2020
DOI: 10.1021/acs.jpclett.0c01713
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Strain Effects of Vertical Separation and Horizontal Sliding in Commensurate Two-Dimensional Homojunctions

Abstract: Strain, as an economic yet controllable approach for structural modulation, frequently plays a vital role in the preparation and performance optimization of two-dimensional nanomaterials (TNMs). Here, utilizing first-principles simulations, the analysis of energetics shows that the biaxial stretching and compressing could facilitate the vertical separation and horizontal sliding in graphene (Gr/Gr), hexagonal boron nitride (h-BN/h-BN), and molybdenum disulfide (MoS2/MoS2) bilayers. The quantification of electr… Show more

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Cited by 13 publications
(15 citation statements)
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“…The sensitivities of interlayer electron density of top and hollow stackings to normal pressure are dissimilar, and the fluctuation of interlayer electron density Δρ diff is monotonically increasing. [ 11 ] This augmentation of Δρ diff means that the relative potential Δ V , which reflects the strength of interlayer coupling, is monotonic. Hence, accompanied by the monotonic increase of the load‐driven Δρ diff , the relative size of sliding energy barriers Δ V between the top and hollow stackings is reversed as normal pressure increases.…”
Section: Resultsmentioning
confidence: 99%
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“…The sensitivities of interlayer electron density of top and hollow stackings to normal pressure are dissimilar, and the fluctuation of interlayer electron density Δρ diff is monotonically increasing. [ 11 ] This augmentation of Δρ diff means that the relative potential Δ V , which reflects the strength of interlayer coupling, is monotonic. Hence, accompanied by the monotonic increase of the load‐driven Δρ diff , the relative size of sliding energy barriers Δ V between the top and hollow stackings is reversed as normal pressure increases.…”
Section: Resultsmentioning
confidence: 99%
“…where ρ Bilayer (x,y, z) indicates the electron density distribution of the bilayers, ρ Top (x,y, z) and ρ Bottom (x,y, z) represent the respective electron density distributions of the isolated top and bottom layers. To further quantify the redistribution of electrons, the distribution curve of charge density perpendicular to the atomic layer ρ(z) is estimated by: [11,30] z ab dy x y z dx b a 1 , ,…”
Section: Methodsmentioning
confidence: 99%
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