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Cu(II)-叠氮多核配合物的 Cu4 建筑簇与席夫碱共配体:合成、结构、磁性行为和 DFT 研究。

Cu(II)-azide polynuclear complexes of Cu4 building clusters with Schiff-base co-ligands: synthesis, structures, magnetic behavior and DFT studies.

机构信息

Department of Inorganic and Physical Chemistry, Indian Institute of Science, Bangalore-560012, India.

出版信息

Dalton Trans. 2013 Mar 21;42(11):4019-30. doi: 10.1039/c2dt32802j. Epub 2013 Jan 22.

Abstract

Three new copper-azido complexes Cu(4)(N(3))(8)(L(1))(2) (1), [Cu(4)(N(3))(6)(L(2))(2)(H(2)O)(2)] (2), and Cu(4)(N(3))(6)(L(3))(2) (3) [L(1) is the imine resulting from the condensation of pyridine-2-carboxaldehyde with N-methylethylenediamine, HL(2) and HL(3) are the condensation products of 2-hydroxy-3-methoxybenzaldehyde with N,N-diethylethylenediamine and N-ethylethylenediamine respectively] have been synthesized by using 0.5 molar equivalents of the Schiff base ligands with Cu(NO(3))(2)·3H(2)O and an excess of NaN(3). Single crystal X-ray structures show that the basic unit of these complexes contains very similar Cu(II)(4) building blocks. While 1 and 3 have overall 1D structures, 2 forms discrete tetranuclear clusters due to blocking of two coordination sites on the tetranuclear cluster by water molecules. Magnetic susceptibility measurements over a wide range of temperatures exhibit the presence of both antiferromagnetic and ferromagnetic exchanges within the tetranuclear unit structures. Density functional theory calculations (using B3LYP functional and two different basis sets) have been performed on the complexes 1-3 to provide a qualitative theoretical interpretation of their overall magnetic behavior.

摘要

三种新型的铜叠氮配合物Cu(4)(N(3))(8)(L(1))(2)(1)、[Cu(4)(N(3))(6)(L(2))(2)(H(2)O)(2)](2)和Cu(4)(N(3))(6)(L(3))(2)(3)[L(1)是由吡啶-2-甲醛与 N-甲基乙二胺缩合而成的亚胺,HL(2)和 HL(3)分别是 2-羟基-3-甲氧基苯甲醛与 N,N-二乙基亚乙基二胺和 N-乙基亚乙基二胺缩合而成的产物],均采用 0.5 摩尔当量的席夫碱配体与 Cu(NO(3))(2)·3H(2)O 和过量的 NaN(3)合成。单晶 X 射线结构表明,这些配合物的基本单元包含非常相似的 Cu(II)(4)构建块。虽然 1 和 3 具有一维结构,但 2 由于水分子占据了四核簇的两个配位位,因此形成离散的四核簇。在很宽的温度范围内进行的磁化率测量显示,在四核单元结构内存在反铁磁和铁磁交换。对配合物 1-3 进行了密度泛函理论计算(使用 B3LYP 函数和两种不同的基组),以提供对其整体磁行为的定性理论解释。

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