2019
DOI: 10.1002/smll.201805145
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Electronic Doping Controlled Migration of Dislocations in Polycrystalline 2D WS2

Abstract: Migration of dislocations not only determines the durability of large‐scale nanoelectronic and opto‐electronic devices based on polycrystalline 2D transition‐metal dichalcogenides (TMDCs), but also plays an important role in enhancing the performance of novel memristors. However, a fundamental question of the migration dependence on the electronic effects, which are inevitable in practical field‐effect transistors based on 2D TMDCs, and its interplay with different dislocations, remains unexplored. Here, takin… Show more

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Cited by 4 publications
(2 citation statements)
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“…Atomic vacancies often induce the reconstruction of the surrounding atoms, which then make the band structures much more complicated such as augmented midgap states. 191 The removal of the MX n units can give rise to enormous transformations of M-X bonds around the atomic vacancies, contributing to the migration of various Fermi levels. 189 In the case of metallic TMDs, atomic vacancies have little impact on their physical behaviour though they induce localized states.…”
Section: Property Transformationsmentioning
confidence: 99%
“…Atomic vacancies often induce the reconstruction of the surrounding atoms, which then make the band structures much more complicated such as augmented midgap states. 191 The removal of the MX n units can give rise to enormous transformations of M-X bonds around the atomic vacancies, contributing to the migration of various Fermi levels. 189 In the case of metallic TMDs, atomic vacancies have little impact on their physical behaviour though they induce localized states.…”
Section: Property Transformationsmentioning
confidence: 99%
“…Tungsten is the heaviest transition metal, and its association with sulfur atoms, forming tungsten disulfide (WS 2 ) in the family of common TMDs, became an emerging 2D nanomaterial. Layered WS 2 is composed of a strong particle covalent bond (S–W) and a weak van der Waals force with an interlayer spacing of 0.7 nm. WS 2 has a P63/mmc hexagonal crystal layer and at room temperature, the stability of the WS 2 structure is due to the strong S–W–S covalent bonds. It has a low bandgap that can change from an indirect bandgap (1.3 eV) to a direct and higher bandgap (∼2 eV) when the thickness approaches the monolayer . The band gap energy can be controlled by the number of layers, which confers to WS 2 nanomaterial's great application potential in the field of optics. , The antibacterial activities of WS 2 nanosheets against two representative bacterial strains, Gram-negative Escherichia coli and Gram-positive Staphylococcus aureus, were evaluated by colony-forming unit (CFU) studies .…”
Section: Introductionmentioning
confidence: 99%