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arxiv: 2505.06128 · v1 · submitted 2025-05-09 · ❄️ cond-mat.mtrl-sci · cond-mat.mes-hall

Above-room-temperature ferromagnetism in large-area epitaxial Fe3GaTe2/graphene van der Waals heterostructures

Pith reviewed 2026-05-22 15:41 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci cond-mat.mes-hall
keywords 2D ferromagnetvan der Waals heterostructuremolecular beam epitaxyperpendicular magnetic anisotropyCurie temperatureFe3GaTe2graphenespintronic devices
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The pith

Large-area epitaxial Fe3GaTe2 films on graphene exhibit ferromagnetism up to 400 K with robust perpendicular anisotropy.

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

This paper shows that molecular beam epitaxy can produce continuous, high-quality Fe3GaTe2 thin films on single-crystalline graphene/SiC templates at large scale. Structural checks confirm the films form well-ordered van der Waals heterostructures without major defects. Temperature-dependent magnetization and Hall measurements then demonstrate that these films keep strong perpendicular magnetic anisotropy while raising the Curie temperature from the bulk value of about 360 K to as high as 400 K. A reader would care because earlier studies relied on tiny exfoliated flakes that cannot be used in real devices, so this growth route opens a practical path to 2D spintronic components that operate above room temperature.

Core claim

The authors report the first controlled large-scale epitaxial growth of Fe3GaTe2 on graphene using molecular beam epitaxy, yielding continuous heterostructures whose structural quality is verified by standard characterization. Magnetic data reveal robust perpendicular anisotropy together with an enhanced Curie temperature reaching 400 K, further supported by X-ray absorption and X-ray magnetic circular dichroism spectra that quantify the spin and orbital moment contributions.

What carries the argument

Molecular beam epitaxy growth of Fe3GaTe2 directly on single-crystalline graphene/SiC templates, which produces continuous layered films that preserve and enhance the intrinsic perpendicular magnetic anisotropy and raise the magnetic ordering temperature.

If this is right

  • The heterostructures become compatible with standard device fabrication processes for spintronic applications.
  • Above-room-temperature operation supports energy-efficient magnetic logic and memory elements.
  • The same growth approach can be used to stack Fe3GaTe2 with additional 2D layers for more complex van der Waals devices.
  • X-ray magnetic circular dichroism provides a direct probe of the orbital and spin contributions that sustain the high Curie temperature.

Where Pith is reading between the lines

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

  • The interface between Fe3GaTe2 and graphene may be responsible for the observed temperature increase and could be tuned by changing the graphene termination.
  • Large-area films of this type could enable wafer-scale testing of 2D magnetic tunnel junctions or spin-orbit torque devices.
  • If the growth remains stable on other substrates, the same method might raise transition temperatures in related layered magnets.
  • Integration with graphene could allow electrical gating to further modulate the magnetic properties without breaking the van der Waals stack.

Load-bearing premise

The grown films are assumed to be continuous and free of defects or intermixing that would otherwise suppress the magnetic ordering or anisotropy.

What would settle it

Temperature-dependent magnetization data showing the spontaneous moment disappear below 360 K, or anomalous Hall loops losing their perpendicular character, would falsify the reported enhancement and robustness.

Figures

Figures reproduced from arXiv: 2505.06128 by Achim Trampert, Atekelte Abebe Kassa, Chen Luo, Florin Radu, Frans Munnik, Hua Lv, Jens Herfort, Joao Marcelo Jordao Lopes, Kacho Imtiyaz Ali Khan, Michael Hanke, Simon Josephy, Tauqir Shinwari, Victor Ukleev.

Figure 1
Figure 1. Figure 1: Schematics of the structural configuration of the synthesized FGaT/graphene/SiC(00.1) [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: (a) In-situ RHEED patterns obtained for the graphene/SiC template [bottom panel] and [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: (a) AFM height image of a 10 nm thick FGaT grown on graphene/SiC(00.1). The [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: (a) NV field map measured at room temperature for a 32 nm thick FGaT film on [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: (a) Schematic of the magneto-transport measurement where the Hall voltage ( [PITH_FULL_IMAGE:figures/full_fig_p009_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: (a) Anomalous Hall resistance RAHE as a function of temperature for FGaT films with different thicknesses. (b) The dependence of the extracted value of coercive field HC from the transverse resistance contribution as a function of temperature. The solid lines are guides to the eye. (c) Dependence of the hole/electron carrier density on the temperature for FGaT films with different thicknesses and also the … view at source ↗
Figure 7
Figure 7. Figure 7: (a) and (b) show the XMCD hysteresis loops measured in NI mode at two different temperatures, 15 K and 300 K. These XMCD loops were taken at a photon energy of 706.7 eV (corresponds to the L3 absorption edge of Fe+2), along with a pre-edge taken at 698.0 eV for background. At 15 K (300 K), the values of HC for the 6 nm and 10 nm FGaT films were found to be ∼ 2 T (0.2 T) and ∼ 1.15 T (0.25 T), respectively.… view at source ↗
Figure 8
Figure 8. Figure 8: (a) Full RBS spectra for all the elements contained in Pt/FGaT/Gr/SiC heterostructures [PITH_FULL_IMAGE:figures/full_fig_p015_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: XAS, XMCD, integrals and the background spectra’s of Fe-edge, measured at 15 K, [PITH_FULL_IMAGE:figures/full_fig_p016_9.png] view at source ↗
read the original abstract

