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. 2024 Nov 15;15:9778. doi: 10.1038/s41467-024-53900-3

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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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Fig. 4 — a The field derivative of the magnetisation isotherms shows the development of the critical field below $T_{N} = 1.3$ K. b The temperature-field phase diagram of RPSO mapped through magnetic susceptibility and isothermal magnetisation measurements reveals the suppression of the zero-field $T_{N} = 1.3$ K upon application of a magnetic field. Above a critical field of $H_{C} = 3.55$ T, $T_{N}$ appears completely suppressed within the temperature range of the measurement.