Carlson Christin N, Scott Brian L, Martin Richard L, Thompson Joe D, Morris David E, John Kevin D
Chemistry Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
Inorg Chem. 2007 Jun 11;46(12):5013-22. doi: 10.1021/ic0702973. Epub 2007 May 11.
The ligand 1-methyl-3,5-bis(2,2':6',2' '-terpyridin-4'-yl)benzene has been employed in the synthesis of a new bimetallic ytterbocene complex [(Cp*)2Yb](1-methyl-3,5-bis(2,2':6',2' '-terpyridin-4'-yl)benzene)[Yb(Cp*)2] (1) and the doubly oxidized congener [1]2+ in an attempt to determine the impact of the bridging ligand geometry on the magnetic/electronic properties as compared to the previously reported 1,4-analog (Cp*)2Yb[Yb(Cp*)2] (2). Electrochemical, electronic, and magnetic data provide compelling evidence that the 1,3-geometry associated with the bridging ligand of 1 has done an effective job of inhibiting electronic communication between metal centers and magnetic coupling of spin carriers at room temperature as compared to 2. In fact, the physical data associated with 1 are quite similar to those reported for the monometallic analog (Cp*)2Yb(tpy) (3). In particular, the f-f profile of [1]2+ is nearly identical to that of [3]+ in its spectral features but with an almost exact doubling of the intensities. Further, the electronic coupling between metal centers as manifested in the potential separation between metal-based reduction waves has for the first time in these bimetallic ytterbocene complexes been found to go to zero for 1. Thus, the linkage isomerism at the phenyl coupling unit has induced a change in the ground-state electronic configuration from the singlet dianion-bridged (4f)13(pi*)2(4f)13 state found in 2 to the diradical-bridged (4f)13(piA*)1(piB*)1(4f)13 state in 1. This diradical formulation on the bridging ligand in 1 is supported by DFT calculations for the uncomplexed doubly reduced ligand that indicate the ground-state configuration is a singlet diradical state with the triplet-diradical state lying to slightly higher energy. Magnetic characterization of 1 is most consistent with the behavior previously observed for monometallic analogs such as 3, and there is no evidence of long-range magnetic ordering such as that observed for 2. In addition, X-ray crystallographic characterization of 1 represents the first case of a structurally characterized 2:1 metal-to-ligand adduct of the 1,3-bis(tpy) framework.
配体1-甲基-3,5-双(2,2':6',2''-三联吡啶-4'-基)苯已用于合成一种新型双金属镱茂配合物(Cp*)2Yb[Yb(Cp*)2] (1) 及其双氧化同系物[1]2+,旨在确定桥连配体几何结构对磁/电子性质的影响,并与先前报道的1,4-类似物(Cp*)2Yb[Yb(Cp*)2] (2) 进行比较。电化学、电子和磁学数据提供了令人信服的证据,表明与2相比,与1的桥连配体相关的1,3-几何结构在室温下有效地抑制了金属中心之间的电子通信和自旋载流子的磁耦合。事实上,与1相关的物理数据与单金属类似物(Cp*)2Yb(tpy) (3) 报道的数据非常相似。特别是,[1]2+的f-f光谱特征与[({3}+)]几乎相同,但强度几乎正好翻倍。此外,在这些双金属镱茂配合物中,首次发现1的基于金属的还原波之间的电位分离所表现出的金属中心之间的电子耦合为零。因此,苯基连接单元处的连接异构导致基态电子构型从2中发现的单重态双阴离子桥连(4f)13(π*)2(4f)13状态变为1中的双自由基桥连(4f)13(πA*)1(πB*)1(4f)13状态。对未配位的双还原配体的DFT计算支持了1中桥连配体上的这种双自由基结构,该计算表明基态构型是单重态双自由基状态,三重态双自由基状态的能量略高。1的磁学表征与先前观察到的单金属类似物(如3)的行为最为一致,没有证据表明存在如2中观察到的长程磁有序。此外,1的X射线晶体学表征代表了1,3-双(三联吡啶)骨架的结构表征的2:1金属-配体加合物的首例。