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. 2024 Dec 11;636(8042):348–353. doi: 10.1038/s41586-024-08234-x

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© The Author(s) 2024

Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.

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Extended Data Fig. 2 — a, XMCD-PEEM image taken at temperature T = 100 K, showing magnetic contrast in open-space region in proximity to a patterned edge. b, The same region re-imaged at T = 250 K, where the XMCD magnetic contrast vanishes, leaving only structural contrast. c, d, Hall resistivity measurements on a 100 μm Hall bar at T = 150 K and 250 K, respectively, showing that the spontaneous anomalous Hall effect is absent at the higher temperature.