu, S.-S. Wang, Z.-M. Yu, S. Guan, X.-L. Sheng, Y. Yao, and S. A. Yang, Nonsymmorphic-symmetry- protected hourglass Dirac loop, nodal line, and Dirac point in bulk and monolayer X3SiTe6 (X=Ta,Nb), Physi- cal Review B97, 045131 (2018)

work page 2018
[20]

Raghu, X.-L

S. Raghu, X.-L. Qi, C. Honerkamp, and S.-C. Zhang, Topological Mott Insulators, Physical Review Letters100, 156401 (2008)

work page 2008
[21]

B.-B. Chen, Y. D. Liao, Z. Chen, O. Vafek, J. Kang, W. Li, and Z. Y. Meng, Realization of topological Mott insulator in a twisted bilayer graphene lattice model, Nature Communications12, 5480 (2021)

work page 2021
[22]

Trivedi, Topological order in Mott insulators, Annals of Physics435, 168636 (2021)

N. Trivedi, Topological order in Mott insulators, Annals of Physics435, 168636 (2021)

work page 2021
[23]

Dzero, K

M. Dzero, K. Sun, V. Galitski, and P. Coleman, Topo- logical Kondo Insulators, Physical Review Letters104, 106408 (2010)

work page 2010
[24]

F. Lu, J. Zhao, H. Weng, Z. Fang, and X. Dai, Corre- lated Topological Insulators with Mixed Valence, Physical Review Letters110, 096401 (2013)

work page 2013
[25]

X. Deng, K. Haule, and G. Kotliar, Plutonium Hexaboride is a Correlated Topological Insulator, Physical Review Letters111, 176404 (2013)

work page 2013
[26]

Cao, G.-X

C. Cao, G.-X. Zhi, and J.-X. Zhu, From Trivial Kondo Insulator C3Pt3Bi4 to Topological Nodal-Line Semimetal Ce3Pd3Bi4, Physical Review Letters124, 166403 (2020)

work page 2020
[27]

D. F. Liu, Y. F. Xu, H. Y. Hu, J. Y. Liu, T. P. Ying, Y. Y. Lv, Y. Jiang, C. Chen, Y. H. Yang, D. Pei, D. Prab- hakaran, M. H. Gao, J. J. Wang, Q. H. Zhang, F. Q. Meng, B. Thiagarajan, C. Polley, M. Hashimoto, D. H. Lu, N. B. M. Schr¨ oter, V. N. Strocov, A. Louat, C. Cacho, D. Biswas, T.-L. Lee, P. Steadman, P. Bencok, Y. B. Chen, L. Gu, T. Hesjeda, G. v...

work page internal anchor Pith review Pith/arXiv arXiv 2024
[28]

H. Hu, Y. Jiang, D. Liu, Y. Chen, A. M. Tsvelik, Y. Xu, and B. A. Bernevig, CeCo 2P2: a unique Co- antiferromagnetic topological heavy-fermion system with P· T -protected Kondo effect and nodal-line excitations (2024), arXiv:2411.13647 [cond-mat]

work page arXiv 2024
[29]

Qi and S.-C

X.-L. Qi and S.-C. Zhang, Topological insulators and superconductors, Reviews of Modern Physics83, 1057 (2011)

work page 2011
[30]

Knebel, D

G. Knebel, D. Aoki, G. Lapertot, B. Salce, J. Flouquet, T. Kawai, H. Muranaka, R. Settai, and Y. ¯Onuki, High Pressure Phase Diagram of the Non-centrosymmetric An- tiferromagnet CeCoGe3, Journal of the Physical Society of Japan78, 074714 (2009)

work page 2009
[31]

Momma and F

K. Momma and F. Izumi,VESTA: a three-dimensional visualization system for electronic and structural analysis, Journal of Applied Crystallography41, 653 (2008)

work page 2008
[32]

H.-H. Lai, S. E. Grefe, S. Paschen, and Q. Si, Weyl–Kondo semimetal in heavy-fermion systems, Proceedings of the National Academy of Sciences115, 93 (2018)

work page 2018
[33]

C. Y. Guo, F. Wu, Z. Z. Wu, M. Smidman, C. Cao, A. Bostwick, C. Jozwiak, E. Rotenberg, Y. Liu, F. Steglich, and H. Q. Yuan, Evidence for Weyl fermions in a canonical heavy-fermion semimetal YbPtBi, Nature Communica- tions9, 4622 (2018)

work page 2018
[34]

V. K. Pecharsky, O.-B. Hyun, and K. A. Gschneidner, Un- usual magnetic properties of the heavy-fermion compound CeCoGe3, Physical Review B47, 11839 (1993)

work page 1993
[35]

