pith. machine review for the scientific record. sign in

arxiv: 2605.07540 · v1 · submitted 2026-05-08 · ❄️ cond-mat.str-el · cond-mat.mtrl-sci· cond-mat.supr-con

Recognition: 2 theorem links

· Lean Theorem

Noncollinear antiferromagnetic structure and physical properties of CrRhAs with distorted kagome lattice

Authors on Pith no claims yet

Pith reviewed 2026-05-11 03:03 UTC · model grok-4.3

classification ❄️ cond-mat.str-el cond-mat.mtrl-scicond-mat.supr-con
keywords CrRhAskagome latticenoncollinear antiferromagnetismneutron diffractionelectrical transportKadowaki-Woods ratiospin fluctuations
0
0 comments X

The pith

CrRhAs has a noncollinear antiferromagnetic order on its distorted kagome lattice with propagation vector (1/3, 1/3, 1/2) unlike theoretical predictions.

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

The paper investigates the magnetic structure and physical properties of CrRhAs, a compound with a distorted chromium kagome lattice that was theoretically proposed as a kagome metal with unusual magnetism. Through powder neutron diffraction, it establishes an antiferromagnetic transition at 149 K with a noncollinear spin arrangement characterized by the wave vector (1/3, 1/3, 1/2). This arrangement includes ferromagnetic coupling between second nearest neighbors within the kagome plane, which contradicts previous density functional theory results. The material also displays unusual electrical transport, including a semiconducting-to-metallic crossover at the magnetic transition, multiple sign changes in the Hall coefficient, and a notably large Kadowaki-Woods ratio indicating strong correlations. These observations position CrRhAs as a strongly correlated kagome metal featuring multiband effects and noncollinear magnetism.

Core claim

CrRhAs is an antiferromagnet below 149 K whose magnetic structure, determined by powder neutron diffraction, is noncollinear with propagation vector k = (1/3, 1/3, 1/2) and features ferromagnetic second-nearest-neighbor interactions in the kagome plane, differing from density functional theory predictions; its transport properties suggest multiband conduction and strong spin fluctuations in this strongly correlated system.

What carries the argument

The noncollinear antiferromagnetic structure with propagation vector k = (1/3, 1/3, 1/2) on the distorted Cr kagome lattice, as revealed by neutron diffraction.

Load-bearing premise

The interpretation of the transport anomalies as arising from multiband effects and strong spin fluctuations, as opposed to sample impurities or other extrinsic factors.

What would settle it

A single-crystal neutron diffraction experiment that either confirms the propagation vector k = (1/3, 1/3, 1/2) and the noncollinear spin arrangement or reveals a different magnetic structure.

Figures

Figures reproduced from arXiv: 2605.07540 by Bingxian Shi, Chenglin Shang, Daye Xu, Hongliang Wang, Hongxia Zhang, Jinchen Wang, Juanjuan Liu, Lijie Hao, Peng Cheng, Xuejuan Gui, Zhongcen Sun.

Figure 1
Figure 1. Figure 1: FIG. 1. Structural characterization of CrRhAs. (a) XRD patt [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Magnetization measurements on CrRhAs. (a) Temperat [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Magnetic structure investigated by neutron diffract [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Electrical transport properties. (a) Resistivity o [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. (a) Specific heat C [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
read the original abstract

CrRhAs was theoretically proposed to be a kagome metal with unusual magnetic ground states; however, little is known about its magnetic structure and physical properties experimentally. Here, we present an experimental investigation of CrRhAs with ZrNiAl-type structure and a distorted Cr kagome lattice. CrRhAs is an antiferromagnet with TN = 149 K. Powder neutron diffraction analysis reveals a noncollinear antiferromagnetic structure with propagation vector k = (1/3, 1/3, 1/2), which features a ferromagnetic second nearest neighbor coupling in the kagome plane that is different from the prediction in previous density functional theory calculations. Furthermore, CrRhAs exhibits anomalous electrical transport properties which are possibly related to multiband effects and strong spin fluctuations. For the temperature-dependent longitudinal resistivity \r{ho}xx, it is semiconductinglike above TN and becomes metallic below TN . The Hall coefficients exhibit two sign changes near 70 and 300 K. Combined with the results of heat capacity measurements, a large Kadowaki-Woods ratio {\alpha} = 33.9 {\mu}{\Omega} cm mol2 K2/J2 is obtained. The above results suggest CrRhAs is a strongly correlated kagome metal with multiband and noncollinear magnetic structure features.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 3 minor

