2021
DOI: 10.1039/d0nr06448c
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Unveiling surface charge on chalcogen atoms toward the high aspect-ratio colloidal growth of two-dimensional transition metal chalcogenides

Abstract: The steric effects of the ligands unveil the charged chalcogen sites which are induced by the ligand adsorption, thus promoting the anisotropic growth of two-dimensional transition metal chalcogenides (TMCs).

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Cited by 2 publications
(2 citation statements)
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“…Additionally, Bi 2 Te 3 has a hetero-epitaxial alliance with crystalline graphene, as discussed previously. In the next step, Sb and Te were introduced and Sb 2 Te 3 starts nucleating at the edge of the Bi 2 Te 3 and also on the graphene and grows laterally (figure 6(b)) plausibly because the edge facets have higher binding energy than that of basal {0001} [36][37][38]. In order to avoid any alloy formation between Bi and Sb, the substrate temperature was reduced by ∼25 • C. To grow lateral heterostructure, it is essential to nucleate the 2nd material successively at the edge of the 1st material [12,39]; the side edge atoms of Bi 2 Te 3 serve as nucleation sites for the Sb 2 Te 3 .…”
Section: Resultsmentioning
confidence: 99%
“…Additionally, Bi 2 Te 3 has a hetero-epitaxial alliance with crystalline graphene, as discussed previously. In the next step, Sb and Te were introduced and Sb 2 Te 3 starts nucleating at the edge of the Bi 2 Te 3 and also on the graphene and grows laterally (figure 6(b)) plausibly because the edge facets have higher binding energy than that of basal {0001} [36][37][38]. In order to avoid any alloy formation between Bi and Sb, the substrate temperature was reduced by ∼25 • C. To grow lateral heterostructure, it is essential to nucleate the 2nd material successively at the edge of the 1st material [12,39]; the side edge atoms of Bi 2 Te 3 serve as nucleation sites for the Sb 2 Te 3 .…”
Section: Resultsmentioning
confidence: 99%
“…However, before moving on to the analysis of the excitation of surface modes with a slow particle under oblique incidence, it is important to emphasize the rich variety of the topology of the surface modes in anisotropic 2D materials. [79][80][81][82] Namely, one may further refer to the azimuthal dependence of the excited modes (see also eqn (4) in ref. 79 and the discussion thereafter) and conclude the alteration of the transmitted and reflected waves (e.g.…”
Section: And 3 Below and Fig S2 In The Esi †)mentioning
confidence: 99%