Palacios María A, Nehrkorn Joscha, Suturina Elizaveta A, Ruiz Eliseo, Gómez-Coca Silvia, Holldack Karsten, Schnegg Alexander, Krzystek Jurek, Moreno José M, Colacio Enrique
Departamento de Química Inorgánica, Facultad de Ciencias, Universidad de Granada, 18071, Granada, Spain.
Department of Chemistry, University of Washington, Box 351700, Seattle, WA, 98195, USA.
Chemistry. 2017 Aug 25;23(48):11649-11661. doi: 10.1002/chem.201702099. Epub 2017 Jul 27.
Three new closely related Co Y complexes of general formula [Co(μ-L)(μ-X)Y(NO ) ] (X =NO 1, benzoate 2, or 9-anthracenecarboxylato 3) have been prepared with the compartmental ligand N,N',N''-trimethyl-N,N''-bis(2-hydroxy-3-methoxy-5-methylbenzyl)diethylenetriamine (H L). In these complexes, Co and Y are triply bridged by two phenoxide groups belonging to the di-deprotonated ligand (L ) and one ancillary anion X . The change of the ancillary bridging group connecting Co and Y ions induces small differences in the trigonally distorted CoN O coordination sphere with a concomitant tuning of the magnetic anisotropy and intermolecular interactions. Direct current magnetic, high-frequency and -field EPR (HFEPR), frequency domain Fourier transform THz electron paramagnetic resonance (FD-FT THz-EPR) measurements, and ab initio theoretical calculations demonstrate that Co ions in compounds 1-3 have large and positive D values (≈50 cm ), which decrease with increasing the distortion of the pseudo-octahedral Co coordination sphere. Dynamic ac magnetic susceptibility measurements indicate that compound 1 exhibits field-induced single-molecule magnet (SMM) behavior, whereas compounds 2 and 3 only display this behavior when they are magnetically diluted with diamagnetic Zn (Zn/Co=10:1). In view of this, it is always advisable to use magnetically diluted complexes, in which intermolecular interactions and quantum tunneling of magnetism (QTM) would be at least partly suppressed, so that "hidden single-ion magnet (SIM)" behavior could emerge. Field- and temperature-dependence of the relaxation times indicate the prevalence of the Raman process in all these complexes above approximately 3 K.
已用间隔配体N,N',N''-三甲基-N,N''-双(2-羟基-3-甲氧基-5-甲基苄基)二亚乙基三胺(H₃L)制备了三种通式为[Co(μ-L)(μ-X)Y(NO₃)₂](X = NO₃⁻ 1、苯甲酸根 2 或 9-蒽甲酸根 3)的紧密相关的新型钴配合物。在这些配合物中,Co和Y通过属于双去质子化配体(L³⁻)的两个酚氧基和一个辅助阴离子X³⁻ 三重桥连。连接Co和Y离子的辅助桥连基团的变化在三角畸变的CoN₅O配位球中引起微小差异,同时伴随着磁各向异性和分子间相互作用的调节。直流磁性、高频和高场电子顺磁共振(HFEPR)、频域傅里叶变换太赫兹电子顺磁共振(FD-FT THz-EPR)测量以及从头算理论计算表明,化合物1-3中的Co离子具有大的正D值(≈50 cm⁻¹),该值随着伪八面体Co配位球畸变的增加而减小。动态交流磁化率测量表明,化合物1表现出场诱导单分子磁体(SMM)行为,而化合物2和3仅在被抗磁性Zn²⁺(Zn/Co = 10:1)磁稀释时才表现出这种行为。鉴于此,使用磁稀释配合物总是明智的,其中分子间相互作用和磁量子隧穿(QTM)将至少部分受到抑制,从而可能出现“隐藏单离子磁体(SIM)”行为。弛豫时间的场和温度依赖性表明,在大约3 K以上的所有这些配合物中,拉曼过程占主导。