Low-dimensional compounds containing cyanido groups. XXVI. Crystal structure, spectroscopic and magnetic properties of Co(II) complexes with non-linear pseudohalide ligands

From the systems Co(II) - L - C(CN)(3)(-)/N(CN)(2)(-) (L = 2,2'-bipyridine (bpy) or 1,10-phenanthroline (phen)) two dicyanamide (dca, N(CN)(2)(-)) and three tricyanomethanide (tcm, C(CN3-) complexes, [Co(phen)(2)(dca)(2)] (1a, 1b) [Co(phen)(3)](tcm)(2) (2), [{Co(phen)(2)(mu(1)-tcm)}(2)(mu(1,5)-tcm)]tcm center dot H2O (3), [CO(bpy)(mu(1,5)-tcm)(2)](n) (4) and [Co(bpy)(mu(1,5)-dca)(2)](n) (5), were isolated and characterized by X-ray crystallography, spectral and magnetic measurements. The Co(II) atoms in all the prepared complexes are coordinated by six nitrogen atoms forming a distorted octahedral environment. The mononuclear molecular complexes 1a and 1b are isomers, in which the Co(II) atoms are coordinated by two phen ligands and two dca anions in cis positions, while 2 is an ionic compound with the [Co(phen)(3)](2+) complex cation and two uncoordinated tcm anions. Their structures are stabilized by a combination of intermolecular pi-pi interactions between phen ligands and weak C-H center dot center dot center dot N hydrogen bonds. Compound 3 is ionic too, containing the binuclear [{Co(phen)(2) (mu(1)-tcm)}(2)(mu(1,5)-tcm)](+) complex cation, in which the Co(II) atoms are separated by 7.149 angstrom, one uncoordinated tcm anion and one disordered molecule of crystal water. Intermolecular pi-pi interactions between the phen ligands, C-N center dot center dot center dot Cg (pi-ring) contacts between tcm anions and phen ligands and hydrogen bonds link the individual components in 3 into a three-dimensional network. Both molecules of the pseudohalide ligands in the isostructural polymeric complexes 4 and 5 act as bridging ligands and link neighboring Co(II) atoms by double bridges, giving zig-zag chains which are connected by pi-pi interactions between L molecules from neighboring chains to form a two-dimensional network. The magnetic properties of the mononuclear complexes 1 and 2 are dominated by a considerable zero-field splitting, D/hc = 80-100 cm(-1). In the dinuclear complex 3 only a weak exchange interaction of an antiferromagnetic nature applies. In the polymeric complexes 4 and 5 the exchange coupling again is low so that a model of mononuclear complexes with sizable zero-field splitting is appropriate. (C) 2014 Elsevier Ltd. All rights reserved.