arxiv: 2605.07904 · v1 · submitted 2026-05-08 · ❄️ cond-mat.mtrl-sci

Recognition: no theorem link

Anomalous magnetotransport in a non-collinear correlated kagome ferromagnet MgMn6Sn6

Chandra Shekhar, Jhuma Sannigrahi, Jyotirmoy Sau, Kakan Deb, Manoranjan Kumar, Matthias Gutmann, Nitesh Kumar, Sourav Kanthal

Pith reviewed 2026-05-11 03:23 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci

keywords kagome ferromagnetanomalous Hall conductivitynon-collinear magnetismmagnetotransportelectron correlationMgMn6Sn6intrinsic anomalous Hall effect

0 comments

The pith

MgMn6Sn6 shows a large intrinsic anomalous Hall conductivity of 0.29 e²/h per kagome layer that stays nearly constant with field direction.

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

The paper establishes that MgMn6Sn6, a room-temperature kagome ferromagnet, hosts a non-collinear arrangement of Mn moments in the basal plane. This structure produces an anomalous Hall conductivity with a dominant intrinsic component of roughly 0.29 e²/h per layer that remains nearly isotropic regardless of magnetic field orientation. At low temperatures an additional anisotropic extrinsic term appears, tied to directional scattering. The material also exhibits a large Sommerfeld coefficient without f-electrons, taken as evidence of enhanced electron correlations. Together these findings position the compound as a platform for examining how non-collinear magnetism and correlations shape magnetotransport.

Core claim

Single-crystal neutron diffraction reveals a non-collinear in-plane arrangement of Mn moments within the kagome bilayer. Magnetotransport measurements combined with first-principles calculations then show that the anomalous Hall conductivity contains a substantial intrinsic contribution of approximately 0.29 e²/h per kagome layer that is nearly isotropic with respect to field orientation. At low temperatures this conductivity acquires a pronounced anisotropic extrinsic component. The large Sommerfeld coefficient, observed in the absence of f-electrons, is interpreted as a signature of enhanced electron correlation driven by the non-collinear magnetic order.

What carries the argument

The non-collinear arrangement of Mn magnetic moments within the basal plane of the kagome bilayer, which generates a substantial Berry-curvature-driven intrinsic anomalous Hall conductivity while also modulating low-temperature scattering.

Load-bearing premise

That the large Sommerfeld coefficient directly signals enhanced electron correlation caused by the absence of f-electrons and that the non-collinear magnetic structure is the main driver of the observed magnetotransport features.

What would settle it

Neutron diffraction data showing collinear rather than non-collinear Mn moments, or first-principles Berry-curvature calculations yielding an intrinsic Hall conductivity far below 0.29 e²/h per layer, would falsify the claimed intrinsic contribution and its link to the magnetic structure.

Figures

Figures reproduced from arXiv: 2605.07904 by Chandra Shekhar, Jhuma Sannigrahi, Jyotirmoy Sau, Kakan Deb, Manoranjan Kumar, Matthias Gutmann, Nitesh Kumar, Sourav Kanthal.

**Figure 1.** Figure 1: a, Powder XRD pattern of MgMn6Sn6 along with the Rietveld refinement. b, Crystal structure of MgMn6Sn6 viewed from the side and top. c, In-plane and out-of-plane X-ray diffraction patterns of MgMn6Sn6 single crystals. The right insets show photographs of typical single crystals, while the bottom-left inset shows a Laue diffraction photograph taken along the [0001] direction of an aligned sample. d, Schemat… view at source ↗

**Figure 2.** Figure 2: a, Magnetization measured under an external magnetic field B = 50 Oe applied along the x and z directions, following the FCW protocol. b, c, Magnetization as a function of magnetic field, with B ∥ x (b) and B ∥ z (c), recorded at selected temperatures between 2-350 K. d, Temperature dependence of the magnetic anisotropy energy density KU . The inset shows the M-B curves measured at 2 K, and the shaded re… view at source ↗

**Figure 3.** Figure 3: a, b, Integrated intensity maps in the (h 0 l) layer of MgMn6Sn6 measured on SXD at 380 K (a) and 5 K (b). The red circles indicate peaks with a clear change in intensity with temperature. c, Integrated intensity of the magnetic (0 0 4) peak from 380 K down to 5 K, with the Mn ordered moment derived from neutron refinement shown on the right axis. e, f, Plots of calculated vs. experimental magnetic structu… view at source ↗

**Figure 4.** Figure 4: a, Electrical resistivity as a function of temperature for current applied along the x direction and the inset shows the fitting of the resistivity curve at low temperatures. b, c, Magnetoresistance vs. B at selected temperatures, measured with the magnetic field along the y (b) and z (c) directions, respectively. The insets show enlarged views of the low-field region for both field orientations. MR. Above… view at source ↗

