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Electronic and magnetic properties of H-terminated graphene nanoribbons deposited on the topological insulator Sb2Te3

机译:沉积在拓扑绝缘体Sb2Te3上的H末端石墨烯纳米带的电子和磁性

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摘要

Magnetism in zigzag graphene nanoribbons (GNRs) has received enormous attention recently, due to the one-dimensional nature of this phenomenon, as well as its potential applications in the field of spintronics. In this work, we present a density functional theory (DFT) investigation of H-passivated GNRs on the (111) surface of the topological insulator Sb2Te3. We show that the chemical interaction between the GNR and the substrate is weak. As a result, the GNR-surface distance is large, of the order of 3.4 Angstrom, doping effects are almost negligible, and the mean-field magnetic properties of the GNR are preserved. Nevertheless, the presence of the substrate affects significantly the magnitude of the exchange coupling constants between the edges. Although our DFT calculations do not properly describe quantum fluctuations that destabilize the edge magnetism in free-standing GNRs, they provide important information about the stabilizing mechanisms which originate from the substrate-induced spin orbit coupling and the decoherence effects due to the surface states of Sb2Te3. We argue that, owing to these mechanisms, Sb2Te3 may be a suitable substrate to investigate experimentally the transition from “quantum” to “classical” magnetism in GNRs.
机译:由于这种现象的一维性质及其在自旋电子学领域的潜在应用,锯齿形石墨烯纳米带(GNR)中的磁性最近受到了极大的关注。在这项工作中,我们提出了在拓扑绝缘子Sb2Te3(111)表面上H钝化GNR的密度泛函理论(DFT)研究。我们表明,GNR和底物之间的化学相互作用很弱。结果,GNR的表面距离大,约为3.4埃,掺杂效应几乎可以忽略不计,并且保留了GNR的平均场磁性能。然而,基板的存在显着影响边缘之间的交换耦合常数的大小。尽管我们的DFT计算未能正确描述使独立式GNR中的边缘磁性不稳定的量子涨落,但它们提供了有关稳定机理的重要信息,这些稳定机理源于基质诱导的自旋轨道耦合以及Sb2Te3的表面态引起的去相干效应。我们认为,由于这些机制,Sb2Te3可能是研究GNRs从“量子”到“经典”磁性跃迁的合适底物。

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