Zhang Yu, Gao Fei, Gao Shiwu, He Lin
Center for Advanced Quantum Studies, Department of Physics, Beijing Normal University, Beijing 100875, China.
Computational Science Research Center, ZPark II, Beijing 100193, China.
Sci Bull (Beijing). 2020 Feb 15;65(3):194-200. doi: 10.1016/j.scib.2019.11.023. Epub 2019 Nov 23.
Creating a single-carbon vacancy introduces (quasi-)localized states for both σ and π electrons in graphene. Theoretically, interactions between the localized σ electrons and quasilocalized π electrons of a single-carbon vacancy in graphene are predicted to control its magnetism. However, experimentally confirming this prediction through manipulating the interactions remains an outstanding challenge. Here we report the manipulation of magnetism in the vicinity of an individual single-carbon vacancy in graphene by using a scanning tunnelling microscopy (STM) tip. Our spin-polarized STM measurements, complemented by density functional theory calculations, indicate that the interactions between the localized σ and quasilocalized π electrons could split the π electrons into two states with opposite spins even when they are well above the Fermi level. Via the STM tip, we successfully manipulate both the magnitude and direction of magnetic moment of the π electrons with respect to that of the σ electrons. Three different magnetic states of the single-carbon vacancy, exhibiting magnetic moments of about 1.6 μ, 0.5 μ, and 0 μ respectively, are realized in our experiment.
在石墨烯中创建一个单碳空位会为σ和π电子引入(准)局域态。从理论上讲,石墨烯中单个碳空位的局域σ电子和准局域π电子之间的相互作用预计会控制其磁性。然而,通过操纵这些相互作用在实验上证实这一预测仍然是一个突出的挑战。在此,我们报告了利用扫描隧道显微镜(STM)针尖对石墨烯中单个单碳空位附近的磁性进行操纵。我们的自旋极化STM测量结果,辅以密度泛函理论计算,表明即使局域σ电子和准局域π电子远高于费米能级,它们之间的相互作用也能将π电子分裂为具有相反自旋的两个态。通过STM针尖,我们成功地相对于σ电子的磁矩操纵了π电子磁矩的大小和方向。在我们的实验中实现了单碳空位的三种不同磁态,其磁矩分别约为1.6μ、0.5μ和0μ。