Nagle-Cocco Liam A V, Bull Craig L, Ridley Christopher J, Dutton Siân E
Cavendish Laboratory, University of Cambridge, JJ Thomson Avenue, Cambridge CB3 0HE, United Kingdom.
ISIS Neutron and Muon Facility, Rutherford Appleton Laboratory, Didcot OX11 0QX, United Kingdom.
Inorg Chem. 2022 Mar 14;61(10):4312-4321. doi: 10.1021/acs.inorgchem.1c03345. Epub 2022 Mar 3.
NaNiO is a layered material consisting of alternating layers of NaO and Jahn-Teller-active NiO edge-sharing octahedra. At ambient pressure, it undergoes a broad phase transition from a monoclinic to rhombohedral structure between 465 and 495 K, associated with the loss of long-range orbital ordering. In this work, we present the results of a neutron powder diffraction study on powdered NaNiO as a function of pressure and temperature from ambient pressure to ∼5 GPa between 290 and 490 K. The 290 and 460 K isothermal compressions remained in the monoclinic phase up to the maximum pressures studied, whereas the 490 K isotherm was mixed-phase throughout. The unit-cell volume was fitted to a second-order Birch-Murnaghan equation of state, where = 119.6(5) GPa at 290 K. We observe at 490 K that the fraction of the Jahn-Teller-distorted phase increases with pressure, from 67.8(6)% at 0.71(2) GPa to 80.2(9)% at 4.20(6) GPa. Using this observation, in conjunction with neutron diffraction measurements at 490 K on removing pressure from 5.46(9) to 0.342(13) GPa, we show that the Jahn-Teller transition temperature increases with pressure. Our results are used to present a structural pressure-temperature phase diagram for NaNiO. To the best of our knowledge, this is the first diffraction study of the effect of pressure on the Jahn-Teller transition temperature in materials with edge-sharing Jahn-Teller-distorted octahedra and the first variable-pressure study focusing on the Jahn-Teller distortion in a nickelate.
NaNiO是一种层状材料,由交替的NaO层和具有 Jahn-Teller 活性的 NiO 边共享八面体层组成。在常压下,它在465至495 K之间经历从单斜结构到菱面体结构的广泛相变,这与长程轨道有序的丧失有关。在这项工作中,我们展示了对粉末状NaNiO进行中子粉末衍射研究的结果,该研究是在290至490 K之间,从常压到约5 GPa的压力和温度范围内进行的。290 K和460 K的等温压缩在研究的最大压力下仍保持在单斜相,而490 K等温线在整个过程中都是混合相。晶胞体积被拟合到二阶Birch-Murnaghan状态方程,其中在290 K时 = 119.6(5) GPa。我们在490 K时观察到,Jahn-Teller畸变相的比例随压力增加,从0.71(2) GPa时的67.8(6)%增加到4.20(6) GPa时的80.2(9)%。利用这一观察结果,结合在490 K下从5.