Abstract <![CDATA[Ferroelastic domain structure and phase transition in single-crystalline [PbZn <ce:inf loc='post'>1/3</ce:inf>Nb <ce:inf loc='post'>2/3</ce:inf>O <ce:inf loc='post'>3</ce:inf>] <ce:inf loc='post'>1-x</ce:inf>[PbTiO <ce:inf loc='post'>3</ce:inf>] <ce:inf loc='post'>x</ce:inf> observed via <ce:italic>in situ</ce:italic> x-ray microbeam]]>
首页> 外文期刊>Journal of the European Ceramic Society >1/3Nb 2/3O 3] 1-x[PbTiO 3] x observed via in situ x-ray microbeam]]>
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1/3Nb 2/3O 3] 1-x[PbTiO 3] x observed via in situ x-ray microbeam]]>

机译:<![CDATA [CDATA [单晶中的铁弹性域结构和相转移[PBZN 1/3 NB 2/3 o 3 ] 1-x [pbtio 3 ] X 通过原位 X射线microbeam]]>

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摘要

Abstract(1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this work, we extensively investigated (1-x)PZN-xPT (x=0.07–0.11) ferroelectric single crystals usingin-situsynchrotron μXRD, complemented by TEM and PFM, to correlate microstructures with phase transitions. The results reveal that (i) at 25°C, the equilibrium state of (1-x)PZN-xPT is a metastable orthorhombic phase for x=0.07 and 0.08, while it shows coexistence of orthorhombic and tetragonal phases for x=0.09 and x=0.11, with all ferroelectric phases accompanied by ferroelastic domains; (ii) upon heating, the phase transformation in x=0.07 is Orthorhombic→Monoclinic→Tetragonal→Cubic. The coexistence of ferroelectric tetragonal and paraelectric cubic phases wasin-situobserved in x=0.08 above Curie temperature (TC), and (iii) phase transition can be explained by the evolution of the ferroelectric and ferroelastic domains. These results disclose that (1-x)PZN-xPT are in an unstable regime, which is possible factor for its anomalous dielectric response and high piezoelectric coefficient.]]>
机译:<![cdata [ 抽象 (1-x)Pb(zn ​​ 1/3 Nb 2/3 )O 3 -XPBTIO 3 < / CE:INF>((1-x)PZN-XPT)是最重要的压电材料之一。在这项工作中,我们使用原位调查(1-x)pzn-xpt(x = 0.07-0.11)铁电单晶:Italic>同步>同步> SynchrotronμXRD,由TEM和PFM补充说将微观结构与相变相关性。结果表明(i)在25℃下,(1-x)PZN-XPT的平衡状态是X = 0.07和0.08的亚稳定性正常相位,而其显示出X = 0.09的正交和四方相的共存。 X = 0.11,所有铁电相伴有铁旋畴; (ii)在加热时,X = 0.07中的相变为正晶→单斜→四方→立方体。铁电四方和琼脂等阶段的共存是原位>斜体>在x = 0.08以上居里温度观察( t C ),(III)相变可以通过铁电和铁弹性结构域的演变来解释。这些结果公开了(1-x)pzn-xpt处于不稳定的状态,这是其异常介电响应和高压电系数的可能因素。 ]]>

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    Shenzhen Key Laboratory of Special Functional Materials Shenzhen Engineering Laboratory for Advanced Technology of Ceramics College of Materials Science and Engineering Shenzhen University;

    Temasek Laboratories Nanyang Technological University;

    Advanced Light Source (ALS) Lawrence Berkeley National Laboratory (LBNL);

    Shenzhen Key Laboratory of Special Functional Materials Shenzhen Engineering Laboratory for Advanced Technology of Ceramics College of Materials Science and Engineering Shenzhen University;

    Shenzhen Key Laboratory of Special Functional Materials Shenzhen Engineering Laboratory for Advanced Technology of Ceramics College of Materials Science and Engineering Shenzhen University;

    University Research Facility in Materials Characterization and Device Fabrication The Hong Kong Polytechnic University;

    Shenzhen Key Laboratory of Special Functional Materials Shenzhen Engineering Laboratory for Advanced Technology of Ceramics College of Materials Science and Engineering Shenzhen University;

    Shenzhen Key Laboratory of Special Functional Materials Shenzhen Engineering Laboratory for Advanced Technology of Ceramics College of Materials Science and Engineering Shenzhen University;

    Department of Applied Physics and Materials Research Center The Hong Kong Polytechnic University;

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