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首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Dilution-induced slow magnetic relaxation and anomalous hysteresis in trigonal prismatic dysprosium(III) and uranium(III) complexes
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Dilution-induced slow magnetic relaxation and anomalous hysteresis in trigonal prismatic dysprosium(III) and uranium(III) complexes

机译:三角棱柱状prism(III)和铀(III)配合物的稀释诱导的慢磁弛豫和异常磁滞现象

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摘要

Magnetically dilute samples of complexes Dy(H_2BPz ~(Me2)_2)_3 (1) and U(H_2BPz _2)_3 (3) were prepared through cocrystallization with diamagnetic Y(H_2BPz~(Me2)_2)_3 (2) and Y(H_2BPz_2)_3. Alternating current (ac) susceptibility measurements performed on these samples reveal magnetic relaxation behavior drastically different from their concentrated counterparts. For concentrated 1, slow magnetic relaxation is not observed under zero or applied dc fields of several hundred Oersteds. However, a 1:65 (Dy:Y) molar dilution results in a nonzero out-of-phase component to the magnetic susceptibility under zero applied dc field, characteristic of a single-molecule magnet. The highest dilution of 3 (1:90, U:Y) yields a relaxation barrier U _(eff) = 16 cm~(-1), double that of the concentrated sample. These combined results highlight the impact of intermolecular interactions in mononuclear single-molecule magnets possessing a highly anisotropic metal center. Finally, dilution elucidates the previously observed secondary relaxation process for concentrated 3. This process is slowed down drastically upon a 1:1 molar dilution, leading to butterfly magnetic hysteresis at temperatures as high as 3 K. The disappearance of this process for higher dilutions reveals it to be relaxation dictated by short-range intermolecular interactions, and it stands as the first direct example of an intermolecular relaxation process competing with single-molecule-based slow magnetic relaxation.
机译:通过与抗磁性Y(H_2BPz〜(Me2)_2)_3(2)和Y(共结晶)制备复合物Dy(H_2BPz〜(Me2)_2)_3(1)和U(H_2BPz _2)_3(3)的磁性稀释样品H_2BPz_2)_3。在这些样品上进行的交流电(ac)磁化率测量表明,其磁弛豫行为与浓缩样品大不相同。对于集中的1,在零或施加数百奥斯特的直流磁场下观察不到缓慢的磁弛豫。但是,1:65(Dy:Y)摩尔稀释会导致在零施加的直流磁场下磁化率的非零异相分量,这是单分子磁体的特征。最高稀释度3(1:90,U:Y)产生弛豫屏障U _(eff)= 16 cm〜(-1),是浓缩样品的两倍。这些综合结果突出了分子间相互作用对具有高各向异性金属中心的单核单分子磁体的影响。最后,稀释说明了先前观察到的浓缩3的二次弛豫过程。在1:1摩尔稀释时,该过程急剧减慢,导致在高达3 K的温度下产生蝶形磁滞。对于更高的稀释度,该过程的消失表明它是由短程分子间相互作用决定的弛豫,它是分子弛豫过程与基于单分子的慢磁弛豫竞争的第一个直接示例。

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