2022
DOI: 10.1007/s12274-022-5190-9
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Thermal stability of Te nanowires and their crystallography-determined surface evolution at elevated temperatures

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Cited by 3 publications
(1 citation statement)
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“…This is quite different from the type-ii and type-iii nanosheets where the {101̅ 0} surfaces are the outer exposure surfaces. Because the surface energy of the {112̅ 0} free surfaces (∼0.36 J/m 2 ) is significantly higher than that of the {101̅ 0} surfaces (∼0.08 J/ m 2 ), 38,39 this discrepancy in surface energy may be one of the critical influencing factors why such crossed nanowires will not turn into nanosheets. As illustrated in Figure 4c, the priority of exposing low-energy surfaces obviously prefers the prism structure, where the outer surfaces are enclosed with {101̅ 0} surfaces.…”
Section: Resultsmentioning
confidence: 99%
“…This is quite different from the type-ii and type-iii nanosheets where the {101̅ 0} surfaces are the outer exposure surfaces. Because the surface energy of the {112̅ 0} free surfaces (∼0.36 J/m 2 ) is significantly higher than that of the {101̅ 0} surfaces (∼0.08 J/ m 2 ), 38,39 this discrepancy in surface energy may be one of the critical influencing factors why such crossed nanowires will not turn into nanosheets. As illustrated in Figure 4c, the priority of exposing low-energy surfaces obviously prefers the prism structure, where the outer surfaces are enclosed with {101̅ 0} surfaces.…”
Section: Resultsmentioning
confidence: 99%