Thamizhavel, T

A. Thamizhavel, T. Takeuchi, T. D Matsuda, Y. Haga, K. Sugiyama, R. Settai, and Y. Onuki, Unique Magnetic Phases in an Antiferromagnet CeCoGe 3, Journal of the Physical Society of Japan74, 1858 (2005)

work page 2005
[36]

Smidman, D

M. Smidman, D. T. Adroja, A. D. Hillier, L. C. Chapon, J. W. Taylor, V. K. Anand, R. P. Singh, M. R. Lees, E. A. Goremychkin, M. M. Koza, V. V. Krishnamurthy, D. M. Paul, and G. Balakrishnan, Neutron scattering and muon spin relaxation measurements of the noncentrosymmetric antiferromagnet CeCoGe3, Physical Review B88, 134416 (2013)

work page 2013
[37]

P. Li, H. Ye, Y. Hu, Y. Fang, Z. Xiao, Z. Wu, Z. Shan, R. P. Singh, G. Balakrishnan, D. Shen, Y.-f. Yang, C. Cao, N. C. Plumb, M. Smidman, M. Shi, J. Kroha, H. Yuan, F. Steglich, and Y. Liu, Photoemission signature of the competition between magnetic order and Kondo effect in CeCoGe3, Physical Review B107, L201104 (2023)

work page 2023
[38]

Kawai, H

T. Kawai, H. Muranaka, M.-A. Measson, T. Shimoda, Y. Doi, T. D. Matsuda, Y. Haga, G. Knebel, G. Laper- tot, D. Aoki, J. Flouquet, T. Takeuchi, R. Settai, and Y. ¯Onuki, Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure, Journal of the Physical Society of Japan77, 064716 (2008)

work page 2008
[39]

Georges, G

A. Georges, G. Kotliar, W. Krauth, and M. J. Rozen- berg, Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions, Re- views of Modern Physics68, 13 (1996)

work page 1996
[40]

Kotliar, S

G. Kotliar, S. Y. Savrasov, K. Haule, V. S. Oudovenko, O. Parcollet, and C. A. Marianetti, Electronic structure calculations with dynamical mean-field theory, Reviews of Modern Physics78, 865 (2006)

work page 2006
[41]

Sheikin, P

I. Sheikin, P. Rodiere, R. Settai, and Y. ¯Onuki, High- Field de Haas–van Alphen Effect in Non-Centrosymmetric CeCoGe3 and LaCoGe3, Journal of the Physical Society of Japan80, SA020 (2011)

work page 2011
[42]

Y. Xu, C. Yue, H. Weng, and X. Dai, Heavy Weyl Fermion State in CeRu 4Sn6, Physical Review X7, 011027 (2017)

work page 2017
[43]

C. Guo, C. Cao, M. Smidman, F. Wu, Y. Zhang, F. Steglich, F.-C. Zhang, and H. Yuan, Possible Weyl fermions in the magnetic Kondo system CeSb, npj Quan- tum Materials2, 39 (2017)

work page 2017
[44]

Settai, T

R. Settai, T. Goto, S. Sakatume, Y. S. Kwon, T. Suzuki, Y. Kaneta, and O. Sakai, Observation of Heavy Hole State in CeSb, Journal of the Physical Society of Japan63, 3026 (1994)

work page 1994
[45]

Pizzi, V

G. Pizzi, V. Vitale, R. Arita, S. Bl¨ ugel, F. Freimuth, G. G´ eranton, M. Gibertini, D. Gresch, C. Johnson, T. Koretsune, J. Iba˜ nez-Azpiroz, H. Lee, J.-M. Lihm, D. Marchand, A. Marrazzo, Y. Mokrousov, J. I. Mustafa, Y. Nohara, Y. Nomura, L. Paulatto, S. Ponc´ e, T. Pon- weiser, J. Qiao, F. Th¨ ole, S. S. Tsirkin, M. Wierzbowska, N. Marzari, D. Vanderbi...

work page 2020
[46]

J. G. Checkelsky, B. A. Bernevig, P. Coleman, Q. Si, and S. Paschen, Flat bands, strange metals and the Kondo effect, Nature Reviews Materials9, 509 (2024)

work page 2024
[47]

X. Chen, L. Wang, J. Ishizuka, R. Zhang, K. Nogaki, Y. Cheng, F. Yang, Z. Chen, F. Zhu, Z. Liu, J. Mei, Y. Yanase, B. Lv, and Y. Huang, Coexistence of near- E F Flat Band and Van Hove Singularity in a Two-Phase Superconductor, Physical Review X14, 021048 (2024)

work page 2024
[48]

