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arXiv 0808.3532cond-mat.mtrl-sci
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准同型相界的动力学起源--0.68 Pb(Mg1/3Nb2/3O3)-0.32 PbTiO_3的软模和相不稳定性

Dynamic origin of the morphotropic phase boundary - Soft modes and phase instability in 0.68Pb(Mg1/3Nb2/3O3)-0.32PbTiO3

Hu Cao, Chris Stock, Guangyong Xu, Peter M. Gehring, Jiefang Li, Dwight Viehland

摘要:

本文报道了0.68Pb(Mg_(1/3)Nb_(2/3)O_3)-0.32PbTiO_3(PMN-0.32PT)单晶的中子非弹性散射。在沿立方[001]方向施加的零和非零电场下,在100 K和600 K之间获得数据。最低能量的、带中心的、横向光学声子在高温下被强烈阻尼并缓慢软化;然而,软模能量的平方开始随着温度线性增加,如在常规铁电体中一样,我们称之为软模“恢复”,在TC下冷却到四极相。我们的数据表明,在PMN-0.32PT的软模式的行为几乎相同的纯PMN,表现出相同的温度依赖性和恢复温度,即使PMN表现出没有明确的结构转变(没有TC)。PMN-0.32PT中软模的温度依赖性也类似于PMN-0.60PT中的软模的温度依赖性;然而,在PMN-0.60PT中,恢复温度等于TC。这些结果表明,PMN-xPT中的软模动力学的温度依赖性和能量尺度与MPB的Ti-贫侧的浓度无关,但与TC的比例为富Ti的组合物。因此,MPB可以在晶格动力学项中被定义为TC首先匹配软模式的恢复温度的浓度。高分辨率的X射线研究表明,在电场的存在下,在MPB区域内的异常量的铁电体的相边界转移到更高的温度。这表明,一个不寻常的不稳定性存在于明显的立方相在MPB。

英文摘要:

We report neutron inelastic scattering on single crystal 0.68Pb(Mg1/3Nb2/3O3)-0.32PbTiO3 (PMN-0.32PT), a relaxor ferroelectric material that lies within the compositional range of the morphotropic phase boundary (MPB). Data were obtained between 100 K and 600 K under zero and non-zero electric field applied along the cubic [001] direction. The lowest energy, zone-center, transverse optic phonon is strongly damped and softens slowly at high temperature; however the square of the soft mode energy begins to increase linearly with temperature as in a conventional ferroelectric, which we term the soft mode "recovery," upon cooling into the tetragonal phase at TC. Our data show that the soft mode in PMN-0.32PT behaves almost identically to that in pure PMN, exhibiting the same temperature dependence and recovery temperature even though PMN exhibits no well-defined structural transition (no TC). The temperature dependence of the soft mode in PMN-0.32PT is also similar to that in PMN-0.60PT; however in PMN-0.60PT the recovery temperature equals TC. These results suggest that the temperature dependence and the energy scale of the soft mode dynamics in PMN-xPT are independent of concentration on the Ti-poor side of the MPB, but scale with TC for Ti-rich compositions. Thus the MPB may be defined in lattice dynamical terms as the concentration where TC first matches the recovery temperature of the soft mode. High-resolution x-ray studies show that the cubic-to-ferroelectric phase boundary shifts to higher temperatures by an abnormal amount within the MPB region in the presence of an electric field. This suggests that an unusual instability exists within the apparently cubic phase at the MPB.

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