Summary. The manuscript experimentally characterizes CrRhAs, which adopts the ZrNiAl-type structure featuring a distorted Cr kagome lattice. It reports an antiferromagnetic transition at TN = 149 K. Powder neutron diffraction determines a noncollinear antiferromagnetic structure with propagation vector k = (1/3, 1/3, 1/2) that exhibits ferromagnetic second-nearest-neighbor coupling within the kagome plane, differing from prior DFT predictions. Transport measurements reveal a semiconducting-to-metallic crossover in longitudinal resistivity below TN, two sign changes in the Hall coefficient (near 70 K and 300 K), and a large Kadowaki-Woods ratio of 33.9 μΩ cm mol² K²/J², which the authors attribute to multiband effects and strong spin fluctuations in a correlated kagome metal.

Significance. If the magnetic structure is robustly determined, the work is significant for providing the first experimental benchmark of the magnetic ground state in CrRhAs, directly challenging existing DFT calculations on kagome antiferromagnets and supplying concrete input for refined theoretical models. The complementary transport and thermodynamic data add context on correlated behavior in this distorted kagome system. Standard techniques (neutron diffraction, resistivity, Hall effect, heat capacity) are employed appropriately, with the experimental focus on falsifiable structural claims representing a strength.

major comments (1)
  1. [Powder neutron diffraction analysis] Powder neutron diffraction analysis: The refined noncollinear structure with k = (1/3, 1/3, 1/2) must report the Cr magnetic moment magnitudes and directions together with their uncertainties, plus the magnetic R-factor or χ² for the fit, to substantiate the claimed ferromagnetic second nearest neighbor coupling and to allow evaluation of model uniqueness.
minor comments (3)
  1. [Abstract] Abstract: Quantitative details such as magnetic moment sizes, error bars on TN, or fit quality metrics are absent, which reduces the standalone informativeness of the summary.
  2. [Transport properties] Transport discussion: The semiconducting-to-metallic crossover and Hall sign changes would benefit from explicit temperature/field ranges and raw data presentation to clarify the multiband interpretation.
  3. [Figures and notation] Notation and presentation: The resistivity symbol appears as a LaTeX artifact (e.g., “r{ho}xx”); ensure consistent, readable notation throughout and include error bars on all plotted data points.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive evaluation of our manuscript and the constructive comment on the neutron diffraction analysis. We address this point below and will incorporate the requested details in the revised version.

read point-by-point responses
  1. Referee: Powder neutron diffraction analysis: The refined noncollinear structure with k = (1/3, 1/3, 1/2) must report the Cr magnetic moment magnitudes and directions together with their uncertainties, plus the magnetic R-factor or χ² for the fit, to substantiate the claimed ferromagnetic second nearest neighbor coupling and to allow evaluation of model uniqueness.

    Authors: We agree that these quantitative details are necessary for a complete and transparent presentation of the magnetic structure refinement. In the revised manuscript, we will include the refined Cr magnetic moment magnitudes and directions (with uncertainties) obtained from the powder neutron diffraction data, along with the magnetic R-factor (or χ² value) for the fit. These additions will allow readers to evaluate the quality of the refinement and the robustness of the claimed ferromagnetic second-nearest-neighbor coupling within the kagome plane. revision: yes

Circularity Check

0 steps flagged

No significant circularity; purely experimental determination

full rationale

The paper reports experimental measurements of magnetic structure via powder neutron diffraction and transport properties. The noncollinear antiferromagnetic order with k = (1/3, 1/3, 1/2) is obtained by direct indexing and Rietveld refinement of diffraction peaks on the ZrNiAl-type lattice; no theoretical derivation or ansatz is introduced that reduces to fitted inputs or prior self-citations. The noted difference from earlier DFT calculations is an external comparison, not an internal loop. Transport observations (resistivity crossover, Hall sign changes, Kadowaki-Woods ratio) are presented as measured data with cautious interpretation and do not rely on any self-definitional or load-bearing self-citation chain. The study is self-contained against external benchmarks with no reduction of claims to their own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard experimental techniques and domain interpretations from condensed matter physics without new free parameters or postulated entities.