Cao and Y.-f

Y. Cao and Y.-f. Yang, Flat bands promoted by Hund’s rule coupling in the candidate double-layer high- temperature superconductor La 3 Ni 2 O 7 under high pressure, Physical Review B109, L081105 (2024)

work page 2024
[49]

B. Xu, R. Liu, H. Wo, Z. Liao, S. Yi, C. Li, J. Zhao, X. Qiu, Z. Yin, and C. Bernhard, Unraveling the origin of Kondo-like behavior in the 3d-electron heavy-fermion com- pound YFe2Ge2, Proceedings of the National Academy of Sciences121, e2401430121 (2024)

work page 2024
[50]

Baglo, J

J. Baglo, J. Chen, K. Murphy, R. Leenen, A. McCollam, M. L. Sutherland, and F. M. Grosche, Fermi Surface and Mass Renormalization in the Iron-Based Superconductor YFe 2 Ge 2, Physical Review Letters129, 046402 (2022)

work page 2022
[51]

Yu and J.-X

S.-L. Yu and J.-X. Li, Chiral superconducting phase and chiral spin-density-wave phase in a Hubbard model on the kagome lattice, Physical Review B85, 144402 (2012)

work page 2012
[52]

X. Wu, T. Schwemmer, T. M¨ uller, A. Consiglio, G. San- giovanni, D. Di Sante, Y. Iqbal, W. Hanke, A. P. Schny- der, M. M. Denner, M. H. Fischer, T. Neupert, and R. Thomale, Nature of Unconventional Pairing in the Kagome Superconductors AV$ 3$Sb$ 5$( A = K , Rb , Cs ), Physical Review Letters127, 177001 (2021)

work page 2021
[53]

S. D. Wilson and B. R. Ortiz, AV3Sb5 kagome supercon- ductors, Nature Reviews Materials9, 420 (2024)

work page 2024
[54]

Q. Wu, S. Zhang, H.-F. Song, M. Troyer, and A. A. Soluyanov, WannierTools: An open-source software pack- age for novel topological materials, Computer Physics Communications224, 405 (2018)

work page 2018
[55]

Ivanov, X

V. Ivanov, X. Wan, and S. Y. Savrasov, Renormalized quasiparticles, topological monopoles, and superconduct- ing line nodes in heavy-fermion Ce T X3 compounds, Phys- ical Review B103, L041112 (2021)

work page 2021
[56]

Liu and B

C.-X. Liu and B. A. Bernevig, Nodal nematic supercon- ductivity in multiple flat-band systems, Physical Review B111, L020502 (2025)

work page 2025
[57]

D. Eom, N. Takeda, and M. Ishikawa, Magnetic Instability around the Quantum Critical Point in CeCoGe 3−xSix (0 ≤x≤ 3), Journal of the Physical Society of Japan75, 093706 (2006)

work page 2006
[58]

D. Eom, M. Ishikawa, and N. Takeda, Non-Fermi liquid-like behavior around the critical concentration in CeCoGe3−xSix (x≃ 1.2), Physica B: Condensed Matter 281-282, 369 (2000)

work page 2000
[59]

M´ easson, H

M.-A. M´ easson, H. Muranaka, T. Matsuda, T. Kawai, Y. Haga, G. Knebel, D. Aoki, G. Lapertot, F. Honda, R. Settai, J.-P. Brison, J. Flouquet, K. Shimizu, and Y. Onuki, Huge upper critical field in the superconductor with non-centrosymmetric crystal structure CeCoGe 3, Physica C: Superconductivity and its Applications470, S536 (2010)

work page 2010
[60]

M. R. Norman, Hund’s rule theory for heavy fermion superconductors, Physical Review Letters72, 2077 (1994), 27 citations (Crossref) [2023-02-28]

work page 2077
[61]

Hoshino and P

S. Hoshino and P. Werner, Superconductivity from Emerg- ing Magnetic Moments, Physical Review Letters115, 247001 (2015)

work page 2015
[62]

Wu and Y

Z. Wu and Y. Wang, Nodal topological superconductivity in nodal-line semimetals, Physical Review B108, 224503 (2023)

work page 2023
[63]

Haule, C.-H

K. Haule, C.-H. Yee, and K. Kim, Dynamical mean-field theory within the full-potential methods: Electronic struc- ture of CeIrIn 5, CeCoIn5, and CeRhIn 5, Phys. Rev. B81, 195107 (2010)

work page 2010
[64]

Blaha, K

P. Blaha, K. Schwarz, F. Tran, R. Laskowski, G. K. H. Madsen, and L. D. Marks, WIEN2k: An APW+lo pro- gram for calculating the properties of solids, J. Chem. Phys.152, 074101 (2020)

work page 2020
[65]

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

work page 1996
[66]

