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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...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Association for the Advancement of Science
2021
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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 |
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. |
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