Abstract
Seven new complexes of nickel(II), derived from azido, thiocyanato and nitrito bridging ligands and N,N,N′-trimethylethylenediamine (N,N,N′-Me3en) as blocking ligand, were synthesised and characterised; four of them are one-dimensional compounds: [Ni(μ1, 3-N3)(N,N,N′-Me3en)2]n(ClO4)n1, [Ni(μ1, 3-N3)(N,N,N′-Me3en)2]n(PF6)n2, [Niμ1, 1-N3)(μ1, 3-N3)(N,N,N′-Me3en)]n3, [Ni(μ-SCN)2(N,N,N′-Me3en)]n4, and three mononuclear: [Ni(NCS)2(N,N,N′-Me3en)2] 5, [Ni(NO2)(N,N,N′-Me3en)2]PF66, [Ni(NO2)2(N,N,N′-Me3en)] 7. Crystal structures for 3 and 6 were determined by X-ray diffraction methods. Compound 3 may be described as a one-dimensional system with double azido bridging ligands alternately in end-on and end-to-end co-ordination modes. Compound 6 is a mononuclear complex in which a nitrito ligand acts as a chelate. The magnetic properties of all the compounds were studied by susceptibility measurements vs. temperature. The χMvs.T plots for 1 and 2 show the typical shape for moderate antiferromagnetic one-dimensional nickel(II) complexes, while global strong antiferromagnetic behaviour with a maximum at about 200 K is observed for 3 and 4 exhibits a very weak ferromagnetic interaction. Compounds 5, 6, and 7 follow the Curie law, typical behaviour of mononuclear NiII compounds. The superexchange parameter J for 1, 2 and 4 was deduced from the spin Hamiltonian −JΣSiSi+1 and from −Σ(JAFS2iS2i+1 + JFS2iS2i−1) for 3. J values for 1 and 2 are −15.5 and −16.6 cm−1, respectively, JAF = −132 cm−1 and JFM = 99 cm−1 for 3, and 1.34 cm−1 for 4.
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