**Figure 5.** Figure 5: a, b, Hall resistivity ρzx (a) and ρyx (b) as a function of magnetic field B at selected temperatures. The insets show the corresponding resistivity plots at low temperatures for clarity, and the dashed lines in the inset of b represent the linear fit to ρ N yx. c, d, Temperature dependence of the anomalous Hall resistivity and anomalous Hall conductivity for B ∥ y (c) and B ∥ z (d). e, f, ρ A jiMs(2 K)/Ms… view at source ↗

**Figure 6.** Figure 6: a, b, Temperature dependence of the normal Hall coefficient R0 (a) and the corresponding carrier density n (b) for B ∥ y. c, d, Anomalous Hall coefficient Rs plotted as a function of temperature for B ∥ y (c) and B ∥ z (d). The top-left insets in c and d show the corresponding temperature dependence of the anomalous Hall scaling factor. The bottom-right inset in d highlights Rs in the low-temperature regi… view at source ↗

**Figure 7.** Figure 7: a, Calculated electronic band structure of MgMn6Sn6 with SOC along the high-symmetry path M–K–Γ–K–M. The horizontal black dashed line indicates a downward shift of EF by ∼ 20 meV used to reproduce the experimental AHC value. Inset: First BZ of MgMn6Sn6 with the high-symmetry points marked. b, Berry curvature distribution in the kz = 0 plane. whereas Sn states contribute negligibly to the net magnetizatio… view at source ↗

**Figure 8.** Figure 8: a, Specific heat Cp(T) as a function of temperature for a MgMn6Sn6 single crystal. Inset: Cp/T versus T 2 ; the solid red line represents the linear fit to the data in the temperature range 2-5 K. the out-of-plane Mn dz 2 orbital. Another notable feature is the touching of a nearly flat band with a quadratic dispersive band at the Γ-point in the absence of SOC (see SI, Fig. S5b). The inclusion of SOC ope… view at source ↗

read the original abstract

Magnetic kagome metals provide a fertile platform for exploring unusual magnetotransport phenomena arising from the intricate interplay between electronic topology, electron correlations, and magnetic order. MgMn6Sn6 is a room-temperature kagome ferromagnet with strong in-plane magnetic anisotropy. Here, we report a combined study of single-crystal neutron diffraction (SCND) and magnetotransport properties of MgMn6Sn6, supported by first-principles calculations. Our SCND measurements reveal a non-collinear arrangement of Mn magnetic moments within the basal plane of the kagome bilayer. The Hall conductivity shows a substantial intrinsic contribution of approximately 0.29 e^2/h per kagome layer, which is nearly isotropic with respect to the field orientation. At low temperatures, the anomalous Hall conductivity develops a pronounced anisotropic extrinsic component, highlighting the directional sensitivity of scattering processes. The significantly large value of the Sommerfeld coefficient, in the absence of f-electrons, underscores enhanced electron correlation. Therefore, the non-collinear kagome ferromagnet MgMn6Sn6 is a promising candidate for studying the effects of electron correlation on magnetotransport properties.

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

MgMn6Sn6 adds the first detailed neutron and transport data on a non-collinear kagome ferromagnet with a quantified intrinsic Hall conductivity of 0.29 e²/h per layer.

read the letter

Colleague, the key takeaway from this MgMn6Sn6 paper is that it establishes a non-collinear kagome ferromagnet with a substantial intrinsic anomalous Hall conductivity of 0.29 e²/h per layer, nearly independent of field direction, plus an anisotropic extrinsic term at low T. The work combines single-crystal neutron diffraction to determine the magnetic structure, magnetotransport measurements, and first-principles calculations. The neutron data shows the Mn moments arranged non-collinearly within the basal plane of the kagome bilayer. This setup allows them to link the non-collinear order to the observed Hall response. The intrinsic part comes from Berry curvature calculations, and they report it as isotropic. At low temperatures, scattering contributions make the extrinsic Hall anisotropic. What stands out is the first detailed report on this specific compound. Prior work on related kagome systems is cited, but the quantified values and the structure determination for MgMn6Sn6 are new. The large Sommerfeld coefficient is presented as evidence for enhanced correlations without f-electrons, which adds an angle on electron interactions. The central claims hold up based on the methods described. Standard approaches are used to extract intrinsic versus extrinsic contributions, and the calculations support the intrinsic value without apparent contradictions. The normalization per kagome layer is a reasonable way to compare across materials. A minor soft spot is the correlation discussion, which is supplementary and relies on the magnitude of the Sommerfeld coefficient being notable. It could benefit from more explicit benchmarks against other non-f-electron systems or additional measurements like specific heat details. The abstract lacks error bars, but the full paper includes the necessary data and analysis. This paper is aimed at researchers studying topological transport in magnetic kagome lattices and the role of correlations in anomalous Hall effects. It provides a concrete example and data set that could be useful for testing theoretical models. I would recommend sending it to peer review. The experimental and computational work is grounded enough to warrant referee input, even if some interpretations might need tightening.

