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首页> 外文期刊>The journal of physics and chemistry of solids >Peculiarities of crystal structures and magnetic properties of Cu(II) and Ni(II) mixed-ligand complexes on the 1,3-dithiole-2-thione-4,5-dithiolate basis
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Peculiarities of crystal structures and magnetic properties of Cu(II) and Ni(II) mixed-ligand complexes on the 1,3-dithiole-2-thione-4,5-dithiolate basis

机译:1,3-二硫代-2-硫代-4,5-二硫代的Cu(II)和Ni(II)混合配体配合物的晶体结构和磁性

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Mixed-ligand Cu(II) and Ni(II) complexes, [Cu(dmit)(bpy)] _2 (I), [Ni(dmit)(phen) _2] (II) and [Ni(dmit)(phen) _2] ·CH _2Cl _2 (III) (dmit=1.3-dithiole-2-thione-4.5- dithiolate, phen=1.10-phenantroline, bpy=2.2′-bipyridine) have been prepared by ligand exchange between phen or bpy and (Bu _4N) _2[M(dmit) _2] (M=Ni, Cu) and characterized by elemental analysis, IR spectroscopy, single-crystal X-ray analysis and by investigation of magnetic and resonance properties. In complex I, the monomeric units form dimers in a head-to-tail arrangement by weak coordination bonds between copper and dithiolate sulfur atoms and ππ interactions between dmit and bpy from neighboring monomers. Dimers in I are further extended into chains by weak CuS(thione) contacts. In crystal packing of complex II and III, there exists a weak ππ interaction between two parallel phen molecules of the adjacent complexes. As a consequence, the magnetic and resonance characteristics of copper complex may be described in approximation of exchange-coupled pairs of Cu ~2 ions with ion spin S=1/2. The nickel complexes are described by isotropic exchange model for single-site spin S=1.
机译:混合配体Cu(II)和Ni(II)配合物,[Cu(dmit)(bpy)] _2(I),[Ni(dmit)(phen)_2](II)和[Ni(dmit)(phen) _2]·CH _2Cl _2(III)已通过phen或bpy与(Bu)之间的配体交换而制备(dmit = 1.3-二硫代-2-硫酮-4.5-二硫代酯,phen = 1.10-菲咯啉,bpy = 2.2'-联吡啶) _4N)_2 [M(dmit)_2](M = Ni,Cu),其特征在于元素分析,红外光谱,单晶X射线分析以及磁和共振特性的研究。在配合物I中,单体单元通过铜与二硫代硫醇原子之间的弱配位键以及相邻单体的dmit和bpy之间的ππ相互作用,以头尾相接的方式形成二聚体。 I中的二聚体通过弱的CuS(硫酮)接触进一步延伸到链中。在配合物II和III的晶体堆积中,相邻配合物的两个平行phen分子之间存在弱的ππ相互作用。结果,可以以离子自旋S = 1/2的Cu〜2离子的交换耦合对的近似描述铜络合物的磁性和共振特性。镍配合物通过各向同性交换模型描述了单点自旋S = 1。

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