M. B. Z¨ olfl, I. A. Nekrasov, T. Pruschke, V. I. Anisimov, and J. Keller, Spectral and Magnetic Properties of α - and γ -Ce from Dynamical Mean-Field Theory and Local Density Approximation, Physical Review Letters 87, 276403 (2001)

work page 2001
[67]

Amadon, S

B. Amadon, S. Biermann, A. Georges, and F. Aryaseti- awan, The γ - α Transition of Cerium Is Entropy Driven, Physical Review Letters96, 066402 (2006)

work page 2006
[68]

Lanat` a, Y.-X

N. Lanat` a, Y.-X. Yao, C.-Z. Wang, K.-M. Ho, J. Schmalian, K. Haule, and G. Kotliar, γ - α Isostruc- tural Transition in Cerium, Physical Review Letters111, 196801 (2013)

work page 2013
[69]

E. Gull, A. J. Millis, A. I. Lichtenstein, A. N. Rubtsov, M. Troyer, and P. Werner, Continuous-time monte carlo methods for quantum impurity models, Rev. Mod. Phys. 83, 349 (2011)

work page 2011
[70]

Haule, Exact double counting in combining the dynam- ical mean field theory and the density functional theory, Phys

K. Haule, Exact double counting in combining the dynam- ical mean field theory and the density functional theory, Phys. Rev. Lett.115, 196403 (2015)

work page 2015
[71]

Birch, Finite Elastic Strain of Cubic Crystals, Physical Review71, 809 (1947)

F. Birch, Finite Elastic Strain of Cubic Crystals, Physical Review71, 809 (1947)

work page 1947
[72]

Kresse and J

G. Kresse and J. Furthm¨ uller, Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set, Physical Review B54, 11169 (1996)

work page 1996
[73]

S. L. Dudarev, G. A. Botton, S. Y. Savrasov, C. J. Humphreys, and A. P. Sutton, Electron-energy-loss spec- tra and the structural stability of nickel oxide: An LSDA+U study, Physical Review B57, 1505 (1998)

work page 1998

[1] [1]

Armitage, E

N. Armitage, E. Mele, and A. Vishwanath, Weyl and Dirac semimetals in three-dimensional solids, Reviews of Modern Physics90, 015001 (2018)

work page 2018

[2] [2]

C. Fang, M. J. Gilbert, X. Dai, and B. A. Bernevig, Multi- Weyl Topological Semimetals Stabilized by Point Group Symmetry, Physical Review Letters108, 266802 (2012)

work page 2012

[3] [3]

Bradlyn, J

B. Bradlyn, J. Cano, Z. Wang, M. G. Vergniory, C. Felser, R. J. Cava, and B. A. Bernevig, Beyond Dirac and Weyl fermions: Unconventional quasiparticles in conventional crystals, Science353, aaf5037 (2016)

work page 2016

[4] [4]

Z. Zhu, G. W. Winkler, Q. Wu, J. Li, and A. A. Soluyanov, Triple Point Topological Metals, Physical Review X6, 031003 (2016)

work page 2016

[5] [5]

Z.-M. Yu, Z. Zhang, G.-B. Liu, W. Wu, X.-P. Li, R.-W. Zhang, S. A. Yang, and Y. Yao, Encyclopedia of emergent particles in three-dimensional crystals, Science Bulletin 67, 375 (2022)

work page 2022

[6] [6]

A. A. Zyuzin and A. A. Burkov, Topological response in Weyl semimetals and the chiral anomaly, Physical Review B86, 115133 (2012)

work page 2012

[7] [7]

D. T. Son and B. Z. Spivak, Chiral anomaly and classi- cal negative magnetoresistance of Weyl metals, Physical Review B88, 104412 (2013)

work page 2013

[8] [8]

Huang, L

X. Huang, L. Zhao, Y. Long, P. Wang, D. Chen, Z. Yang, H. Liang, M. Xue, H. Weng, Z. Fang, X. Dai, and G. Chen, Observation of the Chiral-Anomaly-Induced Negative Magnetoresistance in 3D Weyl Semimetal TaAs, Physical Review X5, 031023 (2015)

work page 2015

[9] [9]

P. E. C. Ashby and J. P. Carbotte, Magneto-optical con- ductivity of Weyl semimetals, Physical Review B87, 245131 (2013)

work page 2013

[10] [10]

De Juan, A

F. De Juan, A. G. Grushin, T. Morimoto, and J. E. Moore, Quantized circular photogalvanic effect in Weyl semimetals, Nature Communications8, 15995 (2017)

work page 2017

[11] [11]

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 B83, 205101 (2011)

work page 2011

[12] [12]