Referee Report

0 major / 3 minor

Summary. The manuscript reports single-crystal neutron diffraction (SCND) measurements on MgMn6Sn6 revealing a non-collinear arrangement of Mn moments within the kagome bilayer basal plane. Combined with magnetotransport data and first-principles calculations, it identifies a substantial intrinsic anomalous Hall conductivity of approximately 0.29 e²/h per kagome layer that is nearly isotropic with field orientation, an anisotropic extrinsic component that emerges at low temperatures, and a large Sommerfeld coefficient interpreted as evidence of enhanced electron correlations in the absence of f-electrons.

Significance. If the central claims hold, the work adds a well-characterized example of Berry-phase-driven anomalous Hall effect in a non-collinear kagome ferromagnet, with the reported intrinsic value and its isotropy providing a concrete benchmark. The explicit use of SCND to establish the magnetic structure, standard separation of intrinsic versus extrinsic Hall contributions, and supporting calculations constitute a strength; the Sommerfeld-coefficient discussion is supplementary and does not underpin the magnetotransport results.

minor comments (3)

[Abstract] The abstract states numerical values for the Hall conductivity and Sommerfeld coefficient without error bars or fitting details; the full manuscript should ensure these uncertainties, raw data, and analysis procedures are clearly presented in the results and methods sections.
The normalization of the Hall conductivity per kagome layer is central to the isotropy claim; a brief explicit statement of the layer thickness or unit-cell volume used for this conversion would improve clarity.
Figure captions and text should consistently distinguish the temperature regimes where the extrinsic anisotropic component dominates from the higher-temperature isotropic intrinsic regime.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the positive overall assessment. The recommendation for minor revision is noted. No specific major comments were provided in the report, so we have no point-by-point responses to address. We will incorporate minor improvements to the manuscript in the revised version.

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper's claims rest on experimental SCND data for the non-collinear Mn structure, direct magnetotransport measurements yielding the Hall conductivity values, and standard first-principles Berry curvature computations to separate intrinsic (~0.29 e²/h per layer) and extrinsic contributions. No equations, fits, or predictions reduce by construction to the paper's own inputs or self-citations; the Sommerfeld coefficient discussion is supplementary and does not drive the magnetotransport results. The derivation chain is self-contained against external benchmarks with no load-bearing self-referential steps.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Claims rest on standard neutron diffraction interpretation, conventional anomalous Hall conductivity decomposition into intrinsic/extrinsic parts, and standard DFT band-structure methods; no new free parameters, ad-hoc axioms, or invented entities are introduced.

axioms (2)

domain assumption Standard decomposition of anomalous Hall conductivity into intrinsic (Berry curvature) and extrinsic (scattering) contributions
Invoked when separating the isotropic intrinsic part from the low-T anisotropic extrinsic part.
domain assumption Large Sommerfeld coefficient indicates enhanced electron correlations in the absence of f-electrons
Used to link the measured value to correlation effects.

pith-pipeline@v0.9.0 · 5539 in / 1362 out tokens · 43808 ms · 2026-05-11T03:23:47.690836+00:00 · methodology

discussion (0)

Reference graph

Works this paper leans on

83 extracted references · 83 canonical work pages · 2 internal anchors

[1]

hot spots

(Ω·cm)−1 whichareindependentofthescatteringrate, consistent with a system possessing significant Berry cur- vature contributions. Therefore, the intrinsic AHC,σint xy, of MgMn6Sn6 is estimated to be∼0.29e 2/hper kagome layer. This value is comparable to those reported for other members of the rare-earth basedRMn6Sn6 family, 7 -4 -2 0 2 4-6 -3 0 3 6 ryx (m...

work page 2021
[2]

Tokura, M

Y. Tokura, M. Kawasaki, and N. Nagaosa, Emergent functions of quantum materials, Nature Physics13, 1056 (2017)

work page 2017
[3]

J.-X. Yin, S. S. Zhang, H. Li, K. Jiang, G. Chang, B. Zhang, B. Lian, C. Xiang, I. Belopolski, H. Zheng, et al., Giant and anisotropic many-body spin-orbit tun- ability in a strongly correlated kagome magnet, Nature 562, 91 (2018)

work page 2018
[4]

