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Discriminating superconducting fluctuations from the pseudogap in Bi2Sr2Can−1CunO2n+4+δ (n = 2, 3): A magnetotransport study

Shunpei Yamaguchi1, Nae Sasaki1, Shintaro Adachi1,2, Keiichi Harada1, Yuki Teramoto1, Shintaro Matsuda1, Tomohiro Usui1, Takenori Fujii3, Takashi Noji4 et al.

Itsuhiro Kakeya5, Haruka Taniguchi6,7, Michiaki Matsukawa6, Atsushi Miyake8,9, Hajime Ishikawa8, Koichi Kindo8, and Takao Watanabe1,10,11,*

  • *Contact author: watanabe.takao@nihon-u.ac.jp; tnmwata313@gmail.com

Phys. Rev. B 114, L200501 – Published 14 October, 2026

DOI: https://doi.org/10.1103/d532-8q2d

Abstract

Understanding the normal state is essential for uncovering the mechanism of high-Tc superconductivity. We investigate magnetotransport in Bi2Sr2CaCu2O8+δ and Bi2Sr2Ca2Cu3O10+δ single crystals over a wide doping range. While the in-plane resistivity and Hall coefficient show strong pseudogap-induced temperature dependence, the T2 Hall-angle behavior and the modified Kohler's rule remain robust across all dopings. The onset temperatures of the pseudogap are clearly distinct from superconducting fluctuations, although they scale with the pseudogap magnitudes with a factor consistent with a d-wave superconductor. These results demonstrate that the pseudogap does not arise from superconducting fluctuations and instead suggest that it may originate from preformed Cooper pairing in the BCS-BEC crossover regime.

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