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Structural and magnetic studies of copper(II) and zinc(II) coordination complexes containing nitroxide radicals as chelating ligands

机译:含氮氧自由基作为螯合配体的铜(II)和锌(II)配合物的结构和磁性研究

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The mononuclear transition metal complexes [Cu(CF3SO3)(2)1(2)] (1a), [Zn(CF3SO3)(2)1(2)] (1b), [Cu(CF3SO3)(2)2(2)]center dot 2CH(3)CN (2a), and [Zn(CF3SO3)(2)2(2)]center dot 2CH(3)CN (2b) have been prepared from the newly synthesized doxyl nitroxide ligands 4,4-dimethyl-2,2-di(2-pyridyl)oxazolidine-N-oxyl (1) and 4,4-dimethyl-2,2-bis[2-(3-methylpyridyl)]oxazolidine-N-oxyl (2) and M(CF3SO3)2 (M = Cu-II or Zn-II). These metal-nitroxide complexes have been structurally and magnetically characterized. In all complexes, the four pyridyl groups coordinate in equatorial coordination sites and the two nitroxide groups in axial coordination sites, which means that the central metal ion acquires a distorted N4O2 octahedral configuration. The variable-temperature magnetic susceptibility data show that complexes 1b and 2b exhibit paramagnetic behavior, and hence a very weak intraligand magnetic interaction could be estimated [J(NO-NO) = -0.64 (1b) and 0.14 cm(-1) (2b)]. The chi T-m values of la and 2a decrease continuously with decreasing temperature until they reach a nearly constant value at around 50 K, thereby indicating an intramolecular antiferromagnetic interaction between the Cu-II ion and the nitroxide ligands for both la and 2a [J(CU-NO) = -81.6 (1a) and -78.1 cm(-1) (2b)]. These magnetic behaviors are supported by density functional theory calculations and are discussed in connection with the specific structural features. ((c) Wiley-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, Germany, 2006)
机译:单核过渡金属络合物[Cu(CF3SO3)(2)1(2)](1a),[Zn(CF3SO3)(2)1(2)](1b),[Cu(CF3SO3)(2)2(2) )]的中心点2CH(3)CN(2a)和[Zn(CF3SO3)(2)2(2)]中心点2CH(3)CN(2b)已从新合成的二甲苯基氮氧化物配体4,4制备-二甲基-2,2-二(2-吡啶基)恶唑烷-N-氧基(1)和4,4-二甲基-2,2-双[2-(3-甲基吡啶基)]恶唑烷-N-氧基(2)和M(CF3SO3)2(M = Cu-II或Zn-II)。这些金属-氮氧化物配合物已经在结构和磁性上进行了表征。在所有络合物中,四个吡啶基在赤道配位部位进行配位,两个氮氧化物在轴向配位部位进行配位,这意味着中心金属离子具有扭曲的N4O2八面体构型。变温磁化率数据表明,配合物1b和2b表现出顺磁行为,因此可以估计非常弱的配体内部磁相互作用[J(NO-NO)= -0.64(1b)和0.14 cm(-1)(2b )]。 1a和2a的chi Tm值随温度降低而连续降低,直到它们在50 K附近达到几乎恒定的值,从而表明1a和2a的Cu-II离子与一氧化氮配体之间的分子内反铁磁相互作用[J(CU -NO)= -81.6(1a)和-78.1 cm(-1)(2b)]。这些磁行为得到密度泛函理论计算的支持,并结合具体的结构特征进行了讨论。 ((c)Wiley-VCH Verlag GmbH&Co.KGaA,69451 Weinheim,Germany,2006)

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