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首页> 外文期刊>Polyhedron: The International Journal for Inorganic and Organometallic Chemistry >Azido-bridged Cu(II) compounds with asymmetric end-to-end and end-on binding modes: magnetic assignments using a spin dimer model
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Azido-bridged Cu(II) compounds with asymmetric end-to-end and end-on binding modes: magnetic assignments using a spin dimer model

机译:具有不对称端对端和端对端结合模式的叠氮桥联Cu(II)化合物:使用自旋二聚体模型的磁性分配

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Dinuclear [Cu(aepi)(N-3)(2)](2) (1) [aepi = 1-(2-aminoethyl)piperidine] and 1D chain [Cu(aepy)(N-3)(2)](n)(2) [aepy = 1-(2-aminoethyl)pyrrolidine] have been prepared and characterized by means of X-ray analysis and magnetic measurements. For 1, the Cu(II) centers are doubly bridged by end-on (EO) azido units in a basal-apical fashion. The molecular structure of 2 features magnetic centers that are linked by alpha-1,1,3 azido groups, forming a 1D chain with alternating EO and end-to-end (EE) azido bridging patterns. The magnetic data for the dinuclear complex 1 were fitted with the Bleaney-Bowers equation derived from the Hamiltonian H = -JS(1) . S-2, affording parameters of g = 2.093(1), J = -3.06(l) cm(-1) and zJ' = -1.32(3) cm(-1). This indicates that the EO azido group mediates an antiferromagnetic interaction. Complex 2 has two possible magnetic pathways: one is through the EO azido bridge (J(eo)) and the other via the EE bridge (J(ee)). The alternating chain model with ferromagnetic and anti ferromagnetic interactions based on the exchange Hamiltonian H = -Sigma(i)[J(1)S(2i) . S2i+1 + J(2)S(2i) . S2i-1] was employed, leading to g = 2.076(2), J(1) = -3.22(5) cm(-1), J(2) = 17.0(5) cm(-1) and zJ' = -1.34(6) cm(-1). By taking into account structural parameters of 1 and 2, it is rationally suggested that J(1) and J(2) are ascribed to J(eo) and J(ee), respectively. These assignments are also ascertained by MO calculations using a spin dimer model. (C) 2004 Elsevier Ltd. All rights reserved.
机译:双核[Cu(aepi)(N-3)(2)](2)(1)[aepi = 1-(2-氨基乙基)哌啶]和一维链[Cu(aepy)(N-3)(2)] (n)(2)[aepy = 1-(2-氨基乙基)吡咯烷]已制备并通过X射线分析和磁测量进行了表征。对于1,Cu(II)中心由底(EO)叠氮基单元以基顶方式双重桥接。 2的分子结构具有磁性中心,这些中心由alpha-1,1,3叠氮基基团链接,形成一维链,具有交替的EO和端到端(EE)叠氮基桥接模式。用从哈密顿量H = -JS(1)导出的Bleaney-Bowers方程拟合双核配合物1的磁数据。 S-2,提供参数g = 2.093(1),J = -3.06(1)cm(-1),z′′=-1.32(3)cm(-1)。这表明EO叠氮基团介导反铁磁相互作用。配合物2具有两种可能的磁路:一种是通过EO叠氮桥(J(eo)),另一种是通过EE桥(J(ee))。基于交换哈密顿量H = -Sigma(i)[J(1)S(2i)的具有铁磁和反铁磁相互作用的交替链模型。 S2i + 1 + J(2)S(2i)使用S2i-1],导致g = 2.076(2),J(1)= -3.22(5)cm(-1),J(2)= 17.0(5)cm(-1)和zJ'= -1.34(6)cm(-1)。通过考虑结构参数1和2,可以合理地建议将J(1)和J(2)分别归因于J(eo)和J(ee)。这些分配也可以通过使用自旋二聚体模型的MO计算来确定。 (C)2004 Elsevier Ltd.保留所有权利。

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