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. 2021 Nov 18;12:6727. doi: 10.1038/s41467-021-27084-z

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© The Author(s) 2021

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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Fig. 4 — Angular dependent c-axis resistivity measured at different temperatures under a magnetic field of a 0.4 and b 5 T. c Temperature dependence of the nematicity. The solid symbols represent the c-axis resistivity difference between θ = 0° and 90° at 0.4 and 5 T, while the open symbols show twice the amplitude of the 180° (or C₂) peak (2A_FT,C2) from FT results (Supplementary Fig. 8a) to ρ_c(θ) curves measured at different temperatures under 5 T. One can see that the latter is more sensitive to show the C₂ symmetry which seems ending near T_CDW.