H. Weng, C. Fang, Z. Fang, B. A. Bernevig, and X. Dai, Weyl Semimetal Phase in Noncentrosymmetric Transition- Metal Monophosphides, Physical Review X5, 011029 (2015)

work page 2015

[13] [13]

Z. Wang, Y. Sun, X.-Q. Chen, C. Franchini, G. Xu, H. Weng, X. Dai, and Z. Fang, Dirac semimetal and topological phase transitions in A 3Bi ( A = Na , K, Rb), Physical Review B85, 195320 (2012)

work page 2012

[14] [14]

Z. Wang, H. Weng, Q. Wu, X. Dai, and Z. Fang, Three- dimensional Dirac semimetal and quantum transport in Cd3As2, Physical Review B88, 125427 (2013)

work page 2013

[15] [15]

Z. K. Liu, B. Zhou, Y. Zhang, Z. J. Wang, H. M. Weng, D. Prabhakaran, S.-K. Mo, Z. X. Shen, Z. Fang, X. Dai, Z. Hussain, and Y. L. Chen, Discovery of a Three- Dimensional Topological Dirac Semimetal, Na 3 Bi, Sci- ence343, 864 (2014)

work page 2014

[16] [16]

Neupane, S.-Y

M. Neupane, S.-Y. Xu, R. Sankar, N. Alidoust, G. Bian, C. Liu, I. Belopolski, T.-R. Chang, H.-T. Jeng, H. Lin, A. Bansil, F. Chou, and M. Z. Hasan, Observation of a 7 three-dimensional topological Dirac semimetal phase in high-mobility Cd3As2, Nature Communications5, 3786 (2014)

work page 2014

[17] [17]

Z. K. Liu, J. Jiang, B. Zhou, Z. J. Wang, Y. Zhang, H. M. Weng, D. Prabhakaran, S.-K. Mo, H. Peng, P. Dudin, T. Kim, M. Hoesch, Z. Fang, X. Dai, Z. X. Shen, D. L. Feng, Z. Hussain, and Y. L. Chen, A stable three- dimensional topological Dirac semimetal Cd 3As2, Nature Materials13, 677 (2014)

work page 2014

[18] [18]

C. Fang, H. Weng, X. Dai, and Z. Fang, Topological nodal line semimetals, Chinese Physics B25, 117106 (2016)

work page 2016

[19] [19]

S. Li, Y. Liu, S.-S. Wang, Z.-M. Yu, S. Guan, X.-L. Sheng, Y. Yao, and S. A. Yang, Nonsymmorphic-symmetry- protected hourglass Dirac loop, nodal line, and Dirac point in bulk and monolayer X3SiTe6 (X=Ta,Nb), Physi- cal Review B97, 045131 (2018)

work page 2018

[20] [20]

Raghu, X.-L

S. Raghu, X.-L. Qi, C. Honerkamp, and S.-C. Zhang, Topological Mott Insulators, Physical Review Letters100, 156401 (2008)

work page 2008

[21] [21]

B.-B. Chen, Y. D. Liao, Z. Chen, O. Vafek, J. Kang, W. Li, and Z. Y. Meng, Realization of topological Mott insulator in a twisted bilayer graphene lattice model, Nature Communications12, 5480 (2021)

work page 2021

[22] [22]

Trivedi, Topological order in Mott insulators, Annals of Physics435, 168636 (2021)

N. Trivedi, Topological order in Mott insulators, Annals of Physics435, 168636 (2021)

work page 2021

[23] [23]

Dzero, K

M. Dzero, K. Sun, V. Galitski, and P. Coleman, Topo- logical Kondo Insulators, Physical Review Letters104, 106408 (2010)

work page 2010

[24] [24]

F. Lu, J. Zhao, H. Weng, Z. Fang, and X. Dai, Corre- lated Topological Insulators with Mixed Valence, Physical Review Letters110, 096401 (2013)

work page 2013

[25] [25]

X. Deng, K. Haule, and G. Kotliar, Plutonium Hexaboride is a Correlated Topological Insulator, Physical Review Letters111, 176404 (2013)

work page 2013

[26] [26]

Cao, G.-X

C. Cao, G.-X. Zhi, and J.-X. Zhu, From Trivial Kondo Insulator C3Pt3Bi4 to Topological Nodal-Line Semimetal Ce3Pd3Bi4, Physical Review Letters124, 166403 (2020)

work page 2020

[27] [27]

D. F. Liu, Y. F. Xu, H. Y. Hu, J. Y. Liu, T. P. Ying, Y. Y. Lv, Y. Jiang, C. Chen, Y. H. Yang, D. Pei, D. Prab- hakaran, M. H. Gao, J. J. Wang, Q. H. Zhang, F. Q. Meng, B. Thiagarajan, C. Polley, M. Hashimoto, D. H. Lu, N. B. M. Schr¨ oter, V. N. Strocov, A. Louat, C. Cacho, D. Biswas, T.-L. Lee, P. Steadman, P. Bencok, Y. B. Chen, L. Gu, T. Hesjeda, G. v...

