Institute of Low Temperature and Structure Research, Polish Academy of Sciences, PO Box 1410, 50-950 Wrocław 2, Poland.
J Phys Condens Matter. 2011 Feb 2;23(4):045401. doi: 10.1088/0953-8984/23/4/045401. Epub 2011 Jan 12.
Lattice dynamics calculations and a high-pressure Raman scattering study of nanocrystalline Bi(2)MoO(6), a member of the bismuth-layered Aurivillius family of ferroelectrics, are presented. These studies showed the onset of two reversible second-order or weakly first-order phase transitions near 2.5 and 4.5 GPa as well as some subtle structural changes at 8.2 GPa. Symmetry increases upon application of pressure and the first phase transition involves, most likely, the loss of the MoO(6) tilt mode around a pseudo-tetragonal axis. The second phase transition is associated with the instability of a low wavenumber mode, which behaves as a soft mode. This soft mode most likely corresponds to the polar E(u) mode of the tetragonal I4/mmm aristotype and Bi(2)MoO(6) transforms at 4.5 GPa into the centrosymmetric orthorhombic phase. The sequence of the pressure-induced phase transitions in nanocrystalline Bi(2)MoO(6) is similar to that observed for bulk Bi(2)WO(6) but the critical pressures are significantly lower for the molybdenum compound. Our results also show that the critical pressure of the first phase transition is slightly lower for the nanocrystalline Bi(2)MoO(6) (2.5 GPa) than for the microcrystalline (bulk) Bi(2)MoO(6) (2.8 GPa).
本文对纳米晶 Bi(2)MoO(6)(属于铋层状钙钛矿型铁电体的 Aurivillius 家族的一员)进行了晶格动力学计算和高压拉曼散射研究。这些研究表明,在 2.5 和 4.5 GPa 附近出现了两个可逆的二级或弱一级相变,以及在 8.2 GPa 时出现了一些细微的结构变化。在施加压力时,对称性增加,第一个相变可能涉及 MoO(6)倾斜模式围绕拟四方轴的丧失。第二个相变与低波数模式的不稳定性有关,该模式表现为软模式。这个软模式很可能对应于四方 I4/mmm 典型的极性 E(u)模式,并且在 4.5 GPa 时,Bi(2)MoO(6)转变为中心对称的正交相。纳米晶 Bi(2)MoO(6)中压力诱导相变的顺序与块状 Bi(2)WO(6)中观察到的顺序相似,但钼化合物的临界压力要低得多。我们的结果还表明,纳米晶 Bi(2)MoO(6)的一级相变的临界压力(2.5 GPa)略低于微晶晶体(块状)Bi(2)MoO(6)(2.8 GPa)。