Strain-tunable anomalous Hall plateau in antiferromagnet CoNb<sub>3</sub>S<sub>6</sub>
ORAL
Abstract
Antiferromagnets exhibiting the anomalous Hall effect (AHE) represent a fascinating convergence of magnetism, topology, and electronic structure. CoNb3S6 is an excellent example of layered antiferromagnets [1,2] that has attracted increasing attentions in recent years due to its rich physics. Nirmal et al [3] first discovered the unexpected large AHE (~27 W-1 cm-1) and later Giulia et al [4] found the AHE can be further enhanced in small exfoliated crystals (~400 W-1 cm-1). In 2020, Smejkal et al rebranded the AHE in CoNb3S6 as the “crystal Hall effect”, with CoNb3S6 being an early altermagnet candidate [5,6]. Moreover, neutron scattering measurements suggested that CoNb3S6 has a non-coplanar antiferromagnetic structure and the AHE should be a spontaneous topological Hall effect from spin chirality [7]. Here, we report a strain tunable anomalous Hall plateau in the antiferromagnet CoNb3S6, which is characterized a flat extended intermediate step of the anomalous Hall hysteresis loop. The remarkable tunability of the plateau indicates the existence of a hidden phase transition that significantly changes the magnetic anisotropy energy but not the magnetic order. As a result, the anomalous Hall plateau reflects the phase coexistence during the hidden transition, which is non-volatile and enables an unusual four-state switching of the anomalous Hall effect. We believe further investigations into the underlying mechanisms and potential applications of this strain-engineered magnetic phenomenon could contribute to the advancement and innovations in data storage and other magnetic technologies.
[1] K. Anzenhofer et al., Journal of Physics and Chemistry of Solids 31, 1057 (1970).
[2] S. S. P. Parkin et al., Journal of Physics C: Solid State Physics 16, 2765 (1983).
[3] N. J. Ghimire et al., Nature Communications 9, 3280 (2018).
[4] G. Tenasini et al., Physical Review Research 2, 023051 (2020).
[5] L. Šmejkal et al., Science Advances 6, eaaz8809 (2020).
[6] L. Šmejkal et al., Physical Review X 12, 040501 (2022).
[7] H. Takagi et al., Nature Physics 19, 961 (2023).
[1] K. Anzenhofer et al., Journal of Physics and Chemistry of Solids 31, 1057 (1970).
[2] S. S. P. Parkin et al., Journal of Physics C: Solid State Physics 16, 2765 (1983).
[3] N. J. Ghimire et al., Nature Communications 9, 3280 (2018).
[4] G. Tenasini et al., Physical Review Research 2, 023051 (2020).
[5] L. Šmejkal et al., Science Advances 6, eaaz8809 (2020).
[6] L. Šmejkal et al., Physical Review X 12, 040501 (2022).
[7] H. Takagi et al., Nature Physics 19, 961 (2023).
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Presenters
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Long Chen
University of Tennessee
Authors
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Long Chen
University of Tennessee
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Richard Lai
University of Tennessee
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Shashi K Pandey
University of Tennessee
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Dapeng Cui
University of Tennessee
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Alexander Brassington
University of Tennessee
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Ryan J Philip
Argonne National Laboratory, Advanced Photon Source, Argonne National Laboratories
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Jong-Woo kim
Argonne National Laboratory, Advanced Photon Source, Argonne National Laboratories
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Jian Liu
University of Tennessee
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Haidong Zhou
University of Tennessee