work page internal anchor Pith review Pith/arXiv arXiv 2024

[28] [28]

H. Hu, Y. Jiang, D. Liu, Y. Chen, A. M. Tsvelik, Y. Xu, and B. A. Bernevig, CeCo 2P2: a unique Co- antiferromagnetic topological heavy-fermion system with P· T -protected Kondo effect and nodal-line excitations (2024), arXiv:2411.13647 [cond-mat]

work page arXiv 2024

[29] [29]

Qi and S.-C

X.-L. Qi and S.-C. Zhang, Topological insulators and superconductors, Reviews of Modern Physics83, 1057 (2011)

work page 2011

[30] [30]

Knebel, D

G. Knebel, D. Aoki, G. Lapertot, B. Salce, J. Flouquet, T. Kawai, H. Muranaka, R. Settai, and Y. ¯Onuki, High Pressure Phase Diagram of the Non-centrosymmetric An- tiferromagnet CeCoGe3, Journal of the Physical Society of Japan78, 074714 (2009)

work page 2009

[31] [31]

Momma and F

K. Momma and F. Izumi,VESTA: a three-dimensional visualization system for electronic and structural analysis, Journal of Applied Crystallography41, 653 (2008)

work page 2008

[32] [32]

H.-H. Lai, S. E. Grefe, S. Paschen, and Q. Si, Weyl–Kondo semimetal in heavy-fermion systems, Proceedings of the National Academy of Sciences115, 93 (2018)

work page 2018

[33] [33]

C. Y. Guo, F. Wu, Z. Z. Wu, M. Smidman, C. Cao, A. Bostwick, C. Jozwiak, E. Rotenberg, Y. Liu, F. Steglich, and H. Q. Yuan, Evidence for Weyl fermions in a canonical heavy-fermion semimetal YbPtBi, Nature Communica- tions9, 4622 (2018)

work page 2018

[34] [34]

V. K. Pecharsky, O.-B. Hyun, and K. A. Gschneidner, Un- usual magnetic properties of the heavy-fermion compound CeCoGe3, Physical Review B47, 11839 (1993)

work page 1993

[35] [35]

Thamizhavel, T

A. Thamizhavel, T. Takeuchi, T. D Matsuda, Y. Haga, K. Sugiyama, R. Settai, and Y. Onuki, Unique Magnetic Phases in an Antiferromagnet CeCoGe 3, Journal of the Physical Society of Japan74, 1858 (2005)

work page 2005

[36] [36]

Smidman, D

M. Smidman, D. T. Adroja, A. D. Hillier, L. C. Chapon, J. W. Taylor, V. K. Anand, R. P. Singh, M. R. Lees, E. A. Goremychkin, M. M. Koza, V. V. Krishnamurthy, D. M. Paul, and G. Balakrishnan, Neutron scattering and muon spin relaxation measurements of the noncentrosymmetric antiferromagnet CeCoGe3, Physical Review B88, 134416 (2013)

work page 2013

[37] [37]

P. Li, H. Ye, Y. Hu, Y. Fang, Z. Xiao, Z. Wu, Z. Shan, R. P. Singh, G. Balakrishnan, D. Shen, Y.-f. Yang, C. Cao, N. C. Plumb, M. Smidman, M. Shi, J. Kroha, H. Yuan, F. Steglich, and Y. Liu, Photoemission signature of the competition between magnetic order and Kondo effect in CeCoGe3, Physical Review B107, L201104 (2023)

work page 2023

[38] [38]

Kawai, H

T. Kawai, H. Muranaka, M.-A. Measson, T. Shimoda, Y. Doi, T. D. Matsuda, Y. Haga, G. Knebel, G. Laper- tot, D. Aoki, J. Flouquet, T. Takeuchi, R. Settai, and Y. ¯Onuki, Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure, Journal of the Physical Society of Japan77, 064716 (2008)

work page 2008

[39] [39]

Georges, G

A. Georges, G. Kotliar, W. Krauth, and M. J. Rozen- berg, Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions, Re- views of Modern Physics68, 13 (1996)

work page 1996

[40] [40]

Kotliar, S

G. Kotliar, S. Y. Savrasov, K. Haule, V. S. Oudovenko, O. Parcollet, and C. A. Marianetti, Electronic structure calculations with dynamical mean-field theory, Reviews of Modern Physics78, 865 (2006)

work page 2006

[41] [41]

