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Structural diversity and magnetic properties of five copper-organic frameworks containing one-, two-, and three-types of organic ligands. | LitMetric

Structural diversity and magnetic properties of five copper-organic frameworks containing one-, two-, and three-types of organic ligands.

Dalton Trans

Department of Chemistry, Key Laboratory of Advanced Energy Material Chemistry, MOE, TKL of Metal and Molecule Based Material Chemistry, Nankai University, Tianjin 300071, China.

Published: March 2013

Five novel compounds {[Cu(CMA)]·0.8H(2)O}(n) (1), {[Cu(CMA)(bpy)(0.5)]·0.5DMF}(n) (2), {[Cu(CMA)(bpy)(H(2)O)]·0.5H(2)O}(n) (3), {[Cu(2)(CMA)(DPA)(bpy)(2)(H(2)O)]ClO(4)}(n) (4) and {[Cu(3)(CMA)(DPA)(bpy)(4)(OH)](ClO(4))(2)·3H(2)O)}(n) (5) (H(2)CMA = 3-(carboxymethoxy)-5-methylbenzoic acid, HDPA = 2-(3,5-dimethylphenoxy)acetic acid, bpy = 4,4'-bipyridine) were synthesized and characterized by single crystal X-ray diffraction. Interestingly, the kinds of ligands included in these compounds are different: 1 contains single-ligand CMA(2-); 2 and 3 comprise two kinds of ligands (CMA(2-) and bpy); 4 and 5 cover three kinds of ligands (CMA(2-), DPA(-) and bpy). Structural analyses reveal that 1-3, and 5 are three-dimensional (3D) frameworks, while 4 is a 2D layer. Noteworthily, 1 possesses two types of channels: six-star and hexagonal ones. 3 displays a three-fold interpenetrating 3D framework. The structural diversity of the compounds may have originated from different anions, solvents and temperatures. Variable-temperature magnetic susceptibility measurements were carried out on compounds 1, 2 and 4, and the magnetic properties are dramatically different due to the structural diversities. The magnetic data of 1 shows an antiferromagnetic interaction with J = -54.84 cm(-1) estimated from the Bonner-Fisher model. The magnetic data of 2 was least-square fitted to the Blenaey-Bowers equation with J = -131.01 cm(-1), indicating the existence of a strong antiferromagnetic interaction between two adjacent Cu(2+). The magnetic data of linear tetranuclear structure 4 was best fitted to the expression derived from the Hamiltonian H = -2(2J(1)S(1)S(2) + J(2)S(1)S(1*)). The best fitting parameters are J(1) = -17.48 cm(-1) and J(2) = -65.26 cm(-1), which also indicate an antiferromagnetic interaction. Simultaneously, the magneto-structural relationship was discussed.

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Source
http://dx.doi.org/10.1039/c2dt32515bDOI Listing

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