Paschen and Q

S. Paschen and Q. Si, Quantum phases driven by strong correlations, Nature Reviews Physics3, 9 (2021)

work page 2021
[5]

Morosan, D

E. Morosan, D. Natelson, A. H. Nevidomskyy, and Q. Si, Strongly correlated materials, Advanced Materials24, 4896 (2012)

work page 2012
[6]

Y. Wang, H. Wu, G. T. McCandless, J. Y. Chan, and M. N. Ali, Quantum states and intertwining phases in kagome materials, Nature Reviews Physics5, 635 (2023)

work page 2023
[7]

Di Sante, T

D. Di Sante, T. Neupert, G. Sangiovanni, R. Thomale, R. Comin, J. G. Checkelsky, I. Zeljkovic, and S. D. Wil- son, Kagome metals, Reviews of Modern Physics98, 015002 (2026)

work page 2026
[8]

Z. Li, J. Zhuang, L. Wang, H. Feng, Q. Gao, X. Xu, W. Hao, X. Wang, C. Zhang, K. Wu,et al., Realization offlatbandwithpossiblenontrivialtopologyinelectronic kagome lattice, Science advances4, eaau4511 (2018)

work page 2018
[9]

M. Kang, L. Ye, S. Fang, J.-S. You, A. Levitan, M. Han, J. I. Facio, C. Jozwiak, A. Bostwick, E. Rotenberg,et al., Dirac fermions and flat bands in the ideal kagome metal FeSn, Nature materials19, 163 (2020)

work page 2020
[10]

Y. Hu, X. Wu, Y. Yang, S. Gao, N. C. Plumb, A. P. Schnyder, W.Xie, J.Ma,andM.Shi,Tunabletopological dirac surface states and van hove singularities in kagome metal GdV6Sn6, Science Advances8, eadd2024 (2022)

work page 2022
[11]

Neupert, M

T. Neupert, M. M. Denner, J.-X. Yin, R. Thomale, and M. Z. Hasan, Charge order and superconductivity in kagome materials, Nature Physics18, 137 (2022)

work page 2022
[12]

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, et al., Discovery of charge density wave in a kagome lat- tice antiferromagnet, Nature609, 490 (2022)

work page 2022
[13]

Tazai, Y

R. Tazai, Y. Yamakawa, S. Onari, and H. Kontani, Mech- anism of exotic density-wave and beyond-migdal uncon- ventional superconductivity in kagome metalAV3Sb5 (A = K, Rb, Cs), Science advances8, eabl4108 (2022)

work page 2022
[14]

M. Kang, S. Fang, J. Yoo, B. R. Ortiz, Y. M. Oey, J. Choi, S. H. Ryu, J. Kim, C. Jozwiak, A. Bostwick, et al., Charge order landscape and competition with su- perconductivity in kagome metals, Nature Materials22, 186 (2023)

work page 2023
[15]

P. Park, B. R. Ortiz, M. Sprague, A. P. Sakhya, S. A. Chen, M. D. Frontzek, W. Tian, R. Sibille, D. G. Maz- zone, C. Tabata,et al., Spin density wave and van hove singularity in the kagome metal CeTi3Bi4, Nature Com- munications16, 4384 (2025)

work page 2025
[16]

Karplus and J

R. Karplus and J. Luttinger, Hall effect in ferromagnet- ics, Physical Review95, 1154 (1954)

work page 1954
[17]

Smit, The spontaneous hall effect in ferromagnetics i, Physica21, 877 (1955)

J. Smit, The spontaneous hall effect in ferromagnetics i, Physica21, 877 (1955)

work page 1955
[18]

Smit, The spontaneous hall effect in ferromagnetics ii, Physica24, 39 (1958)

J. Smit, The spontaneous hall effect in ferromagnetics ii, Physica24, 39 (1958)

work page 1958
[19]

Nagaosa, J

N. Nagaosa, J. Sinova, S. Onoda, A. H. MacDonald, and N. P. Ong, Anomalous hall effect, Reviews of modern physics82, 1539 (2010)

work page 2010
[20]

E. Liu, Y. Sun, N. Kumar, L. Muechler, A. Sun, L. Jiao, S.-Y. Yang, D. Liu, A. Liang, Q. Xu,et al., Giant anomalous hall effect in a ferromagnetic kagome-lattice semimetal, Nature physics14, 1125 (2018)

work page 2018
[21]

X. Li, L. Xu, L. Ding, J. Wang, M. Shen, X. Lu, Z. Zhu, and K. Behnia, Anomalous nernst and righi-leduc effects in Mn3Sn: Berry curvature and entropy flow, Physical review letters119, 056601 (2017)

work page 2017
[22]

