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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Transition between the ferroelectric and relaxor states in 0.8Pb(Mg_(1/3)Nb_(2/3))O_3-0.2PbTiO_3 ceramics
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Transition between the ferroelectric and relaxor states in 0.8Pb(Mg_(1/3)Nb_(2/3))O_3-0.2PbTiO_3 ceramics

机译:0.8Pb(Mg_(1/3)Nb_(2/3))O_3-0.2PbTiO_3陶瓷中铁电态和弛豫态之间的跃迁

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摘要

The phase transition between the ferroelectric and relaxor states for 0.8Pb(Mg_(1/3)Nb_(2/3))O_3-0.2PbTiO_3 ceramics with high chemical homogeneity has been studied by measurements of the dielectric and elastic properties as a function of temperature and of thermal expansion. The room temperature ferroelectric phase structure has been studied in ceramics and powdered samples by Rietveld analysis of x-ray diffraction patterns and by ferroelectric hysteresis loops. Results indicate that the material has well defined, different transition and freezing temperatures, such as the transition is between a monoclinic Cm ferroelectric phase and the noner-godic glass state. The transition presents thermal hysteresis, not only in the transition temperature, but in the kinetics. This indicates that a quite sharp slowing down occurs in the temperature interval between 334 and 344 K: the transition temperatures on cooling and heating.
机译:通过测量介电和弹性特性(随温度变化的函数)研究了0.8Pb(Mg_(1/3)Nb_(2/3))O_3-0.2PbTiO_3陶瓷的铁电和弛豫态之间的相变。温度和热膨胀。通过X射线衍射图的Rietveld分析和铁电磁滞回线,研究了陶瓷和粉末状样品中的室温铁电相结构。结果表明该材料具有定义明确的,不同的转变和冻结温度,例如转变处于单斜Cm铁电相和非高温玻璃状态之间。该转变不仅在转变温度上而且在动力学上都表现出热滞。这表明在334和344 K之间的温度区间(冷却和加热时的转变温度)会发生非常急剧的减速。

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