Oyarzabal Itziar, Ruiz José, Seco José Manuel, Evangelisti Marco, Camón Agustín, Ruiz Eliseo, Aravena Daniel, Colacio Enrique
Departamento de Química Aplicada, Facultad de Química, UPV/EHU, Paseo Manuel de Lardizabal 3, 20018 Donostia-San Sebastián (Spain).
Chemistry. 2014 Oct 27;20(44):14262-9. doi: 10.1002/chem.201403670. Epub 2014 Sep 24.
Two novel trinuclear complexes [ZnCl(μ-L)Ln(μ-L)ClZn][ZnCl3 (CH3 OH)]⋅3 CH3 OH (Ln(III) =Dy (1) and Er (2)) have been prepared from the compartmental ligand N,N'-dimethyl-N,N'-bis(2-hydroxy-3-formyl-5-bromo-benzyl)ethylenediamine (H2 L). X-ray studies reveal that Ln(III) ions are coordinated by two ZnCl(L) units through the phenoxo and aldehyde groups, giving rise to a LnO8 coordination sphere with square-antiprism geometry and strong easy-axis anisotropy of the ground state. Ab initio CASSCF+RASSI calculations carried out on 1 confirm that the ground state is an almost pure MJ =±15/2 Kramers doublet with a marked axial anisotropy, the magnetic moment is roughly collinear with the shortest DyO distances. This orientation of the local magnetic moment of the Dy(III) ion in 1 is adopted to reduce the electronic repulsion between the oblate electron shape of the MJ =±15/2 Kramers doublet and the phenoxo-oxygen donor atoms involved in the shortest DyO bonds. CASSCF+RASSI calculations also show that the ground and first excited states of the Dy(III) ion are separated by 129 cm(-1) . As expected for this large energy gap, compound 1 exhibits, in a zero direct-current field, thermally activated slow relaxation of the magnetization with a large Ueff =140 K. The isostructural Zn-Er-Zn species does not present significant SMM behavior as expected for the prolate electron-density distribution of the Er(III) ion leading to an easy-plane anisotropy of the ground doublet state.
通过隔室配体N,N'-二甲基-N,N'-双(2-羟基-3-甲酰基-5-溴苄基)乙二胺(H₂L)制备了两种新型三核配合物[ZnCl(μ-L)Ln(μ-L)ClZn][ZnCl₃(CH₃OH)]⋅3 CH₃OH (Ln(III)=Dy (1)和Er (2))。X射线研究表明,Ln(III)离子通过苯氧基团和醛基与两个[ZnCl(L)]⁻单元配位,形成具有四方反棱柱几何结构和基态强易轴各向异性的LnO₈配位球。对1进行的从头算CASSCF+RASSI计算证实,基态是几乎纯的MJ =±15/2克莱默斯二重态,具有明显的轴向各向异性,磁矩大致与最短的DyO距离共线。1中Dy(III)离子的局部磁矩的这种取向被采用以减少MJ =±15/2克莱默斯二重态的扁球形电子形状与最短DyO键中涉及的苯氧-氧供体原子之间的电子排斥。CASSCF+RASSI计算还表明,Dy(III)离子的基态和第一激发态被129 cm⁻¹隔开。正如对这个大的能隙所预期的那样,化合物1在零直流场中表现出热激活的磁化缓慢弛豫,Ueff =140 K。如预期的那样,对于具有基态二重态易平面各向异性的Er(III)离子的长球形电子密度分布,同构的Zn-Er-Zn物种没有呈现出显著的单分子磁体行为。