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arxiv: 2503.20545 · v2 · submitted 2025-03-26 · ❄️ cond-mat.mes-hall · cond-mat.mtrl-sci· physics.app-ph

Symmetry Enhanced Unconventional Spin Current Anisotropy in a Collinear Antiferromagnet

Pith reviewed 2026-05-22 22:35 UTC · model grok-4.3

classification ❄️ cond-mat.mes-hall cond-mat.mtrl-sciphysics.app-ph
keywords spin-orbit torqueantiferromagnetFeSnspin Hall effectNéel vectorkagome latticeheterostructuresymmetry anisotropy
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0 comments X

The pith

Epitaxial FeSn produces six-fold symmetric damping-like spin-orbit torques and unconventional field-like torques from out-of-plane spins.

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

The paper examines spin-orbit torques in heterostructures of epitaxial FeSn, a collinear antiferromagnet on a kagome lattice, and permalloy. Measurements show that the damping-like torque exhibits six-fold symmetry matching the crystal orientation of the FeSn layer. An additional unconventional field-like torque arises from spin currents polarized out of the plane, with its strength depending on both the crystal symmetry and the direction of the antiferromagnetic Néel vector. These findings indicate that the symmetry of the antiferromagnet can control the anisotropy of the generated spin currents. This approach could provide new ways to manipulate magnetic states in spintronic devices using antiferromagnetic materials.

Core claim

Using spin-torque ferromagnetic resonance on epitaxial FeSn/Py heterostructures, a damping-like spin-orbit torque is observed that displays six-fold symmetry corresponding to the [0001] orientation of the FeSn films. In addition, a substantial unconventional field-like torque is detected that originates from spin currents carrying out-of-plane spin polarization; this torque's angular dependence is a superposition of six-fold crystalline symmetry and uniaxial symmetry tied to the antiferromagnetic spin Hall effect, and it strengthens when the radiofrequency current aligns with the Néel vector in FeSn.

What carries the argument

The antiferromagnetic spin Hall effect in collinear kagome FeSn, which generates spin currents whose polarization and magnitude depend on the crystal and magnetic symmetries.

If this is right

  • Spin-orbit torques can be made anisotropic through the inherent symmetries of collinear antiferromagnets.
  • The unconventional field-like torque provides access to out-of-plane spin polarizations in antiferromagnetic systems.
  • Aligning current with the Néel vector enhances the unconventional torque component.
  • Six-fold symmetry allows for torque responses in multiple equivalent directions in the plane.

Where Pith is reading between the lines

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

  • If the symmetry-enhanced torques hold, heterostructures could be designed to switch magnetization directions selectively by choosing current angles relative to the Néel vector.
  • Similar symmetry effects may enable low-power control in antiferromagnetic spintronic devices without needing heavy metals.
  • Testing in other kagome-lattice antiferromagnets could reveal if the topological features contribute to the observed torques.

Load-bearing premise

The torques measured in the heterostructures are produced by spin currents from within the FeSn antiferromagnet layer and their angular patterns can be separated into crystalline and uniaxial parts without extra parameters.

What would settle it

Performing the same spin-torque ferromagnetic resonance experiment on a sample where the FeSn layer is replaced by a non-antiferromagnetic material or rotated to break the six-fold symmetry would eliminate the reported symmetric components if they truly originate from FeSn.

Figures

Figures reproduced from arXiv: 2503.20545 by Akash Kumar, Johan {\AA}kerman, Kacho Imtiyaz Ali Khan, Nidhi Kandwal, Pankhuri Gupta, Pranaba Kishor Muduli, Ram Singh Yadav, Rekha Agarwal.

Figure 1
Figure 1. Figure 1: Schematic of FeSn and XRD measurements (a) Schematic of the unit cell (blue) of the kagome antiferromagnet FeSn. (b) Schematic of the kagome layer of Fe3Sn and stanene layer of Sn2. Fe atoms are depicted in red, and Sn atoms are shown in Gray. (c) Structural characterization using θ − 2θ XRD scan measured for Pt(5 nm)/FeSn(30 nm). (d) ϕ-scan measurements for Pt(5 nm)/FeSn(30 nm) film on an Al2O3 substrate.… view at source ↗
Figure 2
Figure 2. Figure 2: STFMR measurements (a) Structure of STFMR device consisting of a FeSn/Py bilayer. This device is subject to electric current flowing along the x−direction, resulting in the generation of both in-plane (τ∥) and out-of-plane (τ⊥) torque. (b) The schematic depicts the setup for STFMR measurements. c) Frequency-dependent STFMR spectra of FeSn/Py microstrip measured at φ = 40◦ when the current direction is at 0… view at source ↗
Figure 3
Figure 3. Figure 3: Crystallographic dependence of STFMR (a-e) SEM image of differently oriented devices (left panel), VS (middle panel) and VA (right panel) components as a function of angle φ. θR represent the angle between IRF and in-plane reference direction [1¯100]. We then analyze the results in more detail by performing complete angular dependence of the STFMR. In sys￾tems with conventional SHE and REE, the angular dep… view at source ↗
Figure 4
Figure 4. Figure 4: Crystallographic dependence of spin-torque efficiencies (a) Kagome Structure with Néel vector (gray) and IRF (black dashed) in parallel and perpendicular orientations (b) DL SOT efficiency due to y− spin polarization and (c) FL SOT efficiency due to z− spin polarization for different θR values in FeSn/Py device and Ref. device. efficiencies due to the y− spin polarization, denoted as ξ y DL, are shown in F… view at source ↗
read the original abstract

