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金属蛋白中非对称活性位点的模型:具有M-(μ-OH)-Fe核心的双金属配合物的结构、氧化还原和磁性性质

Models for Unsymmetrical Active Sites in Metalloproteins: Structural, Redox, and Magnetic Properties of Bimetallic Complexes with M-(μ-OH)-Fe Cores.

作者信息

Sano Yohei, Lau Nathanael, Weitz Andrew C, Ziller Joseph W, Hendrich Michael P, Borovik A S

机构信息

Department of Chemistry, University of California-Irvine , 1102 Natural Sciences II, Irvine, California 92697-2025, United States.

Department of Chemistry, Carnegie Mellon University , Pittsburgh, Pennsylvania 15213, United States.

出版信息

Inorg Chem. 2017 Nov 20;56(22):14118-14128. doi: 10.1021/acs.inorgchem.7b02230. Epub 2017 Nov 7.

Abstract

Bimetallic complexes are important sites in metalloproteins but are often difficult to prepare synthetically. We have previously introduced an approach to form discrete bimetallic complexes with M-(μ-OH)-Fe (M = Mn, Fe) cores using the tripodal ligand N,N',N″-[2,2',2″-nitrilotris(ethane-2,1-diyl)]tris(2,4,6-trimethylbenzenesulfonamido) ([MST]). This series is extended to include the rest of the late 3d transition metal ions (M = Co, Ni, Cu, Zn). All of the bimetallic complexes have similar spectroscopic and structural properties that reflect little change despite varying the M centers. Magnetic studies performed on the complexes in solution using electron paramagnetic resonance spectroscopy showed that the observed spin states varied incrementally from S = 0 through S = 5/2; these results are consistent with antiferromagnetic coupling between the high-spin M and Fe centers. However, the difference in the M ion occupancy yielded only slight changes in the magnetic exchange coupling strength, and all complexes had J values ranging from +26(4) to +35(3) cm.

摘要

双金属配合物是金属蛋白中的重要位点,但通常很难通过合成方法制备。我们之前介绍了一种使用三脚架配体N,N',N″-[2,2',2″-次氮基三(乙烷-2,1-二基)]三(2,4,6-三甲基苯磺酰胺)([MST])形成具有M-(μ-OH)-Fe (M = Mn, Fe)核的离散双金属配合物的方法。该系列扩展到包括其余的3d晚期过渡金属离子(M = Co、Ni、Cu、Zn)。尽管改变了M中心,但所有双金属配合物都具有相似的光谱和结构性质,几乎没有变化。使用电子顺磁共振光谱对溶液中的配合物进行的磁性研究表明,观察到的自旋态从S = 0到S = 5/2逐渐变化;这些结果与高自旋M和Fe中心之间的反铁磁耦合一致。然而,M离子占有率的差异仅导致磁交换耦合强度略有变化,并且所有配合物的J值范围为+26(4)至+35(3) cm。

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