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Giant edge state splitting at atomically precise graphene zigzag edges

机译:原子精确石墨烯之字形边缘处的巨型边缘状态分裂

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摘要

Zigzag edges of graphene nanostructures host localized electronic states that are predicted to be spin-polarized. However, these edge states are highly susceptible to edge roughness and interaction with a supporting substrate, complicating the study of their intrinsic electronic and magnetic structure. Here, we focus on atomically precise graphene nanoribbons whose two short zigzag edges host exactly one localized electron each. Using the tip of a scanning tunnelling microscope, the graphene nanoribbons are transferred from the metallic growth substrate onto insulating islands of NaCl in order to decouple their electronic structure from the metal. The absence of charge transfer and hybridization with the substrate is confirmed by scanning tunnelling spectroscopy, which reveals a pair of occupied/unoccupied edge states. Their large energy splitting of 1.9 eV is in accordance with ab initio many-body perturbation theory calculations and reflects the dominant role of electron–electron interactions in these localized states.
机译:石墨烯纳米结构的之字形边缘具有预测为自旋极化的局部电子态。然而,这些边缘状态极易受到边缘粗糙度和与支撑衬底的相互作用的影响,这使得对其固有的电子和磁性结构的研究变得复杂。在这里,我们专注于原子精确的石墨烯纳米带,其两个短的锯齿形边缘分别恰好承载一个局部电子。使用扫描隧道显微镜的尖端,将石墨烯纳米带从金属生长基质转移到NaCl绝缘岛上,以使它们的电子结构与金属分离。通过扫描隧道光谱法确认不存在电荷转移和与底物的杂化,其揭示了一对占据/未占据的边缘状态。它们的1.9 eV的大能量分裂符合从头算起的多体微扰理论计算,反映了在这些局部状态下电子与电子相互作用的主要作用。

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