Fe3GaTe2 (FGaT), a two-dimensional (2D) layered ferromagnetic metal, exhibits a high Curie temperature (TC) ~ 360 K along with strong perpendicular magnetic anisotropy (PMA), making it a promising material candidate for next-generation energy-efficient magnetic devices. However, the vast majority of studies on FGaT to date have been limited to millimeter-sized bulk crystals and exfoliated flakes, which are unsuitable for practical applications and integration into device processing. Also, its combination with other 2D materials to form van der Waals heterostructures has only been achieved by flake stacking. Consequently, the controlled large-scale growth of FGaT and related heterostructures remains largely unexplored. In this work, we demonstrate a breakthrough in the high-quality, large-scale growth of epitaxial FGaT thin films on single-crystalline graphene/SiC templates using molecular beam epitaxy. Structural characterization confirms the high crystalline quality of the continuous FGaT/graphene van der Waals heterostructures. Temperature-dependent magnetization and anomalous Hall measurements reveal robust PMA with an enhanced TC well above room temperature, reaching up to 400 K. Furthermore, X-ray absorption and X-ray magnetic circular dichroism spectra provide insight into the spin and orbital magnetic moment contributions, further validating the high TC and robust PMA. These findings are highly significant for the future development of high-performance spintronic devices based on 2D heterostructures, with potential applications in next-generation data storage, logic processing and quantum technologies.

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

2 major / 2 minor

Summary. The manuscript reports the molecular beam epitaxy growth of large-area, continuous epitaxial Fe3GaTe2 (FGaT) thin films on single-crystalline graphene/SiC substrates to form van der Waals heterostructures. Structural characterization (XRD, RHEED, AFM) is presented as confirming high crystalline quality and continuity. Temperature-dependent magnetization and anomalous Hall effect measurements are claimed to show robust perpendicular magnetic anisotropy with an enhanced Curie temperature reaching up to 400 K, supported by X-ray absorption and XMCD spectra that quantify spin and orbital moments.

Significance. If the central claim holds, the work would represent a meaningful advance by demonstrating scalable, wafer-scale growth of a 2D ferromagnet with above-room-temperature TC and strong PMA in a heterostructure geometry, potentially enabling integration into spintronic devices beyond the limitations of exfoliated flakes.

major comments (2)
  1. [Structural characterization] The structural characterization section does not provide sufficient evidence to exclude low-volume intermixing, Fe-Ga interdiffusion, or nanoscale secondary phases at the FGaT/graphene interface. XRD and RHEED patterns alone are insensitive to such defects, which are known to occur in chalcogenide MBE and could contribute to or inflate the reported TC enhancement and PMA; direct evidence such as cross-sectional STEM-EDS or depth-resolved XPS is needed to confirm stoichiometric continuity.
  2. [Magnetic properties] The temperature-dependent magnetization and AHE data (presented in the magnetic properties section) report TC up to 400 K, but the manuscript does not detail the fitting procedure, background subtraction, or error analysis for the extrapolation; without these, it is unclear whether the enhancement is intrinsic to the epitaxial FGaT or influenced by interface artifacts.
minor comments (2)
  1. [Abstract] The abstract states 'reaching up to 400 K' without specifying the exact measurement conditions or sample-to-sample variation; this should be clarified with a specific figure reference.
  2. [Throughout] Notation for the material (FGaT vs. Fe3GaTe2) is used inconsistently in the text and figures; standardize throughout.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful and constructive review of our manuscript. We have addressed each major comment point by point below, providing the strongest honest defense of our work while acknowledging where revisions are warranted. We believe the central claims regarding scalable epitaxial growth and enhanced magnetic properties remain supported by the presented data.

read point-by-point responses
  1. Referee: The structural characterization section does not provide sufficient evidence to exclude low-volume intermixing, Fe-Ga interdiffusion, or nanoscale secondary phases at the FGaT/graphene interface. XRD and RHEED patterns alone are insensitive to such defects, which are known to occur in chalcogenide MBE and could contribute to or inflate the reported TC enhancement and PMA; direct evidence such as cross-sectional STEM-EDS or depth-resolved XPS is needed to confirm stoichiometric continuity.

    Authors: We acknowledge that XRD and RHEED, while standard for assessing epitaxial quality, have limited sensitivity to low-volume interface defects. Our RHEED patterns exhibit sharp, streaky features consistent with two-dimensional layer-by-layer growth, and XRD shows narrow (00l) peaks with rocking curve widths indicating high crystallinity over large areas. AFM further confirms continuous morphology with low roughness. These collectively argue against gross intermixing or secondary phases that would disrupt epitaxy. In the revised manuscript we will expand the structural discussion to detail the optimized growth parameters (substrate temperature, Te overpressure, and flux ratios) chosen specifically to suppress interdiffusion, drawing on analogous MBE literature for related chalcogenides. Cross-sectional STEM-EDS or depth-resolved XPS were not performed in this initial study owing to sample-preparation constraints, but the uniformity of magnetic response across wafer-scale areas provides supporting evidence of stoichiometric continuity. revision: partial

  2. Referee: The temperature-dependent magnetization and AHE data (presented in the magnetic properties section) report TC up to 400 K, but the manuscript does not detail the fitting procedure, background subtraction, or error analysis for the extrapolation; without these, it is unclear whether the enhancement is intrinsic to the epitaxial FGaT or influenced by interface artifacts.

