Callista M. SkaggsPeter SiegfriedChang‐Jong KangCraig M. BrownChen FuLu MaSteven N. EhrlichYan XinMark CroftWenqian XuSaul H. LapidusN. GhimireXiaoyan Tan
In this work, a polycrystalline iridate Li<sub>8</sub>IrO<sub>6</sub> material was prepared via heating Li<sub>2</sub>O and IrO<sub>2</sub> starting materials in a sealed quartz tube at 650 °C for 48 h. The structure was determined from Rietveld refinement of room-temperature powder neutron diffraction data. Li<sub>8</sub>IrO<sub>6</sub> adopts the nonpolar space group $R\\bar{3}$ with Li atoms occupying the tetrahedral and octahedral sites, which is supported by the electron diffraction and solid-state 7Li NMR. This results in a crystal structure consisting of LiO<sub>4</sub> tetrahedral layers alternating with mixed IrO<sub>6</sub> and LiO<sub>6</sub> octahedral layers along the crystallographic <em>c</em>-axis. The +4 oxidation state of Ir<sup>4+</sup> was confirmed by near-edge X-ray absorption spectroscopy. An in situ synchrotron X-ray diffraction study of Li<sub>8</sub>IrO<sub>6</sub> indicates that the sample is stable up to 1000 °C and exhibits no structural transitions. Magnetic measurements suggest long-range antiferromagnetic ordering with a Néel temperature (TN) of 4 K, which is corroborated by heat capacity measurements. The localized effective moment $μ_{\\text{eff}}$ (Ir) = 1.73 $μ_{\\text{B}}$ and insulating character indicate that Li<sub>8</sub>IrO<sub>6</sub> is a correlated insulator. First-principles calculations support the nonpolar crystal structure and reveal the insulating behavior both in paramagnetic and antiferromagnetic states.
CallistaM. Skaggs (11649498)Peter E. Siegfried (11649501)Chang-Jong Kang (3000273)Craig M. Brown (1414177)Fu Chen (418017)Lu Ma (46360)Steven N. Ehrlich (1736527)Yan Xin (1392169)Mark Croft (1356261)Wenqian Xu (1446349)Saul H. Lapidus (1453873)Nirmal J. Ghimire (7905785)Xiaoyan Tan (1297425)
P. KroeschellR. H. H. WolfR. HOPPE