μ‐Oxamido‐桥接Cu(II) -Cr (III)和Cu(II) -Fe (III)杂双核配合物的合成和磁性研究

Cui‐Wei Yan, Yan-Tuan Li, Chunyuan Zhu, H. Guan
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引用次数: 8

摘要

摘要合成了两个新的μ‐氧胺桥接杂双核配合物,并鉴定为[Cu(dmoxae)Cr(bpy)2](ClO4)3(1)和[Cu(dmoxae)Fe(bpy)2](ClO4)3(2),其中dmoxae表示N, N′‐双[2‐(二甲氨基)乙基]氧胺二离子,bpy表示2,2′‐联吡啶。这两种配合物尚未以适合x射线结构分析的晶体形式分离出来,但基于元素分析,IR, ESR和电子能谱研究以及摩尔电导率测量,这些配合物被认为具有由平面铜(II)和八面体铬(III)或铁(III)离子组成的扩展氧胺桥接结构。通过变温磁化率(4.2-300 K)测量进一步表征了这两种杂双核配合物,并利用磁数据推断了所指示的杂双核结构。对实验数据进行最小二乘拟合的结果证实,配合物(1)中相邻的铜(II)和铬(III)离子通过oxamido桥发生铁磁耦合,交换积分J (Cu-Cr) = +16.5 cm−1,而配合物(2)中铜(II)和铁(III)离子通过oxamido桥发生反铁磁耦合,交换积分J (Cu-Fe) = - 18.9 cm−1。基于自旋-哈密顿算符,H = - 2J S - Cu S - M (M = Cr和Fe)。本文还讨论了金属离子的电子结构变化对顺磁中心间自旋交换相互作用性质的影响。
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Synthesis and Magnetic Studies of μ‐Oxamido‐Bridged Cu(II)–Cr(III) and Cu(II)–Fe(III) Heterobinuclear Complexes
Abstract Two new μ‐oxamido‐bridged heterobinuclear complexes have been synthesized and identified as [Cu(dmoxae)Cr(bpy)2](ClO4)3 (1) and [Cu(dmoxae)Fe(bpy)2](ClO4)3 (2), where dmoxae denotes N, N′‐bis[2‐(dimethylamino)ethyl]oxamido dianion and bpy represents 2,2′‐bipyridine. The two complexes have not yet been isolated in crystalline form suitable for x‐ray structure analysis, but based on elemental analyses, IR, ESR and electronic spectra studies, and molar conductivity measurements, the complexes are proposed to have an extended oxamido‐bridged structure consisting of planar copper(II) and octahedral chromium(III) or iron(III) ions. The two heterobinuclear complexes were further characterized by variable‐temperature magnetic susceptibility (4.2–300 K) measurements and the magnetic data have also been used to deduce the indicated heterobinuclear structure. The results derived from the least‐squares fit of the experimental data have confirmed that the adjacent copper(II) and chromium(III) ions in complex (1) are ferromagnetically coupled through the oxamido‐bridge with the exchange integral J (Cu–Cr) = +16.5 cm−1, while intramolecular antiferromagnetic coupling is detected between the copper(II) and iron(III) ions through the oxamido‐bridge in complex (2) with the exchange integral J (Cu–Fe) = −18.9 cm−1, on the basis of the spin‐Hamiltonian operator, Hˆ = − 2J Sˆ Cu Sˆ M (M = Cr and Fe). The influence of electronic‐structural variations of the metal ions on the nature of spin‐exchange interaction between the paramagnetic centers is also discussed.
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