axioms (2)
  • domain assumption Magnetic structures can be reliably refined from powder neutron diffraction data using standard symmetry analysis and propagation vector determination.
    Invoked when assigning the k = (1/3, 1/3, 1/2) vector and noncollinear spin arrangement from the diffraction patterns.
  • domain assumption A large Kadowaki-Woods ratio signals strong electron correlations in metallic systems.
    Used to interpret the measured value of 33.9 μΩ cm mol² K²/J² as evidence for strong correlations.

pith-pipeline@v0.9.0 · 5587 in / 1501 out tokens · 73110 ms · 2026-05-11T03:03:49.551782+00:00 · methodology

discussion (0)

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

Lean theorems connected to this paper

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

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

48 extracted references · 48 canonical work pages

  1. [1]

    The dominant ∼ T2 dependence indicates either electron-electron or electron-magnon in- teractions

    0358(2) µ Ω cm/K 2 . The dominant ∼ T2 dependence indicates either electron-electron or electron-magnon in- teractions. Fig. 4(b) presents the magnetoresistance (MR) data and MR is defined as [ ρ(B) - ρ(B = 0)]/ ρ(B = 0). Over- all, MR is quite weak at all temperatures and its max- imum value is lower than 0.4% at 14 T and 2 K. The main feature is that MR ...

  2. [2]

    2117 mJ mol − 1 K− 2 and γ = 32.8mJ mol − 1 K− 2 for sample 2)

    5 mJ mol − 1 K− 2 for sample 1, β = 0 . 2117 mJ mol − 1 K− 2 and γ = 32.8mJ mol − 1 K− 2 for sample 2). The Debye temperature is estimated to be 136.7 K for sample 1 and 145.2 K for sample 2. The obtained electronic specific heat coefficient γ up to 32.8 mJ mol − 1 K− 2 is a very large value comparing with conventional metal. Both γ and the coefficient A in th...

  3. [3]

    J.-X. Yin, B. Lian, and M. Z. Hasan, Topological kagome magnets and superconductors, Nature 612, 647 (2022)

  4. [4]

    S. D. Wilson and B. R. Ortiz, A V 3Sb5 kagome supercon- ductors, Nature Reviews Materials 9, 420 (2024)

  5. [5]

    H. Li, T. T. Zhang, T. Yilmaz, Y. Y. Pai, C. E. Marvin- ney, A. Said, Q. W. Yin, C. S. Gong, Z. J. Tu, E. Vescovo, C. S. Nelson, R. G. Moore, S. Murakami, H. C. Lei, H. N. Lee, B. J. Lawrie, and H. Miao, Observation of uncon- ventional charge density wave without acoustic phonon anomaly in kagome superconductors A V 3Sb5(A = Rb, Cs), Phys. Rev. X 11, 0310...

  6. [6]

    Jiang, J.-X

    Y.-X. Jiang, J.-X. Yin, M. M. Denner, N. Shumiya, B. R. Ortiz, G. Xu, Z. Guguchia, J. He, M. S. Hossain, X. Liu, J. Ruff, L. Kautzsch, S. S. Zhang, G. Chang, I. Belopol- ski, Q. Zhang, T. A. Cochran, D. Multer, M. Litskevich, Z.-J. Cheng, X. P. Yang, Z. Wang, R. Thomale, T. Ne- upert, S. D. Wilson, and M. Z. Hasan, Unconventional chiral charge order in kag...

  7. [7]

    H. W. S. Arachchige, W. R. Meier, M. Marshall, T. Matsuoka, R. Xue, M. A. McGuire, R. P. Hermann, H. Cao, and D. Mandrus, Charge den- sity wave in kagome lattice intermetallic ScV 6Sn6, Phys. Rev. Lett. 129, 216402 (2022)

  8. [8]

    X. Teng, L. Chen, F. Ye, E. Rosenberg, Z. Liu, J.-X. Yin, Y.-X. Jiang, J. S. Oh, M. Z. Hasan, K. J. Neubauer, B. Gao, Y. Xie, M. Hashimoto, D. Lu, C. Jozwiak, A. Bostwick, E. Rotenberg, R. J. Birgeneau, J.-H. Chu, M. Yi, and P. Dai, Discovery of charge density wave in a kagome lattice antiferromagnet, Nature 609, 490 (2022)

  9. [9]

    J.-X. Yin, W. Ma, T. A. Cochran, X. Xu, S. S. Zhang, H.-J. Tien, N. Shumiya, G. Cheng, K. Jiang, B. Lian, Z. Song, G. Chang, I. Belopolski, D. Mul- ter, M. Litskevich, Z.-J. Cheng, X. P. Yang, B. Swi- dler, H. Zhou, H. Lin, T. Neupert, Z. Wang, N. Yao, T.-R. Chang, S. Jia, and M. Zahid Hasan, Quantum- limit chern topological magnetism in TbMn 6Sn6, Nature...