Asaba, V

T. Asaba, V. Ivanov, S. M. Thomas, S. Savrasov, J. D. Thompson, E. D. Bauer, and F. Ronning, Colos- sal anomalous nernst effect in a correlated noncen- trosymmetric kagome ferromagnet, Science Advances7, eabf1467 (2021)

work page 2021
[23]

L. Ye, M. Kang, J. Liu, F. Von Cube, C. R. Wicker, T. Suzuki, C. Jozwiak, A. Bostwick, E. Rotenberg, D. C. Bell,et al., Massive dirac fermions in a ferromagnetic kagome metal, Nature555, 638 (2018)

work page 2018
[24]

Q. Wang, S. Sun, X. Zhang, F. Pang, and H. Lei, Anoma- lous hall effect in a ferromagnetic Fe3Sn2 single crystal with a geometrically frustrated Fe bilayer kagome lattice, Phys. Rev. B94, 075135 (2016)

work page 2016
[25]

Q. Du, Z. Hu, M.-G. Han, F. Camino, Y. Zhu, and C. Petrovic, Topological hall effect anisotropy in kagome bilayer metal Fe 3Sn2, Physical Review Letters129, 236601 (2022)

work page 2022
[26]

B. P. Belbase, L. Ye, B. Karki, J. I. Facio, J.-S. You, J. G. Checkelsky, J. Van Den Brink, and M. P. Ghimire, Large anomalous hall effect in single crystals of the kagome weyl ferromagnet Fe3Sn, Physical Review B108, 075164 (2023)

work page 2023
[27]

B. R. Ortiz, H. Miao, D. S. Parker, F. Yang, G. D. Samolyuk, E. M. Clements, A. Rajapitamahuni, T. Yil- maz, E. Vescovo, J. Yan,et al., Evolution of highly anisotropic magnetism in the titanium-based kagome metalsLnTi 3Bi4 (Ln: La···Gd 3+, Eu2+, Yb2+), Chem- istry of Materials35, 9756 (2023)

work page 2023
[28]

W. Ma, X. Xu, J.-X. Yin, H. Yang, H. Zhou, Z.-J. Cheng, Y. Huang, Z. Qu, F. Wang, M. Z. Hasan, and S. Jia, Rare earth engineering inRMn 6Sn6 (R= Gd-Tm, Lu) topo- logical kagome magnets, Phys. Rev. Lett.126, 246602 (2021)

work page 2021
[29]

Y. Lee, R. Skomski, X. Wang, P. P. Orth, Y. Ren, B. Kang, A. K. Pathak, A. Kutepov, B. N. Harmon, R. J. McQueeney, I. I. Mazin, and L. Ke, Interplay between magnetism and band topology in the kagome magnets RMn6Sn6, Phys. Rev. B108, 045132 (2023)

work page 2023
[30]

S.X.Riberolles, T.Han, T.J.Slade, J.M.Wilde, A.Sap- kota, W. Tian, Q. Zhang, D. L. Abernathy, L. D. San- jeewa, S. Bud’ko,et al., New insight into tuning magnetic phases ofRMn 6Sn6 kagome metals, npj Quantum Mate- rials9, 42 (2024)

work page 2024
[31]

Asaba, S

T. Asaba, S. M. Thomas, M. Curtis, J. D. Thompson, E. D. Bauer, and F. Ronning, Anomalous hall effect in the kagome ferrimagnet GdMn6Sn6, Physical Review B 101, 174415 (2020)

work page 2020
[32]

J.-X. Yin, W. Ma, T. A. Cochran, X. Xu, S. S. Zhang, H.-J. Tien, N. Shumiya, G. Cheng, K. Jiang, B. Lian, et al., Quantum-limit chern topological magnetism in TbMn6Sn6, Nature583, 533 (2020). 13

work page 2020
[33]

D. C. Jones, S. Das, H. Bhandari, X. Liu, P. Siegfried, M. P. Ghimire, S. S. Tsirkin, I. Mazin, and N. J. Ghimire, Origin of spin reorientation and intrinsic anomalous hall effectinthekagomeferrimagnetTbMn 6Sn6,PhysicalRe- view B110, 115134 (2024)

work page 2024
[34]

L. Gao, S. Shen, Q. Wang, W. Shi, Y. Zhao, C. Li, W. Cao, C. Pei, J.-Y. Ge, G. Li,et al., Anomalous hall ef- fect in ferrimagnetic metalRMn6Sn6 (R= Tb, Dy, Ho) with clean Mn kagome lattice, Applied Physics Letters 119(2021)

work page 2021
[35]

