Listorti Andrea, Accorsi Gianluca, Rio Yannick, Armaroli Nicola, Moudam Omar, Gégout Aline, Delavaux-Nicot Béatrice, Holler Michel, Nierengarten Jean-François
Molecular Photoscience Group, Istituto per la Sintesi Organica e la Fotoreattività, Consiglio Nazionale delle Ricerche, Via Gobetti 101, 40129 Bologna, Italy.
Inorg Chem. 2008 Jul 21;47(14):6254-61. doi: 10.1021/ic800315e. Epub 2008 Jun 26.
Heteroleptic copper(I) complexes CuPOP-F and CuFc-F have been prepared from a fullerene-substituted phenanthroline ligand and bis[2-(diphenylphosphino)phenyl] ether (POP) and 1,1'-bis(diphenylphosphino)ferrocene (dppFc), respectively. Electrochemical studies indicate that some ground-state electronic interaction between the fullerene subunit and the metal-complexed moiety are present in both CuPOP-F and CuFc-F. Their photophysical properties have been investigated by steady state and time-resolved UV-vis-NIR luminescence spectroscopy and nanosecond laser flash photolysis in a CH2Cl2 solution and compared to those of the corresponding model copper(I) complexes CuPOP and CuFc and of the fullerene model compound F. Selective excitation of the methanofullerene moiety in CuPOP-F results in regular deactivation of the lowest singlet and triplet states, indicating no intercomponent interactions. Conversely, excitation of the copper(I)-complexed unit (405 nm, 40% selectivity) shows that the strongly luminescent triplet metal-to-ligand charge-transfer ((3)MLCT) excited state located at 2.40 eV is quenched by the carbon sphere with a rate constant of 1.6 x 10(8) s(-1). Details on the mechanism of photodynamic processes in CuPOP-F via transient absorption are hampered by the rather unfavorable partition of light excitation between the two chromophores. By determination of the yield of formation of the lowest fullerene triplet level through sensitized singlet oxygen luminescence in the NIR region, it is shown that the final sink of photoinduced processes is always the fullerene triplet. This can be populated via a two-step charge-separation charge-recombination process and a less favored (3)MLCT --> (3)C60 triplet-triplet energy-transfer pathway. In CuFc-F, both of the photoexcited copper(I)-complexed and fullerene moieties are quenched by the presence of the ferrocene unit, most likely via ultrafast energy transfer.
异质配位的铜(I)配合物CuPOP-F和CuFc-F分别由富勒烯取代的菲咯啉配体与双[2-(二苯基膦基)苯基]醚(POP)和1,1'-双(二苯基膦基)二茂铁(dppFc)制备而成。电化学研究表明,CuPOP-F和CuFc-F中富勒烯亚基与金属配位部分之间均存在一些基态电子相互作用。通过稳态和时间分辨紫外-可见-近红外发光光谱以及在二氯甲烷溶液中的纳秒激光闪光光解研究了它们的光物理性质,并与相应的模型铜(I)配合物CuPOP和CuFc以及富勒烯模型化合物F的光物理性质进行了比较。对CuPOP-F中甲烷富勒烯部分的选择性激发导致最低单重态和三重态的正常失活,表明不存在组分间相互作用。相反,对铜(I)配位单元的激发(405 nm,40%选择性)表明,位于2.40 eV的强发光三重态金属到配体电荷转移((3)MLCT)激发态被碳球淬灭,淬灭速率常数为1.6×10(8) s(-1)。由于光激发在两个发色团之间的分配相当不利,阻碍了通过瞬态吸收对CuPOP-F中光动力过程机制细节的研究。通过在近红外区域通过敏化单线态氧发光测定最低富勒烯三重态能级的形成产率,结果表明光诱导过程的最终归宿始终是富勒烯三重态。这可以通过两步电荷分离-电荷复合过程以及不太有利的(3)MLCT→(3)C60三重态-三重态能量转移途径来实现。在CuFc-F中,光激发的铜(I)配位部分和富勒烯部分都因二茂铁单元的存在而被淬灭,最有可能是通过超快能量转移。