Iron(II) 2-methylimidazolate and copper(II) 1,2,4-triazolate complexes: systems exhibiting long-range ferromagnetic ordering at low temperatures

Crystals of [Fe(2-methylimidazolate)(2). 0.13(FeCp2)](x), 1, are orthorhomb ic, a = 8.0654(11), b = 15.3504(5), c = 19.3388(9) Angstrom, Z = 8, space g roup Pnnm. The structure was solved by direct methods and refined by full-m atrix least-squares procedures to R (F, I greater than or equal to 3 sigma( I)) = 0.057 (R-w (F-2, all data) = 0.142). The structure involves tetrahedr al iron(II) centers linked in chains by single imidazolate ligand bridges. The chains are cross-linked by additional imidazolates to generate a comple x 3-D network of linear channels in which ferrocene molecules are trapped. [Cu(1,2,4-triazolate)(2)](x), 2, is shown by indirect evidence to have a po lymeric structure in which copper(II) ions are bridged by triazolate ligand s. Magnetic susceptibilities were measured on powdered samples over the tem perature range 2-300 K at applied fields of 0-55 000 G. Both materials exhi bit antiferromagnetic exchange at temperatures above a magnetic phase trans ition: 27 K for 1 and 35 K for 2. At temperatures below these transitions t he compounds exhibit weak ferromagnetism, likely resulting from canted spin structures. Cycling the applied magnetic field between +55 000 G and -55 0 00 G at 4.8 K generates hysteresis loops for both materials. Remnant magnet izations of 200 and 55 cm(3) G mol(-1) and coercive fields of 5000 and 2500 G are obtained for 1 and 2, respectively.