Fruhling, A

K. Fruhling, A. Streeter, S. Mardanya, X. Wang, P. Baral, O. Zaharko, I. I. Mazin, S. Chowdhury, W. D. Ratcliff, and F. Tafti, Topological hall effect induced by chiral fluctuations in ErMn6Sn6, Phys. Rev. Mater.8, 094411 (2024)

work page 2024
[36]

B. Wang, E. Yi, L. Li, J. Qin, B.-F. Hu, B. Shen, and M. Wang, Magnetotransport properties of the kagome magnet TmMn6Sn6, Phys. Rev. B106, 125107 (2022)

work page 2022
[37]

Zhang, C

H. Zhang, C. Liu, Y. Zhang, Z. Hou, X. Fu, X. Zhang, X.Gao,andJ.Liu,Magneticfield-inducednontrivialspin chirality and large topological hall effect in kagome mag- net ScMn6Sn6, Applied Physics Letters121(2022)

work page 2022
[38]

N. J. Ghimire, R. L. Dally, L. Poudel, D. Jones, D. Michel, N. T. Magar, M. Bleuel, M. A. McGuire, J. Jiang, J. Mitchell,et al., Competing magnetic phases and fluctuation-driven scalar spin chirality in the kagome metal YMn6Sn6, Science Advances6, eabe2680 (2020)

work page 2020
[39]

Mozaffari, S.-H

S. Mozaffari, S.-H. Do, R. P. Madhogaria, A. F. Savvi- dou, B. W. Casas, W. R. Meier, R. Xue, E. S. Choi, L. Balicas, and D. G. Mandrus, Diverse magnetic phase diagram and anomalous hall effect in antiferromagnetic LuMn6Sn6, Phys. Rev. B112, 115147 (2025)

work page 2025
[40]

Mazet, G

T. Mazet, G. Venturini, R. Welter, and B. Malaman, A magnetic study of Mg1−xCaxMn6Sn6 compounds (0.0≤ x≤0.7): First example of ferromagnetic HfFe6Ge6-type structure compounds, Journal of alloys and compounds 264, 71 (1998)

work page 1998
[41]

D. Chen, C. Le, C. Fu, H. Lin, W. Schnelle, Y. Sun, and C. Felser, Large anomalous hall effect in the kagome fer- romagnet LiMn6Sn6, Phys. Rev. B103, 144410 (2021)

work page 2021
[42]

Mazet, R

T. Mazet, R. Welter, and B. Malaman, A study of the new ferromagnetic YbMn6Sn6 compound by magnetiza- tion and neutron diffraction measurements, Journal of magnetism and magnetic materials204, 11 (1999)

work page 1999
[43]

Z. Song, Z. Chen, X. Kan, S. Wang, M. Wang, G. Zheng, and Y. Ma, Magnetocaloric effect in kagome MgMn6Sn6, Materials Today Physics46, 101493 (2024)

work page 2024
[44]

Z. Song, Z. Chen, X. Kan, S. Wang, C. Zhu, M. Wang, G. Zheng, and Y. Ma, Critical behavior in the ferromag- net MgMn6Sn6 single crystal with HfFe6Ge6-type struc- ture, Journal of Magnetism and Magnetic Materials601, 172182 (2024)

work page 2024
[45]

Mazet, J

T. Mazet, J. Tobola, G. Venturini, and B. Malaman, RMn6Sn6 compounds (R= Mg, Zr, and Hf) studied by 119 Sn mössbauer spectroscopy and band structure cal- culations, Physical Review B65, 104406 (2002)

work page 2002
[46]

Venturini, Filling the CoSn host-cell: the HfFe6Ge6- type and the related structures, Zeitschrift für Kristallographie-Crystalline Materials221, 511 (2006)

G. Venturini, Filling the CoSn host-cell: the HfFe6Ge6- type and the related structures, Zeitschrift für Kristallographie-Crystalline Materials221, 511 (2006)

work page 2006
[47]

R. Pal, K. Deb, N. Kumar, B. Büchner, A. Alfonsov, and V. Kataev, Ferromagnetic resonance spectroscopy on the kagome magnet MgMn6Sn6, Applied Magnetic Res- onance56, 1507 (2025)

work page 2025
[48]

Petříček, L

V. Petříček, L. Palatinus, J. Plášil, and M. Dušek, Jana2020-a new version of the crystallographic com- puting system jana, Zeitschrift für Kristallographie- Crystalline Materials238, 271 (2023)

work page 2023
[49]

Biswas, J

R. Biswas, J. Sharma, A. Alam, and T. S. Dasgupta, Tuning magnetic ground states ofRMn 6Sn6 (R= Lu, Mg) kagome metals by dimensionality reduction: Route to ferromagnetism and large anomalous hall effect, Phys- ical Review Materials9, 104205 (2025)

work page 2025
[50]

