报告摘要 | A topological crystalline insulator (TCI) is a topological phase characterized by crystallographic symmetries. There exist various TCI phases depending on the crystallographic symmetries, such as mirror- symmetric TCIs and glide-symmetric TCIs [1,2]. In these TCIs, whether or not gapless topological surface states appear depends on the surface orientations. Namely, if the surface orientation is mirror/glide invariant, the corresponding gapless surface states appear. For example, in glide-symmetric TCIs, whether topological gapless surface states appear depends on the parity of the Miller index of the surface. In this presentation, we discuss relationships between equilibrium crystal shapes and topological phases. When gapless topological surface states appear, the surface energy for the surface orientation will become higher. It makes this surface orientation less favorable, and its area will become smaller. Therefore, we expect that the equilibrium crystal shape will depend on whether the crystal is in a trivial phase or in a topological phase. By model calculation, we show that this is indeed true for various topological phases [3,4]. [1]K. Shiozaki, M. Sato, K. Gomi, Z2 topology in nonsymmorphic crystalline insulators: Möbius twist in surface states, Phys. Rev. B 91, 155120 (2015). [2]C. Fang, L. Fu, New classes of three-dimensional topological crystalline insulators: Nonsymmorphic and magnetic, Phys. Rev. B 91, 161105 (2015). [3] Y. Tanaka, T. Zhang, M. Uwaha, S. Murakami, Anomalous crystal shapes of topological crystalline insulators, Phys. Rev. Lett. 129, 046802 (2022). [4] Y. Tanaka and S. Murakami, Effects of first- and second-order topological phases on equilibrium crystal shapes, Phys. Rev. B 107, 245148 (2023). |