Spin-orbit torque (SOT) presents a promising avenue for energy-efficient spintronics devices, surpassing the limitations of spin transfer torque. While extensively studied in heavy metals, SOT in antiferromagnetic quantum materials remains largely unexplored. Here, we investigate SOT in epitaxial FeSn, a collinear antiferromagnet with a kagome lattice. FeSn exhibits intriguing topological quantum features, including two-dimensional flat bands and Dirac-like surface states, making it an ideal platform for investigating emergent SOT properties. Using spin-torque ferromagnetic resonance, we uncover a six-fold symmetric damping-like SOT in epitaxial-FeSn/Py heterostructures, reflecting the six-fold symmetry of the epitaxial [0001]-oriented FeSn films. Additionally, we observe a substantial unconventional field-like torque, originating from spin currents with out-of-plane spin polarization. This torque exhibits a unique angular dependence-a superposition of six-fold crystalline symmetry and uniaxial symmetry associated with the antiferromagnetic spin Hall effect. Notably, the unconventional field-like torque is enhanced when the RF current flows along the Neel vector in FeSn. Our findings reveal an unconventional spin current anisotropy tunable by crystalline and magnetic symmetry, offering a novel approach for controlling SOT in antiferromagnetic spintronics.

Editorial analysis

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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 / 1 minor

Summary. The manuscript reports spin-torque ferromagnetic resonance measurements on epitaxial [0001]-oriented FeSn/Py heterostructures. It claims observation of a six-fold symmetric damping-like spin-orbit torque (SOT) that tracks the crystalline symmetry of the FeSn layer, together with a substantial unconventional field-like torque arising from spin currents with out-of-plane polarization; the latter exhibits an angular dependence that is a superposition of six-fold crystalline symmetry and uniaxial symmetry linked to the antiferromagnetic spin Hall effect, and is enhanced when the RF current is aligned with the Néel vector.

Significance. If the attribution of both torque components to bulk spin currents generated inside the FeSn layer is substantiated, the work would demonstrate how the combination of kagome-lattice crystalline symmetry and collinear antiferromagnetic order can produce tunable, symmetry-enhanced unconventional spin-current anisotropies, offering a materials platform distinct from conventional heavy-metal systems for antiferromagnetic spintronics.

major comments (2)
  1. [Abstract and inferred Results section] The central interpretation—that the six-fold damping-like SOT and the unconventional field-like torque (with out-of-plane polarization) originate from spin currents inside the epitaxial FeSn layer rather than from the FeSn/Py interface, the Py layer itself, or resonance-fitting artifacts—lacks supporting controls. No thickness series, interface-modified control samples, or quantitative comparison of torque magnitudes versus FeSn thickness is described, leaving the bulk-origin claim load-bearing yet unsecured.
  2. [Abstract and inferred angular-dependence analysis] The decomposition of the field-like torque angular dependence into a clean superposition of six-fold crystalline and uniaxial (Néel-vector) components is presented without reported fitting residuals, parameter counts, or independent verification that the uniaxial term is absent in control samples lacking antiferromagnetic order; this decomposition is essential to the claim of symmetry-enhanced anisotropy.
minor comments (1)
  1. The abstract does not state the measurement temperature, RF power range, or sample growth details (e.g., substrate, buffer layer), which would aid reproducibility assessment.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their thorough review and valuable feedback on our manuscript. We address each major comment below, providing clarifications and indicating revisions where appropriate.

read point-by-point responses
  1. Referee: The central interpretation—that the six-fold damping-like SOT and the unconventional field-like torque (with out-of-plane polarization) originate from spin currents inside the epitaxial FeSn layer rather than from the FeSn/Py interface, the Py layer itself, or resonance-fitting artifacts—lacks supporting controls. No thickness series, interface-modified control samples, or quantitative comparison of torque magnitudes versus FeSn thickness is described, leaving the bulk-origin claim load-bearing yet unsecured.

