Venkatasubbaiah Krishnan, Doshi Ami, Nowik Israel, Herber Rolfe H, Rheingold Arnold L, Jäkle Frieder
Department of Chemistry, Rutgers University Newark, 73 Warren Street, Newark, NJ 07102, USA.
Chemistry. 2008;14(2):444-58. doi: 10.1002/chem.200701219.
A series of mixed-valent (MV) complexes [(FeCp)2(mu-C10H6(BPh)2)]+X ([1+]X; X=I 5, PF6, SbF6, B(C6F5)4) were prepared by oxidation of diboradiferrocene [(FeCp)2(mu-C10H6(BPh)2)] (1) with I 2, AgPF6, and AgSbF6, respectively, and through anion exchange of the I 5(-) salt with [Li(Et2O)x][B(C6F5)4] in the case of X=B(C6F5)4. The MV state of the cation was investigated in solution by multinuclear NMR spectroscopy, CV, and UV/Vis-NIR absorption spectroscopy, and in the solid state by IR spectroscopy, single-crystal X-ray crystallography, and Mössbauer spectroscopy. The cyclic voltammogram of 1 shows two distinct redox waves with a large redox splitting of Delta E=510 mV in CH2Cl2 and the NIR spectrum for the mono-oxidized species displays an intervalence charge-transfer band at around 1500 to 1700 nm depending on the specific counterion present. The X-ray crystal structures of [1+]X show inversion-symmetric cations with X=I 5 and B(C6F5)4 and unsymmetric valence-trapped structures composed of one ferrocene and one ferrocenium moiety with X=PF6 and SbF6. Mössbauer data for X=PF6 are consistent with valence trapping at all temperatures between 90 and 343 K. In comparison, fast electron transfer is evident on the Mössbauer timescale for X=I 5 and temperature-dependent behavior is observed for X=B(C6F5)4. The anion dependence of the X-ray structural and Mössbauer data is discussed in the context of crystal symmetry and the possibility of static and dynamic disorder effects is considered.
通过分别用I₂、AgPF₆和AgSbF₆氧化二硼二茂铁[(FeCp)₂(μ-C₁₀H₆(BPh)₂)] (1),以及在X = B(C₆F₅)₄的情况下通过I₅⁻盐与[Li(Et₂O)ₓ][B(C₆F₅)₄]进行阴离子交换,制备了一系列混合价态(MV)配合物[(FeCp)₂(μ-C₁₀H₆(BPh)₂)]⁺X ([1⁺]X; X = I₅、PF₆、SbF₆、B(C₆F₅)₄)。通过多核NMR光谱、CV和UV/Vis-NIR吸收光谱在溶液中研究阳离子的MV状态,并通过IR光谱、单晶X射线晶体学和穆斯堡尔光谱在固态中进行研究。1的循环伏安图在CH₂Cl₂中显示出两个明显的氧化还原波,氧化还原分裂较大,ΔE = 510 mV,并且单氧化物种的近红外光谱根据存在的特定抗衡离子在1500至1700 nm左右显示出价间电荷转移带。[1⁺]X的X射线晶体结构显示,X = I₅和B(C₆F₅)₄时为反演对称阳离子,X = PF₆和SbF₆时为由一个二茂铁和一个二茂铁鎓部分组成的不对称价态捕获结构。X = PF₆的穆斯堡尔数据与90至343 K之间所有温度下的价态捕获一致。相比之下,对于X = I₅,在穆斯堡尔时间尺度上快速电子转移明显,对于X = B(C₆F₅)₄观察到温度依赖性行为。在晶体对称性的背景下讨论了X射线结构和穆斯堡尔数据的阴离子依赖性,并考虑了静态和动态无序效应的可能性。