The 70th JSAP Spring Meeting 2023

Presentation information

Oral presentation

10 Spintronics and Magnetics » 10.4 Spintronics in semiconductor, topological material, superconductor, and multiferroics

[16p-D704-1~18] 10.4 Spintronics in semiconductor, topological material, superconductor, and multiferroics

Thu. Mar 16, 2023 1:30 PM - 6:30 PM D704 (Building No. 11)

Tetsuya Fukushima(東大), Kenji Nawa(三重大), Masaki Kobayashi(東大)

6:15 PM - 6:30 PM

[16p-D704-18] Demonstration of Ferroic Behavior of Berry Curvature Dipole in a Topological Crystalline Insulator at 300 K

〇(D)Taiki Nishijima1, Takuto Watanabe2, Hiroaki Sekiguchi2, Yuichiro Ando1, Ei Shigematsu1, Ryo Ohshima1, Shinji Kuroda2, Masashi Shiraishi1 (1.CSRN, Kyoto Univ., 2.Univ. Tsukuba)

Keywords:topological crystalline insulator, Berry curvature, non-volatile

The physics related to Berry curvature is now a central research topic in condensed matter physics. The Berry curvature dipole (BCD) is a significant and intriguing physical parameter that characterizes the antisymmetric distribution of Berry curvature. The BCD exists under inversion symmetry breaking, which induces current-driven out-of-plane magnetization and nonlinear Hall effect (NLHE). However, the creation and controllability of BCDs have been limited to far below room temperature (RT) and nonvolatile (i.e., ferroic) BCDs have not yet been discovered, hindering further progress in topological physics. In this work, we focused on a topological crystalline insulator, Pb1-xSnxTe (PST) to realize the ferroic BCD and demonstrated the ferroic BCD by measuring NLHE induced by BCD in PST.