ISIS Facility, STFC, Didcot, Oxfordshire, UK.
J Phys Condens Matter. 2012 Sep 26;24(38):382201. doi: 10.1088/0953-8984/24/38/382201. Epub 2012 Aug 28.
Analysis of published data gathered on a sample of Na(2)IrO(3), held deep inside the antiferromagnetic phase at 1.58 K, shows that iridium magnetic dipole moments, measured in resonant x-ray Bragg diffraction, lie in the a-c plane of the monoclinic crystal and enclose an angle ≈118° with the c-axis. These findings, together with bulk measurements, are united in a plausible magnetic ground state for an iridium ion constructed from a Kramers doublet. A magnetic space group, derived from the chemical space group C2/m (unique axis b), possesses an anti-translation, to accommodate antiferromagnetic order, and an odd, two-fold axis of rotation symmetry on the b-axis, C'(2b), placing Ir magnetic dipoles perpendicular to the b-axis. Anapoles (toroidal dipoles) are predicted to be likewise confined to the a-c plane, and magnetic charges forbidden.
对储存在 1.58 K 的反铁磁相中的 Na(2)IrO(3)样本进行的已发表数据进行分析表明,在共振 X 射线布拉格衍射中测量的铱磁偶极子位于单斜晶体的 a-c 平面内,并与 c 轴形成约 118°的夹角。这些发现与体测量结果相结合,为 Ir 离子的磁基态提供了一个合理的解释,该基态由一个 Kramers 双重态构建而成。从化学空间群 C2/m(唯一的 b 轴)导出的磁空间群具有反平移,以适应反铁磁有序,以及 b 轴上的奇数、二倍旋转对称轴 C'(2b),将 Ir 磁偶极子垂直于 b 轴排列。预测反磁偶极子(环形偶极子)同样被限制在 a-c 平面内,并且磁荷被禁止。