State Key Laboratory of Mechanics and Control of Mechanical Structures, and Institute of Nano Science, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China.
Phys Chem Chem Phys. 2012 Oct 5;14(37):13035-40. doi: 10.1039/c2cp42181j. Epub 2012 Aug 21.
We investigate the strain-dependent electronic and magnetic properties of two-dimensional (2D) monolayer and bilayer MoS(2), as well as 1D MoS(2) nanoribbons and nanotubes using first-principles calculations. For 2D monolayer MoS(2) subjected to isotropic or uniaxial tensile strain, the direct band gap of MoS(2) changes to an indirect gap that decreases monotonically with increasing strain; while under the compressive strain, the original direct band gap is enlarged first, followed by gap reduction when the strain is beyond -2%. The effect of isotropic strain is even stronger than that of uniaxial strain. For bilayer MoS(2) subjected to isotropic tensile strain, its indirect gap reduces monotonically to zero at strain about 6%; while under the isotropic compressive strain, its indirect gap increases first and then reduces and turns into direct gap when the strain is beyond -4%. For strained 1D metallic zigzag MoS(2) nanoribbons, the net magnetic moment increases slightly with axial strain from about -5% to 5%, but drops to zero when the compressive strain is beyond -5% or increases with a power law beyond 5%. For 1D armchair MoS(2) nanotubes, tensile or compressive axial strain reduces or enlarges the band gap linearly, and the gap can be fully closed for nanotubes with relatively small diameter or under large tensile strain. For zigzag MoS(2) nanotubes, the strain effect becomes nonlinear and the tensile strain can reduce the band gap, whereas compressive strain can initially enlarge the band gap and then decrease it. The strain induced change in projected orbitals energy of Mo and the coupling between the Mo atom d orbital and the S atom p orbital are analyzed to explain the strong strain effect on the band gap and magnetic properties.
我们使用第一性原理计算研究了二维(2D)单层和双层 MoS2 以及 1D MoS2 纳米带和纳米管的应变依赖性电子和磁性。对于二维单层 MoS2,无论是受到各向同性应变还是单轴拉伸应变,MoS2 的直接带隙都会变为间接带隙,且随应变的增加而单调减小;而在压缩应变下,原始直接带隙首先增大,当应变超过-2%时,带隙减小。各向同性应变的影响甚至比单轴应变更强。对于各向同性拉伸应变的双层 MoS2,其间接带隙单调减小到零,应变约为 6%;而在各向同性压缩应变下,其间接带隙先增大后减小,并在应变超过-4%时变为直接带隙。对于受应变的 1D 锯齿状 MoS2 纳米带,轴向应变从约-5%增加到 5%时,净磁矩略有增加,但当压缩应变超过-5%时,磁矩降为零,或者以幂次律增加超过 5%。对于 1D 扶手椅 MoS2 纳米管,拉伸或压缩轴向应变线性减小或增大带隙,对于直径较小或拉伸应变较大的纳米管,带隙可以完全关闭。对于锯齿状 MoS2 纳米管,应变效应变得非线性,拉伸应变可以减小带隙,而压缩应变可以初始增大带隙,然后减小带隙。分析了 Mo 的投影轨道能量与 Mo 原子 d 轨道和 S 原子 p 轨道之间的耦合的应变诱导变化,以解释带隙和磁性对应变的强烈影响。