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过渡金属二硫属化物二维面内异质结构中的应变电子学

Straintronics in two-dimensional in-plane heterostructures of transition-metal dichalcogenides.

作者信息

Wei Wei, Dai Ying, Huang Baibiao

机构信息

School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China.

出版信息

Phys Chem Chem Phys. 2016 Dec 21;19(1):663-672. doi: 10.1039/c6cp07823k.

DOI:10.1039/c6cp07823k
PMID:27918042
Abstract

For in-plane heterostructures between 2D transition-metal dichalcogenides (TMDs), namely, MoSe/MoS, MoS/MoSe, WSe/MoS and MoS/WSe, intrinsic strain can be introduced resulting from lattice mismatch between two constituents, which significantly influences electronic properties (straintronics). Intrinsic strain can reduce or decrease the coupling strength between nonmetal p and metal d orbitals, and therefore modifies the splitting between bonding and antibonding states at the high-symmetry k-points. In this case, relative upward or downward shift of band edge at specific k-points leads to band gap reduction or enhancement and the indirect-direct band gap transition. Upon consideration of spin-orbit coupling (SOC) effects, energy splitting in valence bands will further shift the band edge at a specific k-point, and changes the band gap nature, such as indirect-direct band gap transition. It is of interest that intense states hybridization exists within the interline region, and therefore band alignments for in-plane heterostructures of 2D TMDs should be reconsidered, which is crucial for transport and optical features. In addition, states hybridization plays a role in the amplitude of band edge shift since individual 2D TMDs present different resistance to the strain. However, we found that intrinsic strain has no effects on the SOC-induced energy splitting in valence bands of these in-plane heterostructures, while the extent of states hybridization determines the magnitude of energy splitting. In addition, charge transfer across the interline also has effects on the band gap. In the presence of strain, the bonding strength of two 2D TMDs is reduced.

摘要

对于二维过渡金属二硫属化物(TMDs)之间的面内异质结构,即MoSe/MoS、MoS/MoSe、WSe/MoS和MoS/WSe,由于两种组分之间的晶格失配会引入本征应变,这会显著影响电子性质(应变电子学)。本征应变会降低或减小非金属p轨道和金属d轨道之间的耦合强度,从而改变高对称k点处成键态和反键态之间的分裂。在这种情况下,特定k点处带边的相对向上或向下移动会导致带隙减小或增大以及间接-直接带隙转变。考虑自旋轨道耦合(SOC)效应时,价带中的能量分裂会进一步使特定k点处的带边移动,并改变带隙性质,例如间接-直接带隙转变。有趣的是,在界面区域内存在强烈的态杂化,因此二维TMDs面内异质结构的能带排列应重新考虑,这对输运和光学特性至关重要。此外,由于单个二维TMDs对应变的抵抗力不同,态杂化在带边移动的幅度中起作用。然而,我们发现本征应变对这些面内异质结构价带中SOC诱导的能量分裂没有影响,而态杂化程度决定了能量分裂的大小。此外,跨界面的电荷转移也会对带隙产生影响。在存在应变的情况下,两个二维TMDs的结合强度会降低。

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