磁性衬底上石墨烯中的自旋依赖性 $π$$π^{\ast}$ 间隙

P. M. Sheverdyaeva, G. Bihlmayer, E. Cappelluti, D. Pacilé, F. Mazzola, N. Atodiresei, M. Jugovac, I. Grimaldi, G. Contini, A. K. Kundu, I. Vobornik, J. Fujii, P. Moras, C. Carbone, L. Ferrari
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引用次数: 0

摘要

我们详细分析了石墨烯/Eu/Ni(111)的电子特性。通过使用角度和自旋分辨光发射光谱以及 ab initio 计算,我们发现石墨烯/Eu/Ni(111)的 Eu 互掺恢复了 K 点的($/pi/pi^ast/$)狄拉克锥的近乎独立的分散性,同时由于石墨烯和 Eu 态的混合,额外地解除了自旋不均匀性。与磁性基底的相互作用导致了具有拓扑性质的狄拉克锥中的大自旋间隙,其特征是大贝里曲率和spin-polarized van Hove奇异性,其与费米级的接近性产生了极子带。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spin-dependent $π$$π^{\ast}$ gap in graphene on a magnetic substrate
We present a detailed analysis of the electronic properties of graphene/Eu/Ni(111). By using angle and spin-resolved photoemission spectroscopy and ab initio calculations, we show that the Eu-intercalation of graphene/Ni(111) restores the nearly freestanding dispersion of the $\pi\pi^\ast$ Dirac cones at the K point with an additional lifting of the spin degeneracy due to the mixing of graphene and Eu states. The interaction with the magnetic substrate results in a large spin-dependent gap in the Dirac cones with a topological nature characterized by a large Berry curvature, and a spin-polarized van Hove singularity, whose closeness to the Fermi level gives rise to a polaronic band.
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