Maurice Rémi
SUBATECH, UMR CNRS 6457, IN2P3/IMT Atlantique/Université de Nantes, 4 rue A. Kastler, 44307 Nantes Cedex 3, France.
Inorg Chem. 2021 May 3;60(9):6306-6318. doi: 10.1021/acs.inorgchem.1c00047. Epub 2021 Apr 16.
Magnetic anisotropy, in the absence of an external magnetic field, relates to the degeneracy lift of energy levels. In the standard case of transition metal complexes, this property is usually modeled by an anisotropic spin Hamiltonian and one speaks of "zero-field splitting" (ZFS) of spin states. While the case of mononuclear complexes has been extensively described by means of ab initio quantum mechanical calculations, the literature on polynuclear complexes studied with these methodologies is rather scarce. In this work, advanced multiconfigurational wave function theory methods are applied to compute the ZFS of the ground = 4 state of an actual tetranickel(II) complex, displaying a magnet behavior below 0.5 K. First, the isotropic couplings are computed in the absence of the spin-orbit coupling operator, in the full complex and also in clusters with only two active nickel(II) centers, confirming the occurrence of weak ferromagnetic couplings in this system. Second, the single-site magnetic anisotropies are computed on a cluster bearing only one active nickel(II) site, showing that the single-site anisotropy axes are not oriented in an optimal fashion for generating a large uniaxial molecular anisotropy. Furthermore, the possibility for involving only a few local orbital excited states in the calculation is assessed, actually opening the way for a consistent and manageable treatment of the ZFS of the ground = 4 state. Third, multiconfigurational calculations are performed on the full complex, confirming the weak uniaxial anisotropy occurring for this state and also, interestingly, revealing a significant contribution of the lowest-lying orbitally excited = 3 states. Overall, by comparison with the experiment, the reported results question the common habit of using only one structure, in particular derived from a crystallography experiment, to compute magnetic anisotropy parameters.
在没有外磁场的情况下,磁各向异性与能级的简并解除有关。在过渡金属配合物的标准情形中,此性质通常由各向异性自旋哈密顿量来建模,人们会谈到自旋态的“零场分裂”(ZFS)。虽然单核配合物的情况已通过从头算量子力学计算得到了广泛描述,但用这些方法研究多核配合物的文献却相当稀少。在这项工作中,应用先进的多组态波函数理论方法来计算一个实际的四镍(II)配合物基态(S = 4)的零场分裂,该配合物在低于(0.5K)时表现出磁行为。首先,在没有自旋轨道耦合算符的情况下,在整个配合物以及仅含两个活性镍(II)中心的簇中计算各向同性耦合,证实了该体系中存在弱铁磁耦合。其次,在仅含一个活性镍(II)位点的簇上计算单中心磁各向异性,结果表明单中心各向异性轴的取向并非以产生大的单轴分子各向异性的最佳方式。此外,评估了在计算中仅涉及少数局域轨道激发态的可能性,实际上为基态(S = 4)的零场分裂的一致且可管理的处理开辟了道路。第三,对整个配合物进行多组态计算,证实了该态存在弱单轴各向异性,有趣的是,还揭示了最低的轨道激发态(S = 3)的显著贡献。总体而言,与实验相比,所报道的结果对仅使用一种结构(特别是源自晶体学实验的结构)来计算磁各向异性参数的常见做法提出了质疑。