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Symmetry-mode analysis for intuitive observation of structure–property relationships in the lead-free antiferroelectric (1−x)AgNbO(3)–xLiTaO(3)

Functional materials are of critical importance to electronic and smart devices. A deep understanding of the structure–property relationship is essential for designing new materials. In this work, instead of utilizing conventional atomic coordinates, a symmetry-mode approach is successfully used to...

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Detalles Bibliográficos
Autores principales: Lu, Teng, Tian, Ye, Studer, Andrew, Narayanan, Narendirakumar, Li, Qian, Withers, Ray, Jin, Li, Mendez-González, Y., Peláiz-Barranco, A., Yu, Dehong, McIntyre, Garry J., Xu, Zhuo, Wei, Xiaoyong, Yan, Haixue, Liu, Yun
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6608632/
https://www.ncbi.nlm.nih.gov/pubmed/31316817
http://dx.doi.org/10.1107/S2052252519007711
Descripción
Sumario:Functional materials are of critical importance to electronic and smart devices. A deep understanding of the structure–property relationship is essential for designing new materials. In this work, instead of utilizing conventional atomic coordinates, a symmetry-mode approach is successfully used to conduct structure refinement of the neutron powder diffraction data of (1−x)AgNbO(3)–xLiTaO(3) (0 ≤ x ≤ 0.09) ceramics. This provides rich structural information that not only clarifies the controversial symmetry assigned to pure AgNbO(3) but also explains well the detailed structural evolution of (1−x)AgNbO(3)–xLiTaO(3) (0 ≤ x ≤ 0.09) ceramics, and builds a comprehensive and straightforward relationship between structural distortion and electrical properties. It is concluded that there are four relatively large-amplitude major modes that dominate the distorted Pmc2(1) structure of pure AgNbO(3), namely a Λ3 antiferroelectric mode, a T4+ a (−) a (−) c (0) octahedral tilting mode, an H2 a (0) a (0) c (+)/a (0) a (0) c (−) octahedral tilting mode and a Γ4− ferroelectric mode. The H2 and Λ3 modes become progressively inactive with increasing x and their destabilization is the driving force behind the composition-driven phase transition between the Pmc2(1) and R3c phases. This structural variation is consistent with the trend observed in the measured temperature-dependent dielectric properties and polarization–electric field (P-E) hysteresis loops. The mode crystallography applied in this study provides a strategy for optimizing related properties by tuning the amplitudes of the corresponding modes in these novel AgNbO(3)-based (anti)ferroelectric materials.