  10. [10]

    Pollmann, P

    F. Pollmann, P. Fulde, and K. Shtengel, Ki- netic ferromagnetism on a kagome lattice, Phys. Rev. Lett. 100, 136404 (2008)

  11. [11]

    Lin, J.-H

    Z. Lin, J.-H. Choi, Q. Zhang, W. Qin, S. Yi, P. Wang, L. Li, Y. Wang, H. Zhang, Z. Sun, L. Wei, S. Zhang, T. Guo, Q. Lu, J.-H. Cho, C. Zeng, and Z. Zhang, Flat- bands and emergent ferromagnetic ordering in Fe 3Sn2 kagome lattices, Phys. Rev. Lett. 121, 096401 (2018)

  12. [12]

    Nakatsuji, N

    S. Nakatsuji, N. Kiyohara, and T. Higo, Large anomalous Hall effect in a non-collinear antiferromagnet at room temperature, Nature 527, 212 (2015)

  13. [13]

    Q. Wang, K. J. Neubauer, C. Duan, Q. Yin, S. Fu- jitsu, H. Hosono, F. Ye, R. Zhang, S. Chi, K. Krycka, H. Lei, and P. Dai, Field-induced topological hall ef- fect and double-fan spin structure with a c-axis compo- nent in the metallic kagome antiferromagnetic compound YMn6Sn6, Phys. Rev. B 103, 014416 (2021)

  14. [14]

    Q. Du, Z. Hu, M.-G. Han, F. Camino, Y. Zhu, and C. Petrovic, Topological hall ef- fect anisotropy in kagome bilayer metal Fe 3Sn2, Phys. Rev. Lett. 129, 236601 (2022)

  15. [15]

    Y. Tao, L. Daemen, Y. Cheng, J. C. Neue- feind, and D. Louca, Investigating the magnetoelas- tic properties in fesn and Fe 3Sn2 flat band metals, Phys. Rev. B 107, 174407 (2023)

  16. [16]

    Kuroda, T

    K. Kuroda, T. Tomita, M.-T. Suzuki, C. Bareille, A. A. Nugroho, P. Goswami, M. Ochi, M. Ikhlas, M. Nakayama, S. Akebi, R. Noguchi, R. Ishii, N. In- ami, K. Ono, H. Kumigashira, A. Varykhalov, T. Muro, T. Koretsune, R. Arita, S. Shin, T. Kondo, and S. Nakat- suji, Evidence for magnetic Weyl fermions in a correlated metal, Nature Materials 16, 1090 (2017)

  17. [17]

    L. Zhou, F. Yang, S. Zhang, and T. Zhang, Chemical Rules for Stacked Kagome and Honeycomb Topological Semimetals, Advanced Materials 36, 2309803 (2024)

  18. [18]

    Morosan, S

    E. Morosan, S. Bud’ko, P. Canfield, M. Torikachvili, and A. Lacerda, Thermodynamic and transport properties of RAgGe (R=Tb–Lu) single crystals, Journal of Magnetism and Magnetic Materials 277, 298 (2004)

  19. [19]

    K. Zhao, H. Deng, H. Chen, K. A. Ross, V. Va- clav Petˇ r ´ ıˇ cek, G¨ unther, M. Russina, V. Hutanu, and P. Gegenwart, Realization of the kagome spin ice state in a frustrated intermetallic compound, Science 367, 1218 (2020)

  20. [20]

    K. Zhao, Y. Tokiwa, H. Chen, and P. Gegenwart, Discrete degeneracies distinguished by the anoma- lous Hall effect in a metallic kagome ice compound, Nature Physics 20, 442 (2024)

  21. [21]

