Paulovic Jozef, Cimpoesu Fanica, Ferbinteanu Marilena, Hirao Kimihiko
Department of Applied Chemistry, School of Engineering University of Tokyo, Tokyo, Japan.
J Am Chem Soc. 2004 Mar 17;126(10):3321-31. doi: 10.1021/ja030628k.
This paper offers the first series of state-of-the-art quantum chemical calculations (CASSCF, CASPT2, MS-CASPT2) and analytical models for the well-known problem of quasi-general ferromagnetic coupling in copper-gadolinium complexes. A system chosen from the chemical report of Costes et al. was taken as prototype. At the CASSCF level, calculated results for the experimental structure reproduced the magnetic coupling constant well (J(calcd)( )()= +7.67 cm(-)(1) vs J(exp)( )()= +7.0 cm(-)(1)). For more insight, the study molecule was further idealized by geometry optimization to C(2)(v)() symmetry. Systematic ab initio computation experiments were designed and performed. Owing to specific problems related to the non-aufbau ground configuration of the [CuL-Gd] complexes, the calculations were conducted in a nonstandard manner. We found that the qualitative mechanism of Kahn, assigned to the electron jump from 3d of Cu(II) to 5d shell of Gd(III), can be presented effectively as the cause of the phenomenon, if CASPT2 MOs are taken as magnetic orbitals. We showed that the ferromagnetic coupling is also matched and magnified by spin polarization effects over the ligand, in line with the early assumption of Gatteschi. To be distinguished from the initial hypothesis of Gatteschi, which assumed the role of 6s AO of Gd(III), we found that one 5d-type AO is actually involved in the polarization scheme. In fact, the Gatteschi and Kahn mechanisms are not mutually contradictory, but are even interconvertible with appropriate changes of the magnetic orbitals. Within C(2)(v)() symmetry of complexes, the ferromagnetic coupling can be qualitatively regarded as the preponderant influence of interaction channels exhibiting orbital orthogonality (four 3d-4f contacts) over the nonorthogonal ones (two 3d-4f contacts). The effective preponderance from ferromagnetic pathways is supported by CASPT2 results. One may explain the generality of Cu(II)-Gd(III) ferromagnetic coupling as being correlated with the large occurrence of approximate pseudo-C(2)(v)() geometry of complexes. The observed orbital regularity is lost in lower symmetries. Thus, the antiferromagnetic exceptions occur when the molecular asymmetry is advanced (e.g., owing to strong chemical nonequivalence of the donor atoms).
本文针对铜 - 钆配合物中准一般铁磁耦合这一著名问题,给出了一系列前沿的量子化学计算(CASSCF、CASPT2、MS - CASPT2)及分析模型。从科斯特等人的化学报告中选取的一个体系作为原型。在CASSCF水平下,对实验结构的计算结果很好地重现了磁耦合常数(计算值J(calcd) = +7.67 cm⁻¹,实验值J(exp) = +7.0 cm⁻¹)。为了更深入了解,通过几何优化将研究分子进一步理想化为C₂ᵥ对称性。设计并进行了系统的从头计算实验。由于[CuL - Gd]配合物的非构造基态构型相关的特定问题,计算以非标准方式进行。我们发现,如果将CASPT2分子轨道作为磁轨道,卡恩的定性机制(归因于电子从Cu(II)的3d跃迁到Gd(III)的5d壳层)可以有效地作为该现象的原因呈现出来。我们表明,铁磁耦合也通过配体上的自旋极化效应得到匹配和放大,这与加泰斯基的早期假设一致。与加泰斯基最初假设Gd(III)的6s原子轨道起作用不同,我们发现实际上一个5d型原子轨道参与了极化方案。事实上,加泰斯基机制和卡恩机制并非相互矛盾,而是在磁轨道适当变化时甚至可以相互转换。在配合物的C₂ᵥ对称性内,铁磁耦合可以定性地看作是表现出轨道正交性的相互作用通道(四个3d - 4f接触)比非正交通道(两个3d - 4f接触)具有更大影响。铁磁路径的有效优势得到了CASPT2结果的支持。人们可以将Cu(II) - Gd(III)铁磁耦合的普遍性解释为与配合物近似伪C₂ᵥ几何结构的大量出现相关。在较低对称性下观察到的轨道规律性丧失。因此,当分子不对称性增强时(例如,由于供体原子的强烈化学不等价性)会出现反铁磁例外情况。