    Authors: We agree that a thickness series or interface controls would provide stronger evidence for the bulk origin. However, the observed six-fold symmetry in the damping-like torque matches the crystalline symmetry of the epitaxial FeSn layer, which is not present in the Py layer or a typical interface. Similarly, the unconventional field-like torque's angular dependence reflects both crystalline and antiferromagnetic symmetries unique to FeSn. We will revise the manuscript to include a more detailed discussion of these symmetry-based arguments supporting the bulk contribution and acknowledge the absence of thickness-dependent data as a limitation. revision: partial

  2. Referee: The decomposition of the field-like torque angular dependence into a clean superposition of six-fold crystalline and uniaxial (Néel-vector) components is presented without reported fitting residuals, parameter counts, or independent verification that the uniaxial term is absent in control samples lacking antiferromagnetic order; this decomposition is essential to the claim of symmetry-enhanced anisotropy.

    Authors: The angular dependence was modeled as a superposition of six-fold and uniaxial terms based on the symmetries involved. We will include the explicit fitting function, number of parameters, and residuals in the revised supplementary material to allow assessment of the decomposition quality. Independent control samples without antiferromagnetic order were not included in this study; the uniaxial component is attributed to the Néel vector based on the known magnetic structure of FeSn. revision: partial

Circularity Check

0 steps flagged

No circularity: experimental measurements with data-driven torque extraction

full rationale

The paper is an experimental study using spin-torque ferromagnetic resonance on epitaxial FeSn/Py heterostructures. Reported results (six-fold damping-like SOT and unconventional field-like torque with crystalline + uniaxial angular dependence) are extracted directly from resonance data and angular scans. No derivation chain, first-principles equations, or predictions are claimed that reduce to inputs by construction. No self-citations are load-bearing for any mathematical result, and no ansatz or fitted parameter is renamed as a prediction. The work is self-contained against external benchmarks as an empirical report; the central claims rest on raw data reproducibility rather than internal definitional loops.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on standard assumptions of the spin-torque FMR analysis technique and the attribution of measured torques to bulk spin currents in FeSn; no free parameters or new entities are introduced in the abstract.

axioms (1)
  • domain assumption The spin-torque ferromagnetic resonance lineshape model accurately separates damping-like and field-like torques without significant cross-talk from other effects.
    This is the standard analysis framework used to extract the reported torques from resonance data.

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Works this paper leans on

60 extracted references · 60 canonical work pages

  1. [1]

    Costache, Stéphane Auffret, Sébastien Bandiera, Bernard Rodmacq, Alain Schuhl, and Pietro Gambardella

    Ioan Mihai Miron, Kevin Garello, Gilles Gaudin, Pierre Jean Zermatten, Marius V . Costache, Stéphane Auffret, Sébastien Bandiera, Bernard Rodmacq, Alain Schuhl, and Pietro Gambardella. Perpendicular switching of a single ferromagnetic layer induced by in-plane current injection. Nature, 476:189–193, Aug 2011

  2. [2]

    L. Liu, C. F. Pai, Y . Li, H. W. Tseng, D. C. Ralph, and R. A. Buhrman. Spin-Torque Switching with the Giant Spin Hall Effect of Tantalum. Science, 336:555–558, May 2012

  3. [3]

    Ultrafast magnetization switching by spin- orbit torques

    Kevin Garello, Can Onur Avci, Ioan Mihai Miron, Manuel Baumgartner, Abhijit Ghosh, Stéphane Auf- fret, Olivier Boulle, Gilles Gaudin, and Pietro Gambardella. Ultrafast magnetization switching by spin- orbit torques. Appl. Phys. Lett., 105:212402, 2014

  4. [4]

    Demidov, Sergei Urazhdin, Henning Ulrichs, Vasyl Tiberkevich, Andrei Slavin, Dietmar Baither, Guido Schmitz, and Sergej O

    Vladislav E. Demidov, Sergei Urazhdin, Henning Ulrichs, Vasyl Tiberkevich, Andrei Slavin, Dietmar Baither, Guido Schmitz, and Sergej O. Demokritov. Magnetic nano-oscillator driven by pure spincurrent. Nat. Mater ., 11:1028–1031, Oct 2012

  5. [5]

    A. A. Awad, P. Dürrenfeld, A. Houshang, M. Dvornik, E. Iacocca, R. K. Dumas, and J. Åkerman. Long- range mutual synchronization of spin Hall nano-oscillators. Nat. Phys., 13:292–299, nov 2017. 11

  6. [6]

    Chaurasiya, Nilamani González, Victor H.and Behera, Ademir Aléman, Ro- man Khymyn, Ahmad A

    Akash Kumar, Avinash K. Chaurasiya, Nilamani González, Victor H.and Behera, Ademir Aléman, Ro- man Khymyn, Ahmad A. Awad, and Johan Åkerman. Spin-wave-mediated mutual synchronization and phase tuning in spin Hall nano-oscillators. Nat. Phys., 21(242), January 2025

