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Long-Lived Dark Exciton Emission in Mn-Doped CsPbCl(3) Perovskite Nanocrystals

[Image: see text] The unusual temperature dependence of exciton emission decay in CsPbX(3) perovskite nanocrystals (NCs) attracts considerable attention. Upon cooling, extremely short (sub-ns) lifetimes were observed and were explained by an inverted bright–dark state splitting. Here, we report temp...

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Detalles Bibliográficos
Autores principales: Xu, Kunyuan, Vliem, Jara F., Meijerink, Andries
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2018
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6410607/
https://www.ncbi.nlm.nih.gov/pubmed/30873253
http://dx.doi.org/10.1021/acs.jpcc.8b12035
Descripción
Sumario:[Image: see text] The unusual temperature dependence of exciton emission decay in CsPbX(3) perovskite nanocrystals (NCs) attracts considerable attention. Upon cooling, extremely short (sub-ns) lifetimes were observed and were explained by an inverted bright–dark state splitting. Here, we report temperature-dependent exciton lifetimes for CsPbCl(3) NCs doped with 0–41% Mn(2+). The exciton emission lifetime increases upon cooling from 300 to 75 K. Upon further cooling, a strong and fast sub-ns decay component develops. However, the decay is strongly biexponential and also a weak, slow decay component is observed with a ∼40–50 ns lifetime below 20 K. The slow component has a ∼5–10 times stronger relative intensity in Mn-doped NCs compared to that in undoped CsPbCl(3) NCs. The temperature dependence of the slow component resembles that of CdSe and PbSe quantum dots with an activation energy of ∼19 meV for the dark–bright state splitting. Based on our observations, we propose an alternative explanation for the short, sub-ns exciton decay time in CsPbX(3) NCs. Slow bright–dark state relaxation at cryogenic temperatures gives rise to almost exclusively bright state emission. Incorporation of Mn(2+) or high magnetic fields enhances the bright–dark state relaxation and allows for the observation of the long-lived dark state emission at cryogenic temperatures.