Department of Earth Sciences, University of Cambridge, Cambridge, UK.
J Phys Condens Matter. 2012 Feb 1;24(4):045901. doi: 10.1088/0953-8984/24/4/045901. Epub 2011 Dec 21.
The structural evolution of Pb(Mg(1/3)Nb(2/3))O(3) (PMN) has been reviewed in terms of characteristic temperatures, length scales and timescales, with a view to considering the overall relaxor behaviour from the perspectives of strain and elasticity. A conventional analysis of lattice parameter data in terms of spontaneous strain and strain/order parameter coupling shows that even though a normal phase transition does not occur the relaxor ordering process is accompanied by a significant volume strain which follows the pattern of a static order parameter evolving according to that expected for a tricritical phase transition with T(c) ≈ 350 K. This matches the evolution of the intensity of the elastic central peak in neutron scattering spectra, and reflects the development of static (or quasistatic) polar nanoregions (PNRs) as if by a mean-field phase transition. Use of a Landau free energy expansion, which includes Γ4(-) order parameter components to describe ferroelectric contributions and an R1(+) order parameter to describe cation ordering together with their formal coupling with strain, then allows the pattern of elastic softening expected for a cubic → rhombohedral phase transition to be anticipated. The extent to which observed softening differs from this static mean-field pattern serves to highlight the additional roles of local heterogeneity and relaxation dynamics in determining the relaxor properties of PMN.
PMN 的结构演变从特征温度、长度尺度和时间尺度等方面进行了综述,旨在从应变和弹性的角度考虑弛豫体的整体行为。通过对自发应变和应变/序参量耦合的晶格参数数据进行常规分析表明,即使不发生正常的相变,弛豫体有序化过程伴随着显著的体积应变,其模式符合根据 350 K 左右的三叉点相变预期的静态序参量的演化。这与中子散射谱中弹性中心峰强度的演化相匹配,反映了静态(或准静态)极性纳米区 (PNR) 的发展,就像通过平均场相变一样。使用朗道自由能展开式,其中包括 Γ4(-)序参量分量来描述铁电贡献,以及 R1(+)序参量来描述阳离子有序化及其与应变的正式耦合,然后可以预期到立方-菱面体相变的弹性软化模式。观察到的软化与这种静态平均场模式的差异程度突出了局部非均匀性和弛豫动力学在确定 PMN 弛豫体性质方面的额外作用。