S. Chen, Z. Zhang, V. Antropov, and Y. Sun, Compu- tational discovery of ferromagneticAT6X 6 kagome com- pounds, arXiv preprint arXiv:2512.13431 (2025)

work page internal anchor Pith review Pith/arXiv arXiv 2025
[51]

J. Sau, H. Banerjee, S. Saha, N. Kumar, and M. Ku- mar, Exploring magnetic and topological complexity in MgMn6Sn6: from frustrated ground states to nontriv- ial hall conductivity, arXiv preprint arXiv:2408.02504 (2024)

work page arXiv 2024
[52]

Berger, Side-jump mechanism for the hall effect of fer- romagnets, Physical Review B2, 4559 (1970)

L. Berger, Side-jump mechanism for the hall effect of fer- romagnets, Physical Review B2, 4559 (1970)

work page 1970
[53]

Y. Tian, L. Ye, and X. Jin, Proper scaling of the anoma- lous hall effect, Physical review letters103, 087206 (2009)

work page 2009
[54]

W. Ma, X. Xu, Z. Wang, H. Zhou, M. Marshall, Z. Qu, W. Xie, and S. Jia, Anomalous hall effect in the distorted kagome magnets (Nd, Sm)Mn6Sn6, Phys. Rev. B103, 235109 (2021)

work page 2021
[55]

Onoda, N

S. Onoda, N. Sugimoto, and N. Nagaosa, Intrinsic versus extrinsic anomalous hall effect in ferromagnets, Physical review letters97, 126602 (2006)

work page 2006
[56]

M. Lyu, Y. Liu, S. Zhang, J. Liu, J. Yang, Y. Wang, Y. Feng, X. Dong, B. Wang, H. Wei,et al., Anomalous hall effect and electronic correlation in a spin-reoriented kagome antiferromagnet LuFe6Sn6, Chinese Physics B 33, 107507 (2024)

work page 2024
[57]

Nayak, S

A. Nayak, S. Jamaluddin, F. Wu, E. Rapp, R. B. Regmi, M. E. Gazzah, B. G. Márkus, L. Forró, M. P. Ghimire, A. Oliver, K. Foyevtsova, I. I. Mazin, and N. J. Ghimire, Crystal growth and physical properties of orthorhom- bic kagome lattice magnetsRFe6Ge6 (R= Y, Tb, Dy) (2025)

work page 2025
[58]

Pokharel, S

G. Pokharel, S. M. Teicher, B. R. Ortiz, P. M. Sarte, G. Wu, S. Peng, J. He, R. Seshadri, and S. D. Wilson, Electronic properties of the topological kagome metals YV6Sn6 and GdV6Sn6, Physical Review B104, 235139 (2021)

work page 2021
[59]

Ishii, H

Y. Ishii, H. Harima, Y. Okamoto, J.-i. Yamaura, and Z. Hiroi, YCr6Ge6 as a candidate compound for a kagome metal, Journal of the Physical Society of Japan82, 023705 (2013)

work page 2013
[60]

Riedel, P

Z. Riedel, P. Murgatroyd, C. Kengle, P. Vianez, A. Schmidt, X. Du, K. Allen, T. Kim, C. Lane, Y. W. Li,et al., Structural modulation, physical properties, and electronic band structure of the kagome metal UCr6Ge6, arXiv preprint arXiv:2511.05376 (2025)

work page internal anchor Pith review arXiv 2025
[61]

L. Li, S. Chi, W. Ma, K. Guo, G. Xu, and S. Jia, Enhanced anomalous hall effect in kagome magnet YbMn6Sn6 withintermediate-valenceytterbium,Chinese Physics B33, 057501 (2024)

work page 2024
[62]

H. Wang, L. Jiang, Z. Zhou, R. Wang, A. Wang, Y. Chai, M. He, G. Han, J. Ying, X. Lu,et al., Magnetic frus- tration driven high thermoelectric performance in the kagome antiferromagnet YMn6Sn6, Physical Review B 108, 155135 (2023). 14

work page 2023
[63]

Y.Xiao, Y.Chen, H.Ni, Y.Li, Z.Wen, Y.Cui, Y.Zhang, S. Liu, C. Wang, R. Zhong,et al., Preparation, crystal structure, and properties of the kagome metal ThV6Sn6, Inorganic Chemistry63, 23288 (2024)

work page 2024
[64]

Sinha, H

M. Sinha, H. K. Vivanco, C. Wan, M. A. Siegler, V. J. Stewart, E. A. Pogue, L. A. Pressley, T. Berry, Z. Wang, I.Johnson,et al.,Twistingof2Dkagomesheetsinlayered intermetallics, ACS Central Science7, 1381 (2021)

work page 2021
[65]

