Department of Chemistry, Tulane University, New Orleans, Louisiana 70118-5698, USA.
Inorg Chem. 2011 Apr 4;50(7):2995-3002. doi: 10.1021/ic102493g. Epub 2011 Mar 7.
The dipalladium compound [{(adt)Pd}(2)(μ-tpbz)] (1) (adt = bis(p-anisyl)-1,2-ethylenedithiolate, tpbz = 1,2,4,5-tetrakis(diphenylphosphino)benzene) has been synthesized from [{Cl(2)Pd}(2)(μ-tpbz)] by transmetalation employing (adt)SnMe(2). The cyclic voltammogram (CV) of 1 reveals reversible oxidation waves at 0.00 V and +0.50 V (vs Fc/Fc) with current amplitude twice that for identical processes in the monopalladium compound [(adt)Pd(dppb)] (2) (dppb = 1,2-bis(diphenylphosphino)benzene), an observation indicating each wave involves simultaneous one-electron oxidations at each metallodithiolene fragment. This assignment is affirmed by density functional theory (DFT) calculations that show the redox-active molecular orbital (MO) is principally composed of the dithiolene S(2)C(2) π-system, and by spectroelectrochemical UV-vis of 1, which displays hallmark low energy charge transfer (CT) bands. Dication 1 is a diradical with a near degenerate singlet-triplet ground state; fluid solution electron paramagnetic resonance (EPR) spectra validate the DFT-derived isotropic exchange coupling, J' = -6.3 cm(-1). The frozen solution X-band EPR spectrum of 1 is consistent with a spin-triplet bearing a very faint half-field ("ΔM(S) = 2") signal. It is successfully simulated with an amazingly small zero field splitting, D = -15 × 10(-4) cm(-1) and negligible rhombicity (E/D = 0.008). These zero-field splitting parameters, which stem from the long-range dipolar spin coupling, are very accurately reproduced using a multipoint dipole model with an optimized interspin distance of 12.434 Å. With the framework reported herein for understanding how the weak interaction of two spins is mediated by tpbz, this bridging ligand can now be incorporated into extended systems with tailored chemical and physical properties for use in a variety of molecular-based electronic and magnetic devices.
[{(adt)Pd}(2)(μ-tpbz)] (1) 的合成与电化学性质
[(adt)Pd}(2)(μ-tpbz)] (1)(adt = 双(对茴香基)-1,2-乙二硫醇,tpbz = 1,2,4,5-四(二苯基膦)苯)是通过[(Cl2Pd}(2)(μ-tpbz)]与(adt)SnMe2 的transmetalation 反应合成得到的。1 的循环伏安图(CV)在 0.00 V 和 +0.50 V(相对于 Fc/Fc)处显示出可逆的氧化波,电流幅度是单钯化合物[(adt)Pd(dppb)] (2)(dppb = 1,2-双(二苯基膦)苯)中相同过程的两倍,这一观察结果表明每个波都涉及每个金属二硫烯片段的同时单电子氧化。这一分配得到了密度泛函理论(DFT)计算的证实,该计算表明氧化还原活性分子轨道(MO)主要由二硫烯 S(2)C(2) π 体系组成,并且通过 1 的光谱电化学 UV-vis 显示出特征的低能量电荷转移(CT)带。二阳离子1 是一个近简并的单重态-三重态基态的双自由基;流体溶液电子顺磁共振(EPR)谱验证了 DFT 推导的各向同性交换耦合,J' = -6.3 cm(-1)。1的冻结溶液 X 波段 EPR 谱与带有非常微弱的半场(“ΔM(S) = 2”)信号的三重态一致。它可以通过一个非常小的零场分裂,D = -15 × 10(-4) cm(-1) 和可以忽略的非对角性(E/D = 0.008)的零场分裂参数来成功模拟。这些零场分裂参数源自长程偶极自旋耦合,使用优化的自旋间距离为 12.434 Å 的多点偶极模型可以非常准确地重现。有了本文报告的理解两个自旋的弱相互作用如何被 tpbz 介导的框架,现在可以将这种桥连配体纳入具有定制化学和物理性质的扩展系统中,用于各种基于分子的电子和磁性器件。