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Fatigue endurance enhancement of Sn-doped Pb(LuNb)O-PbTiO ceramics.

作者信息

Wang Chenxi, He Chao, Wang Zujian, Li Xiuzhi, Yang Xiaoming, Liu Ying, Long Xifa

机构信息

Key Laboratory of Optoelectronic Materials Chemistry and Physics, Fujian Institute of Research on the Structure of Matter, Chinese Academy of Sciences Fuzhou 350002 Fujian China

University of Chinese Academy of Sciences Beijing China.

出版信息

RSC Adv. 2018 Mar 26;8(21):11633-11642. doi: 10.1039/c8ra00732b. eCollection 2018 Mar 21.

DOI:10.1039/c8ra00732b
PMID:35542813
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9079097/
Abstract

Several mechanisms and methods have been proposed to study the nature of electric fatigue in ferroelectric materials with perovskite structure, including defect agglomeration, field screening and the reorientation of defect dipoles. To ascertain the effect of defect, defect dipoles in particular on the fatigue behavior in perovskite ferroelectrics, 0.51Pb(LuNb)O-0.49PbTi Sn O ferroelectric ceramics were fabricated in this work. It is found that the fatigue endurance has been enhanced after Sn-doping. An abnormal strong self-rejuvenation of polarization was also detected for un-poled and un-aged samples resulting from the reorientation of defect dipoles. The defect dipoles were determined by the confirmed change of the valence of Sn ions and the appearance of oxygen vacancies. The reorientation was also confirmed by the internal bias of - hysteresis loops during the fatigue process. With more Sn doped into the matrix, the symmetry changed from a coexistence of rhombohedral and tetragonal phase to a rhombohedral phase. The remnant polarization decreased, while the coercive field first decreased then increased as increased, which resulted from the composition variance and the effect of defect dipoles. It indicates that the defect dipoles play an important role in the electric fatigue behavior of Sn-doping PLN-PT ceramics.

摘要
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/7317f7c0e68e/c8ra00732b-f10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/c32e3623f105/c8ra00732b-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/8dc0b17eb985/c8ra00732b-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/6cf1c3381141/c8ra00732b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/120aee2add2c/c8ra00732b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/9cbdc63d68a5/c8ra00732b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/0d8dfd027681/c8ra00732b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/4766a518c6f9/c8ra00732b-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/d27d0c40b760/c8ra00732b-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/e463962e7c6e/c8ra00732b-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/7317f7c0e68e/c8ra00732b-f10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/c32e3623f105/c8ra00732b-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/8dc0b17eb985/c8ra00732b-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/6cf1c3381141/c8ra00732b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/120aee2add2c/c8ra00732b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/9cbdc63d68a5/c8ra00732b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/0d8dfd027681/c8ra00732b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/4766a518c6f9/c8ra00732b-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/d27d0c40b760/c8ra00732b-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/e463962e7c6e/c8ra00732b-f9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/07f2/9079097/7317f7c0e68e/c8ra00732b-f10.jpg

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Structure and properties of Bi(Zn0.5Ti0.5)O3- Pb(Zr(1-x)Ti(x))O3 ferroelectric single crystals grown by a top-seeded solution growth technique.采用顶部籽晶溶液生长技术生长的Bi(Zn0.5Ti0.5)O3 - Pb(Zr(1 - x)Ti(x))O3铁电单晶的结构与性能
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SrTiO₃ 中纳米工程氧空位分布的原子尺度成像。
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