材料科学
钙钛矿(结构)
八面体
蓝移
量子产额
带隙
卤化物
发光二极管
量子效率
光致发光
光电子学
结晶学
晶体结构
光学
物理
化学
无机化学
荧光
作者
Guanwei Sun,Xinyan Liu,Zhe Liu,Denghui Liu,Fanyuan Meng,Zhenchao Li,Linghao Chu,Weidong Qiu,Xiaomei Peng,Wentao Xie,Chenyang Shen,Jiting Chen,Hin‐Lap Yip,Shi‐Jian Su
标识
DOI:10.1002/adfm.202106691
摘要
Abstract The band‐edge electronic structure of lead halide perovskites ( ABX 3 ) is composed of the orbitals of B and X components and can be tuned through the composition and structure of the BX 6 octahedron. Although A‐site cations do not directly contribute to near‐edge states, the bandgap of 3D metal halide perovskites can be affected by A‐cations through BX 6 octahedron tilting or lattice size variation. Here, as confirmed by the Rietveld refinement results of X‐ray diffraction characterization, the competition between lattice expansion and octahedral tilting is identified for the first time in emission wavelength tuning when introducing a large A‐site cation (C 2 H 5 NH 3 + , EA + ) into 1‐naphthylmethylammonium iodide‐passivated CsPbI 3 system. The former dominates spectral redshift, while the latter leads to a blueshift of emission peak, which broadens the way to tune the emission wavelength. In addition, excess cations can also passivate the perovskites, leading to a photoluminescence (PL) quantum yield as high as 61%, increased average PL lifetime of 74.7 ns, and a high radiative and non‐radiative recombination ratio of 15.7. Eventually, spectral‐stable deep‐red perovskite light‐emitting diode with a maximum external quantum efficiency of 17.5% is realized, which is one of the highest efficiencies without using any light outcoupling and anti‐solvent techniques.
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