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Near-IR absorbing donor–acceptor ligand-to-ligand charge-transfer complexes of nickel(ii)

A new series of square-planar nickel(ii) donor–acceptor complexes exhibiting ligand-to-ligand charge-transfer (LL'CT) transitions have been prepared. Whereas the use of a catecholate donor ligand in conjunction with a bipyridyl acceptor ligand affords a complex that absorbs throughout the visib...

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Detalles Bibliográficos
Autores principales: Cameron, Lindsay A., Ziller, Joseph W., Heyduk, Alan F.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Royal Society of Chemistry 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5604403/
https://www.ncbi.nlm.nih.gov/pubmed/28959392
http://dx.doi.org/10.1039/c5sc02703a
Descripción
Sumario:A new series of square-planar nickel(ii) donor–acceptor complexes exhibiting ligand-to-ligand charge-transfer (LL'CT) transitions have been prepared. Whereas the use of a catecholate donor ligand in conjunction with a bipyridyl acceptor ligand affords a complex that absorbs throughout the visible region, the use of a azanidophenolate donor ligands in conjunction with a bipyridyl acceptor ligand affords complexes that absorbs well into the near-IR region of the solar spectrum. Three new complexes, (cat)Ni(bpy(t)Bu(2)) (1; (cat)(2–) = 3,5-di-tert-butyl-1,2-catecholate; bpy(t)Bu(2) = 4,4′-di-tert-butyl-2,2′-bipyridine), (ap)Ni(bpy(t)Bu(2)) (2; (ap)(2–) = 4,6-di-tert-butyl-2-(2,6-diisopropylphenylazanido)phenolate), and (ap(Ph))Ni(bpy(t)Bu(2)) (3; (ap(Ph))(2–) = 10-(2,6-diisopropylphenylazanido)-9-phenanthrolate), have been prepared and characterized by structural, electrochemical, and spectroscopic methods. Whereas all three square-planar complexes show multiple reversible one-electron redox-processes and strong LL'CT absorption bands, in azanidophenolate complexes 2 and 3, the LL'CT absorption covers the near-IR region from 700–1200 nm. The electronic absorption spectra and ground state electrochemical data for 2 and 3 provide an estimate of their excited-state reduction potentials, E (+/)*, of –1.3 V vs. SCE, making them as potent as the singlet excited state of [Ru(bpy)(3)](2+).