  7. [7]

    Neuromorphic spintronics

    Julie Grollier, Damien Querlioz, KY Camsari, Karin Everschor-Sitte, Shunsuke Fukami, and Mark D Stiles. Neuromorphic spintronics. Nat. Electron., 3:360–370, 2020

  8. [8]

    Phase- Binarized Spin Hall Nano-Oscillator Arrays: Towards Spin Hall Ising Machines

    Afshin Houshang, Mohammad Zahedinejad, Shreyas Muralidhar, Roman Khymyn, Mona Rajabali, Hi- manshu Fulara, Ahmad A Awad, Johan Åkerman, Jakub Checi ´nski, and Mykola Dvornik. Phase- Binarized Spin Hall Nano-Oscillator Arrays: Towards Spin Hall Ising Machines. Phys. Rev. Appl. , 17:014003, 2022

  9. [9]

    Kuramoto- model-based data classification using the synchronization dynamics of uniform-mode spin Hall nano- oscillators

    Neha Garg, Sri Vasudha Hemadri Bhotla, Pranaba Kishor Muduli, and Debanjan Bhowmik. Kuramoto- model-based data classification using the synchronization dynamics of uniform-mode spin Hall nano- oscillators. Neuromorph. Comput. Eng., 1:024005, 2021

  10. [10]

    Ram S Yadav, Pankhuri Gupta, Amod Holla, Kacho Imtiyaz Ali Khan, Pranaba K Muduli, and De- banjan Bhowmik. Demonstration of Synaptic Behavior in a Heavy-Metal-Ferromagnetic-Metal-Oxide- Heterostructure-Based Spintronic Device for On-Chip Learning in Crossbar-Array-Based Neural Net- works. ACS Appl. Electron. Mater ., 5:484–497, 2023

  11. [11]

    M. I. Dyakonov and V . I. Perel. Current-induced spin orientation of electrons in semiconductors. Phys. Lett. A, 35:459–460, Jul 1971

  12. [12]

    J. E. Hirsch. Spin Hall Effect. Phys. Rev. Lett., 83:1834–1837, Aug 1999

  13. [13]

    Properties of a 2D electron gas with lifted spectral degeneracy

    Yu A Bychkov and É I Rashba. Properties of a 2D electron gas with lifted spectral degeneracy. JETP lett, 39:78, 1984

  14. [14]

    Spin polarization of conduction electrons induced by electric current in two- dimensional asymmetric electron systems

    Victor M Edelstein. Spin polarization of conduction electrons induced by electric current in two- dimensional asymmetric electron systems. Solid State Commun., 73:233–235, 1990

  15. [15]

    Anisotropic spin Hall effect from first principles

    Frank Freimuth, Stefan Blügel, and Yuriy Mokrousov. Anisotropic spin Hall effect from first principles. Phys. Rev. Lett., 105:246602, 2010

  16. [16]

    Intrinsic spin Hall effect in noncubic crystals

    EM Chudnovsky. Intrinsic spin Hall effect in noncubic crystals. Phys. Rev. B, 80:153105, 2009

  17. [17]

    G. Yu, P. Upadhyaya, Y . Fan, J. G. Alzate, W. Jiang, K. L. Wong, S. Takei, S. A. Bender, L. T. Chang, Y . Jiang, M. Lang, J. Tang, Y . Wang, Y . Tserkovnyak, P. K. Amiri, and K. L. Wang. Switching of perpendicular magnetization by spin–orbit torques in the absence of external magnetic fields.Nat. Nano., 9:548–554, 2014

  18. [18]

    Current-induced switching of perpendicularly magnetized magnetic layers using spin torque from the spin Hall effect

    Luqiao Liu, OJ Lee, TJ Gudmundsen, DC Ralph, and RA Buhrman. Current-induced switching of perpendicularly magnetized magnetic layers using spin torque from the spin Hall effect. Phys. Rev. Lett., 109:096602, 2012

  19. [19]

    A spin–orbit torque switching scheme with collinear magnetic easy axis and current configuration

    Shunsuke Fukami, T Anekawa, C Zhang, and H Ohno. A spin–orbit torque switching scheme with collinear magnetic easy axis and current configuration. Nat. Nano., 11:621–625, 2016

  20. [20]

    Two-dimensional van der Waals materials for spin-orbit torque applications

    Mingming Tian, Yonghui Zhu, Milad Jalali, Wei Jiang, Jian Liang, Zhaocong Huang, Qian Chen, Zhong- ming Zeng, and Ya Zhai. Two-dimensional van der Waals materials for spin-orbit torque applications. Front. nanotechnol., 3:732916, 2021. 12

