材料科学
纳米线
兴奋剂
光电子学
原子探针
量子点
共发射极
相(物质)
发光二极管
表征(材料科学)
基质(水族馆)
晶体生长
透射电子显微镜
图层(电子)
壳体(结构)
Crystal(编程语言)
隧道枢纽
分子物理学
扫描电子显微镜
量子隧道
分析化学(期刊)
量子效率
Atom(片上系统)
扫描透射电子显微镜
量子阱
纳米技术
凝聚态物理
隧道效应
光致发光
增长率
量子
谱线
半最大全宽
岛屿生长
作者
Yoshiya Miyamoto,Weifang Lu,Naoki Sone,Renji Okuda,Kazuma Ito,Koji Okuno,Koichi Mizutani,Kazuyoshi Iida,Masaki Ohya,Motoaki Iwaya,Tetsuya Takeuchi,Satoshi Kamiyama,Isamu Akasaki
标识
DOI:10.1021/acsami.1c09591
摘要
Here, we systematically investigated the growth conditions of an n-GaN cap layer for nanowire-based light emitters with a tunnel junction. Selective-area growth of multiple quantum shell (MQS)/nanowire core-shell structures on a patterned n-GaN/sapphire substrate was performed by metal-organic vapor phase epitaxy, followed by the growth of a p-GaN, an n++/ p++-GaN tunnel junction, and an n-GaN cap layer. Specifically, two-step growth of the n-GaN cap layer was carried out under various growth conditions to determine the optimal conditions for a flat n-GaN cap layer. Scanning transmission electron microscopy characterization revealed that n++-GaN can be uniformly grown on the m-plane sidewall of MQS nanowires. A clear tunnel junction, involving 10-nm-thick p++-GaN and 3-nm-thick n++-GaN, was confirmed on the nonpolar m-planes of the nanowires. The Mg doping concentration and distribution profile of the p++-GaN shell were inspected using three-dimensional atom probe tomography. Afterward, the reconstructed isoconcentration mapping was applied to identify Mg-rich clusters. The density and average size of the Mg clusters were estimated to be approximately 4.3 × 1017 cm-3 and 5 nm, respectively. Excluding the Mg atoms contained in the clusters, the remaining Mg doping concentration in the p++-GaN region was calculated to be 1.1 × 1020 cm-3. Despite the lack of effective activation, a reasonably low operating voltage and distinct light emissions were preliminarily observed in MQS nanowire-based LEDs under the optimal n-GaN cap growth conditions. In the fabricated MQS-nanowire devices, carriers were injected into both the r-plane and m-plane of the nanowires without a clear quantum confinement Stark effect.
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