凝聚态物理
反铁磁性
磁化
自旋极化
自旋晶体管
自旋电子学
铁磁性
电场
材料科学
电子能带结构
物理
电子
自旋霍尔效应
磁场
量子力学
作者
Fengrui Yao,Menghan Liao,Marco Gibertini,Cheol-Yeon Cheon,X. N. Lin,Fan Wu,Kenji Watanabe,Takashi Taniguchi,Ignacio Gutiérrez‐Lezama,Alberto F. Morpurgo
标识
DOI:10.1038/s41565-025-01872-w
摘要
Abstract Antiferromagnetic conductors with suitably broken spatial symmetries host spin-polarized bands, which lead to transport phenomena commonly observed in metallic ferromagnets. In bulk materials, it is the given crystalline structure that determines whether symmetries are broken and spin-polarized bands are present. Here we show that, in the two-dimensional limit, an electric field can control the relevant symmetries. To this end, we fabricate a double-gate transistor based on bilayers of van der Waals antiferromagnetic semiconductor CrPS 4 and show how a perpendicular electric displacement field can switch the spin polarization of the conduction band on and off. Because conduction band states with opposite spin polarizations are hosted in the different layers and are spatially separated, these devices also give control over the magnetization of the electrons that are accumulated electrostatically. Our experiments show that double-gated CrPS 4 transistors provide a viable platform to create gate-induced conductors with near unity spin polarization at the Fermi level, as well as devices with a full electrostatic control of the total magnetization of the system.
科研通智能强力驱动
Strongly Powered by AbleSci AI