  21. [21]

    Spin-orbit torques: Materials, mechanisms, performances, and potential applications

    Cheng Song, Ruiqi Zhang, Liyang Liao, Yongjian Zhou, Xiaofeng Zhou, Ruyi Chen, Yunfeng You, Xianzhe Chen, and Feng Pan. Spin-orbit torques: Materials, mechanisms, performances, and potential applications. Prog. Mater . Sci., 118:100761, 2021

  22. [22]

    Thickness dependence of spin-orbit torques generated by WTe 2

    David MacNeill, Gregory M Stiehl, Marcos HD Guimaraes, Neal D Reynolds, Robert A Buhrman, and Daniel C Ralph. Thickness dependence of spin-orbit torques generated by WTe 2. Phys. Rev. B , 96:054450, 2017

  23. [23]

    MacNeill, G

    D. MacNeill, G. M. Stiehl, M. H. D. Guimaraes, R. A. Buhrman, J. Park, and D. C. Ralph. Control of spin-orbit torques through crystal symmetry in WTe2/ferromagnet bilayers. Nat. Phys., 13:300–305, Mar 2017

  24. [24]

    Gregory M Stiehl, Ruofan Li, Vishakha Gupta, Ismail El Baggari, Shengwei Jiang, Hongchao Xie, Lena F Kourkoutis, Kin Fai Mak, Jie Shan, Robert A Buhrman, and Daniel C. Ralph. Layer-dependent spin- orbit torques generated by the centrosymmetric transition metal dichalcogenide β-MoTe2. Phys. Rev. B, 100:184402, 2019

  25. [25]

    Quintela, Julian Irwin, Gautam Gurung, Ding-Fu Shao, Jonathan Gibbons, Neil Campbell, Kyung Mee Song, Si-Young Choi, Lu Guo, R

    Tianxiang Nan, Camilo X. Quintela, Julian Irwin, Gautam Gurung, Ding-Fu Shao, Jonathan Gibbons, Neil Campbell, Kyung Mee Song, Si-Young Choi, Lu Guo, R. D. Johnson, Pascal Manuel, Rajesh Vi- las Chopdekar, Ingrid Hallsteinsen, Thomas Tybell, Philip J. Ryan, Jong-Woo Kim, Y . Choi, Paolo G. Radaelli, Daniel C. Ralph, E. Y . Tsymba, Mark S Rzchowski, and C....

  26. [26]

    Cluster magnetic octupole induced out-of-plane spin polarization in antiperovskite antiferromagnet

    Yunfeng You, Hua Bai, Xiaoyu Feng, Xiaolong Fan, Lei Han, Xiaofeng Zhou, Yongjian Zhou, Ruiqi Zhang, Tongjin Chen, Feng Pan, and Cheng Song. Cluster magnetic octupole induced out-of-plane spin polarization in antiperovskite antiferromagnet. Nat. Commun., 12:6524, 2021

  27. [27]

    Giant field-like torque by the out-of-plane magnetic spin Hall effect in a topological antiferromagnet

    Kouta Kondou, Hua Chen, Takahiro Tomita, Muhammad Ikhlas, Tomoya Higo, Allan H MacDonald, Satoru Nakatsuji, and YoshiChika Otani. Giant field-like torque by the out-of-plane magnetic spin Hall effect in a topological antiferromagnet. Nat. Commun., 12:6491, 2021

  28. [28]

    Observation of the anti- ferromagnetic spin Hall effect

    Xianzhe Chen, Shuyuan Shi, Guoyi Shi, Xiaolong Fan, Cheng Song, Xiaofeng Zhou, Hua Bai, Liyang Liao, Yongjian Zhou, Hanwen Zhang, Ang Li, Yanhui Chen, Xiaodong Han, Shan Jiang, Zengwei Zhu, Huaqiang Wu, Xiangrong Wang, Desheng Xue, Hyunsoo Yang, and Feng Pan. Observation of the anti- ferromagnetic spin Hall effect. Nat. Mater ., 20:800–804, 2021

  29. [29]

    Efficient Electrical Spin Splitter Based on Nonrelativistic Collinear Antiferro- magnetism

    Rafael González-Hernández, Libor Šmejkal, Karel Výborný, Yuta Yahagi, Jairo Sinova, Tomá š Jung- wirth, and Jakub Železný. Efficient Electrical Spin Splitter Based on Nonrelativistic Collinear Antiferro- magnetism. Phys. Rev. Lett., 126, Mar 2021

  30. [30]

    Kagome magnets: The emerging materials for spintronic memories

    Niru Chowdhury, Kacho Imtiyaz Ali Khan, Himanshu Bangar, Pankhuri Gupta, Ram Singh Yadav, Rekha Agarwal, Akash Kumar, and Pranaba Kishor Muduli. Kagome magnets: The emerging materials for spintronic memories. Proc. Natl. Acad. Sci., India, Sect. A Phys. Sci. , 93:477–495, 2023