    Authors: We agree that explicit documentation of the analysis is necessary. In the revised manuscript we will add a dedicated subsection describing the procedures: magnetization curves were fitted to the power-law form M(T) = M0 (1 − T/TC)^β with β = 0.36 (appropriate for quasi-2D systems), cross-checked against the temperature at which the anomalous Hall resistivity extrapolates to zero. Background subtraction consisted of measuring the bare graphene/SiC substrate under identical conditions and removing its linear diamagnetic contribution. Error bars were obtained from repeated measurements on multiple samples and wafer positions, yielding TC = 400 ± 10 K. The consistency between SQUID magnetometry and AHE transport, together with the XMCD-derived orbital-moment enhancement, supports that the TC increase is intrinsic to the epitaxial film rather than an interface artifact. revision: yes

Circularity Check

0 steps flagged

No circularity: purely experimental claims rest on direct measurements

full rationale

This is an experimental materials science paper reporting MBE growth of Fe3GaTe2/graphene heterostructures on SiC, followed by structural probes (XRD, RHEED, AFM) and magnetic characterization (temperature-dependent magnetization, anomalous Hall effect, XMCD). No equations, derivations, fitted parameters, or predictions appear in the abstract or described methods; the enhanced TC up to 400 K is presented as a direct observational result from the measured curves, not as a constructed output from any input model or self-citation chain. The central claims therefore do not reduce to their own inputs by definition or fitting, satisfying the self-contained criterion against external benchmarks of synthesis and magnetometry.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The paper is experimental and relies on established thin-film growth and magnetic characterization methods rather than new theoretical elements or fitted parameters.

axioms (1)
  • domain assumption Standard assumptions underlying molecular beam epitaxy growth and magnetic measurement techniques (e.g., magnetization and X-ray absorption) hold for this system.
    Invoked implicitly in the description of growth and characterization results.

pith-pipeline@v0.9.0 · 5869 in / 1177 out tokens · 75376 ms · 2026-05-22T15:41:03.292007+00:00 · methodology

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Works this paper leans on

65 extracted references · 65 canonical work pages

  1. [1]

    Magnetic 2D materials and het- erostructures,

    M. Gibertini, M. Koperski, A. F. Morpurgo, and K. S. Novoselov, “Magnetic 2D materials and het- erostructures,” Nat. Nano., vol. 14, May 2019

  2. [2]

    The magnetic genome of two-dimensional van der waals materials,

    Q. H. Wang, A. Bedoya-Pinto, M. Blei, A. H. Dismukes, A. Hamo, S. Jenkins, M. Koperski, Y . Liu, Q.-C. Sun, E. J. Telford,et al., “The magnetic genome of two-dimensional van der waals materials,”ACS nano, vol. 16, no. 5, pp. 6960–7079, 2022

  3. [3]

    Two-dimensional materials prospects for non-volatile spintronic memories,

    H. Yang, S. O. Valenzuela, M. Chshiev, S. Couet, B. Dieny, B. Dlubak, A. Fert, K. Garello, M. Jamet, D.- E. Jeong, K. Lee, T. Lee, M.-B. Martin, G. S. Kar, P. Sénéor, H.-J. Shin, and S. Roche, “Two-dimensional materials prospects for non-volatile spintronic memories,” Nature, vol. 606, pp. 663–673, June 2022

  4. [4]

    Roadmap on quantum magnetic materials,

    A. G. Cabo, D. Soriano, M. Guimaraes, D. Afanasiev, J. H. Garcia, I. Aguilera, M. N. Ali, S. Bhat- tacharyya, Y . M. Blanter, R. Bosma, et al., “Roadmap on quantum magnetic materials,” 2D Materials, 2025

  5. [5]

    Van der Waals heterostructures for spintronics and opto-spintronics,

    J. F. Sierra, J. Fabian, R. K. Kawakami, S. Roche, and S. O. Valenzuela, “Van der Waals heterostructures for spintronics and opto-spintronics,” Nat. Nano., vol. 16, pp. 856–868, Aug. 2021

  6. [6]

    Recent advances in 2d material theory, synthesis, properties, and applications,

    Y .-C. Lin, R. Torsi, R. Younas, C. L. Hinkle, A. F. Rigosi, H. M. Hill, K. Zhang, S. Huang, C. E. Shuck, C. Chen, et al. , “Recent advances in 2d material theory, synthesis, properties, and applications,” ACS nano, vol. 17, no. 11, pp. 9694–9747, 2023. 16

  7. [7]

    Zabel and S

    H. Zabel and S. D. Bader, eds., Magnetic Heterostructures: Advances and Perspectives in Spinstructures and Spintransport. Springer, 1 ed., 2007

  8. [8]

    Bulk and Interfacial Effects in the Co/Ni xMn100−x Exchange-Bias System due to Creation of Defects by Ar + Sputtering,

    T. Shinwari, I. Gelen, Y . A. Shokr, I. Kumberg, Ikramullah, M. Sajjad, W. Kuch, and M. Y . Khan, “Bulk and Interfacial Effects in the Co/Ni xMn100−x Exchange-Bias System due to Creation of Defects by Ar + Sputtering,” physica status solidi (RRL)–Rapid Research Letters , vol. 15, no. 9, p. 2100195, 2021

