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. 2020 Oct 14;10:17274. doi: 10.1038/s41598-020-74156-z

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© The Author(s) 2020

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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Temperature variation of the structural transition field H_ST (determined as in Fig. 2), the onset field H_on(T), and the peak field H_p(T). The vertical segments on H_ST(T) illustrate the transition width extracted for several temperatures (by taking the structural transition symmetric relative to H_ST). The continuous line represents the fit of the H_ST(T) dependence with (2), by considering the two-fluid model for the temperature variation of the magnetic penetration depth. The filed-symbol H_p(T) values have been determined from the magnetic hysteresis curves registered with the PPMS.