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Excited-State Dynamics of Crossing-Controlled Energy Transfer in Europium Complexes

[Image: see text] Photosensitized energy transfer (EnT) phenomena occur frequently in a variety of photophysical and photochemical processes and have traditionally been treated with the donor–acceptor distance-dependent Förster and Dexter models. However, incorrect arguments and formulae were employ...

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Detalles Bibliográficos
Autores principales: Wu, Liangliang, Fang, Yu, Zuo, Wanlong, Wang, Juanjuan, Wang, Ju, Wang, Shufeng, Cui, Zhifeng, Fang, Weihai, Sun, Hao-Ling, Li, Yunliang, Chen, Xuebo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9088298/
https://www.ncbi.nlm.nih.gov/pubmed/35557757
http://dx.doi.org/10.1021/jacsau.1c00584
Descripción
Sumario:[Image: see text] Photosensitized energy transfer (EnT) phenomena occur frequently in a variety of photophysical and photochemical processes and have traditionally been treated with the donor–acceptor distance-dependent Förster and Dexter models. However, incorrect arguments and formulae were employed by ignoring energy resonance conditions and the selection rules of the state-to-state transition in special cases, especially for the sensitive intramolecular EnT of lanthanide complexes. Herein, we proposed an innovative model of energy-degeneracy-crossing-controlled EnT, which can be experimentally confirmed by time-resolved two-dimensional photoluminescence measurements. The computationally determined energy resonance region provides the most effective channel to achieve metal-to-ligand EnT beyond the distance-dependent model and sensitively bifurcates into symmetry-allowed or -forbidden channels for some representative europium antenna complexes. The outcomes of the multidisciplinary treatment contribute to a complementary EnT model that can be tuned by introducing a phosphorescence modulator and altering the antenna-related parameters of the ligand-centered energy level of the (3)ππ* state and its spin–orbit coupling for the (3)ππ* → S(0)(*) transition through mechanism-guided crystal engineering and should motivate further development of mechanistic models and applications.