    Manni, S

    S. Manni, S. L. Bud’ko, and P. C. Canfield, GdPtPb: A noncollinear antiferromagnet with distorted kagome lat- tice, Phys. Rev. B 96, 054435 (2017)

  22. [22]

    Liu, S.-S

    H.-X. Liu, S.-S. Miao, H. L. Feng, and Y.-G. Shi, Ev- idence of a first-order magnetic transition in HoPtSn, Phys. Rev. Mater. 7, 074405 (2023)

  23. [23]

    J.-K. Bao, D. E. Bugaris, H. Zheng, D. Y. Chung, and M. G. Kanatzidis, A Noncentrosymmetric Polymorph of LuRuGe, Inorganic Chemistry 60, 7827 (2021)

  24. [24]

    Morosan, S

    E. Morosan, S. L. Bud’ko, and P. C. Canfield, Angular-dependent planar metamagnetism in the hexagonal compounds TbPtIn and TmAgGe, Phys. Rev. B 71, 014445 (2005) . 9

  25. [25]

    Tokiwa, M

    Y. Tokiwa, M. Garst, P. Gegenwart, S. L. Bud’ko, and P. C. Canfield, Quantum bicritical- ity in the heavy-fermion metamagnet YbAgGe, Phys. Rev. Lett. 111, 116401 (2013)

  26. [26]

    Baran, D

    S. Baran, D. Kaczorowski, A. Arulraj, B. Penc, and A. Szytu/suppress La, Magnetic struc- ture and thermodynamic properties of TmPtIn, Journal of Magnetism and Magnetic Materials 322, 2177 (2010)

  27. [27]

    W. Wu, W. J. Guo, P. Zheng, Z. Li, G. Li, and J. L. Luo, Field-induced metamagnetism tran- sition with anisotropic magnetoresistance in he- lical magnetic order on MnRuP single crystals, Phys. Rev. Res. 5, 043133 (2023)

  28. [28]

    Balli, D

    M. Balli, D. Fruchart, and R. Zach, Negative and conven- tional magnetocaloric effects of a MnRhAs single crystal, Journal of Applied Physics 115, 203909 (2014)

  29. [29]

    Y. N. Huang, H. O. Jeschke, and I. I. Mazin, CrRhAs: a member of a large family of metallic kagome antiferro- magnets, npj Quantum Materials 8, 32 (2023)

  30. [30]

    S. Ohta, T. Kanomata, and T. Kaneko, Mag- netic properties of CrRhAs and CrRuAs, Journal of Magnetism and Magnetic Materials 90–91, 171 (1990)

  31. [31]

    Cheng, H

    P. Cheng, H. Zhang, W. Bao, A. Schneidewind, P. Link, A. Gr¨ unwald, R. Georgii, L. Hao, and Y. Liu, Design of the cold neutron triple-axis spec- trometer at the China Advanced Research Reactor, Nuclear Instruments and Methods in Physics Research Sectio n A: Accelerators, Spectrometers, Detectors and Associate d Equipment 821

  32. [32]

    Kanomata, T

    T. Kanomata, T. Kawashima, H. Utsugi, T. Goto, H. Hasegawa, and T. Kaneko, Mag- netic properties of the intermetallic compounds M M′(M=Cr, Mn, M ′=Ru, Rh, Pd, and X=P, As), Journal of Applied Physics 69, 4639 (1991)

  33. [33]

    Sheng, X

    J. Sheng, X. Li, C. Tian, J. Song, X. Li, G. Sun, T. Xia, J. Wang, J. Liu, D. Xu, H. Zhang, X. Tong, W. Luo, L. Wu, W. Bao, and P. Cheng, Evolution of superconductivity and antiferromagnetic order in Ba(Fe 0. 92− xCo0. 08Vx)2as2, Phys. Rev. B 101, 174516 (2020)

  34. [34]

    M. I. Aroyo, J. M. Perez-Mato, C. Capillas, E. Kroumova, S. Ivantchev, G. Madariaga, A. Kirov, and H. Wondratschek, Bilbao crystallographic server: I. databases and crystallographic computing programs, Zeitschrift f¨ ur Kristallographie-Crystalline Materials 221, 15 (2006)

  35. [35]

