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Designing a mononuclear Dy-III single-molecule magnet (SMM) by using a N,O,N,O-based multichelating Schiff base ligand and a -diketonate ligand

机译:通过使用N,O,N,O基杂种席夫碱配体和 - 酮酸盐配体设计单核Dy-III单分子磁体(SMM)

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摘要

Two mononuclear Ln(III) compounds, in which each Ln(III) is eight-coordinated, namely [Ln(L)(tmpd)] (Ln = Dy (1) or Er (2)), have been prepared using a multichelating Schiff base ligand N,N-bis(2-hydroxy-5-methyl-3-formylbenzyl)-N,N-bis-(pyridin-2-ylmethyl)ethylenediamine (H2L) and a bidentate chelating -diketonate ligand (tmpd). The local geometry of the Ln(III) ions in 1 and 2 is close to the D-2d symmetry. Notably, magnetic studies reveal that compound 2 displays no slow relaxation of magnetization while compound 1 exhibits single-molecule magnet (SMM) behaviour in the absence of a static magnetic field, with an effective energy barrier (U-eff) of 66.81 cm(-1) (96.63 K). To deeply understand their different magnetic behaviours, the magnetic anisotropy of 1 and 2 is systematically studied by ab initio calculations. There was an obvious difference between the first excited state (KD1) and the experimental U-eff in 1 because the QTM within KD0 is not completely prohibited and the residual QTM could lead to a large discrepancy between experimentally-fitted U-eff and ab initio calculated crystal field splitting. No temperature/frequency dependence is recorded in the ac susceptibility of 2 because the ab initio magnetic easy axis of 2 does not lie close to any atom of the first sphere since it tries to avoid any strong electrostatic repulsion. Moreover, the g(XY) value of KD0 of 2 is larger than that of 1 by three orders of magnitude leading to the probability of stronger QTM within KD0 of 2.
机译:两种单核LN(III)化合物,其中每个LN(III)是八个协调的,即[LN(L)(TMPD)](LN = DY(1)或ER(2)),使用多核制备Schiff碱配体N,N-BIS(2-羟基-5-甲基-3-甲甲苄基)-N,N-双(吡啶-2-基甲基)乙二胺(H2L)和二齿螯合 - 酮配体(TMPD)。 1和2中LN(III)离子的局部几何形状接近D-2D对称性。值得注意的是,磁性研究揭示了化合物2在没有静磁场的情况下显示出在没有静磁场的单分子磁体(SMM)行为的同时,无需静电(U-EFF)的单分子磁体(SMM)行为,具有66.81cm( - 1)(96.63 k)。为了深入理解其不同的磁行为,通过AB Initio计算系统地研究了1和2的磁各向异性。第一个激发态(KD1)和实验U-EFF之间存在明显的差异,因为KD0内的QTM没有完全禁止,并且残留的QTM可能导致实验拟合U-EFF和AB INITIO之间的大量差异计算的水晶场分裂。没有温度/频率依赖性在2的AC敏感度中记录,因为2的AB Initio磁性容易轴线不会靠近第一球体的任何原子,因为它试图避免任何强大的静电排斥。此外,kd0的g(xy)值为2大于1的三个数量级,导致QTM在KD0中的较强QTM的可能性。

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  • 来源
    《New Journal of Chemistry》 |2019年第1期|共9页
  • 作者单位

    Baoji Univ Arts &

    Sci Coll Chem &

    Chem Engn Baoji 721013 Peoples R China;

    Baoji Univ Arts &

    Sci Coll Chem &

    Chem Engn Baoji 721013 Peoples R China;

    Northwest Univ Coll Chem &

    Mat Sci Key Lab Synthet &

    Nat Funct Mol Chem Minist Educ Xian 710069 Shaanxi Peoples R China;

    Northwest Univ Shaanxi Key Lab Degradable Med Mat Sch Chem Engn Xian 710069 Shaanxi Peoples R China;

    Chinese Acad Sci Dalian Inst Chem Phys Dalian 116023 Peoples R China;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 化学;
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