Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12

The frequency dependences of AC conductivity and dielectric constant spectra of polycrystalline CCTO are reappraised. The physical significance of the related spectra has been solved based on the present model constructed by the super-linear and the extended power laws, which is composed of five rel...

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Main Authors: Tsang-Tse Fang, Hsuan-Jung Hsu, Hsing-I. Hsiang
Format: Article
Language:English
Published: AIP Publishing LLC 2025-04-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0253162
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author Tsang-Tse Fang
Hsuan-Jung Hsu
Hsing-I. Hsiang
author_facet Tsang-Tse Fang
Hsuan-Jung Hsu
Hsing-I. Hsiang
author_sort Tsang-Tse Fang
collection DOAJ
description The frequency dependences of AC conductivity and dielectric constant spectra of polycrystalline CCTO are reappraised. The physical significance of the related spectra has been solved based on the present model constructed by the super-linear and the extended power laws, which is composed of five relaxations: region I′: super-linear power law relaxation, region I: grain intra-clusters relaxation and grain inter-clusters relaxation, and region II: overall intra-clusters relaxation and overall inter-clusters relaxation. It is found that the existence of super-linear power law is related to the electrons hopping in the asymmetric double-well potential caused by the lattice strain. The frequency-independent conductivity in Jonscher’s power law equation is redefined, denoted as quasi-DC conductivity at a critical frequency as inter-clusters become percolation clusters between blocks. The blocks can be either grain boundary (region I) or electrode (region II). The obtained activation energy of the quasi-DC conductivity is high ascribed to the electrons surmounting the barriers caused by lattice strain for region I and grain boundary barrier for region II. In comparing the evaluated values of the activation energy of temperature dependence of loss peak frequency and the quasi-DC conductivity, it implies that the occurrence of the loss peak may be attributed to the most charge carriers surmounting the largest barrier arising from lattice strain or grain boundary in order to form the percolation path. The defect structure of the grain boundary barrier of CCTO is proposed.
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institution DOAJ
issn 2158-3226
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publishDate 2025-04-01
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spelling doaj-art-86343afde6804ee4a656eb3eb5d136c32025-08-20T03:11:02ZengAIP Publishing LLCAIP Advances2158-32262025-04-01154045302045302-910.1063/5.0253162Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12Tsang-Tse Fang0Hsuan-Jung Hsu1Hsing-I. Hsiang2Department of Materials Science and Engineering, National Cheng Kung University, Tainan 70101, Taiwan and Department of Resources Engineering, National Cheng Kung University, Tainan 70101, TaiwanDepartment of Materials Science and Engineering, National Cheng Kung University, Tainan 70101, Taiwan and Department of Resources Engineering, National Cheng Kung University, Tainan 70101, TaiwanDepartment of Materials Science and Engineering, National Cheng Kung University, Tainan 70101, Taiwan and Department of Resources Engineering, National Cheng Kung University, Tainan 70101, TaiwanThe frequency dependences of AC conductivity and dielectric constant spectra of polycrystalline CCTO are reappraised. The physical significance of the related spectra has been solved based on the present model constructed by the super-linear and the extended power laws, which is composed of five relaxations: region I′: super-linear power law relaxation, region I: grain intra-clusters relaxation and grain inter-clusters relaxation, and region II: overall intra-clusters relaxation and overall inter-clusters relaxation. It is found that the existence of super-linear power law is related to the electrons hopping in the asymmetric double-well potential caused by the lattice strain. The frequency-independent conductivity in Jonscher’s power law equation is redefined, denoted as quasi-DC conductivity at a critical frequency as inter-clusters become percolation clusters between blocks. The blocks can be either grain boundary (region I) or electrode (region II). The obtained activation energy of the quasi-DC conductivity is high ascribed to the electrons surmounting the barriers caused by lattice strain for region I and grain boundary barrier for region II. In comparing the evaluated values of the activation energy of temperature dependence of loss peak frequency and the quasi-DC conductivity, it implies that the occurrence of the loss peak may be attributed to the most charge carriers surmounting the largest barrier arising from lattice strain or grain boundary in order to form the percolation path. The defect structure of the grain boundary barrier of CCTO is proposed.http://dx.doi.org/10.1063/5.0253162
spellingShingle Tsang-Tse Fang
Hsuan-Jung Hsu
Hsing-I. Hsiang
Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
AIP Advances
title Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
title_full Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
title_fullStr Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
title_full_unstemmed Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
title_short Revisit of the AC conductivity behavior and the colossal dielectric constant of CaCu3Ti4O12
title_sort revisit of the ac conductivity behavior and the colossal dielectric constant of cacu3ti4o12
url http://dx.doi.org/10.1063/5.0253162
work_keys_str_mv AT tsangtsefang revisitoftheacconductivitybehaviorandthecolossaldielectricconstantofcacu3ti4o12
AT hsuanjunghsu revisitoftheacconductivitybehaviorandthecolossaldielectricconstantofcacu3ti4o12
AT hsingihsiang revisitoftheacconductivitybehaviorandthecolossaldielectricconstantofcacu3ti4o12