Yb3+ speciation and energy-transfer dynamics in quantum-cutting Yb3+ -doped CsPbCl3 perovskite nanocrystals and single crystals

光致发光 材料科学 纳米晶 激发态 钙钛矿(结构) 量子点 纳米晶材料 化学物理 量子效率 光谱学 量子 光电子学 化学 纳米技术 原子物理学 物理 结晶学 量子力学
作者
Joo Yeon D. Roh,Matthew D. Smith,Matthew J. Crane,Daniel Biner,Tyler J. Milstein,Karl W. Krämer,Daniel R. Gamelin
出处
期刊:Cornell University - arXiv
标识
DOI:10.7892/boris.148071
摘要

Yb3+-doped inorganic metal-halide perovskites (Yb3+:CsPbX3, X = Cl, Br) have recently been discovered to display highly efficient quantum cutting, in which the energy from individual blue or UV photons absorbed by the material is re-emitted in the form of pairs of near-infrared photons by Yb3+ dopants. Experimental photoluminescence quantum yields approaching 200{%} have been reported. As the first quantum-cutting materials that combine such high photoluminescence quantum yields with strong, broadband absorption in the visible, these materials offer unique opportunities for enhancing the efficiencies of solar technologies. Little is known about the fundamental origins of this quantum cutting, however. Here, we describe variable-temperature and time-resolved photoluminescence studies of Yb3+:CsPbCl3 in two disparate forms - colloidal nanocrystals and macroscopic single crystals. Both forms show very similar spectroscopic properties, demonstrating that quantum cutting is an intrinsic property of the Yb3+:CsPbX3 composition itself. Diverse Yb3+ speciation is observed in both forms by low-temperature photoluminescence spectroscopy, but remarkably, quantum cutting is dominated by the same specific Yb3+ species in both cases. Time-resolved photoluminescence measurements provide direct evidence of the previously hypothesized intermediate state in the quantum-cutting mechanism. This intermediate state mediates relaxation from the photogenerated excited state of the perovskite to the emissive excited state of Yb3+, and hence is of critical mechanistic importance. At room temperature, this intermediate state is populated within a few picoseconds and has a decay time of only ~ 7 ns in both nanocrystalline and single-crystal Yb3+:CsPbCl3. The mechanistic implications of these observations are discussed.

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