Kharwar Ajit Kumar, Mondal Arpan, Konar Sanjit
Department of Chemistry, Indian Institute of Science Education and Research Bhopal, Bhopal Bypass Road, Bhouri, MP, India.
Dalton Trans. 2021 Mar 2;50(8):2832-2840. doi: 10.1039/d0dt04065g.
Two CoII based complexes namely [Co(IAP)(SCN)2] (1) and {[Co(IPEH)2(SCN)2]·H2O}n (2) (where IPEH = (((1E,2E)-1,2-bis(1-(4-(1H-imidazol-1-yl)phenyl)ethylidene)hydrazine) and IAP = (4'-(imidazol-1-yl)acetophenone)) have been synthesized and characterized by single-crystal X-ray diffraction, magnetic measurements and ab initio calculations. Structural analysis revealed that complex 1 has a zero-dimensional mononuclear structure and complex 2 has a two-dimensional framework where the CoII centers are bridged by bis(monodentate) ligand IPEH. In both the complexes, the CoII center has a distorted octahedral geometry with a CoN6 coordination environment, formed by four equatorial N atoms from the neutral ligand and two NCS- at the axial positions. Detailed magnetic measurements reveal the presence of easy-plane magnetic anisotropy for both the complexes, whereas the field-induced slow relaxation of magnetization is observed at a relatively higher temperature in 1 (above 2 K, Ueff = 30 K) as compared to 2 (below 2 K, Ueff = 6.5 K). The ab initio calculations show the negligible effect of the first coordination sphere as similar anisotropic parameters are obtained for both the complexes. Additionally, it was found that the anisotropic axes are aligned well in a particular direction in complex 1 whereas it is randomly oriented in the framework of 2. The parallel orientation of the anisotropic axes enhances the axial anisotropy and reduces the transverse component, resulting in a higher energy barrier (Ueff = 30 K) in complex 1. The detailed analysis of field and temperature dependence of relaxation time indicates that Raman, direct and QTM processes mainly play an important role in the relaxation dynamics of complex 1.
合成了两种基于钴的配合物,即[Co(IAP)(SCN)₂] (1) 和 {[Co(IPEH)₂(SCN)₂]·H₂O}ₙ (2)(其中IPEH = (((1E,2E)-1,2-双(1-(4-(1H-咪唑-1-基)苯基)亚乙基)肼) 且IAP = (4'-(咪唑-1-基)苯乙酮)),并通过单晶X射线衍射、磁性测量和从头算进行了表征。结构分析表明,配合物1具有零维单核结构,配合物2具有二维框架结构,其中CoII中心由双(单齿)配体IPEH桥连。在这两种配合物中,CoII中心具有扭曲的八面体几何结构,具有CoN₆配位环境,由来自中性配体的四个赤道面N原子和轴向位置的两个NCS⁻形成。详细的磁性测量表明,这两种配合物都存在易平面磁各向异性,而与配合物2(低于2 K,Ueff = 6.5 K)相比,在配合物1中在相对较高的温度(高于2 K,Ueff = 30 K)下观察到场诱导的磁化慢弛豫。从头算计算表明,第一配位层的影响可忽略不计,因为两种配合物获得了相似的各向异性参数。此外,发现配合物1中各向异性轴在特定方向上排列良好,而在配合物2的框架中则随机取向。各向异性轴的平行取向增强了轴向各向异性并降低了横向分量,导致配合物1中具有更高的能垒(Ueff = 30 K)。对弛豫时间的场和温度依赖性的详细分析表明,拉曼、直接和量子隧穿过程在配合物1的弛豫动力学中主要起重要作用。