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首页> 外文期刊>CERAMICS INTERNATIONAL >Evolution of polar nano-regions under electric field around ferro-paraelectric transition temperature and its contribution to piezoelectric property in Pb(Mg1/3Nb2/3)O-3-0.30PbTiO(3) crystal
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Evolution of polar nano-regions under electric field around ferro-paraelectric transition temperature and its contribution to piezoelectric property in Pb(Mg1/3Nb2/3)O-3-0.30PbTiO(3) crystal

机译:电气场下极光纳米区的进化及其对Pb(Mg1 / 3NB2 / 3)o-3-0.30pbtio(3)晶体中压电性能的贡献及其对压电性能的贡献

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摘要

As one of the most pronounced structural features, polar nano-regions (PNRs) is believed to have significant contribution to the outstanding piezoelectric property of relaxor-based ferroelectrics. However, direct experimental investigation on the connection between the-PNRs behavior under-electric field and piezoelectric responses is still insufficient. In this work, by the combined use of piezoresponse force microscopy, polarization light microscopy, and the electrical property measurements, we investigate the structure evolution from macro domains to PNRs around ferro-paraelectric phase transition temperature (T-m, 140 degrees C) in Pb(Mg1/3Nb2/3)O-3-0.30PbTiO(3) single crystal. Most importantly, based on the corresponding analysis of unipolar strain-electric-field (5-E) curves at different temperatures and the direct observation of electric-field-induced structure evolution at T-m, we intensively investigate the response of PNRs to electric field and its contribution to piezoelectric property. We conclude that, under electric field, the active PNRs around T-m first serve as polar seeds to induce macro domains from the non-polar matrix, then promote the switching of macro-domains. The large-field strain coefficient d(33)* in these two processes can achieve maximum of about 5410 pm/V and 61710 pm/V at T-m, and gradually decreases at higher temperature with lower PNRs content.
机译:作为最明显的结构特征之一,据信极性纳米区(PNRS)对基于松弛剂的铁电性的优异压电性能具有显着贡献。然而,对-PNR行为之间的连接的直接实验研究仍然不足。在这项工作中,通过组合使用压电响应力显微镜,偏振光显微镜和电性能测量,我们研究了PB中的铁琼脂相转变温度(TM,140℃)周围的宏观结构域的结构演变( MG1 / 3NB2 / 3)O-3-0.30PBTIO(3)单晶。最重要的是,基于不同温度下的单极应变电场(5-e)曲线的相应分析以及TM的电场诱导结构演进的直接观察,我们深入研究了PNR对电场的响应和它对压电性质的贡献。我们得出结论,在电场下,T-M周围的活性PNRS首先用作极性种子以诱导来自非极性矩阵的宏观域,然后促进宏观域的切换。在这两种过程中,大场应变系数D(33)*在T-M处可以获得约5410μm/ v和61710pm / v,并且在较低的pnr含量下逐渐降低。

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