VIII2LnIII2蝴蝶配合物中单离子各向异性与磁性3d - 4f相互作用的相互作用

Jan Arneth, Dr. Xian-Feng Li, Dr. Jonas Braun, Dr. Sagar Paul, Dr. Michael Schulze, Dr. Christopher E. Anson, Prof. Dr. Wolfgang Wernsdorfer, Prof. Dr. Annie K. Powell, Prof. Dr. Rüdiger Klingeler
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引用次数: 0

摘要

在3d-4f分子磁体的框架内,研究最彻底的结构是蝴蝶形状的配位团簇,因为它为研究基本的磁相互作用提供了理想的测试平台。本文报道了一系列同构蝴蝶配合物VIII2LnIII2的合成和表征,其中Ln=Y (1Y), Tb (2Tb), Dy (3Dy), Ho (4Ho), Er (5Er), Tm (6Tm), Yb (7Yb),扩展了先前对CrIII, MnIII和FeIII同构蝴蝶的研究。在零外场条件下,化合物2Tb、3Dy和4Ho在交流磁化率的非相分量中表现出明显的最大值,而在6Tm条件下,需要较小的磁场才能抑制量子隧道效应。结合高场电子顺磁共振波谱和磁化测量明确地揭示了VIII离子和反铁磁Ising-like 3d-4f交换耦合的易平面各向异性。J3d-4f的强度随着4f离子从Tb到Ho的变化而降低,而从Ho到Tm的反铁磁相互作用增加。在3d和4f主各向异性轴之间的相对角度上发现了完全相反的化学趋势,这突出了镧系元素4f电子分布各向异性对3d - 4f交换的重要作用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Interplay of Single Ion Anisotropy and Magnetic 3 d-4 f Interactions in VIII2LnIII2 Butterfly Complexes

Within the framework of 3d–4f molecular magnets, the most thoroughly investigated architecture is that of butterfly-shaped coordination clusters as it provides an ideal testbed to study fundamental magnetic interactions. Here, we report the synthesis and characterisation of a series of isostructural VIII2LnIII2 butterfly complexes, where Ln=Y (1Y), Tb (2Tb), Dy (3Dy), Ho (4Ho), Er (5Er), Tm (6Tm), Yb (7Yb), which extends the previous study on isostructural butterflies with CrIII, MnIII and FeIII. In zero external field, compounds 2Tb, 3Dy and 4Ho show clear maxima in the out-of-phase component of the ac susceptibility whereas small magnetic fields are needed to suppress quantum tunnelling in 6Tm. Combined high-field electron paramagnetic resonance spectroscopy and magnetisation measurements unambiguously reveal an easy-plane anisotropy of the VIII ion and antiferromagnetic Ising-like 3d–4f exchange couplings. The strength of J3d-4f is shown to decrease upon variation of the 4 f ion from Tb to Ho, while increasing antiferromagnetic interaction can be observed from Ho to Tm. The exact inverse chemical trend is found for the relative angle between the 3d and 4 f main anisotropy axes, which highlights the important role of the lanthanide 4 f electron distribution anisotropy for 3d–4f exchange.

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