首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Vibronic Coupling in Dicyano-Complex-Bridged Mixed-Valence Complexes. Relaxation of Vibronic Constraints in Systems with Degenerate Bridging-Ligand and Electron-Transfer Excited States
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Vibronic Coupling in Dicyano-Complex-Bridged Mixed-Valence Complexes. Relaxation of Vibronic Constraints in Systems with Degenerate Bridging-Ligand and Electron-Transfer Excited States

机译:Dicyano-复杂桥混合价络合物中的电子振动耦合。简并桥联配体和电子转移激发态的系统中振动约束的弛豫

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Intense near-infrared (NIR) absorption bands have been found in mixed-valence Ru(NH_3)_5~(2+,3+) complexes bridged by trans-Ru(py)_4(CN)_2 and cis-Os(bpy)_2(CN)_2, #epsilon#_(max) approx1.5X10~3 cm~(-1) and #DELTA#_(v1/2) approx 5X10~3 cm~(-1) for bands at 1000 and 1300 nm, respectively. The NIR transitions implecate substantial comproportionation constants (64 and 175, respectvely) characteristic of moderately strong electronic coupling in the mixed-valence complexes. This stands in contrast to the weakly forbidded electronic coupling of Ru(NH_3)_5~(2+,3+) couples bridged by M(MCL)-(CN)_2~+ complexes (MCL=a tetraazamacrocyclic ligand) (Macatangay; et al. J. Phys. Chem.1998, 102, 7537). A straightforward perturbation theory argument is used to account for this contrasting behavior. The electronic coupling between a cyanide-bridged, donor-acceptor pair, D-(CN~-)-A, alters the properties of the bridging ligand. Such systems are described by a “vibronic” model in which the electronic matrix element, H_(DA), is a function of the nuclear coordinates, O_N, of the bridging ligand: H_(DA)=H_(DA)+bO_N. Electronic coupling in the dicyano-complex-bridged, D-[(NC)M(CN)]-A, systems is treated as the consequence of the perturbational mixing of the “local”, D(NC)M and M(CN)A, vibronic interactions. If M is an electron-transfer acceptor, then the nuclear coordinates are assumed to be configured so that bO_N is larger for D(NC)M but very small(bO_N approx 0) for M(CN)A. When the vertical energies of the corresponding charge-transfer transitions, E_(DM) and E_(DA), differ significantly, a perturbation theory treatment results in H_(DA)=H_(DA)H_(AM)/E_(ave) independent of M and consistent with the earlier report. When E_(DM)ident to E_(DA), configurational mixing of the excited states leads to H_(DA) proportional to H_(DM), consistent with the relatively intense intervalence bands reported in this paper. Some implications of the model are discussed.
机译:在由反式Ru(py)_4(CN)_2和顺式Os(bpy)桥接的混合价Ru(NH_3)_5〜(2 +,3 +)配合物中发现了强烈的近红外吸收带_2(CN)_2,#epsilon #_(max)约1.5X10〜3 cm〜(-1)和#DELTA #_(v1 / 2)约5X10〜3 cm〜(-1)适用于1000和1300波段纳米。 NIR跃迁实现了混合价络合物中中等强度电子耦合的相当大的比例常数(分别为64和175)。这与由M(MCL)-(CN)_2〜+配合物(MCL =四氮杂大环配体)桥接的Ru(NH_3)_5〜(2 +,3 +)偶合的弱禁止电子偶合相反(Macatangay; et al J. Phys。Chem。1998,102,7537)。一个简单的摄动理论论点被用来解释这种相反的行为。氰化物桥接的供体-受体对D-(CN〜-)-A之间的电子偶联改变了桥连配体的性质。这样的系统由“振动”模型描述,其中电子矩阵元素H_(DA)是桥联配体的核坐标O_N的函数:H_(DA)= H_(DA)+ bO_N。 D-[((NC)M(CN)]-A,双氰基复合桥联系统中的电子耦合被视为“局部”,D(NC)M和M(CN)扰动混合的结果A,振动相互作用。如果M是电子转移受体,则假定核坐标已配置为使得D(NC)M的bO_N较大,而M(CN)A的bO_N非常小(bO_N约为0)。当相应的电荷转移跃迁的垂直能量E_(DM)和E_(DA)显着不同时,微扰理论处理导致H_(DA)= H_(DA)H_(AM)/ E_(ave)独立M并与先前的报告一致。当E_(DM)与E_(DA)相同时,激发态的结构混合导致H_(DA)与H_(DM)成比例,这与本文报道的相对强烈的间隔带一致。讨论了该模型的一些含义。

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