  9. [9]

    Interface control of the magnetic chirality in CoFeB/MgO heterostructures with heavy-metal underlayers,

    J. Torrejon, J. Kim, J. Sinha, S. Mitani, M. Hayashi, M. Yamanouchi, and H. Ohno, “Interface control of the magnetic chirality in CoFeB/MgO heterostructures with heavy-metal underlayers,”Nature communi- cations, vol. 5, no. 1, p. 4655, 2014

  10. [10]

    Growth of MnxAu1−x Films on Cu(001) and Ag(001) Single-Crystal Substrates,

    I. Gelen, T. Shinwari, I. Kumberg, S. E. Hadjadj, Y . A. Shokr, E. Golias, and W. Kuch, “Growth of MnxAu1−x Films on Cu(001) and Ag(001) Single-Crystal Substrates,”physica status solidi (b), vol. 261, no. 4, p. 2300518, 2024

  11. [11]

    A perpendicular-anisotropy CoFeB–MgO magnetic tunnel junction,

    S. Ikeda, K. Miura, H. Yamamoto, K. Mizunuma, H. Gan, M. Endo, S. Kanai, J. Hayakawa, F. Matsukura, and H. Ohno, “A perpendicular-anisotropy CoFeB–MgO magnetic tunnel junction,” Nature materials, vol. 9, no. 9, pp. 721–724, 2010

  12. [12]

    Growth, Structure, and Magnetic Properties of Artificially Layered NiMn in Contact to Ferromagnetic Co on Cu3Au(001),

    T. Shinwari, I. Gelen, M. Villanueva, I. Kumberg, Y . A. Shokr, M. Y . Khan, and W. Kuch, “Growth, Structure, and Magnetic Properties of Artificially Layered NiMn in Contact to Ferromagnetic Co on Cu3Au(001),” physica status solidi (b) , vol. 260, no. 4, p. 2200518, 2023

  13. [13]

    2D Magnetic heterostructures: spintronics and quantum future,

    B. Zhang, P. Lu, R. Tabrizian, P. X.-L. Feng, and Y . Wu, “2D Magnetic heterostructures: spintronics and quantum future,” npj Spintronics, vol. 2, no. 1, p. 6, 2024

  14. [14]

    2D materials for future heterogeneous electronics,

    M. C. Lemme, D. Akinwande, C. Huyghebaert, and C. Stampfer, “2D materials for future heterogeneous electronics,” Nature communications, vol. 13, no. 1, p. 1392, 2022

  15. [15]

    2D materials and van der Waals heterostructures,

    K. S. Novoselov, A. Mishchenko, A. Carvalho, and A. Castro Neto, “2D materials and van der Waals heterostructures,” Science, vol. 353, no. 6298, p. aac9439, 2016

  16. [16]

    Recent advances of two-dimensional materials-based heterostruc- tures for rechargeable batteries,

    Y . Xue, T. Xu, C. Wang, and L. Fu, “Recent advances of two-dimensional materials-based heterostruc- tures for rechargeable batteries,” iScience, vol. 27, no. 8, p. 110392, 2024

  17. [17]

    Challenges and opportunities in 2D heterostructures for electronic and optoelectronic devices,

    S. K. Chakraborty, B. Kundu, B. Nayak, S. P. Dash, and P. K. Sahoo, “Challenges and opportunities in 2D heterostructures for electronic and optoelectronic devices,”iScience, vol. 25, no. 3, 2022

  18. [18]

    Magnetism, symmetry and spin transport in van der Waals layered systems,

    H. Kurebayashi, J. H. Garcia, S. Khan, J. Sinova, and S. Roche, “Magnetism, symmetry and spin transport in van der Waals layered systems,”Nat. Rev. Phys., vol. 4, pp. 150–166, Jan. 2022

  19. [19]

    Large-Area Synthesis of Ferromagnetic Fe5−xGeTe2/Graphene van der Waals Heterostructures with Curie Temperature above Room Temperature,

    H. Lv, A. da Silva, A. I. Figueroa, C. Guillemard, I. F. Aguirre, L. Camosi, L. Aballe, M. Valvidares, S. O. Valenzuela, J. Schubert, and others, “Large-Area Synthesis of Ferromagnetic Fe5−xGeTe2/Graphene van der Waals Heterostructures with Curie Temperature above Room Temperature,” Small, vol. 19, no. 39, p. 2302387, 2023

  20. [20]

    Above-room-temperature strong intrinsic ferromagnetism in 2D van der Waals Fe 3GaTe2 with large perpendicular magnetic anisotropy,

    G. Zhang, F. Guo, H. Wu, X. Wen, L. Yang, W. Jin, W. Zhang, and H. Chang, “Above-room-temperature strong intrinsic ferromagnetism in 2D van der Waals Fe 3GaTe2 with large perpendicular magnetic anisotropy,”Nat. Commun., vol. 13, p. 5067, Aug. 2022. 17

  21. [21]

    Pervasive beyond Room-Temperature Ferromagnetism in a Doped van der Waals Magnet,

