Wong Chun-Yuen, Lee Fu-Wa, Che Chi-Ming, Cheng Yung Fong, Phillips David Lee, Zhu Nianyong
Department of Chemistry and HKU-CAS Joint Laboratory on New Materials, The University of Hong Kong, Pokfulam Road, Hong Kong SAR, China.
Inorg Chem. 2008 Nov 17;47(22):10308-16. doi: 10.1021/ic800743a. Epub 2008 Oct 14.
trans-[Ru(16-TMC)(C[triple bond]N)2] (1; 16-TMC = 1,5,9,13-tetramethyl-1,5,9,13-tetraazacyclohexadecane) was prepared by the reaction of trans-[Ru(16-TMC)Cl2]Cl with KCN in the presence of zinc powder. The oxidation of 1 with bromine gave trans-[Ru(16-TMC)(CN)2]+ isolated as PF6 salt (2.PF6). The Ru-C/C-N distances are 2.061(4)/1.130(5) and 2.069(5)/1.140(7) A for 1 and 2, respectively. Both complexes show a Ru(III/II) couple at 0.10 V versus FeCp2+/0. The UV-vis absorption spectrum of 1 is dominated by an intense high-energy absorption at lambda(max) = 230 nm, which is mainly originated from dpi(RuII) --> pi*(N[triple bond]C-Ru-C[triple bond]N) charge-transfer transition. Complex 2 shows intense absorption bands at lambda(max) <or= 228 nm and weaker vibronically structured absorption bands with peak maxima at 315-441 nm (epsilon(max) approximately (5-8) x 10(2) dm3 mol-1 cm-1), which are assigned to dpi(RuIII) --> pi*(N[triple bond]C-Ru-C[triple bond]N) and sigma(-CN) --> d(RuIII) charge-transfer transition, respectively. Density functional theory and time-dependent density-functional theory calculations have been performed on trans-[(NH3)4Ru(C[triple bond]N)2] (1') and trans-[(NH3)4Ru(C[triple bond]N)2]+ (2') to examine the Ru-cyanide interaction and the nature of associated electronic transition(s). The 230 nm band of 1 has been probed by resonance Raman spectroscopy. Simulations of the absorption band and the resonance Raman intensities show that the nominal nuC[triple bond]N stretch mode accounts for ca. 66% of the total vibrational reorganization energy. A change of nominal bond order for the cyanide ligand from 3 to 2.5 is estimated upon the electronic excitation.
反式-[Ru(16-TMC)(C≡N)₂](1;16-TMC = 1,5,9,13-四甲基-1,5,9,13-四氮杂环十六烷)通过反式-[Ru(16-TMC)Cl₂]Cl与KCN在锌粉存在下反应制备。1与溴反应氧化得到反式-[Ru(16-TMC)(CN)₂]⁺,以PF₆盐(2.PF₆)形式分离出来。对于1和2,Ru-C/C-N距离分别为2.061(4)/1.130(5) Å和2.069(5)/1.140(7) Å。两种配合物相对于FeCp₂⁺/0在0.10 V处均显示出Ru(III/II)电对。1的紫外-可见吸收光谱以λ(max) = 230 nm处的强高能吸收为主,其主要源于dpi(RuII)→π*(N≡C-Ru-C≡N)电荷转移跃迁。配合物2在λ(max)≤228 nm处显示出强吸收带,在315 - 441 nm处有较弱的振动结构吸收带(ε(max)约为(5 - 8)×10² dm³ mol⁻¹ cm⁻¹),分别归属于dpi(RuIII)→π*(N≡C-Ru-C≡N)和σ(-CN)→d(RuIII)电荷转移跃迁。已对反式-[(NH₃)₄Ru(C≡N)₂](1')和反式-[(NH₃)₄Ru(C≡N)₂]⁺(2')进行密度泛函理论和含时密度泛函理论计算,以研究Ru-氰基相互作用及相关电子跃迁的性质。1的230 nm吸收带已通过共振拉曼光谱进行探测。吸收带和共振拉曼强度的模拟表明,名义上的νC≡N伸缩模式约占总振动重组能的66%。据估计,在电子激发时,氰基配体的名义键级从3变为2.5。