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具有非常规 Mn(III)6Mn(II) 交换耦合核的半整数自旋七核单分子磁体。

Half-integer spin heptanuclear single-molecule magnet with an unusual Mn(III)6Mn(II) exchange-coupled core.

机构信息

Department of Chemistry, Fu Jen Catholic University, Hsinchuang, Taipei, 24205, Taiwan, Republic of China.

出版信息

Inorg Chem. 2012 Apr 16;51(8):4448-57. doi: 10.1021/ic2019154. Epub 2012 Apr 3.

Abstract

The synthesis, X-ray crystallography, magnetic properties, and high-field electron paramagnetic resonance (HFEPR) of a new heptanuclear manganese complex Mn(7)(heamp)(6)(2)·4CH(2)Cl(2)·H(2)O (complex 2), in which heampH(3) is 2-[N,N-di(2-hydroxyethyl)aminomethyl]phenol (compound 1), is reported. Complex 2 has a hexagonal, disk-shaped topology and contains six Mn(III) ions and a central Mn(II) ion. It crystallizes in the monoclinic space group P2(1)/c with two molecular orientations. Consideration of the cluster topology, together with variable-temperature and variable-field DC magnetic susceptibility data, suggest that complex 2 exists in a half-integer, S = (19)/(2) ± 1 spin ground state, with appreciable uniaxial zero-field splitting (D = -0.16 cm(-1)). AC magnetic susceptibility measurements clearly show out-of-phase signals, which are frequency- and temperature-dependent, indicating slow magnetization relaxation behavior. An analysis of the relaxation data employing the Arrhenius formula yielded an effective relaxation barrier of 12.9 cm(-1). Simulations of HFEPR studies agree with the assignment of an S ≈ (19)/(2) spin ground state, with g = 1.96, D = -4.71 GHz (-0.16 cm(-1)), and a longitudinal fourth-order zero-field splitting parameter B(4)(0) = -2.7 × 10(-4) GHz (-9.0 × 10(-6) cm(-1)).

摘要

一种新的七核锰配合物Mn(7)(heamp)(6)(2)·4CH(2)Cl(2)·H(2)O(配合物 2)的合成、X 射线晶体学、磁性和高场电子顺磁共振(HFEPR)研究,其中 heampH(3)是 2-[N,N-二(2-羟乙基)氨甲基]苯酚(化合物 1)。配合物 2 具有六方盘形拓扑结构,包含六个 Mn(III)离子和一个中心 Mn(II)离子。它在单斜空间群 P2(1)/c 中结晶,存在两种分子取向。考虑到簇拓扑结构,以及变温变场直流磁化率数据,表明配合物 2 存在半整数自旋 S = (19)/(2) ± 1 的基态,具有可观的单轴零场分裂(D = -0.16 cm(-1))。交流磁化率测量清楚地显示出具有频率和温度依赖性的非相信号,表明存在缓慢的磁化弛豫行为。对弛豫数据的分析采用阿仑尼乌斯公式得出有效弛豫势垒为 12.9 cm(-1)。HFEPR 研究的模拟结果与 S ≈ (19)/(2)自旋基态的分配结果一致,g = 1.96,D = -4.71 GHz(-0.16 cm(-1)),以及纵向四阶零场分裂参数 B(4)(0) = -2.7 × 10(-4) GHz(-9.0 × 10(-6) cm(-1))。

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