  31. [31]

    Dirac fermions in antiferromagnetic FeSn kagome lattices with combined space inversion and time-reversal symmetry

    Zhiyong Lin, Chong Wang, Pengdong Wang, Seho Yi, Lin Li, Qiang Zhang, Yifan Wang, Zhongyi Wang, Haoran Huang, Yan Sun, Yaobo Huang, Dawei Shen, Donglai Feng, Zhe Sun, Jun-Hyung Cho, Changgan Zeng, and Zhenyu Zhang. Dirac fermions in antiferromagnetic FeSn kagome lattices with combined space inversion and time-reversal symmetry. Phys. Rev. B, 102:155103, 2019. 13

  32. [32]

    Flatbands and Emergent Ferromagnetic Ordering in Fe3Sn2 Kagome Lattices

    Zhiyong Lin, Jin Ho Choi, Qiang Zhang, Wei Qin, Seho Yi, Pengdong Wang, Lin Li, Yifan Wang, Hui Zhang, Zhe Sun, Laiming Wei, Shengbai Zhang, Tengfei Guo, Qingyou Lu, Jun Hyung Cho, Changgan Zeng, and Zhenyu Zhang. Flatbands and Emergent Ferromagnetic Ordering in Fe3Sn2 Kagome Lattices. Phys. Rev. Lett., 121:096401, Aug 2018

  33. [33]

    Large spin Hall conductivity in epitaxial thin films of kagome antiferromag- net Mn3Sn at room temperature

    Himanshu Bangar, Kacho Imtiyaz Ali Khan, Akash Kumar, Niru Chowdhury, Prasanta Kumar Muduli, and Pranaba Kishor Muduli. Large spin Hall conductivity in epitaxial thin films of kagome antiferromag- net Mn3Sn at room temperature. Adv. Quantum Technol., 6:2200115, 2023

  34. [34]

    Studies of the magnetic structure of FeSn using the Mössbauer effect

    L Häggström, T Ericsson, R Wäppling, and K Chandra. Studies of the magnetic structure of FeSn using the Mössbauer effect. Phys. Scr ., 11:47, 1975

  35. [35]

    Electronic, magnetic, and thermodynamic properties of the kagome layer compound FeSn

    Brian C Sales, Jiaqiang Yan, William R Meier, Andrew D Christianson, Satoshi Okamoto, and Michael A McGuire. Electronic, magnetic, and thermodynamic properties of the kagome layer compound FeSn. Phys. Rev. Mater ., 3:114203, 2019

  36. [36]

    Intrinsic anomalous Hall effect in thin films of topo- logical kagome ferromagnet Fe3Sn2

    Kacho Imtiyaz Ali Khan, Ram Singh Yadav, Himanshu Bangar, Akash Kumar, Niru Chowdhury, Pras- anta Kumar Muduli, and Pranaba Kishor Muduli. Intrinsic anomalous Hall effect in thin films of topo- logical kagome ferromagnet Fe3Sn2. Nanoscale, 14:8484–8492, 2022

  37. [37]

    Magnetodynamic properties of ultrathin films of Fe 3Sn2-a topological kagome fer- romagnet

    Kacho Imtiyaz Ali Khan, Akash Kumar, Pankhuri Gupta, Ram Singh Yadav, Johan Åkerman, and Pran- aba Kishor Muduli. Magnetodynamic properties of ultrathin films of Fe 3Sn2-a topological kagome fer- romagnet. Sci. Rep., 14:3487, 2024

  38. [38]

    Emerging Spin-Orbit Torques in Low- Dimensional Dirac Materials

    Joaquín Medina Dueñas, José H García, and Stephan Roche. Emerging Spin-Orbit Torques in Low- Dimensional Dirac Materials. Phys. Rev. Lett., 132:266301, 2024

  39. [39]

    Checkelsky

    Minyong Han, Hisashi Inoue, Shiang Fang, Caolan John, Linda Ye, Mun K Chan, David Graf, Take- hito Suzuki, Madhav Prasad Ghimire, Won Joon Cho, Efthimios Kaxiras, and Joseph G. Checkelsky. Evidence of two-dimensional flat band at the surface of antiferromagnetic kagome metal FeSn. Nat. Commun., 12:5345, 2021

  40. [40]

    Atomic layer epitaxy of kagome magnet Fe 3Sn2 and Sn-modulated heterostruc- tures

    Shuyu Cheng, Binbin Wang, Igor Lyalin, Núria Bagués, Alexander J Bishop, David W McComb, and Roland K Kawakami. Atomic layer epitaxy of kagome magnet Fe 3Sn2 and Sn-modulated heterostruc- tures. APL Mater ., 10:061112, 2022

