Pandey Priya, Chauhan Deepanshu, Walawalkar Mrinalini G, Gupta Sandeep K, Meyer Franc, Rajaraman Gopalan, Murugavel Ramaswamy
Department of Chemistry, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India.
Institute of Inorganic Chemistry, University of Göttingen, Göttingen D-37077, Germany.
Inorg Chem. 2024 Jul 1;63(26):11963-11976. doi: 10.1021/acs.inorgchem.4c00332. Epub 2024 Jun 13.
Synthesis of nonameric cationic clusters [Dy(acac)(μ-OH)(μ-OH)]OH·6HO (), [DyTb (acac)(μ-OH)(μ-OH)]OH·2HO (), and [Gd(acac)(μ-OH)(μ-OH)]OH·6HO () (acac = acetylacetonate) is reported. The emission spectrum of shows Dy(III) ion characteristic bands assignable to the F → H ( = 15/2 to 9/2) transitions. Emission due to both Dy(III) and Tb(III) ions is observed for in the visible range, with Tb(III) specific bands appearing due to the D → F ( = 6, 4, and 3) transitions. Cluster exhibits a significant magnetocaloric effect (MCE), with -Δ values increasing with decrease in temperature and increase in field, reaching -Δ = 20.98 J kg K at 2 K and 9 T. Isotropic magnetic coupling constants () in derived from density functional theory (DFT) calculations reveal that the exchange interactions are antiferromagnetic and weak. Compound possesses = 7/2 ground state arising from the central Gd(III) ion along with several nested excited states due to competing antiferromagnetic interactions that yield reasonably large MCE values. Utilizing computed exchange coupling interactions, we have performed ab initio CASSCF/RASSI-SO/POL_ANISO calculations on antiferromagnetic and to estimate the exchange interactions using the Lines model. For , Dy(III)···Tb(III) exchange interactions were extracted for the first time and were found to be weakly antiferromagnetically coupled.
报道了九聚体阳离子簇合物[Dy(acac)(μ-OH)(μ-OH)]OH·6H₂O()、[DyTb(acac)(μ-OH)(μ-OH)]OH·2H₂O()和[Gd(acac)(μ-OH)(μ-OH)]OH·6H₂O()(acac = 乙酰丙酮)的合成。的发射光谱显示了可归因于F→H(J = 15/2至9/2)跃迁的Dy(III)离子特征带。对于,在可见光范围内观察到了Dy(III)和Tb(III)离子的发射,由于D→F(J = 6、4和3)跃迁出现了Tb(III)的特定谱带。簇合物表现出显著的磁热效应(MCE),-ΔS值随着温度降低和磁场增加而增大,在2 K和9 T时达到-ΔS = 20.98 J kg⁻¹ K⁻¹。从密度泛函理论(DFT)计算得出的中的各向同性磁耦合常数(J)表明,交换相互作用是反铁磁性的且较弱。化合物由于中心Gd(III)离子产生了S = 7/2基态以及由于竞争反铁磁相互作用导致的几个嵌套激发态,从而产生了相当大的MCE值。利用计算得到的交换耦合相互作用,我们对反铁磁性的和进行了从头算CASSCF/RASSI-SO/POL_ANISO计算,以使用Lines模型估计交换相互作用。对于,首次提取了Dy(III)···Tb(III)交换相互作用,发现其为弱反铁磁耦合。