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The Excited‐State Creutz–Taube Ion

The excited‐state version of the Creutz–Taube ion was prepared via visible light excitation of [(NH(3))(5)Ru(II)(μ‐pz)Ru(II)(NH(3))(5)](4+). The resulting excited state is a mixed valence {Ru(III–δ)(μ‐pz⋅(−))Ru(II+δ)} transient species, which was characterized using femtosecond transient absorption...

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Detalles Bibliográficos
Autores principales: Pieslinger, German E., Ramírez‐Wierzbicki, Ivana, Cadranel, Alejandro
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10092683/
https://www.ncbi.nlm.nih.gov/pubmed/36161441
http://dx.doi.org/10.1002/anie.202211747
Descripción
Sumario:The excited‐state version of the Creutz–Taube ion was prepared via visible light excitation of [(NH(3))(5)Ru(II)(μ‐pz)Ru(II)(NH(3))(5)](4+). The resulting excited state is a mixed valence {Ru(III–δ)(μ‐pz⋅(−))Ru(II+δ)} transient species, which was characterized using femtosecond transient absorption spectroscopy with vis‐NIR detection. Very intense photoinduced intervalence charge transfers were observed at 7500 cm(−1), revealing an excited‐state electronic coupling element H(DA)=3750 cm(−1). DFT calculations confirm a strongly delocalized excited state. A notable consequence of strong electron delocalization is the nanosecond excited state lifetime, which was exploited in a proof‐of‐concept intermolecular electron transfer. The excited‐state Creutz–Taube ion is established as a reference, and demonstrates that electron delocalization in the excited state can be leveraged for artificial photosynthesis or other photocatalytic schemes based on electron transfer chemistry.