2024
DOI: 10.1021/acs.nanolett.4c00453
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Room-Temperature Ferroelectric Epitaxial Nanowire Arrays with Photoluminescence

Han K. D. Le,
Ye Zhang,
Piush Behera
et al.

Abstract: The development of large-scale, high-quality ferroelectric semiconductor nanowire arrays with interesting light-emitting properties can address limitations in traditional wide-bandgap ferroelectrics, thus serving as building blocks for innovative device architectures and next-generation high-density optoelectronics. Here, we investigate the optical properties of ferroelectric CsGeX 3 (X = Br, I) halide perovskite nanowires that are epitaxially grown on muscovite mica substrates by vapor phase deposition. Detai… Show more

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“…Initially, when the precursor of CdS reaches the mica surface, it prefers to nucleate at the sites with higher energy on mica to reduce the system energy, which results in the early-stage formation of CdS nanosheets that have a relatively larger thickness due to the longer growth time (see the brighter sheets in Figure b and steps 1 and 2 schematically shown in Figure e). Because the surface nonuniformity of mica is usually resulted from the nonuniform distribution of K + ions formed when it is cleaved, the surface energy difference of various sites should be small. , With the time extension, therefore, the growth of the early formed sheets and the formation of new ones can simultaneously take place, which leads to the different thickness sheets (see the darker sheets in Figure b and step 3 schematically shown in Figure e). Interestingly, the sheets formed at both stages have the same lateral growth orientation, which indicates an identical growth mechanism.…”
Section: Resultsmentioning
confidence: 99%
“…Initially, when the precursor of CdS reaches the mica surface, it prefers to nucleate at the sites with higher energy on mica to reduce the system energy, which results in the early-stage formation of CdS nanosheets that have a relatively larger thickness due to the longer growth time (see the brighter sheets in Figure b and steps 1 and 2 schematically shown in Figure e). Because the surface nonuniformity of mica is usually resulted from the nonuniform distribution of K + ions formed when it is cleaved, the surface energy difference of various sites should be small. , With the time extension, therefore, the growth of the early formed sheets and the formation of new ones can simultaneously take place, which leads to the different thickness sheets (see the darker sheets in Figure b and step 3 schematically shown in Figure e). Interestingly, the sheets formed at both stages have the same lateral growth orientation, which indicates an identical growth mechanism.…”
Section: Resultsmentioning
confidence: 99%