Phase Transformations of Pb_(0.995)La_(0.005)[Zr_(0.95-y)Sn_(0.05)(Mg_(1/3)Nb_(2/3))_y]_(0.99875)O_3 Solid Solutions

E. A. Bikyashev; E. A. Reshetnikova; I. V. Lisnevskaya; T. G. Lupeiko

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Phase Transformations of Pb_(0.995)La_(0.005)[Zr_(0.95-y)Sn_(0.05)(Mg_(1/3)Nb_(2/3))_y]_(0.99875)O_3 Solid Solutions

机译：Pb_（0.995）La_（0.005）[Zr_（0.95-y）Sn_（0.05）（Mg_（1/3）Nb_（2/3））_ y] _（0.990.99）O_3固溶体的相变

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We have constructed phase diagrams of Pb_(0.995)La_(0.005)[Zr_(0.95-y)Sn_(0.05)(Mg_(1/3)Nb_(2/3))_y]_(0.99875)O_3 (y = 0-0.02) solid solutions in different electric fields. Our results demonstrate that, by cooling in a constant electric field, the low-temperature rhombohedral ferroelectric phase can be stabilized in a narrow temperature range. It is shown that the phase state below the Curie temperature strongly depends on the temperature-field history of the material. In particular, the low-temperature rhombohedral ferroelectric phase only appears during cooling. At the same time, the temperature-field stability region of the tetragonal antiferroelectric phase is much broader during heating.

机译：我们构建了Pb_（0.995）La_（0.005）[Zr_（0.95-y）Sn_（0.05）（Mg_（1/3）Nb_（2/3））_ y] _（0.99875）O_3（y = 0的相图-0.02）在不同电场中的固溶体。我们的结果表明，通过在恒定电场中冷却，低温菱面体铁电相可以在狭窄的温度范围内稳定。结果表明，居里温度以下的相态很大程度上取决于材料的温度场历史。特别是，低温菱形铁电相仅在冷却期间出现。同时，四方反铁电相的温度场稳定区域在加热期间要宽得多。

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来源
《Inorganic materials》 |2008年第6期|p.615-621|共7页
作者
E. A. Bikyashev; E. A. Reshetnikova; I. V. Lisnevskaya; T. G. Lupeiko;
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作者单位

Southern Federal University, ul. Zorge 7, Rostov-on-Don, 344090 Russia;

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收录信息美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
原文格式 PDF
正文语种 eng
中图分类工程材料学;
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机译：电场对Pb_（0.9975）La_（0.005）[Zr_（0.9-y）Sn_（0.1）Ti_y] _（0.99875）O_3和Pb_（0.9975）[Zr_（0.895）Sn_（0.1）Ti_yNb_（ 0.005）] O_3固体溶液
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机译：电场对固体溶液中相变的影响Pb_（0.995）La_（0.005）[Zr_（0.9-y）Sn_（0.1）Ti_y] _（0.99875）O_3和Pb_（0.9975）[Zr_（0.895-y）Sn_ ）Ti_yNb_（0.005）] O_3
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Phase Transformations of Pb_(0.995)La_(0.005)[Zr_(0.95-y)Sn_(0.05)(Mg_(1/3)Nb_(2/3))_y]_(0.99875)O_3 Solid Solutions

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