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Configurable antiferromagnetic domains and lateral exchange bias in atomically thin CrPS4

Abstract

Interfacial exchange coupling between antiferromagnets (AFMs) and ferromagnets (FMs) crucially makes it possible to shift the FM hysteresis, known as exchange bias, and to switch AFM states. Two-dimensional magnets unlock opportunities to combine AFM and FM materials; however, the buried AFM–FM interfaces obtained by stacking remains challenging to understand. Here we demonstrate interfacial control via intralayer exchange coupling in the layered AFM CrPS4, where connected even and odd layers realize pristine lateral interfaces between AFM-like and FM-like regions. We distinguish antiphase even-layer states by scanning nitrogen-vacancy centre magnetometry due to a weak surface magnetization. This surface magnetization enables control over the even-layer state, with different regions switching at distinct fields due to their own lateral couplings. We toggle three AFM domains adjacent to a FM-like region and demonstrate a tunable multilevel exchange bias. Our nanoscale visualization unveils the microscopic origins of exchange bias and advances single two-dimensional crystals for hybrid AFM–FM technologies.

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Fig. 1: Layered AFM in atomically thin CrPS4.
Fig. 2: Antiphase domains in even-layer CrPS4.
Fig. 3: Lateral exchange bias at the even–odd interface.
Fig. 4: Controlled nucleation and translation of AFM domain walls.
Fig. 5: Multilevel exchange bias through digital control of AFM domains.

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Data availability

All data that support the findings of this study are available from the corresponding author upon request. Source data are provided with this paper.

Code availability

The codes that support the findings of this study are available upon request. Codes include scripts for data analysis and micromagnetic simulations.

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Acknowledgements

The authors thank Y. Ran, P. Aynajian for valuable discussions and Q. Ma and K. S. Burch for use of some laboratory facilities. B.B.Z. and Y.-X.W. acknowledge support from the Department of Energy Early Career Program under award number DE-SC0024177 for NV centre measurements. B.B.Z., Y.-X.W. and T.K.M.G. acknowledge support from the National Science Foundation (NSF) award DMR-2047214 for development of the scanning NV microscope. B.B.Z. and X.-Y.Z. were supported by NSF ECCS-2041779 for sample fabrication and magnetization analysis. Z.L., M.A.I., R.N.G., G.P.T. and T.A. acknowledge a start-up fund from Binghamton University. Funding for the ADL Small Grants Program is made possible by support to S3IP from New York Empire State Development Division of Science, Technology, and Research. E.J.G.S. acknowledges computational resources through CIRRUS Tier-2 HPC Service (ec131 Cirrus Project) at EPCC, which is funded by the University of Edinburgh and EPSRC (EP/P020267/1); and ARCHER2 UK National Supercomputing Service via the UKCP consortium (Project e89) funded by EPSRC grant reference EP/X035891/1. E.J.G.S. acknowledges the EPSRC Open Fellowship (EP/T021578/1) and the Donostia International Physics Center for funding support. E.J.G.S. and R.R.-E. acknowledge support from the Royal Society through the International Newton Fellowship (NIF/R1/241532). K.W. and T.T. acknowledge support from the JSPS KAKENHI (grant numbers 21H05233 and 23H02052) and the World Premier International Research Center Initiative (WPI), MEXT, Japan.

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Contributions

Y.-X.W., Z.L. and B.B.Z. conceived the experiments. M.A.I. and G.P.T. synthesized the bulk crystals. M.A.I., R.N.G., G.P.T. and T.A. performed bulk crystal characterizations and RMCD measurements. C.B. performed X-ray diffraction measurements. Z.L. supervised the research at Binghamton University. Y.-X.W. and T.K.M.G. developed the scanning NV magnetometry instrumentation and protocols. Y.-X.W. fabricated the samples and performed the scanning NV experiments, with the assistance of T.K.M.G. and X.-Y.Z. Y.-X.W. analysed the data and performed micromagnetic simulations, with the assistance of X.-Y.Z. and B.B.Z. Atomistic spin dynamics simulations were performed by R.R.-E., and the Stoner–Wohlfarth model was developed by M.H.B., both under the guidance of E.J.G.S. K.W. and T.T. synthesized the hexagonal boron nitride crystals. B.B.Z., Y.-X.W., R.R.-E., M.H.B. and E.J.G.S. wrote the manuscript, with input from all authors.

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Correspondence to Brian B. Zhou.

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Supplementary Information (download PDF )

Supplementary Figs. 1–21, Tables 1–3 and Discussion.

Supplementary Video 1 (download MP4 )

Video of the dynamical evolution of a thermally nucleated even-layer domain wall in atomistic simulations at an applied magnetic field of +200 mT. The video plots the components of the total magnetization summed over all layers.

Supplementary Video 2 (download MP4 )

Same simulation as Supplementary Video 1 at +200 mT, but the magnetization components of only the third layer are plotted.

Supplementary Video 3 (download MP4 )

Video of the dynamical evolution of a thermally nucleated even-layer domain wall in atomistic simulations at an applied magnetic field of − 200 mT. The video plots the components of the total magnetization summed over all layers.

Supplementary Video 4 (download MP4 )

Same simulation as Supplementary Video 3 at − 200 mT, but the magnetization components of only the third layer are plotted.

Source data

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Statistical source data and analysed reconstruction data.

Source Data Fig. 2 (download XLSX )

Statistical source data.

Source Data Fig. 3 (download XLSX )

Statistical source data and classified hysteresis data.

Source Data Fig. 4 (download XLSX )

Statistical source data and classified hysteresis data.

Source Data Fig. 5 (download XLSX )

Statistical source data and classified hysteresis data.

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Wang, YX., Graham, T.K.M., Rama-Eiroa, R. et al. Configurable antiferromagnetic domains and lateral exchange bias in atomically thin CrPS4. Nat. Mater. 24, 1414–1423 (2025). https://doi.org/10.1038/s41563-025-02259-x

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