Bräuer Björn, Weigend Florian, Fittipaldi Maria, Gatteschi Dante, Reijerse Edward J, Guerri Annalisa, Ciattini Samuele, Salvan Georgeta, Rüffer Tobias
Department of Chemistry, Chemnitz University of Technology, 09107 Chemnitz, Germany.
Inorg Chem. 2008 Aug 4;47(15):6633-44. doi: 10.1021/ic702460t. Epub 2008 Jul 2.
In this work we present the investigation of the influence of electronic and structural variations induced by varying the N,N'-bridge on the magnetic properties of Cu(II)- bis(oxamato) complexes. For this study the complexes [Cu(opba)] (2-) ( 1, opba = o-phenylene- bis(oxamato)), [Cu(nabo)] (2-) ( 2, nabo = 2,3-naphthalene- bis(oxamato)), [Cu(acbo)] (2-) ( 3, acbo = 2,3-anthrachinone- bis(oxamato)), [Cu(pba)] (2-) ( 4, pba = propylene- bis(oxamato)), [Cu(obbo)] (2-) ( 5, obbo = o-benzyl- bis(oxamato)), and [Cu(npbo)] (2-) ( 6, npbo = 1,8-naphthalene- bis(oxamato)), and the respective structurally isomorphic Ni(II) complexes ( 8- 13) have been prepared as ( (n)Bu 4N) (+) salts. The new complex ( (n)Bu 4N) 2[Cu(R-bnbo)].2H 2O ( 7, R-bnbo = (R)-1,1'-binaphthalene-2,2'- bis(oxamato)) was synthesized and is the first chiral complex in the series of Cu(II)-bis(oxamato) complexes. The molecular structure of 7 has been determined by single crystal X-ray analysis. The Cu(II) ions of the complexes 1- 7 are eta (4)(kappa (2) N, kappa (2) O) coordinated with a more or less distorted square planar geometry for 1- 6 and a distorted tetrahedral geometry for 7. Using pulsed Electron Nuclear Double Resonance on complex 6, detailed information about the relative orientation of the hyperfine ( A) and nuclear quadrupole tensors ( Q) of the coordinating nitrogens with respect to the g tensor were obtained. Electron Paramagnetic Resonance studies in the X, Q, and W-band at variable temperatures were carried out to extract g and A values of N ligands and Cu ion for 1- 7. The hyperfine values were interpreted in terms of spin population on the corresponding atoms. The obtained trends of the spin population for the monomeric building blocks were shown to correlate to the trends obtained in the dependence of the exchange interaction of the corresponding trinuclear complexes on their geometry.
在本工作中,我们研究了通过改变N,N'-桥所引起的电子和结构变化对Cu(II)-双(草酰胺)配合物磁性的影响。为此项研究,制备了配合物[Cu(opba)](2 -)(1,opba = 邻亚苯基-双(草酰胺))、[Cu(nabo)](2 -)(2,nabo = 2,3-萘-双(草酰胺))、[Cu(acbo)](2 -)(3,acbo = 2,3-蒽醌-双(草酰胺))、[Cu(pba)](2 -)(4,pba = 亚丙基-双(草酰胺))、[Cu(obbo)](2 -)(5,obbo = 邻苄基-双(草酰胺))和[Cu(npbo)](2 -)(6,npbo = 1,8-萘-双(草酰胺)),以及各自结构同构的Ni(II)配合物(8 - 13),它们均为((n)Bu₄N)(+)盐。合成了新配合物((n)Bu₄N)₂[Cu(R - bnbo)].2H₂O(7,R - bnbo = (R)-1,1'-联萘-2,2'-双(草酰胺)),它是Cu(II)-双(草酰胺)配合物系列中的首个手性配合物。通过单晶X射线分析确定了7的分子结构。配合物1 - 7的Cu(II)离子以η(4)(κ(2)N, κ(2)O)方式配位,其中1 - 6具有或多或少扭曲的平面正方形几何构型,7具有扭曲的四面体几何构型。利用对配合物6进行的脉冲电子核双共振,获得了关于配位氮的超精细(A)张量和核四极张量(Q)相对于g张量的相对取向的详细信息。在可变温度下于X、Q和W波段进行电子顺磁共振研究,以提取配合物1 - 7中N配体和Cu离子的g值和A值。根据相应原子上的自旋布居对超精细值进行了解释。结果表明,单体结构单元的自旋布居趋势与相应三核配合物的交换相互作用对其几何构型的依赖性所得到的趋势相关。