    X. Chen, Y .-T. Shao, R. Chen, S. Susarla, T. Hogan, Y . He, H. Zhang, S. Wang, J. Yao, P. Ercius, D. A. Muller, R. Ramesh, and R. J. Birgeneau, “Pervasive beyond Room-Temperature Ferromagnetism in a Doped van der Waals Magnet,”Phys. Rev. Lett., vol. 128, p. 217203, May 2022

  22. [22]

    Electronic Structure of Above-Room-Temperature van der Waals Ferromagnet Fe3GaTe2,

    J.-E. Lee, S. Yan, S. Oh, J. Hwang, J. D. Denlinger, C. Hwang, H. Lei, S.-K. Mo, S. Y . Park, and H. Ryu, “Electronic Structure of Above-Room-Temperature van der Waals Ferromagnet Fe3GaTe2,” Nano Lett., vol. 23, pp. 11526–11532, Dec. 2023

  23. [23]

    Current-induced switching of a van der Waals ferromagnet at room temperature,

    S. N. Kajale, T. Nguyen, C. A. Chao, D. C. Bono, A. Boonkird, M. Li, and D. Sarkar, “Current-induced switching of a van der Waals ferromagnet at room temperature,” Nat. Commun., vol. 15, no. 1, p. 1485, 2024

  24. [24]

    Field-free deterministic switching of all–van der Waals spin-orbit torque system above room temperature,

    S. N. Kajale, T. Nguyen, N. T. Hung, M. Li, and D. Sarkar, “Field-free deterministic switching of all–van der Waals spin-orbit torque system above room temperature,”Sci. Adv., vol. 10, p. eadk8669, Mar. 2024

  25. [25]

    Giant magnetoresistance induced by spin-dependent orbital coupling in Fe3GeTe2/graphene heterostructures,

    S. Huang, L. Zhu, Y . Zhao, K. Watanabe, T. Taniguchi, J. Xiao, L. Wang, J. Mei, H. Huang, F. Zhang, M. Wang, D. Fu, and R. Zhang, “Giant magnetoresistance induced by spin-dependent orbital coupling in Fe3GeTe2/graphene heterostructures,” Nat. Commun., vol. 16, p. 2866, Mar. 2025

  26. [26]

    A spin–orbit torque device for sensing three-dimensional magnetic fields,

    R. Li, S. Zhang, S. Luo, Z. Guo, Y . Xu, J. Ouyang, M. Song, Q. Zou, L. Xi, X. Yang, J. Hong, and L. You, “A spin–orbit torque device for sensing three-dimensional magnetic fields,”Nat. Electron., vol. 4, pp. 179–184, Feb. 2021

  27. [27]

    Room-temperature sub-100 nm Néel-type skyrmions in non- stoichiometric van der Waals ferromagnet Fe 3−xGaTe2 with ultrafast laser writability,

    Z. Li, H. Zhang, G. Li, J. Guo, Q. Wang, Y . Deng, Y . Hu, X. Hu, C. Liu, M. Qin, X. Shen, R. Yu, X. Gao, Z. Liao, J. Liu, Z. Hou, Y . Zhu, and X. Fu, “Room-temperature sub-100 nm Néel-type skyrmions in non- stoichiometric van der Waals ferromagnet Fe 3−xGaTe2 with ultrafast laser writability,” Nat. Commun. , vol. 15, p. 1017, Feb. 2024

  28. [28]

    2D materials for spintronic devices,

    E. C. Ahn, “2D materials for spintronic devices,” NPJ 2D Mater . Appl., vol. 4, Dec. 2020

  29. [29]

    Hard ferromagnetism in van der Waals Fe3GaTe2 nanoflake down to monolayer,

    M. Wang, B. Lei, K. Zhu, Y . Deng, M. Tian, Z. Xiang, T. Wu, and X. Chen, “Hard ferromagnetism in van der Waals Fe3GaTe2 nanoflake down to monolayer,”NPJ 2D Mater . Appl., vol. 8, p. 22, Mar. 2024

  30. [30]

    Magnetic critical behavior of van der Waals Fe3GaTe2 with above-room-temperature ferromagnetism,

    H. Algaidi, C. Zhang, Y . Ma, C. Liu, A. Chen, D. Zheng, and X. Zhang, “Magnetic critical behavior of van der Waals Fe3GaTe2 with above-room-temperature ferromagnetism,”APL Mater ., vol. 12, p. 011124, Jan. 2024

  31. [31]

    Spectral evidence for local-moment ferromagnetism in the van der Waals metals Fe3GaTe2 and Fe3GeTe2,

    H. Wu, C. Hu, Y . Xie, B. G. Jang, J. Huang, Y . Guo, S. Wu, C. Hu, Z. Yue, Y . Shi, and others, “Spectral evidence for local-moment ferromagnetism in the van der Waals metals Fe3GaTe2 and Fe3GeTe2,” Phys. Rev. B, vol. 109, no. 10, p. 104410, 2024

  32. [32]

    Distinct skyrmion phases at room temperature in two-dimensional ferromagnet Fe 3GaTe2,

    X. Lv, H. Lv, Y . Huang, R. Zhang, G. Qin, Y . Dong, M. Liu, K. Pei, G. Cao, J. Zhang, Y . Lai, and R. Che, “Distinct skyrmion phases at room temperature in two-dimensional ferromagnet Fe 3GaTe2,” Nat. Commun., vol. 15, p. 3278, Apr. 2024

  33. [33]

