Kumar Pawan, Swain Abinash, Acharya Joydev, Li Yanling, Kumar Vierandra, Rajaraman Gopalan, Colacio Enrique, Chandrasekhar Vadapalli
Department of Chemistry, Indian Institute of Technology Kanpur, Kanpur 208016, India.
Department of Chemistry, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India.
Inorg Chem. 2022 Aug 1;61(30):11600-11621. doi: 10.1021/acs.inorgchem.2c01041. Epub 2022 Jul 18.
The synthesis, structure, and magnetic properties of three Dy complexes of different nuclearity, [Dy(HL)(NO)] [NO]·2HO·CHOH (), [Dy(HL)(piv)(OH)] (), and [Dy(HL)(μ-OH)(μ-CO)(CHOH)(HO)] 5Cl·3HO () [(HL) = 6-((bis(2-hydroxyethyl)amino)-'-(2-hydroxybenzylidene)picolinohydrazide)], are described. This variety of complexes with the same ligand could be obtained by playing with the metal-to-ligand molar ratio, the type of Dy salt, the kind of base, and the presence/absence of coligand. is a dinuclear complex, while is a tetranuclear assembly with a butterfly-shaped topology. is a homometallic hexanuclear complex that exhibits a propeller-shaped topology. Interestingly, in this complex , three atmospheric carbon dioxide molecules are trapped in the form of carbonate ions, which assist in holding the hexanuclear complex together. All of the complexes reveal a slow relaxation of magnetization even in zero applied field. Complex is a zero-field SMM with an effective energy barrier () of magnetization reversal equal to 87(1) K and a relaxation time of τ = 6.4(3) × 10 s. Under an applied magnetic field of 0.1 T, these parameters change to = 101(3) K, τ = 2.5(1) × 10 s. Complex shows zero-field SMM behavior with = 31(2) K, τ = 4.2(1) × 10 s or τ = 2(1) × 10 s, = 37(8) K, τ = 5(6) × 10 s, and = 8(4) by considering two Orbach relaxation processes, while , also a zero-field SMM, shows a double relaxation of magnetization [ = 62.4(3) K, τ = 4.6(3) × 10 s, and = 2(1) K, τ = 4.6(2) × 10 s]. The calculations indicated that in these complexes, the Kramer's ground doublet is characterized by an axial g-tensor with the prevalence of the = ±15/2 component, as well as that due to the weak magnetic coupling between the metal centers, the magnetic relaxation, which is dominated by the single Dy centers rather than by the exchange-coupled states, takes place via Raman/Orbach or TA-QTM. Moreover, theoretical calculations support a toroidal magnetic state for complex .
描述了三种不同核数的镝配合物[Dy(HL)(NO)] [NO]·2HO·CHOH ()、[Dy(HL)(piv)(OH)] ()和[Dy(HL)(μ - OH)(μ - CO)(CHOH)(HO)] 5Cl·3HO ()的合成、结构和磁性,其中[(HL) = 6 - ((双(2 - 羟乙基)氨基)-'-(2 - 羟基亚苄基)吡啶酰肼)]。通过改变金属与配体的摩尔比、镝盐的类型、碱的种类以及共配体的存在与否,可以得到具有相同配体的多种配合物。是双核配合物,而 是具有蝶形拓扑结构的四核组装体。是具有螺旋桨形拓扑结构的同金属六核配合物。有趣的是,在这种配合物 中,三个大气二氧化碳分子以碳酸根离子的形式被困住,有助于将六核配合物保持在一起。所有配合物即使在零外加磁场下也显示出磁化的缓慢弛豫。配合物 是零场单分子磁体,磁化反转的有效能垒()等于87(1) K,弛豫时间为τ = 6.4(3)×10 s。在0.1 T的外加磁场下,这些参数变为 = 101(3) K,τ = 2.5(1)×10 s。配合物 显示零场单分子磁体行为,考虑两个奥巴赫弛豫过程时, = 31(2) K,τ = 4.2(1)×10 s或τ = 2(1)×10 s, = 37(8) K,τ = 5(6)×10 s, = 8(4),而同样是零场单分子磁体的 显示出磁化的双重弛豫[ = 62.4(3) K,τ = 4.6(3)×10 s, = 2(1) K,τ = 4.6(2)×10 s]。计算表明,在这些配合物中,克莱默斯基态双重态的特征是轴向g张量,其中 = ±15/2分量占主导,并且由于金属中心之间的弱磁耦合,磁化弛豫主要由单个镝中心而非交换耦合态主导,通过拉曼/奥巴赫或TA - QTM发生。此外,理论计算支持配合物 的环形磁态。