†Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan.
‡ISIS, Rutherford Appleton Laboratory, Harwell Oxford, Didcot OX11 0QX, United Kingdom.
J Am Chem Soc. 2015 Jun 17;137(23):7468-73. doi: 10.1021/jacs.5b03712. Epub 2015 Jun 8.
The crystal and magnetic structures of charge-disproportionated Ca2FeMnO6 were analyzed by neutron powder diffraction. Ca2FeMnO6 is a layered double perovskite oxide with a two-dimensional arrangement of Mn(4+) and unusual high valence Fe(4+) at room temperature. When cooled, the compound shows charge disproportionation followed by magnetic transition. Around 200 K, the Fe(4+) shows the charge disproportionation to Fe(3+) and Fe(5+), which are ordered in a checkerboard pattern in the two-dimensional FeO6 octahedral layers. The magnetic transition occurs at 95 K, which is much lower than the charge disproportionation temperature. The magnetic structure is commensurate but noncollinear, and the antiferromagnetic coupling of Fe(3+) and Fe(5+) spins in the FeO6 octahedral layers gives the ferrimagnetic moments. The unique magnetic structure is described as a result of two-dimensional localization of the ligand holes with effective spins.
通过中子粉末衍射分析了电荷离解的 Ca2FeMnO6 的晶体和磁性结构。Ca2FeMnO6 是一种具有二维排列的 Mn(4+)和异常高价 Fe(4+)的层状双钙钛矿氧化物,在室温下。当冷却时,化合物表现出电荷离解,然后发生磁性转变。在 200 K 左右,Fe(4+)发生电荷离解为 Fe(3+)和 Fe(5+),它们在二维 FeO6 八面体层中以棋盘格图案有序排列。磁性转变发生在 95 K,远低于电荷离解温度。磁结构是相符的,但不是共线的,FeO6 八面体层中 Fe(3+)和 Fe(5+)自旋的反铁磁耦合给出了亚铁磁矩。这种独特的磁结构是由于配体空穴的二维局域化和有效自旋的结果。