Osa Shutaro, Sunatsuki Yukinari, Yamamoto Yoko, Nakamura Masaaki, Shimamoto Tomoshige, Matsumoto Naohide, Re Nazzareno
Department of Chemistry, Faculty of Science, Kumamoto University, Japan.
Inorg Chem. 2003 Sep 8;42(18):5507-12. doi: 10.1021/ic0344012.
A series of heterometal cyclic tetranuclear complexes Cu(II)LM(II)(hfac) (M(II) = Zn (1), Cu (2), Ni (3), Co (4), Fe(5), and Mn (6)) have been synthesized by the assembly reaction of K[CuL] and [M(II)(hfac)(2)(H(2)O)(2)] with a 1:1 mole ratio in methanol, where H(3)L = 1-(2-hydroxybenzamido)-2-((2-hydroxy-3-methoxybenzylidene)amino)ethane and Hhfac = hexafluoroacetylacetone. The crystal structures of 2, 4, and Cu(II)LMn(II)(acac) (6a) (Hacac = acetylacetone) were determined by single-crystal X-ray analyses. Each complex has a cyclic tetranuclear Cu(II)(2)M(II)(2) structure, in which the Cu(II) complex functions as a "bridging ligand complex", and the Cu(II) and M(II) ions are alternately arrayed. One side of the planar Cu(II) complex coordinates to one M(II) ion at the two phenoxo and the methoxy oxygen atoms, and the opposite side of the Cu(II) complex coordinates to another M(II) ion at the amido oxygen atom. The temperature-dependent magnetic susceptibilities revealed spin states of S(M) = 0, 1/2, 1, 3/2, 2, and 5/2 for the Zn(II), Cu(II), Ni(II), Co(II), Fe(II), and Mn(II) ions, respectively. Satisfactory fittings to the observed magnetic susceptibility data were obtained by assuming a rectangular arrangement with two different g-factors for the Cu(II) and M(II) ions, two different isotropic magnetic exchange interactions, J(1) and J(2), between the Cu(II) and M(II) ions, and a zero-field splitting term for the M(II) ion. In all cases, the antiferromagnetic coupling constants were found for both exchange interactions suggesting nonzero spin ground states with S(T) = 2/S(M) - S(Cu)/, which were confirmed by the analysis of the field-dependent magnetization measurements.
通过在甲醇中以1:1的摩尔比使K[CuL]与[M(II)(hfac)₂(H₂O)₂]进行组装反应,合成了一系列异金属环状四核配合物[Cu(II)LM(II)(hfac)]₂(M(II) = Zn (1)、Cu (2)、Ni (3)、Co (4)、Fe (5)和Mn (6)),其中H₃L = 1-(2-羟基苯甲酰胺基)-2-((2-羟基-3-甲氧基亚苄基)氨基)乙烷,Hhfac = 六氟乙酰丙酮。通过单晶X射线分析确定了2、4和[Cu(II)LMn(II)(acac)]₂(6a)(Hacac = 乙酰丙酮)的晶体结构。每个配合物都具有环状四核Cu(II)₂M(II)₂结构,其中Cu(II)配合物充当“桥联配体配合物”,Cu(II)和M(II)离子交替排列。平面Cu(II)配合物的一侧在两个苯氧基和甲氧基氧原子处与一个M(II)离子配位,Cu(II)配合物的另一侧在酰胺氧原子处与另一个M(II)离子配位。温度依赖的磁化率分别揭示了Zn(II)、Cu(II)、Ni(II)、Co(II)、Fe(II)和Mn(II)离子的自旋态为S(M) = 0、1/2、1、3/2、2和5/2。通过假设Cu(II)和M(II)离子具有两个不同的g因子的矩形排列、Cu(II)和M(II)离子之间的两种不同的各向同性磁交换相互作用J(1)和J(2)以及M(II)离子的零场分裂项,对观察到的磁化率数据进行了令人满意的拟合。在所有情况下,两种交换相互作用均发现了反铁磁耦合常数,表明自旋基态非零,S(T) = 2/S(M) - S(Cu)/,这通过对场依赖磁化测量的分析得到了证实。