Korzeniak Tomasz, Desplanches Cédric, Podgajny Robert, Giménez-Saiz Carlos, Stadnicka Katarzyna, Rams Michał, Sieklucka Barbara
Faculty of Chemistry, Jagiellonian University, Ingardena 3, 30-060 Krakow, Poland.
Inorg Chem. 2009 Apr 6;48(7):2865-72. doi: 10.1021/ic801989b.
We report on the syntheses, crystal structures, and magnetic properties of two cyano-bridged molecular assemblies: Cu(II)(phen)(3){Cu(II)(phen)(2)W(V)(CN)(8)}(ClO(4))(2) x 10 H(2)O (phen = 1,10-phenanthroline) (1) and {Cu(II)(bpy)(2)[W(V)(CN)(8)]} {[Cu(II)(bpy)(2)][W(V)(CN)(8)]} x 4 H(2)O (bpy = 2,2'-bipyridyl) (2). Compound 1 consists of cyano-bridged Cu(II)(2)W(V)(2) molecular rectangles and isolated Cu(II)(phen)(3) complexes. The molecular structure of 2 reveals cyano-bridged trinuclear Cu(II)(2)W(V) and dinuclear Cu(II)W(V) ions. Magnetic interactions in 1 are interpreted in terms of the model of a tetranuclear moiety consisting of two ferromagnetic Cu(II)-NC-W(V) units (J(1) = +39(4) cm(-1)) interacting antiferromagnetically (J(2) = -1.6(4) cm(-1)). The analysis of the magnetic response of 2 reveals ferromagnetic interaction within the Cu(II)-NC-W(V)-CN-Cu(II) and Cu(II)-NC-W(V) isolated units, characterized by J = +35(7) cm(-1) and antiferromagnetic coupling between them (4J' = -0.30(8) cm(-1)). The discussion of the magnetic behavior and the correlation of the J(CuW) parameters with the geometry of cyano bridges at copper(II) centers of 1 and 2 is based on the DFT calculations, which yield J(av) = +13.2 cm(-1) for 1 and J = +31 cm(-1) for 2. The domination of the ferromagnetic Cu(II)-NC-W(V) interaction in 1 and 2 originates from the mutual orthogonality of natural magnetic orbitals in the case of coordination of cyano bridges at the equatorial sites of Cu(II) moieties.
我们报道了两种氰基桥联分子组装体的合成、晶体结构和磁性:Cu(II)(phen)(3){Cu(II)(phen)(2)W(V)(CN)(8)}(ClO(4))(2)·10H(2)O(phen = 1,10 - 菲咯啉)(1)和{Cu(II)(bpy)(2)[W(V)(CN)(8)]}{[Cu(II)(bpy)(2)][W(V)(CN)(8)]}·4H(2)O(bpy = 2,2'-联吡啶)(2)。化合物1由氰基桥联的[Cu(II)(2)W(V)(2)](2 - )分子矩形和孤立的[Cu(II)(phen)(3)](2 + )配合物组成。2的分子结构揭示了氰基桥联的三核Cu(II)(2)W(V)和双核Cu(II)W(V)离子。1中的磁相互作用根据由两个铁磁Cu(II)-NC-W(V)单元(J(1) = +39(4) cm(-1))反铁磁相互作用(J(2) = -1.6(4) cm(-1))组成的四核部分模型来解释。对2的磁响应分析揭示了Cu(II)-NC-W(V)-CN-Cu(II)和Cu(II)-NC-W(V)孤立单元内的铁磁相互作用,其特征为J = +35(7) cm(-1),以及它们之间的反铁磁耦合(4J' = -0.30(8) cm(-1))。对1和2的磁性行为以及J(CuW)参数与1和2的铜(II)中心处氰基桥几何结构的相关性的讨论基于密度泛函理论计算,其得出1的J(av) = +13.2 cm(-1),2的J = +31 cm(-1)。1和2中铁磁Cu(II)-NC-W(V)相互作用的主导源于在Cu(II)部分赤道位置处氰基桥配位情况下自然磁轨道的相互正交性。