de Souza Mateus S, Reis Samira G, Stinghen Danilo, Escobar Lívia B L, Allão Cassaro Rafael A, Poneti Giordano, S Bortolot Carolina, Marbey Jonathan, Hill Stephen, Vaz Maria G F
Instituto de Química, Universidade Federal Fluminense, Niterói, Rio de Janeiro 24020-150, Brazil.
Instituto de Física, Universidade Federal Fluminense, Niterói, Rio de Janeiro 24210-346, Brazil.
Inorg Chem. 2022 Aug 8;61(31):12118-12128. doi: 10.1021/acs.inorgchem.2c00679. Epub 2022 Jul 25.
Using the 1-(-tolyl)-1-1,2,3-triazole-4-(4,4,5,5-tetramethylimidazoline-1-oxyl-3-oxide) (TlTrzNIT) radical and metal β-diketonate complexes [M(hfac)(HO)], where hfac is hexafluoroacetylacetonato, three new 2p-3d heterospin complexes were synthesized. Their structures were solved using single crystal X-ray diffraction data, and magnetic investigation was performed by DC and AC measurements and multifrequency EPR spectroscopy. Compounds and are isostructural complexes with molecular formula [M(TlTrzNIT)(hfac)] (M = Mn or Cu) while compound is the mononuclear [Co(TlTrzNIT)(hfac)] complex. In all complexes, the radical acts as a bidentate ligand through the oxygen atom of the nitroxide moiety and the nitrogen atom from the triazole group. Furthermore, in compounds and , the TlTrzNIT is bridge-coordinated between two metal centers, leading to the formation of trinuclear complexes. The fitting of the static magnetic behavior reveals antiferromagnetic and ferromagnetic intramolecular interactions for complexes and , respectively. The EPR spectra of are well described by an isolated ferrimagnetic = / (= / - / + / - / + /) ground state with a biaxial zero-field splitting (ZFS) interaction characterized, respectively, by 2nd order axial and rhombic parameters, and , such that / is close to the maximum of 0.33. Meanwhile, EPR spectra for are explained in terms of a ferromagnetic model with weakly anisotropic Cu-radical exchange interactions, giving rise to an isolated = / (= 5 × /) ground state with both an anisotropic tensor and a weak ZFS interaction. Complex represents one of only a few examples of Cu-radical moieties with measurable exchange anisotropy.
使用1 -(对甲苯基)-1 - 1,2,3 - 三唑 - 4 -(4,4,5,5 - 四甲基咪唑啉 - 1 - 氧基 - 3 - 氧化物)(TlTrzNIT)自由基和金属β - 二酮配合物[M(hfac)(HO)],其中hfac为六氟乙酰丙酮,合成了三种新型的2p - 3d异自旋配合物。通过单晶X射线衍射数据解析了它们的结构,并通过直流和交流测量以及多频电子顺磁共振光谱进行了磁性研究。化合物 和 是具有分子式[M(TlTrzNIT)(hfac)](M = Mn或Cu)的同构配合物,而化合物 是单核[Co(TlTrzNIT)(hfac)]配合物。在所有配合物中,自由基通过氮氧化物部分的氧原子和三唑基团的氮原子作为双齿配体。此外,在化合物 和 中,TlTrzNIT在两个金属中心之间桥连配位,导致形成三核配合物。静态磁性行为的拟合分别揭示了配合物 和 中的反铁磁和铁磁分子内相互作用。 的电子顺磁共振光谱可以用具有双轴零场分裂(ZFS)相互作用的孤立亚铁磁 = /(= / - / + / - / + /)基态很好地描述,该相互作用分别由二阶轴向和菱形参数 和 表征,使得 /接近最大值0.33。同时, 的电子顺磁共振光谱根据具有弱各向异性的Cu - 自由基交换相互作用的铁磁模型进行解释,产生具有各向异性 张量和弱ZFS相互作用的孤立 = /(= 5× /)基态。配合物 代表了少数具有可测量交换各向异性的Cu - 自由基部分的例子之一。