Department of Chemistry, University of Central Arkansas, Conway, Arkansas 72035, USA.
Inorg Chem. 2012 Mar 5;51(5):2793-805. doi: 10.1021/ic201775c. Epub 2012 Feb 15.
The previously reported Ni(II) complex, TpNi(κ(3)-BH(4)) (Tp = hydrotris(3,5-dimethylpyrazolyl)borate anion), which has an S = 1 spin ground state, was studied by high-frequency and -field electron paramagnetic resonance (HFEPR) spectroscopy as a solid powder at low temperature, by UV-vis-NIR spectroscopy in the solid state and in solution at room temperature, and by paramagnetic (11)B NMR. HFEPR provided its spin Hamiltonian parameters: D = 1.91(1) cm(-1), E = 0.285(8) cm(-1), g = [2.170(4), 2.161(3), 2.133(3)]. Similar, but not identical parameters were obtained for its borodeuteride analogue. The previously unreported complex, TpZn(κ(2)-BH(4)), was prepared, and IR and NMR spectroscopy allowed its comparison with analogous closed shell borohydride complexes. Ligand-field theory was used to model the electronic transitions in the Ni(II) complex successfully, although it was less successful at reproducing the zero-field splitting (zfs) parameters. Advanced computational methods, both density functional theory (DFT) and ab initio wave function based approaches, were applied to these TpMBH(4) complexes to better understand the interaction between these metals and borohydride ion. DFT successfully reproduced bonding geometries and vibrational behavior of the complexes, although it was less successful for the spin Hamiltonian parameters of the open shell Ni(II) complex. These were instead best described using ab initio methods. The origin of the zfs in Tp*Ni(κ(3)-BH(4)) is described and shows that the relatively small magnitude of D results from several spin-orbit coupling (SOC) interactions of large magnitude, but with opposite sign. Spin-spin coupling (SSC) is also shown to be significant, a point that is not always appreciated in transition metal complexes. Overall, a picture of bonding and electronic structure in open and closed shell late transition metal borohydrides is provided, which has implications for the use of these complexes in catalysis and hydrogen storage.
先前报道的 Ni(II) 配合物 TpNi(κ(3)-BH(4))(Tp = 三(3,5-二甲基吡唑基)硼酸盐阴离子),具有 S = 1 自旋基态,通过高频和高场电子顺磁共振(HFEPR)光谱在低温下作为固体粉末进行了研究,通过室温下的固态和溶液的紫外可见近红外光谱以及顺磁(11)B NMR 进行了研究。HFEPR 提供了其自旋哈密顿参数:D = 1.91(1) cm(-1),E = 0.285(8) cm(-1),g = [2.170(4),2.161(3),2.133(3)]。其硼氘化物类似物得到了类似但不完全相同的参数。制备了先前未报道的配合物 TpZn(κ(2)-BH(4)),并通过红外和 NMR 光谱对其与类似的满壳层硼氢化物配合物进行了比较。通过配位场理论成功地对 Ni(II) 配合物的电子跃迁进行了建模,尽管它在复制零场分裂(zfs)参数方面效果较差。应用了先进的计算方法,包括密度泛函理论(DFT)和基于从头算波函数的方法,对这些 TpMBH(4) 配合物进行了研究,以更好地理解这些金属与硼氢化物离子之间的相互作用。DFT 成功地复制了配合物的键合几何形状和振动行为,尽管对于开壳层 Ni(II) 配合物的自旋哈密顿参数效果较差。相反,使用从头算方法可以最好地描述这些参数。描述了 Tp*Ni(κ(3)-BH(4)) 中 zfs 的起源,表明 D 的相对较小值是由几个具有较大绝对值但符号相反的自旋轨道耦合(SOC)相互作用引起的。还表明自旋-自旋耦合(SSC)也是显著的,这在过渡金属配合物中并不总是被注意到。总体而言,提供了开放和封闭壳层后过渡金属硼氢化物的成键和电子结构的图像,这对这些配合物在催化和储氢中的应用具有重要意义。