材料科学
光致发光
纳米晶材料
光电子学
基质(水族馆)
波长
蓝移
纳米晶
绿灯
红灯
薄膜
航程(航空)
光学
发射光谱
红移
增长率
纳米技术
红色
可见光谱
纳米结构
电流密度
发射强度
场电子发射
受激发射
句号(音乐)
放大自发辐射
宽禁带半导体
作者
K. Hoshino,Rie Togashi,Katsumi Kishino
标识
DOI:10.1002/pssa.202500261
摘要
Using nanotemplate selective‐area growth methods, InGaN/GaN nanocolumn arrays with bulk‐InGaN active layers are fabricated on AlN/Si(111) substrates by varying the nanocolumn period ( L = 200–400 nm) and InGaN growth time ( t InGaN = 5–20 min). For t InGaN = 12 and 20 min, the photoluminescence emission peak wavelength ( λ ) increases with L . Red emission is observed over a wide range of L (220–300 nm) at t InGaN = 12 min, and the emission color shifts from green to red at t InGaN = 20 min as L increases from 200 to 320 nm. In contrast, for t InGaN = 5 and 8 min, λ shifts toward shorter wavelengths with increasing L . Specifically, at t InGaN = 8 min, three distinct emission regions—red, green, and blue—are achieved within the bulk InGaN, with the emission switching from red to green to blue as L increases, where high‐purity red ( λ = 622 nm), green (544 nm), and blue (477 nm) emissions are obtained for L = 200, 300, and 400 nm, respectively. Notably, red–green–blue‐emitting nanocolumn arrays are achieved in a single‐growth process, with red emission realized even in thin nanocolumns where the nanocrystalline effect is pronounced.
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