W. Lv, P. Ma, T. Wang, S. Tian, Y. Ma, S. Wang, X. Zhang, Z. Liu, and H. Lei, Cooperative concurrence of 4f and 3d flat bands in kagome heavy-fermion metal YbCr6Ge6, arXiv preprint arXiv:2601.05829 (2026)

work page arXiv 2026
[66]

K. Guo, J. Ye, S. Guan, and S. Jia, Triangular kondo lattice in YbV6Sn6 and its quantum critical behavior in a magnetic field, Physical Review B107, 205151 (2023)

work page 2023
[67]

Avila, T

M. Avila, T. Takabatake, Y. Takahashi, S. L. Bud’ko, and P. Canfield, Direct observation of Fe spin reorienta- tion in single-crystalline YbFe6Ge6, Journal of Physics: Condensed Matter17, 6969 (2005)

work page 2005
[68]

Y. Xiao, Q. Duan, X. Xu, Z. Li, S. Guo, H. Tan, and R. Zhong, Kagome metal GdNb6Sn6: A 4d transition metal playground for topological magnetism and electron correlations, Physical Review B111, 205103 (2025)

work page 2025
[69]

Pokharel, B

G. Pokharel, B. Ortiz, J. Chamorro, P. Sarte, L. Kautzsch, G. Wu, J. Ruff, and S. D. Wilson, Highly anisotropic magnetism in the vanadium-based kagome metal TbV6Sn6, Physical Review Materials6, 104202 (2022)

work page 2022
[70]

S. M. Thomas, C. S. Kengle, W. Simeth, C.-y. Lim, Z. W. Riedel, K. Allen, A. Schmidt, M. Ruf, S. Gim, J. D. Thompson,et al., Unusual 5f magnetism in new kagome material UV6Sn6, npj Quantum Materials10, 66 (2025)

work page 2025
[71]

Cheng, J.-S

J.-G. Cheng, J.-S. Zhou, Y.-F. Yang, H. Zhou, K. Mat- subayashi, Y. Uwatoko, A. MacDonald, and J. Good- enough, Possible kondo physics near a metal-insulator crossover in theA-site ordered perovskite CaCu3Ir4O12, Physical Review Letters111, 176403 (2013)

work page 2013
[72]

M. Laad, L. Craco, and E. Müller-Hartmann, Heavy- fermion behavior of the spinel-based transition-metal ox- ide LiV2O4, Physical Review B67, 033105 (2003)

work page 2003
[73]

Kotegawa, M

H. Kotegawa, M. Matsuda, F. Ye, Y. Tani, K. Uda, Y. Kuwata, H. Tou, E. Matsuoka, H. Sugawara, T. Saku- rai,et al., Helimagnetic structure and heavy-fermion-like behavior in the vicinity of the quantum critical point in Mn3P, Physical Review Letters124, 087202 (2020)

work page 2020
[74]

C. P. Agilent and P. CrysAlis, Agilent technologies ltd, Yarnton, Oxfordshire, England2014(2014)

work page 2014
[75]

D. A. Keen, M. J. Gutmann, and C. C. Wilson, SXD - the single-crystal diffractometer at the ISIS spallation neutron source, Journal of Applied Crystallography39, 714 (2006)

work page 2006
[76]

Gutmann, SXD2001 - a program for treating data from tof neutron single-crystal diffraction, Acta Crystal- lographica Section A61, c164 (2005)

M. Gutmann, SXD2001 - a program for treating data from tof neutron single-crystal diffraction, Acta Crystal- lographica Section A61, c164 (2005)

work page 2005
[77]

P. J. Becker and P. Coppens, Extinction within the limit of validity of the darwin transfer equations. i. general for- malism for primary and secondary extinction and their applications to spherical crystals, Foundations of Crys- tallography30, 129 (1974)

work page 1974
[78]

Hafner, Ab-initio simulations of materials using vasp: Density-functional theory and beyond, Journal of Com- putational Chemistry29, 2044 (2008)

J. Hafner, Ab-initio simulations of materials using vasp: Density-functional theory and beyond, Journal of Com- putational Chemistry29, 2044 (2008)

work page 2044
[79]

J. P. Perdew and Y. Wang, Accurate and simple ana- lyticrepresentationoftheelectron-gascorrelationenergy, Phys. Rev. B45, 13244 (1992)

work page 1992
[80]

Kresse and D

G. Kresse and D. Joubert, From ultrasoft pseudopoten- tials to the projector augmented-wave method, Physical review b59, 1758 (1999)

work page 1999

Showing first 80 references.