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

机译:镍的近红外吸收供体-受体配体-配体电荷转移络合物(ii)

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摘要

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(bpytBu2) (>1; (cat)2– = 3,5-di-tert-butyl-1,2-catecholate; bpytBu2 = 4,4′-di-tert-butyl-2,2′-bipyridine), (ap)Ni(bpytBu2) (>2; (ap)2– = 4,6-di-tert-butyl-2-(2,6-diisopropylphenylazanido)phenolate), and (apPh)Ni(bpytBu2) (>3; (apPh)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+.
机译:制备了一系列新的方形平面镍(ii)供体-受体配合物,它们显示出配体到配体的电荷转移(LL'CT)跃迁。邻苯二酚供体配体与联吡啶基受体配体一起使用可提供在整个可见光区域吸收的复合物,而氮杂苯酚酚酸酯供体配体与联吡啶基受体配体一起使用可提供在近红外区域吸收良好的复合物太阳光谱的三种新的配合物(cat)Ni(bpy t Bu2)(> 1 ;(cat) 2 – = 3,5-di-tert -1,2-邻苯二酚丁基; bpy t Bu2 = 4,4'-二叔丁基-2,2'-联吡啶),(ap)Ni(bpy t < / sup> Bu2)(> 2 ;(ap) 2- = 4,6-二叔丁基-2-(2,6-二异丙基苯基叠氮基)酚盐),和(ap Ph )Ni(bpy t Bu2)(> 3 ;(ap Ph 2 – = 10-(2,6-二异丙基苯基叠氮基)-9-菲咯啉酸酯,已通过结构,电化学和光谱法进行了表征。尽管所有三个正方形平面复合物都显示出多个可逆的单电子氧化还原过程,并且具有很强的LL'CT吸收带,但在氮杂多酚盐复合物> 2 和> 3 中,LL'CT吸收覆盖700-1200 nm的近红外区域。 > 2 和> 3 的电子吸收光谱和基态电化学数据提供了其激发态还原电位E + / *的估计值,相对于SCE为–1.3 V,使其具有与[Ru(bpy)3] 2 + 的单重激发态一样强大的能力。

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