Ohtsuka Yusuke, Kanazawa Naoya, Hirayama Motoaki, Matsui Akira, Nomoto Takuya, Arita Ryotaro, Nakajima Taro, Hanashima Takayasu, Ukleev Victor, Aoki Hiroyuki, Mogi Masataka, Fujiwara Kohei, Tsukazaki Atsushi, Ichikawa Masakazu, Kawasaki Masashi, Tokura Yoshinori
Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan.
RIKEN Center for Emergent Matter Science (CEMS), Wako 351-0198, Japan.
Sci Adv. 2021 Nov 19;7(47):eabj0498. doi: 10.1126/sciadv.abj0498. Epub 2021 Nov 17.
FeSi is a nonmagnetic narrow-gap insulator, exhibiting peculiar charge and spin dynamics beyond a simple band structure picture. Those unusual features have been attracting renewed attention from topological aspects. Although the surface conduction was demonstrated according to size-dependent resistivity in bulk crystals, its topological characteristics and consequent electromagnetic responses remain elusive. Here, we demonstrate an inherent surface ferromagnetic-metal state of FeSi thin films and its strong spin-orbit coupling (SOC) properties through multiple characterizations of two-dimensional conductance, magnetization, and spintronic functionality. Terminated covalent bonding orbitals constitute the polar surface state with momentum-dependent spin textures due to Rashba-type spin splitting, as corroborated by unidirectional magnetoresistance measurements and first-principles calculations. As a consequence of the spin-momentum locking, nonequilibrium spin accumulation causes magnetization switching. These surface properties are closely related to the Zak phase of the bulk band topology. Our findings propose another route to explore noble metal–free materials for SOC-based spin manipulation.
FeSi是一种非磁性窄带隙绝缘体,展现出超越简单能带结构图像的奇特电荷和自旋动力学。这些不寻常的特性一直吸引着拓扑学领域的新关注。尽管根据块状晶体中与尺寸相关的电阻率证明了表面传导现象,但其拓扑特性以及随之而来的电磁响应仍然难以捉摸。在此,我们通过对二维电导、磁化和自旋电子功能的多重表征,证明了FeSi薄膜固有的表面铁磁金属态及其强自旋轨道耦合(SOC)特性。由于Rashba型自旋分裂,终止的共价键轨道构成了具有动量依赖自旋纹理的极性表面态,这一点得到了单向磁阻测量和第一性原理计算的证实。作为自旋动量锁定的结果,非平衡自旋积累导致磁化翻转。这些表面特性与体带拓扑的Zak相密切相关。我们的发现为探索用于基于SOC的自旋操控的无贵金属材料提出了另一条途径。