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Ultrabright Au@Cu(14) nanoclusters: 71.3% phosphorescence quantum yield in non-degassed solution at room temperature

The photoluminescence of metal nanoclusters is typically low, and phosphorescence emission is rare due to ultrafast free-electron dynamics and quenching by phonons. Here, we report an electronic engineering approach to achieving very high phosphorescence (quantum yield 71.3%) from a [Au@Cu(14)(SPh(t...

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Detalles Bibliográficos
Autores principales: Song, Yongbo, Li, Yingwei, Zhou, Meng, Liu, Xuan, Li, Hao, Wang, He, Shen, Yuhua, Zhu, Manzhou, Jin, Rongchao
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7787487/
https://www.ncbi.nlm.nih.gov/pubmed/33523969
http://dx.doi.org/10.1126/sciadv.abd2091
Descripción
Sumario:The photoluminescence of metal nanoclusters is typically low, and phosphorescence emission is rare due to ultrafast free-electron dynamics and quenching by phonons. Here, we report an electronic engineering approach to achieving very high phosphorescence (quantum yield 71.3%) from a [Au@Cu(14)(SPh(t)Bu)(12)(PPh(C(2)H(4)CN)(2))(6)](+) nanocluster (abbreviated Au@Cu(14)) in non-degassed solution at room temperature. The structure of Au@Cu(14) has a single-Au-atom kernel, which is encapsulated by a rigid Cu(I) complex cage. This core-shell structure leads to highly efficient singlet-to-triplet intersystem crossing and suppression of nonradiative energy loss. Unlike the phosphorescent organic materials and organometallic complexes—which require de-aerated conditions due to severe quenching by air (i.e., O(2))—the phosphorescence from Au@Cu(14) is much less sensitive to air, which is important for lighting and biomedical applications.