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用于直观观察无铅反铁电体(1-)AgNbO-LiTaO中结构-性能关系的对称模式分析

Symmetry-mode analysis for intuitive observation of structure-property relationships in the lead-free antiferroelectric (1-)AgNbO-LiTaO.

作者信息

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

机构信息

Research School of Chemistry, Australian National University, Canberra, ACT 2601, Australia.

Electronic Materials Research Laboratory, Xi'an Jiaotong University, Xi'an, Shannxi 710049, People's Republic of China.

出版信息

IUCrJ. 2019 Jun 21;6(Pt 4):740-750. doi: 10.1107/S2052252519007711. eCollection 2019 Jul 1.

DOI:10.1107/S2052252519007711
PMID:31316817
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6608632/
Abstract

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-)AgNbO-LiTaO (0 ≤ ≤ 0.09) ceramics. This provides rich structural information that not only clarifies the controversial symmetry assigned to pure AgNbO but also explains well the detailed structural evolution of (1-)AgNbO-LiTaO (0 ≤ ≤ 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 2 structure of pure AgNbO, namely a Λ3 antiferroelectric mode, a T4+ octahedral tilting mode, an H2 / octahedral tilting mode and a Γ4- ferroelectric mode. The H2 and Λ3 modes become progressively inactive with increasing and their destabilization is the driving force behind the composition-driven phase transition between the 2 and 3 phases. This structural variation is consistent with the trend observed in the measured temperature-dependent dielectric properties and polarization-electric field (-) 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-based (anti)ferroelectric materials.

摘要

功能材料对电子和智能设备至关重要。深入理解结构与性能的关系对于设计新材料至关重要。在这项工作中,成功地使用了一种对称模式方法,而不是利用传统的原子坐标,对(1 - x)AgNbO₃ - xLiTaO₃(0 ≤ x ≤ 0.09)陶瓷的中子粉末衍射数据进行结构精修。这提供了丰富的结构信息,不仅澄清了赋予纯AgNbO₃的有争议的对称性,还很好地解释了(1 - x)AgNbO₃ - xLiTaO₃(0 ≤ x ≤ 0.09)陶瓷的详细结构演变,并建立了结构畸变与电学性能之间全面而直接的关系。得出的结论是,有四种相对较大振幅的主要模式主导着纯AgNbO₃的畸变钙钛矿结构,即一个Λ₃反铁电模式、一个T₄⁺八面体倾斜模式、一个H₂/Γ八面体倾斜模式和一个Γ₄⁻铁电模式。随着x的增加,H₂和Λ₃模式逐渐失去活性,它们的失稳是2相和3相之间成分驱动相变的驱动力。这种结构变化与在测量的温度相关介电性能和极化 - 电场(P - E)滞后回线中观察到的趋势一致。本研究中应用的模式晶体学提供了一种通过调整这些新型AgNbO₃基(反)铁电材料中相应模式的振幅来优化相关性能的策略。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/ebaaf6b2731d/m-06-00740-fig12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/54ffb017c209/m-06-00740-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/141a75909af2/m-06-00740-fig2.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/1c76e21d8b24/m-06-00740-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/9c9eb8d5dd14/m-06-00740-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/c1e9c4f236c2/m-06-00740-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/288141cbd011/m-06-00740-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/902a141c9342/m-06-00740-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/3364a2217fee/m-06-00740-fig9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/8cbeaed74ad5/m-06-00740-fig10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/82a835d2f777/m-06-00740-fig11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/ebaaf6b2731d/m-06-00740-fig12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/54ffb017c209/m-06-00740-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/141a75909af2/m-06-00740-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/a0c32b84ada7/m-06-00740-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/1c76e21d8b24/m-06-00740-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/9c9eb8d5dd14/m-06-00740-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/c1e9c4f236c2/m-06-00740-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/288141cbd011/m-06-00740-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/902a141c9342/m-06-00740-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/3364a2217fee/m-06-00740-fig9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/8cbeaed74ad5/m-06-00740-fig10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/82a835d2f777/m-06-00740-fig11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9be2/6608632/ebaaf6b2731d/m-06-00740-fig12.jpg

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