Sheikin, P

I. Sheikin, P. Rodiere, R. Settai, and Y. ¯Onuki, High- Field de Haas–van Alphen Effect in Non-Centrosymmetric CeCoGe3 and LaCoGe3, Journal of the Physical Society of Japan80, SA020 (2011)

work page 2011

[42] [42]

Y. Xu, C. Yue, H. Weng, and X. Dai, Heavy Weyl Fermion State in CeRu 4Sn6, Physical Review X7, 011027 (2017)

work page 2017

[43] [43]

C. Guo, C. Cao, M. Smidman, F. Wu, Y. Zhang, F. Steglich, F.-C. Zhang, and H. Yuan, Possible Weyl fermions in the magnetic Kondo system CeSb, npj Quan- tum Materials2, 39 (2017)

work page 2017

[44] [44]

Settai, T

R. Settai, T. Goto, S. Sakatume, Y. S. Kwon, T. Suzuki, Y. Kaneta, and O. Sakai, Observation of Heavy Hole State in CeSb, Journal of the Physical Society of Japan63, 3026 (1994)

work page 1994

[45] [45]

Pizzi, V

G. Pizzi, V. Vitale, R. Arita, S. Bl¨ ugel, F. Freimuth, G. G´ eranton, M. Gibertini, D. Gresch, C. Johnson, T. Koretsune, J. Iba˜ nez-Azpiroz, H. Lee, J.-M. Lihm, D. Marchand, A. Marrazzo, Y. Mokrousov, J. I. Mustafa, Y. Nohara, Y. Nomura, L. Paulatto, S. Ponc´ e, T. Pon- weiser, J. Qiao, F. Th¨ ole, S. S. Tsirkin, M. Wierzbowska, N. Marzari, D. Vanderbi...

work page 2020

[46] [46]

J. G. Checkelsky, B. A. Bernevig, P. Coleman, Q. Si, and S. Paschen, Flat bands, strange metals and the Kondo effect, Nature Reviews Materials9, 509 (2024)

work page 2024

[47] [47]

X. Chen, L. Wang, J. Ishizuka, R. Zhang, K. Nogaki, Y. Cheng, F. Yang, Z. Chen, F. Zhu, Z. Liu, J. Mei, Y. Yanase, B. Lv, and Y. Huang, Coexistence of near- E F Flat Band and Van Hove Singularity in a Two-Phase Superconductor, Physical Review X14, 021048 (2024)

work page 2024

[48] [48]

Cao and Y.-f

Y. Cao and Y.-f. Yang, Flat bands promoted by Hund’s rule coupling in the candidate double-layer high- temperature superconductor La 3 Ni 2 O 7 under high pressure, Physical Review B109, L081105 (2024)

work page 2024

[49] [49]

B. Xu, R. Liu, H. Wo, Z. Liao, S. Yi, C. Li, J. Zhao, X. Qiu, Z. Yin, and C. Bernhard, Unraveling the origin of Kondo-like behavior in the 3d-electron heavy-fermion com- pound YFe2Ge2, Proceedings of the National Academy of Sciences121, e2401430121 (2024)

work page 2024

[50] [50]

Baglo, J

J. Baglo, J. Chen, K. Murphy, R. Leenen, A. McCollam, M. L. Sutherland, and F. M. Grosche, Fermi Surface and Mass Renormalization in the Iron-Based Superconductor YFe 2 Ge 2, Physical Review Letters129, 046402 (2022)

work page 2022

[51] [51]

Yu and J.-X

S.-L. Yu and J.-X. Li, Chiral superconducting phase and chiral spin-density-wave phase in a Hubbard model on the kagome lattice, Physical Review B85, 144402 (2012)

work page 2012

[52] [52]

X. Wu, T. Schwemmer, T. M¨ uller, A. Consiglio, G. San- giovanni, D. Di Sante, Y. Iqbal, W. Hanke, A. P. Schny- der, M. M. Denner, M. H. Fischer, T. Neupert, and R. Thomale, Nature of Unconventional Pairing in the Kagome Superconductors AV$ 3$Sb$ 5$( A = K , Rb , Cs ), Physical Review Letters127, 177001 (2021)

work page 2021

[53] [53]

S. D. Wilson and B. R. Ortiz, AV3Sb5 kagome supercon- ductors, Nature Reviews Materials9, 420 (2024)

work page 2024

[54] [54]

Q. Wu, S. Zhang, H.-F. Song, M. Troyer, and A. A. Soluyanov, WannierTools: An open-source software pack- age for novel topological materials, Computer Physics Communications224, 405 (2018)

work page 2018

[55] [55]