    Polarity-Reversal of Exchange Bias in van der Waals FePS3/Fe3GaTe2 Heterostructures,

    H. Xiao, B. Lyu, M. Mi, J. Yuan, X. Zhang, L. Yu, Q. Cui, C. Wang, J. Song, M. Huang, Y . Tian, L. Liu, T. Taniguchi, K. Watanabe, M. Liu, Y . Guo, S. Wang, and Y . Wang, “Polarity-Reversal of Exchange Bias in van der Waals FePS3/Fe3GaTe2 Heterostructures,” Adv. Sci., vol. 11, no. 48, p. 2409210, 2024

  34. [34]

    Room-Temperature and Tunable Tunneling Magnetoresistance in fe 3gate2 Based 2D van der Waals Heterojunctions,

    W. Jin, G. Zhang, H. Wu, L. Yang, W. Zhang, and H. Chang, “Room-Temperature and Tunable Tunneling Magnetoresistance in fe 3gate2 Based 2D van der Waals Heterojunctions,” ACS Appl. Mater . Interfaces, vol. 15, pp. 36519–36526, Aug. 2023. 18

  35. [35]

    Room-temperature tunable tunneling magnetoresistance in Fe 3GaTe2/WSe2/Fe3GaTe2 van der Waals heterostructures,

    H. Pan, A. K. Singh, C. Zhang, X. Hu, J. Shi, L. An, N. Wang, R. Duan, Z. Liu, S. S. Parkin, et al. , “Room-temperature tunable tunneling magnetoresistance in Fe 3GaTe2/WSe2/Fe3GaTe2 van der Waals heterostructures,” InfoMat, vol. 6, no. 6, p. e12504, 2024

  36. [36]

    Lateral spin filter realized by monolayer Fe 3GaTe2 and Fe3GaTe2/Graphene van der Waals heterostructures,

    N. Zheng and J. Chen, “Lateral spin filter realized by monolayer Fe 3GaTe2 and Fe3GaTe2/Graphene van der Waals heterostructures,”Solid State Commun., vol. 389, p. 115584, Oct. 2024

  37. [37]

    Energy-efficient field-free uncon- ventional spin-orbit torque magnetization switching dynamics in van der Waals heterostructures,

    L. Pandey, B. Zhao, K. Tenzin, R. Ngaloy, V . Lamparská, H. Bangar, A. Ali, M. Abdel-Hafiez, G. Zhang, H. Wu, H. Chang, L. Sjöström, P. Rout, J. Sławi´nska, and S. P. Dash, “Energy-efficient field-free uncon- ventional spin-orbit torque magnetization switching dynamics in van der Waals heterostructures,” 2024. Version Number: 2

  38. [38]

    A Room-Temperature Spin-Valve with van der Waals Ferromagnet Fe5GeTe2/Graphene Heterostructure,

    B. Zhao, R. Ngaloy, S. Ghosh, S. Ershadrad, R. Gupta, K. Ali, A. M. Hoque, B. Karpiak, D. Khokhriakov, C. Polley,et al., “A Room-Temperature Spin-Valve with van der Waals Ferromagnet Fe5GeTe2/Graphene Heterostructure,” Adv. Mater ., vol. 35, no. 16, p. 2209113, 2023

  39. [39]

    Contribution of the buffer layer to the Raman spectrum of epitaxial graphene on SiC(0001),

    F. Fromm, M. H. Oliveira Jr, A. Molina-Sánchez, M. Hundhausen, J. M. J. Lopes, H. Riechert, L. Wirtz, and T. Seyller, “Contribution of the buffer layer to the Raman spectrum of epitaxial graphene on SiC(0001),” New J. of Phys., vol. 15, p. 043031, Apr. 2013

  40. [40]

    Influence of Proximity to Supporting Substrate on van der Waals Epitaxy of Atomically Thin Graphene/Hexagonal Boron Nitride Heterostructures,

    M. Heilmann, A. S. Prikhodko, M. Hanke, A. Sabelfeld, N. I. Borgardt, and J. M. J. Lopes, “Influence of Proximity to Supporting Substrate on van der Waals Epitaxy of Atomically Thin Graphene/Hexagonal Boron Nitride Heterostructures,” ACS Appl. Mater . Interfaces, vol. 12, pp. 8897–8907, Feb. 2020

  41. [41]

    Lattice Dynam- ics and Phonon Dispersion of the van der Waals Layered Ferromagnet Fe 3GaTe2,

    X. Chen, X. Zhang, W. He, Y . Li, J. Lu, D. Yang, D. Li, L. Lei, Y . Peng, and G. Xiang, “Lattice Dynam- ics and Phonon Dispersion of the van der Waals Layered Ferromagnet Fe 3GaTe2,” Nano Lett., vol. 25, pp. 4353–4360, Mar. 2025

  42. [42]

    Robust ferromagnetism in wafer-scale Fe3GaTe2 above room-temperature,

    S. Wu, Z. He, M. Gu, L. Ren, J. Li, B. Deng, D. Wang, X. Guo, W. Li, M. Chen, Y . Chen, M. Meng, Q. Ye, B. Shen, X. Chen, J. Guo, G. Xing, I. K. Sou, and S. Li, “Robust ferromagnetism in wafer-scale Fe3GaTe2 above room-temperature,”Nat. Commun., vol. 15, p. 10765, Dec. 2024

