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High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System

[Image: see text] This research study examines the high-temperature dielectric relaxation and electric conduction mechanisms in (x)LaCoO(3)-(1 – x)Na(0.5)Bi(0.5)TiO(3) samples, where x is 0.05, 0.10, and 0.15. The findings demonstrate that all the samples exhibit two dielectric transitions: first, a...

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Autores principales: Singh, Surinder, Kaur, Anumeet, Kaur, Parwinder, Singh, Lakhwant
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10357530/
https://www.ncbi.nlm.nih.gov/pubmed/37483226
http://dx.doi.org/10.1021/acsomega.3c04490
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author Singh, Surinder
Kaur, Anumeet
Kaur, Parwinder
Singh, Lakhwant
author_facet Singh, Surinder
Kaur, Anumeet
Kaur, Parwinder
Singh, Lakhwant
author_sort Singh, Surinder
collection PubMed
description [Image: see text] This research study examines the high-temperature dielectric relaxation and electric conduction mechanisms in (x)LaCoO(3)-(1 – x)Na(0.5)Bi(0.5)TiO(3) samples, where x is 0.05, 0.10, and 0.15. The findings demonstrate that all the samples exhibit two dielectric transitions: first, a frequency-dispersive shoulder at a lower temperature (T(s)) around 425–450 K, which is associated with polar nanoregions (PNRs), and second, from ferroelectric to paraelectric transition at the Curie temperature (T(c)) approximately between 580 and 650 K. The impedance analysis reveals the negative temperature coefficient of resistance behavior of the specimens. The broad and asymmetric relaxation peaks obtained from modulus spectroscopy demonstrate a wide range of relaxations, suggesting non-Debye-type behavior. Furthermore, the conductivity studies provide insights into understanding the transport phenomena in the samples. The oxygen vacancies resulting from the addition of LaCoO(3) into the Na(0.5)Bi(0.5)TiO(3) ceramics are responsible for the relaxation and conduction processes, and the charge carrier is doubly ionized oxygen ion vacancies. All samples except for LCNBT10 at 1 kHz exhibit a negative magnetodielectric response.
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spelling pubmed-103575302023-07-21 High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System Singh, Surinder Kaur, Anumeet Kaur, Parwinder Singh, Lakhwant ACS Omega [Image: see text] This research study examines the high-temperature dielectric relaxation and electric conduction mechanisms in (x)LaCoO(3)-(1 – x)Na(0.5)Bi(0.5)TiO(3) samples, where x is 0.05, 0.10, and 0.15. The findings demonstrate that all the samples exhibit two dielectric transitions: first, a frequency-dispersive shoulder at a lower temperature (T(s)) around 425–450 K, which is associated with polar nanoregions (PNRs), and second, from ferroelectric to paraelectric transition at the Curie temperature (T(c)) approximately between 580 and 650 K. The impedance analysis reveals the negative temperature coefficient of resistance behavior of the specimens. The broad and asymmetric relaxation peaks obtained from modulus spectroscopy demonstrate a wide range of relaxations, suggesting non-Debye-type behavior. Furthermore, the conductivity studies provide insights into understanding the transport phenomena in the samples. The oxygen vacancies resulting from the addition of LaCoO(3) into the Na(0.5)Bi(0.5)TiO(3) ceramics are responsible for the relaxation and conduction processes, and the charge carrier is doubly ionized oxygen ion vacancies. All samples except for LCNBT10 at 1 kHz exhibit a negative magnetodielectric response. American Chemical Society 2023-07-07 /pmc/articles/PMC10357530/ /pubmed/37483226 http://dx.doi.org/10.1021/acsomega.3c04490 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Singh, Surinder
Kaur, Anumeet
Kaur, Parwinder
Singh, Lakhwant
High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title_full High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title_fullStr High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title_full_unstemmed High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title_short High-Temperature Dielectric Relaxation and Electric Conduction Mechanisms in a LaCoO(3)-Modified Na(0.5)Bi(0.5)TiO(3) System
title_sort high-temperature dielectric relaxation and electric conduction mechanisms in a lacoo(3)-modified na(0.5)bi(0.5)tio(3) system
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10357530/
https://www.ncbi.nlm.nih.gov/pubmed/37483226
http://dx.doi.org/10.1021/acsomega.3c04490
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