Departament de Química Inorgànica, Universitat de València, Vicent Andrés Estellés s/n, 46100 Burjassot, Valencia, Spain.
Inorg Chem. 2012 Jan 16;51(2):985-1001. doi: 10.1021/ic2020034. Epub 2011 Dec 23.
Two new trinuclear copper(II) complexes, Cu(3)(μ(3)-OH)(daat)(Hdat)(2)(ClO(4))(2)(H(2)O)(3)(2)·2H(2)O (1) and Cu(3)(μ(3)-OH)(aaat)(3)(H(2)O)(3)(2)·3H(2)O (2) (daat = 3,5-diacetylamino-1,2,4-triazolate, Hdat = 3,5-diamino-1,2,4-triazole, and aaat = 3-acetylamino-5-amino-1,2,4-triazolate), have been prepared from 1,2,4-triazole derivatives and structurally characterized by X-ray crystallography. The structures of 1 and 2 consist of cationic trinuclear copper(II) complexes with a Cu(3)OH core held by three N,N-triazole bridges between each pair of copper(II) atoms. The copper atoms are five-coordinate with distorted square-pyramidal geometries. The magnetic properties of 1 and 2 and those of five other related 1,2,4-triazolato tricopper(II) complexes with the same triangular structure (3-7) (whose crystal structures were already reported) have been investigated in the temperature range of 1.9-300 K. The formulas of 3-7 are Cu(3)(μ(3)-OH)(aaat)(3)(H(2)O)(3)(2)·H(2)O (3), {[Cu(3)(μ(3)-OH)(aat)(3)(μ(3)-SO(4))]·6H(2)O}(n) (4), and [Cu(3)(μ(3)-OH)(aat)(3)A(H(2)O)(2)]A·xH(2)O [A = NO(3)(-) (5), CF(3)SO(3)(-) (6), or ClO(4)(-) (7); x = 0 or 2] (aat =3-acetylamino-1,2,4-triazolate). The magnetic and electron paramagnetic resonance (EPR) data have been analyzed by using the following isotropic and antisymmetric exchange Hamiltonian: H = -J[S(1)S(2) + S(2)S(3)] - j[S(1)S(3)] + G[S(1) × S(2) + S(2) × S(3) + S(1) × S(3)]. 1-7 exhibit strong antiferromagnetic coupling (values for both -J and -j in the range of 210-142 cm(-1)) and antisymmetric exchange (G varying from to 27 to 36 cm(-1)). At low temperatures, their EPR spectra display high-field (g < 2.0) signals indicating that the triangles present symmetry lower than equilateral and that the antisymmetric exchange is operative. A magneto-structural study showing a lineal correlation between the Cu-O-Cu angle of the Cu(3)OH core and the isotropic exchange parameters (J and j) has been conducted. Moreover, a model based on Moriya's theory that allows the prediction of the occurrence of antisymmetric exchange in the tricopper(II) triangles, via analysis of the overlap between the ground and excited states of the local Cu(II) ions, has been proposed. In addition, analytical expressions for evaluating both the isotropic and antisymmetric exchange parameters from the experimental magnetic susceptibility data of triangular complexes with local spins (S) of (1)/(2), (3)/(2), or (5)/(2) have been purposely derived. Finally, the magnetic and EPR results of this work are discussed and compared with those of other tricopper(II) triangles reported in the literature.
两种新的三核铜(II)配合物,Cu(3)(μ(3)-OH)(daat)(Hdat)(2)(ClO(4))(2)(H(2)O)(3)(2)·2H(2)O(1)和Cu(3)(μ(3)-OH)(aaat)(3)(H(2)O)(3)(2)·3H(2)O(2)(daat = 3,5-二乙酰氨基-1,2,4-三唑,Hdat = 3,5-二氨基-1,2,4-三唑,aaat = 3-乙酰氨基-5-氨基-1,2,4-三唑),已通过 1,2,4-三唑衍生物的合成和 X 射线晶体学结构表征得到。1 和 2 的结构由三核铜(II)配合物组成,带有 Cu(3)OH 核,由每个铜(II)原子对之间的三个 N,N-三唑桥连接。铜原子具有五配位的扭曲的四方锥几何形状。1 和 2 的磁性性质以及其他五个具有相同三角形结构(3-7)的相关 1,2,4-三唑三铜(II)配合物(其晶体结构已报道)的磁性性质已在 1.9-300 K 的温度范围内进行了研究。3-7 的化学式为Cu(3)(μ(3)-OH)(aaat)(3)(H(2)O)(3)(2)·H(2)O(3),{[Cu(3)(μ(3)-OH)(aat)(3)(μ(3)-SO(4))]·6H(2)O}(n)(4),以及[Cu(3)(μ(3)-OH)(aat)(3)A(H(2)O)(2)]A·xH(2)O[A = NO(3)(-)(5),CF(3)SO(3)(-)(6),或 ClO(4)(-)(7);x = 0 或 2](aat = 3-乙酰氨基-1,2,4-三唑)。使用以下各向同性和反对称交换哈密顿量对磁性和电子顺磁共振(EPR)数据进行了分析:H = -J[S(1)S(2) + S(2)S(3)] - j[S(1)S(3)] + G[S(1)×S(2) + S(2)×S(3) + S(1)×S(3)]。1-7 表现出强的反铁磁耦合(-J 和-j 的值在 210-142 cm(-1)范围内)和反对称交换(G 在 27 到 36 cm(-1)之间变化)。在低温下,它们的 EPR 光谱显示出高场(g < 2.0)信号,表明三角形的对称性低于等边,并且反对称交换是有效的。进行了一项磁结构研究,表明 Cu(3)OH 核的 Cu-O-Cu 角与各向同性交换参数(J 和 j)之间存在线性相关性。此外,提出了一种基于 Moriya 理论的模型,该模型通过分析局部 Cu(II)离子的基态和激发态之间的重叠,可以预测三铜(II)三角形中的反对称交换的发生。此外,还专门推导出了从具有局部自旋(S)为(1)/(2),(3)/(2)或(5)/(2)的三角形配合物的实验磁化率数据中评估各向同性和反对称交换参数的解析表达式。最后,讨论了这项工作的磁性和 EPR 结果,并与文献中报道的其他三铜(II)三角形进行了比较。