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理解 N2(3-)自由基桥联镧系配合物家族中的磁各向异性:密度泛函理论和从头算计算。

Understanding the magnetic anisotropy in a family of N2(3-) radical-bridged lanthanide complexes: density functional theory and ab initio calculations.

机构信息

College of Chemistry and Molecular Engineering, Peking University , Beijing, 100871 P. R. China.

出版信息

J Phys Chem A. 2013 Oct 24;117(42):10873-80. doi: 10.1021/jp4044495. Epub 2013 Oct 15.

DOI:10.1021/jp4044495
PMID:24079453
Abstract

Density functional theory (DFT) and ab initio methods were used to investigate the influence of both intramolecular exchange coupling and single-ion anisotropy on the relaxation barriers of a series of N2(3-) radical-bridged lanthanide complexes {[(Me3Si)2N]2(THF)Ln}2(μ-η(2):η(2)-N2) (Ln = Gd(III) (1), Tb(III) (2), Dy(III) (3), Ho(III) (4), and Er(III) (5)) reported by Long and co-workers. DFT calculations show that the exchange coupling between the lanthanide ions is very weak, but the Ln-N2(3-) coupling is strong for each complex. Moreover, the exchange couplings of Ln-N2(3-) are antiferromagnetic for Ln = Gd(III), Tb(III), Dy(III), and Ho(III) but ferromagnetic for Er(III) for the nearly orthogonal magnetic orbitals on Er(III) and N2(3-). Ab initio calculations show that both of the large magnetic anisotropy of single Tb fragment and the strong Tb-N2(3-) antiferromagnetic couplings lead to the largest energy barrier of complex 2. Although the energy barrier of a single Er fragment is the second largest, the relaxation barrier of complex 5 is only 36.0 cm(-1) due to the weak Er(III)-N2(3-) coupling. This study suggests that both intramolecular exchange coupling and single-ion anisotropy contribute greatly to the full relaxation barrier of lanthanide-based single-molecule magnets (SMMs), which expands the understanding of SMMs using only the giant-spin model.

摘要

密度泛函理论(DFT)和从头算方法被用来研究分子内交换耦合和单离子各向异性对一系列 N2(3-)自由基桥联镧系配合物弛豫势垒的影响,这些配合物是由 Long 和同事报道的 [{[(Me3Si)2N]2(THF)Ln}2(μ-η(2):η(2)-N2)]-(Ln = Gd(III) (1),Tb(III) (2),Dy(III) (3),Ho(III) (4),和 Er(III) (5))。DFT 计算表明,镧系离子之间的交换耦合非常弱,但每个配合物中 Ln-N2(3-)的耦合很强。此外,对于 Ln = Gd(III)、Tb(III)、Dy(III)和 Ho(III),Ln-N2(3-)的交换耦合是反铁磁的,而对于 Er(III),由于 Er(III)和 N2(3-)上的近正交磁轨道,Ln-N2(3-)的交换耦合是铁磁的。从头算计算表明,Tb 片段的大磁各向异性和强烈的 Tb-N2(3-)反铁磁耦合导致配合物 2 的最大能垒。尽管单个 Er 片段的能量势垒是第二大的,但由于 Er(III)-N2(3-)耦合较弱,配合物 5 的弛豫势垒仅为 36.0 cm(-1)。这项研究表明,分子内交换耦合和单离子各向异性都对镧系基单分子磁体(SMM)的完全弛豫势垒有很大贡献,这扩展了仅用巨自旋模型对 SMM 的理解。

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