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双(六氟乙酰丙酮)锰(II)、铜(II)和锌(II)与4,4'-双(N-叔丁基-N-氧自由基氨基)-2,2'-联吡啶的混合配体配合物的分子结构和磁性。由氨氧自由基和金属离子组成的等腰三角形异三自旋体系。

Molecular structures and magnetic properties of the mixed-ligand complexes of bis(hexafluoroacetylacetonato)manganese(II), -copper(II), and -zinc(II) with 4,4'-bis(N-tert-butyl-N-oxylamino)-2,2'-bipyridine. Isosceles triangular hetero-three-spin systems consisting of aminoxyls and metal ions.

作者信息

Sakane A, Kumada H, Karasawa S, Koga N, Iwamura H

机构信息

Graduate School of Pharmaceutical Sciences, Kyushu University, Fukuoka, Japan.

出版信息

Inorg Chem. 2000 Jun 26;39(13):2891-6. doi: 10.1021/ic991205f.

DOI:10.1021/ic991205f
PMID:11232829
Abstract

4,4'-Bis(N-tert-butyloxylamino)-2,2'-bipyridine (4) and its 1:1 complexes with bis(hexafluoroacetylacetonato)manganese(II), -copper(II), and -zinc(II) were prepared. An X-ray structure analysis of free ligand 4 reveals that the molecule has a trans conformation with Ci symmetry and the aminoxyl radical center has a short contact of 2.36 A with one of the neighboring molecules. The three 1:1 complexes have mutually similar molecular structures in which the 2,2'-bipyridine moiety has a cis conformation and serves as a bidentate ligand and coordination geometry around the metal atom is a distorted octahedron. The EPR experiments for free ligand 4 and [Zn(hfac)2.4] in frozen solution suggested that the exchange couplings between the two aminoxyls (R) through the 2,2'-bipyridine rings are antiferromagnetic with JR-R/kB = -19.3 +/- 0.5 and -24.3 +/- 0.4 K, respectively. Isosceles triangular three-spin models were applied to the 1:1 magnetic metal complexes to give JR-M/kB = -19.1 +/- 0.2 K and JR-R/kB = -32.9 +/- 0.3 K for [Mn(hfac)2.4] and JR-M/kB = +73 +/- 18 K and JR-R/kB = -24.5 +/- 6.5 K for [Cu(hfac)2.4].

摘要

制备了4,4'-双(N-叔丁氧基氨基)-2,2'-联吡啶(4)及其与双(六氟乙酰丙酮)锰(II)、铜(II)和锌(II)的1:1配合物。对游离配体4的X射线结构分析表明,该分子具有C i对称性的反式构象,且氨氧基自由基中心与相邻分子之一有2.36 Å的短接触。这三种1:1配合物具有相互相似的分子结构,其中2,2'-联吡啶部分具有顺式构象并作为双齿配体,金属原子周围的配位几何形状为扭曲的八面体。对游离配体4和[Zn(hfac)2·4]在冷冻溶液中的电子顺磁共振实验表明,两个氨氧基(R)通过2,2'-联吡啶环的交换耦合是反铁磁性的,J R-R/k B分别为-19.3±0.5 K和-24.3±0.4 K。等腰三角形三自旋模型应用于1:1磁性金属配合物,对于[Mn(hfac)2·4],J R-M/k B = -19.1±0.2 K,J R-R/k B = -32.9±0.3 K;对于[Cu(hfac)2·4],J R-M/k B = +73±18 K,J R-R/k B = -24.5±6.5 K。

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