Manzur Jorge, Mora Hector, Vega Andrés, Spodine Evgenia, Venegas-Yazigi Diego, Garland María Teresa, El Fallah M Salah, Escuer Albert
Departamento de Ciencia de los Materiales, Facultad de Ciencias Físicas y Matemáticas, Universidad de Chile, Tupper 2069, Santiago, Chile.
Inorg Chem. 2007 Aug 20;46(17):6924-32. doi: 10.1021/ic700544b. Epub 2007 Jul 26.
Two new ligands, 2-[(bis(2-pyridylmethyl)amino)methyl]-4-methylphenol (HL) and 2-[(bis(2-pyridylmethyl)amino)methyl]-4-methyl-6-(methylthio)phenol (HSL), were synthesized and were used to prepare the trinuclear copper(II) complex {[CuSL(Cl)]2Cu}(PF6)2.H2O (1) and the corresponding binuclear complexes Cu2(SL)22 (2) and Cu2L22 (3). The crystal structure of 1 shows two different coordination environments: two square base pyramidal centers (Cu1 and Cu1a, related by a C2 axes), acting as ligands of a distorted square planar copper center (Cu2) by means of the sulfur atom of the SCH3 substituent and the bridging phenoxo oxygen atom of the ligand (Cu2-S = 2.294 A). Compounds 2 and 3 show two equivalent distorted square base pyramidal copper(II) centers, bridged in an axial-equatorial fashion by two phenoxo groups, thus defining an asymmetric Cu2O2 core. A long copper-sulfur distance measured in 2 (2.9261(18) A) suggests a weak bonding interaction. This interaction induces a torsion angle between the methylthio group and the phenoxo plane resulting in a dihedral angle of 41.4(5) degrees. A still larger distortion is observed in 1 with a dihedral angle of 74.0(6) degrees. DFT calculations for 1 gave a ferromagnetic exchange between first neighbors interaction, the calculated J value for this interaction being +11.7 cm-1. In addition, an antiferromagnetic exchange for 1 was obtained for the second neighbor interaction with a J value of -0.05 cm-1. The Bleaney-Bowers equation was used to fit the experimental magnetic susceptibility data for 2 and 3; the best fit was obtained with J values of +3.4 and -16.7 cm-1, respectively. DFT calculations for 2 and 3 confirm the nature and the values of the J constants obtained by the fit of the experimental data. ESR and magnetic studies on the reported compounds show a weak exchange interaction between the copper(II) centers. The low values obtained for the coupling constants can be explained in terms of a poor overlap between the magnetic orbitals, due to the axial-equatorial phenoxo bridging mode observed in these complexes.
合成了两种新的配体,2-[(双(2-吡啶甲基)氨基)甲基]-4-甲基苯酚(HL)和2-[(双(2-吡啶甲基)氨基)甲基]-4-甲基-6-(甲硫基)苯酚(HSL),并用于制备三核铜(II)配合物{[CuSL(Cl)]2Cu}(PF6)2·H2O(1)以及相应的双核配合物Cu2(SL)22(2)和Cu2L22(3)。1的晶体结构显示出两种不同的配位环境:两个方形底锥中心(Cu1和Cu1a,通过C2轴相关),通过SCH3取代基的硫原子和配体的桥连苯氧原子作为扭曲方形平面铜中心(Cu2)的配体(Cu2-S = 2.294 Å)。化合物2和3显示出两个等效的扭曲方形底锥铜(II)中心,由两个苯氧基以轴向-赤道方式桥连,从而定义了一个不对称的Cu2O2核。在2中测得的长铜-硫距离(2.9261(18) Å)表明存在弱键相互作用。这种相互作用导致甲硫基与苯氧平面之间产生扭转角,从而产生41.4(5)度的二面角。在1中观察到更大的扭曲,二面角为74.0(6)度。对1的密度泛函理论(DFT)计算给出了第一近邻相互作用之间的铁磁交换,该相互作用的计算J值为+11.7 cm-1。此外,对于1的第二近邻相互作用获得了反铁磁交换,J值为-0.05 cm-1。使用Bleaney-Bowers方程拟合2和3的实验磁化率数据;分别用+3.4和-16.7 cm-1的J值获得了最佳拟合。对2和3的DFT计算证实了通过拟合实验数据获得的J常数的性质和值。对所报道化合物的电子顺磁共振(ESR)和磁性研究表明铜(II)中心之间存在弱交换相互作用。由于在这些配合物中观察到的轴向-赤道苯氧基桥连模式,耦合常数的低值可以用磁轨道之间的重叠不佳来解释。