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. 2018 Aug 28;8:12959. doi: 10.1038/s41598-018-31201-2

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© The Author(s) 2018

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 license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license 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 license, visit http://creativecommons.org/licenses/by/4.0/.

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Current-induced effective fields after the planar Hall effect correction. (a–d) SOT-induced damping-like and field-like effective fields for Pt/Co/SmO_x (Pt/Co/AlO_x) as a function of the amplitude I₀ of the sinusoidal current. The blue and green symbols denote “up” and “down” magnetized states, respectively. The field-like effective fields against $I_{0}^{2}$ for Pt/Co/SmO_x (e) and Pt/Co/AlO_x (f), respectively.