    E. Yi, D. F. Zheng, F. Pan, H. Zhang, B. Wang, B. Chen, D. Wu, H. Liang, Z. X. Mei, H. Wu, S. A. Yang, P. Cheng, M. Wang, and B. Shen, Topological hall ef- fect driven by short-range magnetic order in EuZn 2As2, Phys. Rev. B 107, 035142 (2023)

  36. [36]

    Huang, C

    J. Huang, C. Shang, J. Qin, F. Pan, B. Shi, J. Wang, J. Liu, D. Xu, H. Zhang, H. Wang, L. Hao, W. Bao, and P. Cheng, FeGe 1 – xSbx: A series of kagome metals with noncollinear antiferromagnetism, Phys. Rev. B 108, 184431 (2023)

  37. [37]

    B. Shi, Y. Geng, H. Wang, J. Yang, C. Shang, M. Wang, S. Mi, J. Huang, F. Pan, X. Gui, J. Wang, J. Liu, D. Xu, H. Zhang, J. Qin, H. Wang, L. Hao, M. Tian, Z. Cheng, G. Zheng, and P. Cheng, FePd 2Te2: An anisotropic two- dimensional ferromagnet with one-dimensional fe chains, Journal of the American Chemical Society 146, 21546 (2024)

  38. [38]

    A. B. Pippard, Magnetoresistance in Metals (Cambridge Uni versity Press, Cambridge, 1989)

  39. [39]

    J. M. Ziman, Electrons and Phonons the Theory of Trans- port Phenomena in Solids (Oxford University Press, Ox- ford, 1960)

  40. [40]

    Q. Yin, Z. Tu, C. Gong, Y. Fu, S. Yan, and H. Lei, Superconductivity and Normal-State Prop- erties of Kagome Metal RbV 3Sb5 Single Crystals, Chinese Physics Letters 38, 037403 (2021)

  41. [41]

    E. Mun, H. Ko, G. J. Miller, G. D. Samolyuk, S. L. Bud’ko, and P. C. Canfield, Magnetic field effects on transport properties of PtSn 4, Phys. Rev. B 85, 035135 (2012)

  42. [42]

    Lau, Anomalous Electronic Transport in the Hexag- onal Ternary Arsenides FeCrAs, CrNiAs, and CrPdAs , Ph.D

    B. Lau, Anomalous Electronic Transport in the Hexag- onal Ternary Arsenides FeCrAs, CrNiAs, and CrPdAs , Ph.D. thesis

  43. [43]

    A. C. Jacko, J. O. Fjærestad, and B. J. Powell, A uni- fied explanation of the Kadowaki–Woods ratio in strongly correlated metals, Nature Physics 5, 422 (2009)

  44. [44]

    Z. Wang, M. Huang, J. Zhao, C. Chen, H. Huang, X. Wang, P. Liu, J. Wang, J. Xiang, C. Feng, Z. Zhang, X. Cui, Y. Lu, S. A. Yang, and B. Xiang, Fermi liq- uid behavior and colossal magnetoresistance in layered MoOCl2, Phys. Rev. Mater. 4, 041001 (2020)

  45. [45]

    F. L. Ruta, Y. Shao, S. Acharya, A. Mu, N. H. Jo, S. H. Ryu, D. Balatsky, Y. Su, D. Pashov, B. S. Y. Kim, M. I. Katsnelson, J. G. Analytis, E. Rotenberg, A. J. Millis, M. van Schilfgaarde, and D. N. Basov, Good plasmons in a bad metal, Science 387, 786 (2025)

  46. [46]

    Trovarelli, C

    O. Trovarelli, C. Geibel, R. Cardoso, S. Mederle, R. Borth, B. Buschinger, F. M. Grosche, Y. Grin, G. Sparn, and F. Steglich, Low-temperature properties of the Yb-based heavy-fermion antiferromagnets YbPtIn, YbRhSn, and YbNiGa, Phys. Rev. B 61, 9467 (2000)

  47. [47]

    S. L. Bud’ko, E. Morosan, and P. C. Canfield, Magnetic field induced non-fermi-liquid behavior in YbAgGe single crystals, Phys. Rev. B 69, 014415 (2004)

  48. [48]

    A. C. V, A. Ptok, P. Sobieszczyk, G. Vaitheeswaran, and V. Kanchana, Correlation stabilized ferro- magnetic MnRuAs with distorted kagome lattice, Physical Review B 111, 035125 (2025)