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. 2022 May 12;13:2655. doi: 10.1038/s41467-022-30302-x

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© The Author(s) 2022

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. 3 — Evolution of the Fermi surface (FS) from non-interacting system with H_f in a, to the nFL FS subjected to strong FM correlation at U = 5.9, T = 0.1 in b, and eventually to the FS in the PG phase at U = 5.9, T = 0.05 in c. The spectral weights are normalized with the same scale. The system size is L = 12 and the twisted boundary condition in the fermion hopping is applied such that the momentum resolution is 4 times larger in both k_x and k_y directions.