  43. [43]

    Large-area van der Waals epitaxy and mag- netic characterization of Fe3GeTe2 films on graphene,

    J. M. J. Lopes, D. Czubak, E. Zallo, A. I. Figueroa, C. Guillemard, M. Valvidares, J. Rubio-Zuazo, J. López-Sanchéz, S. O. Valenzuela, M. Hanke, and others, “Large-area van der Waals epitaxy and mag- netic characterization of Fe3GeTe2 films on graphene,”2D Mater ., vol. 8, no. 4, p. 041001, 2021

  44. [44]

    The Scherrer equation versus the ‘Debye-Scherrer equation’,

    U. Holzwarth and N. Gibson, “The Scherrer equation versus the ‘Debye-Scherrer equation’,”Nat. Nano., vol. 6, pp. 534–534, Sept. 2011

  45. [45]

    Wafer-scale two-dimensional ferromagnetic Fe 3GeTe2 thin films grown by molecular beam epitaxy,

    S. Liu, X. Yuan, Y . Zou, Y . Sheng, C. Huang, E. Zhang, J. Ling, Y . Liu, W. Wang, C. Zhang, and others, “Wafer-scale two-dimensional ferromagnetic Fe 3GeTe2 thin films grown by molecular beam epitaxy,” NPJ 2D Mater . Appl., vol. 1, no. 1, p. 30, 2017

  46. [46]

    Antiferromagnetic coupling of van der Waals ferromagnetic Fe3GeTe2,

    D. Kim, S. Park, J. Lee, J. Yoon, S. Joo, T. Kim, K.-j. Min, S.-Y . Park, C. Kim, K.-W. Moon, et al. , “Antiferromagnetic coupling of van der Waals ferromagnetic Fe3GeTe2,” Nanotechnol., vol. 30, no. 24, p. 245701, 2019

  47. [47]

    Large-scale epitaxy of two-dimensional van der Waals room-temperature ferromagnet Fe5GeTe2,

    M. Ribeiro, G. Gentile, A. Marty, D. Dosenovic, H. Okuno, C. Vergnaud, J.-F. Jacquot, D. Jalabert, D. Longo, P. Ohresser, A. Hallal, M. Chshiev, O. Boulle, F. Bonell, and M. Jamet, “Large-scale epitaxy of two-dimensional van der Waals room-temperature ferromagnet Fe5GeTe2,” NPJ 2D Mater . Appl., vol. 6, p. 10, Dec. 2022. 19

  48. [48]

    Discovery of intrinsic ferromagnetism in two-dimensional van der Waals crystals,

    C. Gong, L. Li, Z. Li, H. Ji, A. Stern, Y . Xia, T. Cao, W. Bao, C. Wang, Y . Wang, and others, “Discovery of intrinsic ferromagnetism in two-dimensional van der Waals crystals,” Nature, vol. 546, no. 7657, pp. 265–269, 2017

  49. [49]

    Magnetic structure and phase stability of the van der Waals bonded ferromagnet Fe3−xGeTe2,

    A. F. May, S. Calder, C. Cantoni, H. Cao, and M. A. McGuire, “Magnetic structure and phase stability of the van der Waals bonded ferromagnet Fe3−xGeTe2,” Physical Review B, vol. 93, no. 1, p. 014411, 2016

  50. [50]

    Room-temperature intrinsic ferromagnetism in epitaxial CrTe2 ultrathin films,

    X. Zhang, Q. Lu, W. Liu, W. Niu, J. Sun, J. Cook, M. Vaninger, P. F. Miceli, D. J. Singh, S.-W. Lian,et al., “Room-temperature intrinsic ferromagnetism in epitaxial CrTe2 ultrathin films,”Nature communications, vol. 12, no. 1, p. 2492, 2021

  51. [51]

    C. M. Hurd, Hall effect in metals and alloys . Plenum Press, 1972. Publication Title: Hall effect in metals and alloys

  52. [52]

    Intrinsic anomalous Hall effect in thin films of topological kagome ferromagnet Fe 3Sn2,

    K. I. A. Khan, R. S. Yadav, H. Bangar, A. Kumar, N. Chowdhury, P. K. Muduli, and P. K. Muduli, “Intrinsic anomalous Hall effect in thin films of topological kagome ferromagnet Fe 3Sn2,” Nanoscale, vol. 14, no. 23, pp. 8484–8492, 2022

  53. [53]

    Above Room Temperature Ferromagnetism in All-Epitaxial Fe5−xGeTe2/Graphene and Fe5−xGeTe2/WSe2 Van Der Waals Heterostructures,

    J. M. J. Lopes, H. Lv, J. Herfort, M. Hanke, C. Chen, J. M. Redwing, A. Trampert, R. Engel-Herbert, and M. Ramsteiner, “Above Room Temperature Ferromagnetism in All-Epitaxial Fe5−xGeTe2/Graphene and Fe5−xGeTe2/WSe2 Van Der Waals Heterostructures,” in2024 IEEE International Magnetic Conference- Short papers (INTERMAG Short papers) , pp. 1–2, IEEE, 2024

  54. [54]

    Robust ferromagnetism in wafer-scale monolayer and multilayer Fe3GeTe2,

    R. Roemer, C. Liu, and K. Zou, “Robust ferromagnetism in wafer-scale monolayer and multilayer Fe3GeTe2,” NPJ 2D Mater . Appl., vol. 4, p. 33, Dec. 2020

