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Formation of quantum spin Hall state on Si surface and energy gap scaling with strength of spin orbit coupling

机译:si表面和能隙上量子自旋霍尔态的形成   用自旋轨道耦合强度缩放

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摘要

For potential applications in spintronics and quantum computing, it isdesirable to place a quantum spin Hall insulator [i.e., a 2D topologicalinsulator (TI)] on a substrate while maintaining a large energy gap. Here, wedemonstrate a unique approach to create the large-gap 2D TI state on asemiconductor surface, based on first-principles calculations and effectiveHamiltonian analysis. We show that when heavy elements with strong spin orbitcoupling (SOC) such as Bi and Pb atoms are deposited on a patterned H-Si(111)surface into a hexagonal lattice, they exhibit a 2D TI state with a largeenergy gap of over 0.5 eV. The TI state arises from an intriguing substrateorbital filtering effect that selects a suitable orbital composition around theFermi level, so that the system can be matched onto a four-band effective modelHamiltonian. Furthermore, it is found that within this model, the SOC gap doesnot increase monotonically with the increasing strength of SOC. Theseinteresting results may shed new light in future design and fabrication oflarge-gap topological quantum states.
机译:对于自旋电子学和量子计算中的潜在应用,期望在保持大的能隙的同时将量子自旋霍尔绝缘体[即,2D拓扑绝缘体(TI)]放置在基板上。在这里,我们展示了一种基于第一性原理计算和有效哈密顿分析的独特方法,可以在半导体表面上创建大间隙2D TI状态。我们显示,当具有强自旋轨道耦合(SOC)的重元素(例如Bi和Pb原子)沉积在带图案的H-Si(111)表面上形成六方晶格时,它们会显示2D TI状态,且能隙大于0.5 eV 。 TI状态是由有趣的底物轨道滤波效应产生的,该效应选择了费米能级附近的合适轨道组成,因此该系统可与四频带有效汉密尔顿模型匹配。此外,发现在该模型内,SOC间隙不会随着SOC强度的增加而单调增加。这些有趣的结果可能为未来的大间隙拓扑量子态的设计和制造提供新的思路。

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