Department of Chemistry, Indian Institute of Technology Bombay, Powai, Mumbai-400076 (India).
Chemistry. 2012 Nov 5;18(45):14434-43. doi: 10.1002/chem.201201785. Epub 2012 Sep 23.
New compounds Ru(pap)(2)(L), [Ru(pap)(L)(2)], and [Ru(acac)(2)(L)] (pap = 2-phenylazopyridine, L(-) = 9-oxidophenalenone, acac(-) = 2,4-pentanedionate) have been prepared and studied regarding their electron-transfer behavior, both experimentally and by using DFT calculations. Ru(pap)(2)(L) and [Ru(acac)(2)(L)] were characterized by crystal-structure analysis. Spectroelectrochemistry (EPR, UV/Vis/NIR), in conjunction with cyclic voltammetry, showed a wide range of about 2 V for the potential of the Ru(III/II) couple, which was in agreement with the very different characteristics of the strongly π-accepting pap ligand and the σ-donating acac(-) ligand. At the rather high potential of +1.35 V versus SCE, the oxidation of L(-) into L(⋅) could be deduced from the near-IR absorption of Ru(III)(pap)(L(⋅))(L(-)). Other intense long-wavelength transitions, including LMCT (L(-) → Ru(III)) and LL/CT (pap(⋅-) → L(-)) processes, were confirmed by TD-DFT results. DFT calculations and EPR data for the paramagnetic intermediates allowed us to assess the spin densities, which revealed two cases with considerable contributions from L-radical-involving forms, that is, Ru(III)(pap(0))(2)(L(-)) ↔ Ru(II)(pap(0))(2)(L(⋅)) and Ru(III)(pap(0))(L(-))(2) ↔ Ru(II)(pap(0))(L(⋅))(L(-)). Calculations of electrogenerated complex [Ru(II)(pap(⋅-))(pap(0))(L(-))] displayed considerable negative spin density (-0.188) at the bridging metal.
已制备并研究了新化合物 Ru(pap)(2)(L)、[Ru(pap)(L)(2)]和 [Ru(acac)(2)(L)](pap = 2-苯基偶氮吡啶,L(-) = 9-氧化菲咯啉,acac(-) = 2,4-戊二酮),其电子转移行为通过实验和 DFT 计算进行了研究。Ru(pap)(2)(L)和 [Ru(acac)(2)(L)]通过晶体结构分析进行了表征。光谱电化学(EPR、UV/Vis/NIR)与循环伏安法相结合,表明 Ru(III/II) 偶对的电位范围很宽,约为 2 V,这与强 π-接受 pap 配体和 σ-供体 acac(-) 配体的非常不同特性相吻合。在 +1.35 V 相对于 SCE 的相当高的电势下,可以从近红外吸收推断出 L(-) 氧化成 L(⋅)。其他强烈的长波长跃迁,包括 LMCT(L(-) → Ru(III))和 LL/CT(pap(⋅-) → L(-))过程,通过 TD-DFT 结果得到了证实。DFT 计算和顺磁中间体的 EPR 数据使我们能够评估自旋密度,这表明两种情况下 L-自由基参与的形式有相当大的贡献,即 Ru(III)(pap(0))(2)(L(-)) ↔ Ru(II)(pap(0))(2)(L(⋅)) 和 Ru(III)(pap(0))(L(-))(2) ↔ Ru(II)(pap(0))(L(⋅))(L(-))。生成的配合物 [Ru(II)(pap(⋅-))(pap(0))(L(-))]的计算显示桥接金属处有相当大的负自旋密度 (-0.188)。