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三角棱柱体镝(III)和铀(III)配合物的稀释诱导的缓慢磁弛豫和异常滞后。

Dilution-induced slow magnetic relaxation and anomalous hysteresis in trigonal prismatic dysprosium(III) and uranium(III) complexes.

机构信息

Department of Chemistry, University of California, Berkeley, Berkeley, California 94720, USA.

出版信息

Inorg Chem. 2011 Sep 5;50(17):8484-9. doi: 10.1021/ic201078r. Epub 2011 Aug 11.

DOI:10.1021/ic201078r
PMID:21834501
Abstract

Magnetically dilute samples of complexes Dy(H(2)BPz(Me2)(2))(3) (1) and U(H(2)BPz(2))(3) (3) were prepared through cocrystallization with diamagnetic Y(H(2)BPz(Me2)(2))(3) (2) and Y(H(2)BPz(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.

摘要

通过与反磁性的 Y(H(2)BPz(Me2)(2))(3) (2) 和 Y(H(2)BPz(2))(3) 共结晶,制备了复合物 Dy(H(2)BPz(Me2)(2))(3) (1) 和 U(H(2)BPz(2))(3) (3) 的磁性稀释样品。对这些样品进行交流 (ac) 磁化率测量,结果表明其磁弛豫行为与浓缩样品有很大不同。对于浓缩的 1,在零场或几百奥斯特的外加直流场下,没有观察到缓慢的磁弛豫。然而,1:65 (Dy:Y) 的摩尔稀释导致在零施加直流场下,磁磁化率出现非零的反相分量,这是单分子磁体的特征。最高稀释度为 3 (1:90, U:Y) 产生的弛豫势 U(eff) = 16 cm(-1),是浓缩样品的两倍。这些综合结果突出了具有高各向异性金属中心的单核单分子磁体中分子间相互作用的影响。最后,稀释法阐明了浓缩 3 中以前观察到的二次弛豫过程。在 1:1 摩尔稀释后,这个过程会大大减慢,导致在高达 3 K 的温度下出现蝴蝶状磁滞。对于更高的稀释度,这个过程的消失表明它是由短程分子间相互作用决定的弛豫过程,这是首例竞争单分子基缓慢磁弛豫的分子间弛豫过程的直接实例。

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