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The Origin of Magnetic Anisotropy and Single-Molecule Magnet Behavior in Chromium(II)-Based Extended Metal Atom Chains

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https://figshare.com/articles/dataset/The_Origin_of_Magnetic_Anisotropy_and_Single-Molecule_Magnet_Behavior_in_Chromium_II_-Based_Extended_Metal_Atom_Chains/11688027
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Chromium­(II)-based extended metal atom chains have been the focus of considerable discussion regarding their symmetric versus unsymmetric structure and magnetism. We have now investigated four complexes of this class, namely, [Cr3(dpa)4X2] and [Cr5(tpda)4X2] with X = Cl– and SCN– [Hdpa = dipyridin-2-yl-amine; H2tpda = N2,N6-di­(pyridin-2-yl)­pyridine-2,6-diamine]. By dc/ac magnetic techniques and EPR spectroscopy, we found that all these complexes have easy-axis anisotropies of comparable magnitude in their S = 2 ground state (|D| = 1.5–1.8 cm–1) and behave as single-molecule magnets at low T. Ligand-field and DFT/CASSCF calculations were used to explain the similar magnetic properties of tri- versus pentachromium­(II) strings, in spite of their different geometrical preferences and electronic structure. For both X ligands, the ground structure is unsymmetric in the pentachromium­(II) species (i.e., with an alternation of long and short Cr–Cr distances) but is symmetric in their shorter congeners. Analysis of the electronic structure using quasi-restricted molecular orbitals (QROs) showed that the four unpaired electrons in Cr5 species are largely localized in four 3d-like QROs centered on the terminal, “isolated” Cr2+ ion. In Cr3 complexes, they occupy four nonbonding combinations of 3d-like orbitals centered only on the two terminal metals. In both cases, then, QRO eigenvalues closely mirror the 3d-level pattern of the terminal ions, whose coordination environment remains quite similar irrespective of chain length. We conclude that the extent of unpaired-electron delocalization has little impact on the magnetic anisotropy of these wire-like molecular species.

基于二价铬的延展金属原子链(extended metal atom chains)因其对称与非对称结构及磁学特性,长期以来备受学界关注。本研究针对该类别配合物中的四个体系展开探究,分别为X=Cl⁻与SCN⁻的[Cr3(dpa)4X2]及[Cr5(tpda)4X2]配合物,其中Hdpa为二(2-吡啶基)胺(dipyridin-2-yl-amine),H2tpda为N2,N6-二(2-吡啶基)吡啶-2,6-二胺(N2,N6-di(pyridin-2-yl)pyridine-2,6-diamine)。借助直流/交流磁学测试技术与电子顺磁共振(EPR)波谱分析,我们发现所有上述配合物在S=2基态下均具有量级相近的易轴各向异性(|D|=1.5~1.8 cm⁻¹),且在低温条件下表现为单分子磁体(single-molecule magnets)。尽管三核与五核二价铬金属链在几何偏好与电子结构上存在差异,本研究通过配体场计算以及密度泛函理论/完全活化空间自洽场(DFT/CASSCF)计算,阐明了二者磁学性质相似的原因。对于两种X配体而言,五核二价铬物种的基态结构呈非对称特征(即Cr-Cr键长呈现长、短交替分布),而其同系的三核配合物则为对称结构。借助准受限分子轨道(quasi-restricted molecular orbitals, QROs)对电子结构进行分析后发现,五核铬物种中的四个未成对电子主要定域在四个以端基“孤立”Cr²+离子为中心的类3d QRO中;而在三核铬配合物中,未成对电子则占据仅以两个端基金属为中心的四个类3d非成键分子轨道组合。综上,两种体系中的QRO本征值均与端基离子的3d能级分布高度吻合,且无论金属链长度如何,端基离子的配位环境均保持高度相似。本研究最终得出结论:未成对电子的离域程度对这类线状分子物种的磁各向异性影响极小。
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2020-02-03
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