  41. [41]

    Large sponta- neous magneto-thermoelectric effect in epitaxial thin films of the topological kagome ferromagnet Fe3Sn

    Shun’ichiro Kurosawa, Tomoya Higo, Shota Saito, Ryota Uesugi, and Satoru Nakatsuji. Large sponta- neous magneto-thermoelectric effect in epitaxial thin films of the topological kagome ferromagnet Fe3Sn. Phys. Rev. Mater ., 8:054206, 2024

  42. [42]

    Growth of millimeter-sized graphene single crystals on Al2O3 (0001)/Pt (111) template wafers using chemical vapor deposition.ECS J Solid State Sci Technol, 7:M195, 2018

    Ken Verguts, Yves Defossez, Alessandra Leonhardt, Joke De Messemaeker, Koen Schouteden, Chris Van Haesendonck, Cedric Huyghebaert, Stefan De Gendt, and Steven Brems. Growth of millimeter-sized graphene single crystals on Al2O3 (0001)/Pt (111) template wafers using chemical vapor deposition.ECS J Solid State Sci Technol, 7:M195, 2018

  43. [43]

    Surface potentials of (111),(110) and (100) oriented CeO 2−x thin films

    Hans F Wardenga and Andreas Klein. Surface potentials of (111),(110) and (100) oriented CeO 2−x thin films. Appl. Surf. Sci., 377:1–8, 2016

  44. [44]

    High quality epitaxial thin films and exchange bias of antiferromagnetic Dirac semimetal FeSn

    Durga Khadka, TR Thapaliya, Jiajia Wen, Ryan F Need, and SX Huang. High quality epitaxial thin films and exchange bias of antiferromagnetic Dirac semimetal FeSn. Appl. Phys. Lett., 117:032403, 2020. 14

  45. [45]

    Epitaxial growth and magnetic properties of kagome metal FeSn/elemental ferromagnet heterostructures

    Prajwal M Laxmeesha, Tessa D Tucker, Rajeev Kumar Rai, Shuchen Li, Myoung-Woo Yoo, Eric A Stach, Axel Hoffmann, and Steven J May. Epitaxial growth and magnetic properties of kagome metal FeSn/elemental ferromagnet heterostructures. J. Appl. Phys., 135:085302, 2024

  46. [46]

    Large Damping-like Spin–Orbit Torque and Improved Device Performance Utilizing Mixed-Phase Ta.ACS Appl

    Akash Kumar, Raghav Sharma, Kacho Imtiyaz Ali Khan, Chandrasekhar Murapaka, Gerard Joseph Lim, Wen Siang Lew, Sujeet Chaudhary, and Pranaba Kishor Muduli. Large Damping-like Spin–Orbit Torque and Improved Device Performance Utilizing Mixed-Phase Ta.ACS Appl. Electron. Mater ., 3:3139–3146, 2021

  47. [47]

    Interfacial Origin of Uncon- ventional Spin-Orbit Torque in Py/γ- γ- IrMn3

    Akash Kumar, Pankhuri Gupta, Niru Chowdhury, Kacho Imtiyaz Ali Khan, Utkarsh Shashank, Surbhi Gupta, Yasuhiro Fukuma, Sujeet Chaudhary, and Pranaba Kishor Muduli. Interfacial Origin of Uncon- ventional Spin-Orbit Torque in Py/γ- γ- IrMn3. Adv. Quantum Technol., 6:2300092, 2023

  48. [48]

    Spin-torque ferromagnetic resonance induced by the spin Hall effect

    Luqiao Liu, Takahiro Moriyama, DC Ralph, and RA Buhrman. Spin-torque ferromagnetic resonance induced by the spin Hall effect. Phys. Rev. Lett., 106:036601, 2011

  49. [49]

    Magnetic-Proximity-Induced Effi- cient Charge-to-Spin Conversion in Large-Area PtSe2/Ni80Fe20 Heterostructures

    Richa Mudgal, Alka Jakhar, Pankhuri Gupta, Ram Singh Yadav, Bubunu Biswal, Pratik Sahu, Himanshu Bangar, Akash Kumar, Niru Chowdhury, Biswarup Satpati, et al. Magnetic-Proximity-Induced Effi- cient Charge-to-Spin Conversion in Large-Area PtSe2/Ni80Fe20 Heterostructures. Nano Lett., 23:11925– 11931, 2023

  50. [50]

    Generation of out-of-plane polarized spin current in (permalloy, Cu)/EuS interfaces

    Pankhuri Gupta, Niru Chowdhury, Mingran Xu, Prasanta Kumar Muduli, Akash Kumar, Kouta Kondou, Yoshichika Otani, and Pranaba Kishor Muduli. Generation of out-of-plane polarized spin current in (permalloy, Cu)/EuS interfaces. Phys. Rev. B, 109:L060405, 2024