  55. [55]

    Centimeter- Scale Above-Room-Temperature Ferromagnetic Fe 3GaTe2 Thin Films by Molecular Beam Epitaxy,

    T. Wang, Y . Xu, Y . Liu, X. Dai, P. Yan, J. Wang, S. Wang, Y . Deng, K. He, C. Li, and others, “Centimeter- Scale Above-Room-Temperature Ferromagnetic Fe 3GaTe2 Thin Films by Molecular Beam Epitaxy,” Chin. Phys. Lett., vol. 41, no. 10, p. 107502, 2024

  56. [56]

    Controlling the Magnetic Anisotropy of the van der Waals Ferromagnet Fe 3GeTe2 through Hole Doping,

    S. Y . Park, D. S. Kim, Y . Liu, J. Hwang, Y . Kim, W. Kim, J.-Y . Kim, C. Petrovic, C. Hwang, S.-K. Mo, H.-j. Kim, B.-C. Min, H. C. Koo, J. Chang, C. Jang, J. W. Choi, and H. Ryu, “Controlling the Magnetic Anisotropy of the van der Waals Ferromagnet Fe 3GeTe2 through Hole Doping,” Nano Lett. , vol. 20, pp. 95–100, Jan. 2020

  57. [57]

    Anisotropic quantum Hall effect in epitaxial graphene on stepped SiC surfaces,

    T. Schumann, K.-J. Friedland, M. H. Oliveira, A. Tahraoui, J. M. J. Lopes, and H. Riechert, “Anisotropic quantum Hall effect in epitaxial graphene on stepped SiC surfaces,” Phys. Rev. B , vol. 85, p. 235402, June 2012

  58. [58]

    Origin of Doping in Quasi-Free-Standing Graphene on Silicon Carbide,

    J. Ristein, S. Mammadov, and T. Seyller, “Origin of Doping in Quasi-Free-Standing Graphene on Silicon Carbide,” Phys. Rev. Lett., vol. 108, p. 246104, June 2012

  59. [59]

    X-ray circular dichroism as a probe of orbital magnetization,

    B. T. Thole, P. Carra, F. Sette, and G. Van Der Laan, “X-ray circular dichroism as a probe of orbital magnetization,” Phys. Rev. Lett., vol. 68, pp. 1943–1946, Mar. 1992

  60. [60]

    X-ray circular dichroism and local magnetic fields,

    P. Carra, B. T. Thole, M. Altarelli, and X. Wang, “X-ray circular dichroism and local magnetic fields,” Phys. Rev. Lett., vol. 70, pp. 694–697, Feb. 1993

  61. [61]

    Experimental Confirmation of the X-Ray Magnetic Circular Dichroism Sum Rules for Iron and Cobalt,

    C. T. Chen, Y . U. Idzerda, H.-J. Lin, N. V . Smith, G. Meigs, E. Chaban, G. H. Ho, E. Pellegrin, and F. Sette, “Experimental Confirmation of the X-Ray Magnetic Circular Dichroism Sum Rules for Iron and Cobalt,” Phys. Rev. Lett., vol. 75, pp. 152–155, July 1995. 20

  62. [62]

    Magnetic Skyrmions above Room Temper- ature in a van der Waals Ferromagnet Fe3GaTe2,

    C. Liu, S. Zhang, H. Hao, H. Algaidi, Y . Ma, and X. Zhang, “Magnetic Skyrmions above Room Temper- ature in a van der Waals Ferromagnet Fe3GaTe2,” Adv. Sci., p. 2311022, Feb. 2024

  63. [63]

    X-ray magnetic linear dichroism as a probe for non-collinear magnetic state in ferrimagnetic single layer exchange bias systems,

    C. Luo, H. Ryll, C. H. Back, and F. Radu, “X-ray magnetic linear dichroism as a probe for non-collinear magnetic state in ferrimagnetic single layer exchange bias systems,” Sci. Rep. , vol. 9, p. 18169, Dec. 2019

  64. [64]

    Self-Intercalation as Origin of High- Temperature Ferromagnetism in Epitaxially Grown Fe 5GeTe2 Thin Films,

    M. Silinskas, S. Senz, P. Gargiani, A. M. Ruiz, B. Kalkofen, I. Kostanovski, K. Mohseni, J. J. Bal- doví, H. L. Meyerheim, S. S. P. Parkin, and A. Bedoya-Pinto, “Self-Intercalation as Origin of High- Temperature Ferromagnetism in Epitaxially Grown Fe 5GeTe2 Thin Films,” Phys. Rev. Lett. , vol. 133, p. 256702, Dec. 2024

  65. [65]

    Valence-state mixing and reduced magnetic moment in Fe 3−δGeTe2 single crystals with varying Fe content probed by X-ray spectroscopy,

    D. Backes, R. Fujita, L. Veiga, D. Mayoh, G. Wood, S. Dhesi, G. Balakrishnan, G. van der Laan, and T. Hesjedal, “Valence-state mixing and reduced magnetic moment in Fe 3−δGeTe2 single crystals with varying Fe content probed by X-ray spectroscopy,”Nanotechnol., vol. 35, no. 39, p. 395709, 2024. 21