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Published July 13, 2022 | Supplemental Material
Journal Article Open

Hard Ferromagnetism Down to the Thinnest Limit of Iron-Intercalated Tantalum Disulfide

Abstract

Two-dimensional (2D) magnetic crystals hold promise for miniaturized and ultralow power electronic devices that exploit spin manipulation. In these materials, large, controllable magnetocrystalline anisotropy (MCA) is a prerequisite for the stabilization and manipulation of long-range magnetic order. In known 2D magnetic crystals, relatively weak MCA typically results in soft ferromagnetism. Here, we demonstrate that ferromagnetic order persists down to the thinnest limit of FeₓTaS₂ (Fe-intercalated bilayer 2H-TaS b) with giant coercivities up to 3 T. We prepare Fe-intercalated TaS₂ by chemical intercalation of van der Waals-layered 2H-TaS₂ crystals and perform variable-temperature transport, transmission electron microscopy, and confocal Raman spectroscopy measurements to shed new light on the coupled effects of dimensionality, degree of intercalation, and intercalant order/disorder on the hard ferromagnetic behavior of FeₓTaS₂. More generally, we show that chemical intercalation gives access to a rich synthetic parameter space for low-dimensional magnets, in which magnetic properties can be tailored by the choice of the host material and intercalant identity/amount, in addition to the manifold distinctive degrees of freedom available in atomically thin, van der Waals crystals.

Additional Information

© 2022 American Chemical Society. Received 16 March 2022. Published online 22 June 2022. Published in issue 13 July 2022. The authors thank Oscar Gonzalez, Zhizhi Kong, Lilia Xie, and Steven Zeltmann for helpful discussion. This material is based upon work supported by the Air Force Office of Scientific Research under AFOSR Award no. FA9550-20-1-0007. We would like to thank Gatan, Inc. as well as P. Denes, A. Minor, J. Ciston, C. Ophus, J. Joseph, and Ian Johnson at LBNL, who contributed to the development of the 4D Camera used for STEM-DPC measurements. This research used resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility located at Lawrence Berkeley National Laboratory, operated under Contract no. DE-AC02-05CH11231 using NERSC award ERCAP0020898 and ERCAP0020897. M.V.W. acknowledges support from a UCB Chancellor's Fellowship and NSF Graduate Research Fellowship. Instrumentation used in this work was supported by grants from the W.M. Keck Foundation (Award # 993922), the Canadian Institute for Advanced Research (CIFAR–Azrieli Global Scholar, Award # GS21-011), the Gordon and Betty Moore Foundation EPiQS Initiative (Award #10637), and the 3M Foundation through the 3M Non-Tenured Faculty Award (#67507585). N.P.K. acknowledges support from the Hertz Fellowship and from the National Science Foundation Graduate Research Fellowship under grant no. DGE-1745301. Confocal Raman spectroscopy was supported by a DURIP grant through the Office of Naval Research under Award no. N00014-20-1-2599 (D.K.B.). Experimental and theoretical work at the Molecular Foundry, LBNL was supported by the Office of Science, Office of Basic Energy Sciences, the U.S. Department of Energy under Contract no. DE-AC02-05CH11231. Computational studies were carried out using supercomputing resources of the National Energy Research Scientific Computing Center (NERSC) and the TMF clusters managed by the High-Performance Computing Services Group at LBNL. K.W. and T.T. acknowledge support from the Elemental Strategy Initiative conducted by the MEXT, Japan, grant number JPMXP0112101001, JSPS KAKENHI grant number JP20H00354, and the CREST (JPMJCR15F3), JST. The authors declare no competing financial interest.

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Additional details

Created:
August 22, 2023
Modified:
October 24, 2023