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Magnetic chains of Fe-3 clusters in the {Fe3YO2} butterfly molecular compound

机译:Fe-3簇的磁链【FE3YO2】蝴蝶分子化合物

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摘要

The "butterfly" molecule [Fe3Y(mu 3-O)(2)(CCl3COO)(8)(H2O)(THF)(3)] (in brief {Fe3YO2}) includes three Fe3+ ions which build a robust Fe-3 cluster with a strong intracluster antiferromagnetic exchange and a total spin S = 5/2. It represents the starting magnetic system to study further interactions with magnetic rare earths when Y is replaced with lanthanides. We present heat capacity and equilibrium susceptibility measurements below 2 K, which show that each cluster has a sizeable magnetic anisotropy pointing to the existence of intercluster interactions. However, no phase transition to a long-range magnetically ordered phase is observed down to 20 mK. The intercluster interaction is analysed in the framework of the one-dimensional Blume-Capel model with an antiferromagnetic chain interaction constant J/k(B) = -40(2) mK between Fe-3 cluster spins, and a uniaxial anisotropy with parameter D/k(B) = -0.56(3) K. This is associated to single chains of Fe-3 clusters oriented along the shortest intercluster distances displayed by the crystal structure of {Fe3YO2}. Ac susceptibility measurements reveal that the magnetic relaxation is dominated by a quantum tunnelling process below 0.2 K, and by thermally activated processes above this temperature. The experimental activation energy of this single chain magnet, E-a/k(B) = 3.4(6) K, can be accounted for by the combination of contributions arising from single-molecule magnetic anisotropy and spin-spin correlations along the chains.
机译:“蝴蝶”分子[Fe3-O)(2)(2)(CCL3COO)(8)(H2O)(THF)(3)](简要{Fe3YO2})包括三种Fe3 +离子,该Fe3 +离子构建鲁棒Fe-3群体具有强大的内部内部反铁磁交换和全旋转S = 5/2。它代表了当Y被镧系所取代时,研究与磁性稀土的进一步相互作用的起始磁系统。我们呈现低于2 k的热容量和平衡易感性测量,表明每个簇具有相当大的磁各向异性,指向搅拌机相互作用的存在。然而,未观察到远程磁排序相的相转变为20 mk。在用反铁磁链相互作用常数J / K(B)= -40(2)MK与Fe-3簇旋转之间的反铁磁链相互作用常数J / K(B)= -40(2)MK和具有参数D的单轴各向异性的框架中分析了帧内簇相互作用。与参数D的单轴各向异性/ k(b)= -0.56(3)K.这与沿着{Fe3YO2}的晶体结构显示的最短的搅拌机距离为导向的单链。 AC敏感度测量表明,磁性松弛是由0.2K以下的量子隧道工艺支配,并且通过高于该温度的热活化过程。该单链磁体的实验激活能量E-A / K(B)= 3.4(6)k可以通过从链子磁各向异性和旋转 - 旋转相关的贡献的组合来算是局部的组合。

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