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在铌酸钠反铁电体中存在明确的双滞后回线。

Well-defined double hysteresis loop in NaNbO antiferroelectrics.

机构信息

Center on Nanoenergy Research, State Key Laboratory of Featured Metal Materials and Life-cycle Safety for Composite Structures; School of Resources, Environment and Materials; Guangxi University, 530004, Nanning, China.

School of Chemistry & Chemical Engineering, Guangxi University, 530004, Nanning, China.

出版信息

Nat Commun. 2023 Mar 30;14(1):1776. doi: 10.1038/s41467-023-37469-x.

DOI:10.1038/s41467-023-37469-x
PMID:36997552
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10063644/
Abstract

Antiferroelectrics (AFEs) are promising candidates in energy-storage capacitors, electrocaloric solid-cooling, and displacement transducers. As an actively studied lead-free antiferroelectric (AFE) material, NaNbO has long suffered from its ferroelectric (FE)-like polarization-electric field (P-E) hysteresis loops with high remnant polarization and large hysteresis. Guided by theoretical calculations, a new strategy of reducing the oxygen octahedral tilting angle is proposed to stabilize the AFE P phase (Space group Pbma) of NaNbO. To validate this, we judiciously introduced CaHfO with a low Goldschmidt tolerance factor and AgNbO with a low electronegativity difference into NaNbO, the decreased cation displacements and [BO] octahedral tilting angles were confirmed by Synchrotron X-ray powder diffraction and aberration-corrected scanning transmission electron microscopy. Of particular importance is that the 0.75NaNbO-0.20AgNbO-0.05CaHfO ceramic exhibits highly reversible phase transition between the AFE and FE states, showing well-defined double P-E loops and sprout-shaped strain-electric field curves with reduced hysteresis, low remnant polarization, high AFE-FE phase transition field, and zero negative strain. Our work provides a new strategy for designing NaNbO-based AFE material with well-defined double P-E loops, which can also be extended to discover a variety of new lead-free AFEs.

摘要

反铁电体(AFE)在储能电容器、电卡固体制冷和位移传感器等领域具有广阔的应用前景。作为一种备受关注的无铅反铁电(AFE)材料,NaNbO 长期以来一直存在铁电(FE)类似的极化-电场(P-E)滞后回线,表现出较高的剩余极化和较大的滞后。受理论计算的启发,提出了一种新的策略来降低氧八面体倾斜角,以稳定 NaNbO 的 AFE P 相(空间群 Pbma)。为了验证这一点,我们巧妙地引入了 Goldschmidt 容忍因子较低的 CaHfO 和电负性差较小的 AgNbO 到 NaNbO 中,通过同步加速器 X 射线粉末衍射和像差校正扫描透射电子显微镜证实了阳离子位移和 [BO] 八面体倾斜角度的降低。特别重要的是,0.75NaNbO-0.20AgNbO-0.05CaHfO 陶瓷表现出 AFE 和 FE 状态之间高度可逆的相变,表现出明确的双 P-E 回线和具有较小滞后、低剩余极化、高 AFE-FE 相变场和零负应变的芽状应变-电场曲线。我们的工作为设计具有明确双 P-E 回线的 NaNbO 基 AFE 材料提供了一种新策略,也可扩展到发现各种新型无铅 AFE。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/70e8a1197886/41467_2023_37469_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/9e8aa36dfc98/41467_2023_37469_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/79987a10d9a3/41467_2023_37469_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/c1cf6b741473/41467_2023_37469_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/b814d7b1b39e/41467_2023_37469_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/70e8a1197886/41467_2023_37469_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/9e8aa36dfc98/41467_2023_37469_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/79987a10d9a3/41467_2023_37469_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/c1cf6b741473/41467_2023_37469_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/b814d7b1b39e/41467_2023_37469_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/00a6/10063644/70e8a1197886/41467_2023_37469_Fig5_HTML.jpg

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