化学
量子点
离域电子
光致发光
量子产额
光电子学
自发辐射
存水弯(水管)
暗状态
分子物理学
热的
量子
产量(工程)
电子
重组
宽带
芯(光纤)
荧光
物理
量子效率
激发态
原子物理学
热平衡
联轴节(管道)
光子学
发光
发光二极管
作者
Jiakuan Zhang,Peipei Jin,Boyi Xu,Jing Wang,Jiongzhao Li,Xing Lin,Haiyan Qin,Haiming Zhu,Xiaogang Peng
摘要
Abstract Broadband emission from single quantum dot (QD) inherently relies on localized states that are conventionally regarded as nonradiative trap manifolds and suffer from low synthetic reproducibility. Here we show that photogenerated holes in a AgInxGa1–xS2/ZnS core/shell QD can be controllably partitioned into two parallel, kinetically isolated, and nonthermalized localized states, each of which then radiatively recombines with the delocalized electron with distinct formation and recombination kinetics. The high-energy and low-energy photoluminescence (PL) peaks are related to a small-polaron-like state in the core and a manifold of trap states near the core–shell boundary, respectively. The nonequilibrated dual-state architecture yields composition-tunable and ultrabroad emission with a PL full width at half maximum (fwhm) of 120–130 nm, near-unity quantum yield (QY), negligible Urbach tail, and robust operation under thermal and optical stress. Integrated with a blue GaN chip, a single type of QD produces efficient and stable warm-white light with a wall-plug efficiency as ∼150 lm W–1 and an electron-to-photon QY > 50%. Our results indicate localized states should be revisited as a valid paradigm for optoelectronic QD materials.
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