Hale Ashlyn R, Lott Megan E, Peralta Juan E, Foguet-Albiol Dolos, Abboud Khalil A, Christou George
Department of Chemistry, University of Florida, Gainesville, Florida 32611-7200, Unites States.
Department of Physics and Science of Advanced Materials, Central Michigan University, Mount Pleasant, Michigan 48859, United States.
Inorg Chem. 2022 Jul 25;61(29):11261-11276. doi: 10.1021/acs.inorgchem.2c01371. Epub 2022 Jul 11.
The synthesis, structure, and magnetic properties of three related iron(III)-oxo clusters are reported, [FeO(OCPh)(mda)(HO)] (), FeO(OH)(OCMe)(mda) (), and FeO(OH)(OEt)(OCMe)(mda) (), where mdaH is -methyldiethanolamine. was prepared from the reaction of FeO(OCPh)(HO) with mdaH in a 1:2 ratio in MeCN, whereas and were prepared from the reaction of FeCl/NaOCMe/mdaH in a 2:∼13:2 ratio and FeCl/NaOCMe/mdaH/pyridine in a 2:∼13:2:25 ratio, respectively, both in EtOH. The core of consists of a central octahedral Fe ion held within a nonplanar Fe loop by three μ-O and three μ-RO arms from the three mda chelates. The cores of the cations of and consist of an :: three-layer topology, in which a central Fe () or Fe () layer is sandwiched between two Fe layers . The layers structurally resemble with the additional Fe added at the center to retain virtual symmetry. The central Fe layer of consists of a {Fe(μ-O)(μ-OH)} cubane with an Fe on either side attached to cubane O ions, whereas that of has the same cubane but with an {Fe(μ-O)(μ-OH)} unit attached on one side and a single Fe on the other. Variable-temperature dc and ac magnetic susceptibility studies revealed dominant antiferromagnetic coupling in all complexes leading to ground-state spins of = / for and = 0 for and . All Fe pairwise exchange parameters () for - were estimated by two independent methods: density functional theory (DFT) calculations using broken symmetry methods and a magnetostructural correlation previously developed for high-nuclearity Fe/O complexes. The two approaches gave satisfyingly similar values, and the latter allowed rationalization of the experimental ground states by identification of the spin frustration effects operative and the resultant relative spin vector alignments at each Fe ion.
报道了三种相关的铁(III)-氧簇合物的合成、结构和磁性,即[FeO(OCPh)(mda)(HO)] ()、FeO(OH)(OCMe)(mda) ()和FeO(OH)(OEt)(OCMe)(mda) (),其中mdaH为N-甲基二乙醇胺。通过FeO(OCPh)(HO)与mdaH以1:2的比例在乙腈中反应制备得到 ,而 和 分别通过FeCl/NaOCMe/mdaH以2:13:2的比例以及FeCl/NaOCMe/mdaH/吡啶以2:13:2:25的比例在乙醇中反应制备得到。 的核心由一个中心八面体铁离子组成,该铁离子通过来自三个mda螯合物的三个μ-O和三个μ-RO臂保持在一个非平面的铁环内。 和 的阳离子核心由一种::三层拓扑结构组成,其中一个中心Fe()或Fe()层夹在两个Fe层之间。 层在结构上类似于 ,只是在中心添加了额外的Fe以保持近似 对称性。 的中心Fe层 由一个{Fe(μ-O)(μ-OH)}立方烷组成,其两侧各有一个Fe连接到立方烷的O离子上,而 的中心Fe层具有相同的立方烷,但一侧连接有一个{Fe(μ-O)(μ-OH)}单元,另一侧有一个单个的Fe。变温直流和交流磁化率研究表明,所有配合物中均存在主导的反铁磁耦合,导致 的基态自旋为S = / , 和 的基态自旋为S = 0。对于 - 的所有铁对交换参数()通过两种独立方法进行估计:使用破缺对称性方法的密度泛函理论(DFT)计算以及先前为高核Fe/O配合物开发的磁结构相关性。这两种方法给出了令人满意的相似 值,并且后者通过识别起作用的自旋挫折效应以及每个铁离子处产生的相对自旋矢量排列,对实验基态进行了合理化解释。