2020
DOI: 10.1088/1361-6528/ab6bf2
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Selective area formation of GaN nanowires on GaN substrates by the use of amorphous Al x O y nucleation layer

Abstract: Examples are presented that application of amorphous Al x O y nucleation layer is an efficient way of controlling spatial distribution of GaN nanowires grown by plasma-assisted molecular beam epitaxy. On GaN/sapphire substrates Al x O y stripes induce formation of GaN nanowires while a compact GaN layer is formed outside the stripes. We show that the rati… Show more

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Cited by 10 publications
(8 citation statements)
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“…Recently, there is an increasing interest in the application of amorphous AlO y films deposited by ALD as nucleation layers for the PAMBE growth of GaN nanostructures. Such buffers effectively induce selective area formation of GaN NWs on sapphire [33] and GaN [69,70]. As shown in previous studies [34,41,71,72], AlO y buffer layers significantly enhance the nucleation rate of GaN with respect to nitridated Si without a loss of structural and optical quality [34].…”
Section: Resultsmentioning
confidence: 52%
“…Recently, there is an increasing interest in the application of amorphous AlO y films deposited by ALD as nucleation layers for the PAMBE growth of GaN nanostructures. Such buffers effectively induce selective area formation of GaN NWs on sapphire [33] and GaN [69,70]. As shown in previous studies [34,41,71,72], AlO y buffer layers significantly enhance the nucleation rate of GaN with respect to nitridated Si without a loss of structural and optical quality [34].…”
Section: Resultsmentioning
confidence: 52%
“…As discussed above, this nonuniformity initially originates from the diffusion barrier which prevents Ga diffusion onto the mask surface and is further enhanced by nucleation and growth of GaN islands and NWs within the stripe. According to ref , MBE growth of GaN NWs on Al x O y layers on Si(111) involves very long nucleation times which are required to nucleate the first GaN islands from which the NW growth subsequently starts. ,,,, Nucleation of GaN islands is limited by the kinetics of Ga adatoms. ,,,, Difficult nucleation is observed when DσN 0 t des ≪ 1, where D is the diffusion coefficient of Ga adatoms on a-Al x O y , σ as the capture coefficient, N 0 is the surface concentration of nucleation centers, and t des is the mean stay time of Ga adatom on the surface before desorption. Under such conditions, formation of GaN islands occurs in the incomplete condensation regime, and most probably by heterogeneous nucleation .…”
Section: Modelingmentioning
confidence: 99%
“…It is remarkable that the whole set of data can be reasonably fitted with the same parameters, including the Ga diffusion length λ on a-Al x O y of 600 nm. This value nicely correlates with the one of ref , where it was roughly estimated at 500 nm. As for the Ga diffusion length on SiN x (λ 0 ), it equals to approximately 1000–1100 nm from λ 0 /λ = 1.7–1.9.…”
Section: Modelingmentioning
confidence: 99%
See 1 more Smart Citation
“…4,6,7 Recently there is an increasing interest in application of amorphous AlO x lms grown by ALD as nucleation layers for plasma-assisted molecular beam epitaxy (PAMBE) of GaN nanostructures. Such buffers effectively induce catalyst-free nucleation of GaN nanowires on sapphire 8 and GaN 9 substrates. As shown in previous studies, [10][11][12][13] AlO x buffer layers signicantly enhance the nucleation rate of GaN with respect to nitridated Si (the most common substrate for growing GaN nanowires), without loss of structural and optical properties.…”
Section: Introductionmentioning
confidence: 99%