Tolis Evangelos I, Engelhardt Larry P, Mason Pamela V, Rajaraman Gopalan, Kindo Koichi, Luban Marshall, Matsuo Akira, Nojiri Hiroyuki, Raftery James, Schröder Christian, Timco Grigore A, Tuna Floriana, Wernsdorfer Wolfgang, Winpenny Richard E P
School of Chemistry, The University of Manchester, Oxford Road, Manchester, M13 9PL, UK.
Chemistry. 2006 Dec 4;12(35):8961-8. doi: 10.1002/chem.200600400.
The synthesis and structural characterization of a nonanuclear FeIII cage complex is reported. The nine iron centers in [Fe9(mu3-O)4(O3PPh)3(O2CCMe3)13] lie on the vertices of an incomplete icosahedron, with the P atoms of triphenylphosphonate at the other three vertices. The paramagnetic core therefore describes a tridiminished icosahedron. Magnetic studies suggest an S=1/2 ground state for the molecule. Analysis of exchange paths and the susceptibility data point to the interpretation that the cluster can be divided into two nearly decoupled sections: an {Fe6O3} section, with an S=0 ground state, in which three oxo-centered triangles bound a central triangle that is not oxo-centered; and an {Fe3O} triangle with S=1/2. The analysis of the susceptibility data leads to a Heisenberg model based on three significant antiferromagnetic exchange interactions, with values of 173.7 cm-1 in the {Fe3O} triangle, and 30.9 and 19.1 cm-1 within the {Fe6O3} section, while the exchange between them is <1 cm-1. With these assignments, the theoretical low-temperature differential susceptibility is also in very good agreement with measurements up to 50 T. Magnetic measurements in the milli-kelvin range reveal striking hysteresis loops and magnetization reversals associated with a Landau-Zener-Stückelberg (LZS) transition as enhanced by the occurrence of a phonon bottleneck.
报道了一种九核FeIII笼状配合物的合成及结构表征。[Fe9(μ3 - O)4(O3PPh)3(O2CCMe3)13]中的九个铁中心位于一个不完全二十面体的顶点上,三苯基膦酸酯的P原子位于另外三个顶点。因此,顺磁核心描述了一个截顶二十面体。磁性研究表明该分子的基态为S = 1/2。对交换路径和磁化率数据的分析表明,该簇合物可分为两个几乎解耦的部分:一个{Fe6O3}部分,基态为S = 0,其中三个以氧为中心的三角形包围着一个不以氧为中心的中心三角形;以及一个S = 1/2的{Fe3O}三角形。对磁化率数据的分析得出了一个基于三种显著反铁磁交换相互作用的海森堡模型,{Fe3O}三角形中的值为173.7 cm-1,{Fe6O3}部分内的值为30.9和19.1 cm-1,而它们之间的交换小于1 cm-1。基于这些赋值,理论低温微分磁化率也与高达50 T的测量结果非常吻合。毫开尔文范围内的磁性测量揭示了与声子瓶颈增强的朗道 - 齐纳 - 施图克尔贝格(LZS)转变相关的显著磁滞回线和磁化反转。