Department of Chemistry, North Carolina State University, Raleigh, North Carolina 27695-8204, United States.
Inorg Chem. 2011 Oct 3;50(19):9400-5. doi: 10.1021/ic201023j. Epub 2011 Aug 11.
We evaluated the spin-exchange interactions of Li(3)RuO(4) by performing energy-mapping analysis based on density functional calculations and examined the nature of its magnetic transition at T(1) = 66 K and the divergence of the field-cooled and zero-field-cooled susceptibilities below T(2) = 32 K. Our study shows that T(1) is associated with a three-dimensional antiferromagnetic ordering, in which the two-dimensional antiferromagnetic lattices parallel to the ab plane are antiferromagnetically coupled along the c direction. We examined how the substitutional defects, Ru atoms residing in the Li sites, affect the antiferromagnetic coupling along the c direction to explain why the expected c-axis doubling is not detected from powder neutron diffraction measurements. The susceptibility divergence below T(2) is attributed to a slight spin canting out of the ab plane.
我们通过基于密度泛函计算的能量映射分析评估了 Li(3)RuO(4)的自旋交换相互作用,并研究了其在 T(1) = 66 K 时的磁转变性质以及在 T(2) = 32 K 以下的场冷和零场冷磁化率的发散。我们的研究表明,T(1)与三维反铁磁有序有关,其中平行于 ab 平面的二维反铁磁晶格沿 c 方向反铁磁耦合。我们研究了取代缺陷,即占据 Li 位的 Ru 原子,如何影响沿 c 方向的反铁磁耦合,以解释为什么从粉末中子衍射测量中没有检测到预期的 c 轴加倍。低于 T(2)的磁化率发散归因于 ab 平面外的轻微自旋倾斜。