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High-pressure neutron study of the morphotropic lead-zirconate-titanate: Phase transitions in a two-phase system

机译:高压变质锆钛酸铅的中子研究:两相系统中的相变

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摘要

The present study was dedicated to the classical piezoelectric, lead-zirconate-titanate ceramic with composition Pb(Zr0.54Ti0.46)O3 at the Zr-rich side of the morphotropic phase boundary at which two phases co-exists. The pressure-induced changes in the phase fractions were studied by high-pressureneutronpowder diffraction technique up to 3 GPa and 773 K. The two co-existing phases were rhombohedral R3c and monoclinic Cm at room temperature and R3c and P4mm above 1 GPa and 400 K. The experiments show that pressure favors the R3c phase over the Cm and P4mm phases, whereas at elevated temperatures entropy favours the P4mm phase. At 1 GPa pressure, the transition to the cubic Pm3¯m phase occurred at around 600 K. Pressure lowers the Cm→P4mm transition temperature. The Cm phase was found to continuously transform to the P4mm phase with increasing pressure, which is inline with the usual notion that the hydrostatic pressure favours higher symmetry structures. At the same time, the phase fraction of the R3c phase was increasing, implying discontinuous Cm→R3cphase transition. This is in clear contrast to the polarization rotation model according to which the Cm would link the tetragonal and rhombohedral phases by being a phase in which the polarization would, more or less continuously, rotate from the tetragonal polarization direction to the rhombohedral direction. Pressure induces large changes in phase fractions contributing to the extrinsic piezoelectricity. The changes are not entirely reversible, as was revealed by noting that after high-pressure experiments the amount of rhombohedral phase was larger than initially, suggesting that on the Zr-rich side of the phase boundary the monoclinic phase is metastable. An important contribution to the intrinsic piezoelectricity was revealed: a large displacement of the B cations (Zr and Ti) with respect to the oxygen anions is induced by pressure.
机译:本研究致力于经典压电压电锆钛酸铅陶瓷,在变质相边界的富Zr侧(两相共存)组成为Pb(Zr0.54Ti0.46)O3。通过高压中子粉末衍射技术研究了相分数在压力高达3 changesGPa和773 K时的相变变化,两个共存相分别是室温下的菱形R3c和单斜Cm以及高于1 GPa和400 K的R3c和P4mm。实验表明,压力有利于R3c相优于Cm和P4mm相,而在高温下,熵有利于P4mm相。在1 GPa的压力下,向立方Pm3′m相的转变发生在600 K附近,压力降低了Cm→P4mm的转变温度。发现Cm相随着压力的增加而连续转变为P4mm相,这与通常的观点一致,即静水压力有利于更高的对称结构。同时,R3c相的相分数增加,这意味着Cm→R3c相的转变是不连续的。这与极化旋转模型形成鲜明对比,在极化旋转模型中,Cm通过使极化或多或少连续地从四边形极化方向旋转到菱面体方向而链接四方和菱面体相。压力引起相分数的大变化,从而有助于外部压电。这些变化不是完全可逆的,这可以通过注意到在高压实验后菱面体相的数量大于初始值来表明,这表明在相边界的富Zr侧单斜晶相是亚稳的。揭示了对固有压电性的重要贡献:压力引起B阳离子(Zr和Ti)相对于氧阴离子的大位移。

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