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CaNaTiNbO陶瓷的结构特性与介电弛豫

Structure properties and dielectric relaxation of CaNaTiNbO ceramic.

作者信息

Ghoudi Hanen, Chkoundali Souad, Raddaoui Zeineb, Aydi Abdelhedi

机构信息

Laboratoire de physique des Matériaux et des Nanomatériaux Appliquée à l'environnement, Faculté des Sciences de Gabès, Université de Gabès Tunisia

Laboratoire des Matériaux Multifonctionnels et Applications, Faculté des Sciences de Sfax (FSS), Université de Sfax B. P.1171 3018 Sfax Tunisia.

出版信息

RSC Adv. 2019 Aug 13;9(44):25358-25367. doi: 10.1039/c9ra03967h.

DOI:10.1039/c9ra03967h
PMID:35530109
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9070096/
Abstract

In this paper, the synthesis of CaNaTiNbO (CNTN) ceramic by a solid-state reaction method is reported. The results of Rietveld refinement of X-ray diffraction (XRD) patterns at room temperature showed a pure tetragonal perovskite (4 space group). Raman spectroscopy analysis, ranging from of 50 to 1000 cm, at room temperature, validates the results of XRD. The dielectric properties was studied by complex impedance spectroscopy examined in broad frequency range, 100 Hz to 200 kHz, at different temperatures. The dielectric permittivity for our CNTN compound confirms the typical relaxor behavior. The investigation of the diffuseness of the transition was conducted by fitting the experimental data with modified Curie-Weiss law; Gaussian distribution and Power law confirm the presence of a short-range association between the polar nanoregions (PNRs). The obtained values of the diffuseness coefficient are of the order 1.6, which corresponds to the diffuse phase transition (DPT) ascribed to the existence of various states of polarization, thus various relaxation times in different regions. The value of diffuseness is of the order 85 and the degree of relaxor (Δ = 65 K) is interesting as far as microelectric applications are concerned. Moreover, based on the frequency dependence of temperature at dielectric maxima using Vogel-Fulcher relationship, a strong evidence for a static freezing temperature with regards to thermally-activated polarization fluctuations was found.

摘要

本文报道了采用固态反应法合成CaNaTiNbO(CNTN)陶瓷。室温下X射线衍射(XRD)图谱的Rietveld精修结果显示为纯四方钙钛矿(4种空间群)。室温下50至1000 cm范围内的拉曼光谱分析验证了XRD的结果。通过在100 Hz至200 kHz的宽频率范围和不同温度下进行复阻抗谱研究介电性能。我们的CNTN化合物的介电常数证实了典型的弛豫铁电体行为。通过用修正的居里 - 外斯定律拟合实验数据来研究转变的漫散性;高斯分布和幂律证实了极性纳米区域(PNR)之间存在短程关联。得到的漫散系数值约为1.6,这对应于归因于各种极化状态存在的漫散相变(DPT),因此不同区域有不同的弛豫时间。就微电子应用而言,漫散度值约为85且弛豫铁电体程度(Δ = 65 K)很有意思。此外,基于使用Vogel - Fulcher关系在介电最大值处温度的频率依赖性,发现了关于热激活极化涨落的静态冻结温度的有力证据。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/066b5ed5a6ad/c9ra03967h-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/8c6b5493caf1/c9ra03967h-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/120df15a8cbe/c9ra03967h-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/0fe8cfa625eb/c9ra03967h-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/066b5ed5a6ad/c9ra03967h-f8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/8c6b5493caf1/c9ra03967h-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/120df15a8cbe/c9ra03967h-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/0fe8cfa625eb/c9ra03967h-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3725/9070096/066b5ed5a6ad/c9ra03967h-f8.jpg

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本文引用的文献

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2
Dielectric, structural and Raman studies on (Na(0.5)Bi(0.5)TiO(3))((1 - x))(BiCrO(3))(x) ceramic.介电、结构和拉曼研究(Na(0.5)Bi(0.5)TiO(3))((1 - x))(BiCrO(3))(x)陶瓷。
J Phys Condens Matter. 2011 Feb 9;23(5):055901. doi: 10.1088/0953-8984/23/5/055901. Epub 2011 Jan 19.
3
Diffuse phase transitions and random-field-induced domain states of the "relaxor" ferroelectric PbMg1/3Nb2/3O3.
“弛豫铁电体”PbMg1/3Nb2/3O3的弥散相变及随机场诱导的畴态
Phys Rev Lett. 1992 Feb 10;68(6):847-850. doi: 10.1103/PhysRevLett.68.847.