Yang Boxuan, Bhujel Bibek, Chica Daniel G, Telford Evan J, Roy Xavier, Ibrahim Fatima, Chshiev Mairbek, Cosset-Chéneau Maxen, Wees Bart J van
Zernike Institute for Advanced Materials, University of Groningen, 9747, AG, Groningen, The Netherlands.
Department of Chemistry, Columbia University, New York, NY, 10027, USA.
Nat Commun. 2024 May 25;15(1):4459. doi: 10.1038/s41467-024-48809-w.
The magnetic proximity effect can induce a spin dependent exchange shift in the band structure of graphene. This produces a magnetization and a spin polarization of the electron/hole carriers in this material, paving the way for its use as an active component in spintronics devices. The electrostatic control of this spin polarization in graphene has however never been demonstrated so far. We show that interfacing graphene with the van der Waals antiferromagnet CrSBr results in an unconventional manifestation of the quantum Hall effect, which can be attributed to the presence of counterflowing spin-polarized edge channels originating from the spin-dependent exchange shift in graphene. We extract an exchange shift ranging from 27 - 32 meV, and show that it also produces an electrostatically tunable spin polarization of the electron/hole carriers in graphene ranging from - 50% to + 69% in the absence of a magnetic field. This proof of principle provides a starting point for the use of graphene as an electrostatically tunable source of spin current and could allow this system to generate a large magnetoresistance in gate tunable spin valve devices.
磁近邻效应可在石墨烯的能带结构中诱导自旋相关的交换位移。这会在该材料中产生电子/空穴载流子的磁化和自旋极化,为其用作自旋电子器件中的有源组件铺平了道路。然而,迄今为止,石墨烯中这种自旋极化的静电控制从未得到证实。我们表明,将石墨烯与范德华反铁磁体CrSBr相接触会导致量子霍尔效应的非常规表现,这可归因于源自石墨烯中自旋相关交换位移的反向流动的自旋极化边缘通道的存在。我们提取出范围为27 - 32毫电子伏特的交换位移,并表明在没有磁场的情况下,它还会在石墨烯中产生电子/空穴载流子的静电可调自旋极化,范围为 - 50%至 + 69%。这一原理验证为将石墨烯用作自旋电流的静电可调源提供了一个起点,并可能使该系统在栅极可调自旋阀器件中产生大的磁电阻。