<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Lu T</submitter><funding>Centre of Excellence for Integrative Brain Function, Australian Research Council</funding><pagination>740-750</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC6608632</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>6(Pt 4)</volume><pubmed_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-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub> (0 ≤ &lt;i>x&lt;/i> ≤ 0.09) ceramics. This provides rich structural information that not only clarifies the controversial symmetry assigned to pure AgNbO&lt;sub>3&lt;/sub> but also explains well the detailed structural evolution of (1-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub> (0 ≤ &lt;i>x&lt;/i> ≤ 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 &lt;i>Pmc&lt;/i>2&lt;sub>1&lt;/sub> structure of pure AgNbO&lt;sub>3&lt;/sub>, namely a Λ3 antiferroelectric mode, a T4+ &lt;i>a&lt;/i> &lt;sup>-&lt;/sup> &lt;i>a&lt;/i> &lt;sup>-&lt;/sup> &lt;i>c&lt;/i> &lt;sup>0&lt;/sup> octahedral tilting mode, an H2 &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>c&lt;/i> &lt;sup>+&lt;/sup>/&lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>c&lt;/i> &lt;sup>-&lt;/sup> octahedral tilting mode and a Γ4- ferroelectric mode. The H2 and Λ3 modes become progressively inactive with increasing &lt;i>x&lt;/i> and their destabilization is the driving force behind the composition-driven phase transition between the &lt;i>Pmc&lt;/i>2&lt;sub>1&lt;/sub> and &lt;i>R&lt;/i>3&lt;i>c&lt;/i> phases. This structural variation is consistent with the trend observed in the measured temperature-dependent dielectric properties and polarization-electric field (&lt;i>P&lt;/i>-&lt;i>E&lt;/i>) 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&lt;sub>3&lt;/sub>-based (anti)ferroelectric materials.</pubmed_abstract><journal>IUCrJ</journal><pubmed_title>Symmetry-mode analysis for intuitive observation of structure-property relationships in the lead-free antiferroelectric (1-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub>.</pubmed_title><pmcid>PMC6608632</pmcid><funding_grant_id>DP160104780</funding_grant_id><pubmed_authors>McIntyre GJ</pubmed_authors><pubmed_authors>Pelaiz-Barranco A</pubmed_authors><pubmed_authors>Li Q</pubmed_authors><pubmed_authors>Yu D</pubmed_authors><pubmed_authors>Wei X</pubmed_authors><pubmed_authors>Liu Y</pubmed_authors><pubmed_authors>Studer A</pubmed_authors><pubmed_authors>Tian Y</pubmed_authors><pubmed_authors>Lu T</pubmed_authors><pubmed_authors>Yan H</pubmed_authors><pubmed_authors>Narayanan N</pubmed_authors><pubmed_authors>Withers R</pubmed_authors><pubmed_authors>Xu Z</pubmed_authors><pubmed_authors>Jin L</pubmed_authors><pubmed_authors>Mendez-Gonzalez Y</pubmed_authors></additional><is_claimable>false</is_claimable><name>Symmetry-mode analysis for intuitive observation of structure-property relationships in the lead-free antiferroelectric (1-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub>.</name><description>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-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub> (0 ≤ &lt;i>x&lt;/i> ≤ 0.09) ceramics. This provides rich structural information that not only clarifies the controversial symmetry assigned to pure AgNbO&lt;sub>3&lt;/sub> but also explains well the detailed structural evolution of (1-&lt;i>x&lt;/i>)AgNbO&lt;sub>3&lt;/sub>-&lt;i>x&lt;/i>LiTaO&lt;sub>3&lt;/sub> (0 ≤ &lt;i>x&lt;/i> ≤ 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 &lt;i>Pmc&lt;/i>2&lt;sub>1&lt;/sub> structure of pure AgNbO&lt;sub>3&lt;/sub>, namely a Λ3 antiferroelectric mode, a T4+ &lt;i>a&lt;/i> &lt;sup>-&lt;/sup> &lt;i>a&lt;/i> &lt;sup>-&lt;/sup> &lt;i>c&lt;/i> &lt;sup>0&lt;/sup> octahedral tilting mode, an H2 &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>c&lt;/i> &lt;sup>+&lt;/sup>/&lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>a&lt;/i> &lt;sup>0&lt;/sup> &lt;i>c&lt;/i> &lt;sup>-&lt;/sup> octahedral tilting mode and a Γ4- ferroelectric mode. The H2 and Λ3 modes become progressively inactive with increasing &lt;i>x&lt;/i> and their destabilization is the driving force behind the composition-driven phase transition between the &lt;i>Pmc&lt;/i>2&lt;sub>1&lt;/sub> and &lt;i>R&lt;/i>3&lt;i>c&lt;/i> phases. This structural variation is consistent with the trend observed in the measured temperature-dependent dielectric properties and polarization-electric field (&lt;i>P&lt;/i>-&lt;i>E&lt;/i>) 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&lt;sub>3&lt;/sub>-based (anti)ferroelectric materials.</description><dates><release>2019-01-01T00:00:00Z</release><publication>2019 Jul</publication><modification>2025-05-29T22:10:30.506Z</modification><creation>2025-05-29T22:10:30.506Z</creation></dates><accession>S-EPMC6608632</accession><cross_references><pubmed>31316817</pubmed><doi>10.1107/S2052252519007711</doi></cross_references></HashMap>