Department of Chemistry and Biochemistry, California State University, Long Beach, 1250 Bellflower Boulevard, Long Beach, California 90840, USA.
Inorg Chem. 2012 Nov 5;51(21):11493-9. doi: 10.1021/ic3013377. Epub 2012 Oct 15.
The novel osmium-based oxide Li(3)Mg(2)OsO(6) was synthesized in polycrystalline form by reducing Li(5)OsO(6) by osmium metal and osmium(IV) oxide in the presence of stoichiometric amounts of magnesium oxide. The crystal structure was refined using powder X-ray diffraction data in the orthorhombic Fddd space group with a = 5.88982(5) Å, b = 8.46873(6) Å, and c = 17.6825(2) Å. This compound is isostructural and isoelectronic with the ruthenium-based system Li(3)Mg(2)RuO(6). The magnetic ion sublattice Os(5+) (S = 3/2) consists of chains of interconnected corner- and edge-shared triangles, which brings about the potential for geometric magnetic frustration. The Curie-Weiss law holds over the range 80-300 K with C = 1.42(3) emu·K/mol [μ(eff) = 3.37(2) μ(B)] and θ(C) = -105.8(2) K. Below 80 K, there are three anomalies at 75, 30, and 8 K. Those at 75 and 30 K are suggestive of short-range antiferromagnetic correlations, while that at 8 K is a somewhat sharper maximum showing a zero-field-cooled/field-cooled divergence suggestive of perhaps spin freezing. The absence of magnetic Bragg peaks at 3.9 K in the neutron diffraction pattern supports this characterization, as does the absence of a sharp peak in the heat capacity, which instead shows only a very broad maximum at ∼12 K. A frustration index of f = 106/8 = 13 indicates a high degree of frustration. The magnetic properties of the osmium phase differ markedly from those of the isostructural ruthenium material, which shows long-range antiferromagnetic order below 17 K, f = 6, and no unusual features at higher temperatures. Estimates of the magnetic exchange interactions at the level of spin-dimer analysis for both the ruthenium and osmium materials support a more frustrated picture for the latter. Errors in the calculation and assignment of the exchange pathways in the previous report on Li(3)Mg(2)RuO(6) are identified and corrected.
通过用锇金属和四氧化锇还原五氧化二锂,并在化学计量量的氧化镁存在下,合成了新的基于锇的氧化物 Li(3)Mg(2)OsO(6) 的多晶形式。使用粉末 X 射线衍射数据在正交 Fddd 空间群中对晶体结构进行了细化,a = 5.88982(5) Å, b = 8.46873(6) Å, c = 17.6825(2) Å。该化合物与基于钌的系统 Li(3)Mg(2)RuO(6) 是等结构和等电子的。磁离子亚晶格 Os(5+) (S = 3/2) 由相互连接的角和边缘共享三角形链组成,这带来了几何磁挫折的可能性。居里-外斯定律在 80-300 K 范围内成立,C = 1.42(3) emu·K/mol [μ(eff) = 3.37(2) μ(B)],θ(C) = -105.8(2) K。在 80 K 以下,在 75、30 和 8 K 处有三个异常。在 75 和 30 K 处的异常表明存在短程反铁磁相关性,而在 8 K 处的异常则是一个更为尖锐的最大值,表明在零场冷却/场冷却时存在发散,可能表明自旋冻结。在 3.9 K 时的中子衍射图中没有出现磁布拉格峰,这支持了这种特征,热容中也没有出现尖锐的峰,而只在约 12 K 处显示出非常宽的最大值。挫折指数 f = 106/8 = 13 表明挫折程度很高。锇相的磁性性质与等结构的钌材料明显不同,后者在 17 K 以下表现出长程反铁磁有序,f = 6,在较高温度下没有异常特征。对钌和锇材料进行自旋二聚体分析水平的磁交换相互作用的估计支持了后者更具挫折感的图像。识别并纠正了之前关于 Li(3)Mg(2)RuO(6) 的报告中计算和分配交换途径的错误。