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Electric-field-induced AFE-FE transitions and associated strain/preferred orientation in antiferroelectric PLZST

Electric-field-induced, antiferroelectric-ferroelectric (AFE-FE) phase transitions are common for AFE materials. To date, the strain and preferred orientation evolution as well as the role of the intermediate FE state during the successive AFE-FE-AFE phase transitions has not been clear. To this end...

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Detalles Bibliográficos
Autores principales: Lu, Teng, Studer, Andrew J., Noren, Lasse, Hu, Wanbiao, Yu, Dehong, McBride, Bethany, Feng, Yujun, Withers, Ray L., Chen, Hua, Xu, Zhuo, Liu, Yun
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4812248/
https://www.ncbi.nlm.nih.gov/pubmed/27025685
http://dx.doi.org/10.1038/srep23659
Descripción
Sumario:Electric-field-induced, antiferroelectric-ferroelectric (AFE-FE) phase transitions are common for AFE materials. To date, the strain and preferred orientation evolution as well as the role of the intermediate FE state during the successive AFE-FE-AFE phase transitions has not been clear. To this end, we have herein studied a typical AFE Pb(0.97)La(0.02)(Zr(0.56)Sn(0.33)Ti(0.11))O(3) (PLZST) material using in-situ neutron diffraction. It is striking that the AFE-FE phase transition is not fully reversible: in the electric-field-induced FE state, the induced strain exhibits an elliptical distribution, which in turn leads to significant preferred orientation in the final AFE state after withdrawal of the applied electric-field. The ω-dependent neutron diffraction patterns show clear evidence of the induced strain distribution and associated preferred orientation arising from the AFE-FE phase transition. The current work also provides an explanation for several temperature and electric-field dependent dielectric anomalies as well as unrecovered strain change which appear in AFE materials after exposure to sufficiently high electric fields.