Ivanov, X

V. Ivanov, X. Wan, and S. Y. Savrasov, Renormalized quasiparticles, topological monopoles, and superconduct- ing line nodes in heavy-fermion Ce T X3 compounds, Phys- ical Review B103, L041112 (2021)

work page 2021

[56] [56]

Liu and B

C.-X. Liu and B. A. Bernevig, Nodal nematic supercon- ductivity in multiple flat-band systems, Physical Review B111, L020502 (2025)

work page 2025

[57] [57]

D. Eom, N. Takeda, and M. Ishikawa, Magnetic Instability around the Quantum Critical Point in CeCoGe 3−xSix (0 ≤x≤ 3), Journal of the Physical Society of Japan75, 093706 (2006)

work page 2006

[58] [58]

D. Eom, M. Ishikawa, and N. Takeda, Non-Fermi liquid-like behavior around the critical concentration in CeCoGe3−xSix (x≃ 1.2), Physica B: Condensed Matter 281-282, 369 (2000)

work page 2000

[59] [59]

M´ easson, H

M.-A. M´ easson, H. Muranaka, T. Matsuda, T. Kawai, Y. Haga, G. Knebel, D. Aoki, G. Lapertot, F. Honda, R. Settai, J.-P. Brison, J. Flouquet, K. Shimizu, and Y. Onuki, Huge upper critical field in the superconductor with non-centrosymmetric crystal structure CeCoGe 3, Physica C: Superconductivity and its Applications470, S536 (2010)

work page 2010

[60] [60]

M. R. Norman, Hund’s rule theory for heavy fermion superconductors, Physical Review Letters72, 2077 (1994), 27 citations (Crossref) [2023-02-28]

work page 2077

[61] [61]

Hoshino and P

S. Hoshino and P. Werner, Superconductivity from Emerg- ing Magnetic Moments, Physical Review Letters115, 247001 (2015)

work page 2015

[62] [62]

Wu and Y

Z. Wu and Y. Wang, Nodal topological superconductivity in nodal-line semimetals, Physical Review B108, 224503 (2023)

work page 2023

[63] [63]

Haule, C.-H

K. Haule, C.-H. Yee, and K. Kim, Dynamical mean-field theory within the full-potential methods: Electronic struc- ture of CeIrIn 5, CeCoIn5, and CeRhIn 5, Phys. Rev. B81, 195107 (2010)

work page 2010

[64] [64]

Blaha, K

P. Blaha, K. Schwarz, F. Tran, R. Laskowski, G. K. H. Madsen, and L. D. Marks, WIEN2k: An APW+lo pro- gram for calculating the properties of solids, J. Chem. Phys.152, 074101 (2020)

work page 2020

[65] [65]

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

work page 1996

[66] [66]

M. B. Z¨ olfl, I. A. Nekrasov, T. Pruschke, V. I. Anisimov, and J. Keller, Spectral and Magnetic Properties of α - and γ -Ce from Dynamical Mean-Field Theory and Local Density Approximation, Physical Review Letters 87, 276403 (2001)

work page 2001

[67] [67]

Amadon, S

B. Amadon, S. Biermann, A. Georges, and F. Aryaseti- awan, The γ - α Transition of Cerium Is Entropy Driven, Physical Review Letters96, 066402 (2006)

work page 2006

[68] [68]

Lanat` a, Y.-X

N. Lanat` a, Y.-X. Yao, C.-Z. Wang, K.-M. Ho, J. Schmalian, K. Haule, and G. Kotliar, γ - α Isostruc- tural Transition in Cerium, Physical Review Letters111, 196801 (2013)

work page 2013

[69] [69]

E. Gull, A. J. Millis, A. I. Lichtenstein, A. N. Rubtsov, M. Troyer, and P. Werner, Continuous-time monte carlo methods for quantum impurity models, Rev. Mod. Phys. 83, 349 (2011)

work page 2011

[70] [70]

Haule, Exact double counting in combining the dynam- ical mean field theory and the density functional theory, Phys

K. Haule, Exact double counting in combining the dynam- ical mean field theory and the density functional theory, Phys. Rev. Lett.115, 196403 (2015)

work page 2015

[71] [71]

Birch, Finite Elastic Strain of Cubic Crystals, Physical Review71, 809 (1947)

F. Birch, Finite Elastic Strain of Cubic Crystals, Physical Review71, 809 (1947)

work page 1947

[72] [72]

Kresse and J

G. Kresse and J. Furthm¨ uller, Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set, Physical Review B54, 11169 (1996)

work page 1996

[73] [73]

S. L. Dudarev, G. A. Botton, S. Y. Savrasov, C. J. Humphreys, and A. P. Sutton, Electron-energy-loss spec- tra and the structural stability of nickel oxide: An LSDA+U study, Physical Review B57, 1505 (1998)

work page 1998