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卤化物钙钛矿纳米片材中的暗激子和亮激子

Dark and Bright Excitons in Halide Perovskite Nanoplatelets.

作者信息

Gramlich Moritz, Swift Michael W, Lampe Carola, Lyons John L, Döblinger Markus, Efros Alexander L, Sercel Peter C, Urban Alexander S

机构信息

Nanospectroscopy Group, Nano-Institute Munich, Department of Physics, Ludwig-Maximilians-Universität München (LMU), Munich, 80539, Germany.

Center for Computational Materials Science, U.S. Naval Research Laboratory, Washington D.C., 20375, USA.

出版信息

Adv Sci (Weinh). 2022 Feb;9(5):e2103013. doi: 10.1002/advs.202103013. Epub 2021 Dec 23.

DOI:10.1002/advs.202103013
PMID:34939751
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8844578/
Abstract

Semiconductor nanoplatelets (NPLs), with their large exciton binding energy, narrow photoluminescence (PL), and absence of dielectric screening for photons emitted normal to the NPL surface, could be expected to become the fastest luminophores amongst all colloidal nanostructures. However, super-fast emission is suppressed by a dark (optically passive) exciton ground state, substantially split from a higher-lying bright (optically active) state. Here, the exciton fine structure in 2-8 monolayer (ML) thick Cs Pb Br NPLs is revealed by merging temperature-resolved PL spectra and time-resolved PL decay with an effective mass model taking quantum confinement and dielectric confinement anisotropy into account. This approach exposes a thickness-dependent bright-dark exciton splitting reaching 32.3 meV for the 2 ML NPLs. The model also reveals a 5-16 meV splitting of the bright exciton states with transition dipoles polarized parallel and perpendicular to the NPL surfaces, the order of which is reversed for the thinnest NPLs, as confirmed by TR-PL measurements. Accordingly, the individual bright states must be taken into account, while the dark exciton state strongly affects the optical properties of the thinnest NPLs even at room temperature. Significantly, the derived model can be generalized for any isotropically or anisotropically confined nanostructure.

摘要

半导体纳米片(NPLs)具有较大的激子结合能、窄的光致发光(PL)以及对于垂直于NPL表面发射的光子不存在介电屏蔽,有望成为所有胶体纳米结构中发光最快的发光体。然而,超快发射受到暗(光学无源)激子基态的抑制,该基态与较高能态的亮(光学有源)态有很大的分裂。在此,通过将温度分辨PL光谱和时间分辨PL衰减与考虑量子限制和介电限制各向异性的有效质量模型相结合,揭示了2 - 8个单层(ML)厚的Cs Pb Br NPLs中的激子精细结构。这种方法揭示了厚度依赖的亮 - 暗激子分裂,对于2 ML的NPLs,分裂达到32.3 meV。该模型还揭示了亮激子态在跃迁偶极矩平行和垂直于NPL表面时存在5 - 16 meV的分裂,如时间分辨PL测量所证实的,对于最薄的NPLs,其顺序相反。因此,必须考虑各个亮态,而暗激子态即使在室温下也会强烈影响最薄NPLs的光学性质。值得注意的是,所推导的模型可以推广到任何各向同性或各向异性限制的纳米结构。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/f1ccd3da7216/ADVS-9-2103013-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/950a6bc5d5c8/ADVS-9-2103013-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/16d9498fd56e/ADVS-9-2103013-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/d7ccf12752a3/ADVS-9-2103013-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/f1ccd3da7216/ADVS-9-2103013-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/950a6bc5d5c8/ADVS-9-2103013-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/16d9498fd56e/ADVS-9-2103013-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/d7ccf12752a3/ADVS-9-2103013-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9d1b/8844578/f1ccd3da7216/ADVS-9-2103013-g002.jpg

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