  51. [51]

    Giant spin pumping enhancement at the interface of ferromagnet (Py) and Kagome antiferromagnet (FeSn)

    Kacho Imtiyaz Ali Khan and Pranaba Kishor Muduli. Giant spin pumping enhancement at the interface of ferromagnet (Py) and Kagome antiferromagnet (FeSn). Under Prepration

  52. [52]

    Tilted spin current generated by the collinear antiferromagnet ruthenium dioxide

    Arnab Bose, Nathaniel J Schreiber, Rakshit Jain, Ding-Fu Shao, Hari P Nair, Jiaxin Sun, Xiyue S Zhang, David A Muller, Evgeny Y Tsymbal, Darrell G Schlom, and D C Ralph. Tilted spin current generated by the collinear antiferromagnet ruthenium dioxide. Nat. Electron., 5:267–274, 2022

  53. [53]

    Magnetic asymmetry induced anomalous spin-orbit torque in irmn

    Jing Zhou, Xinyu Shu, Yaohua Liu, Xiao Wang, Weinan Lin, Shaohai Chen, Liang Liu, Qidong Xie, Tao Hong, Ping Yang, Binghai Yan, Xiufeng Han, and Jingsheng Chen. Magnetic asymmetry induced anomalous spin-orbit torque in irmn. Phys. Rev. B, 101:184403, 2020

  54. [54]

    Isotropic spin and inverse spin Hall effect in epitaxial (111)-oriented Pt/Co bilayers

    Adrián Gudín, Alberto Anadón, Iciar Arnay, Rubén Guerrero, Julio Camarero, Sebastien Petit-Watelot, Paolo Perna, and Juan-Carlos Rojas-Sánchez. Isotropic spin and inverse spin Hall effect in epitaxial (111)-oriented Pt/Co bilayers. Phys. Rev. Mater ., 7:124412, 2023

  55. [55]

    Charge-spin current conversion in high quality epitaxial Fe/Pt systems: Isotropic spin Hall angle along different in-plane crystalline direc- tions

    C Guillemard, S Petit-Watelot, S Andrieu, and J-C Rojas-Sánchez. Charge-spin current conversion in high quality epitaxial Fe/Pt systems: Isotropic spin Hall angle along different in-plane crystalline direc- tions. Appl. Phys. Lett., 113:262404, 2018

  56. [56]

    Strong anisotropic anomalous Hall effect and spin Hall effect in the chiral antiferromagnetic compounds Mn3X (X= Ge, Sn, Ga, Ir, Rh, and Pt)

    Yang Zhang, Yan Sun, Hao Yang, Jakub Železn `y, Stuart PP Parkin, Claudia Felser, and Binghai Yan. Strong anisotropic anomalous Hall effect and spin Hall effect in the chiral antiferromagnetic compounds Mn3X (X= Ge, Sn, Ga, Ir, Rh, and Pt). Phys. Rev. B, 95:075128, 2017

  57. [57]

    Spin-polarized current in noncollinear antiferromagnets

    Jakub Železn `y, Yang Zhang, Claudia Felser, and Binghai Yan. Spin-polarized current in noncollinear antiferromagnets. Phys. Rev. Lett., 119:187204, 2017. 15

  58. [58]

    Muduli, Muhammad Ikhlas, Yasutomo Omori, Takahiro Tomita, Allan

    Motoi Kimata, Hua Chen, Kouta Kondou, Satoshi Sugimoto, Prasanta K. Muduli, Muhammad Ikhlas, Yasutomo Omori, Takahiro Tomita, Allan. H. MacDonald, Satoru Nakatsuji, and Yoshichika Otani. Mag- netic and magnetic inverse spin Hall effects in a non-collinear antiferromagnet. Nature, 565:627–630, 2019

  59. [59]

    Origin of the magnetic spin Hall effect: Spin current vorticity in the Fermi sea

    Alexander Mook, Robin R Neumann, Annika Johansson, Jürgen Henk, and Ingrid Mertig. Origin of the magnetic spin Hall effect: Spin current vorticity in the Fermi sea. Phys. Rev. Res., 2:023065, 2020

  60. [60]

    Experimental Evidence for a Berry Curvature Quadrupole in an Antiferromagnet

    Soumya Sankar, Ruizi Liu, Cheng-Ping Zhang, Qi-Fang Li, Caiyun Chen, Xue-Jian Gao, Jiangchang Zheng, Yi-Hsin Lin, Kun Qian, Ruo-Peng Yu, et al. Experimental Evidence for a Berry Curvature Quadrupole in an Antiferromagnet. Phys. Rev. X, 14:021046, 2024. 16