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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. 2 — a Angular dependence of c-axis resistivity measured at different in-plane magnetic fields. The featureless ρ_c(θ) curve measured at 2.4 T separates two sets of ρ_c(θ) curves holding phase-reversed oscillations with twofold symmetry. Angular dependent c-axis resistivity plotted in polar coordinate measured with rotating in-plane magnetic field of the magnitude (b) below and (c) above 2.4 T. Local minima in curves measured at μ₀H < 2.4 T change to local maxima in curves at μ₀H > 2.4 T in the direction along a-axis. In addition, ρ_c(θ) curves measured at μ₀H > 2.4 T show extra oscillation of six-fold symmetry besides the major twofold signal. d FT result to the ρ_c(θ) curve measured at 7 T.