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Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions

Ferroelectric materials exhibiting switchable and spontaneous polarization have strong potential to be utilized in various novel electronic devices. Solid solutions of different perovskite structures induce the coexistence of various phases and enhance the physical functionalities around the phase c...

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Autores principales: Sahoo, Satyaranjan, Pradhan, Dhiren K., Kumari, Shalini, Samantaray, Koyal Suman, Singh, Charanjeet, Mishra, Anupam, Rahaman, Md. Mijanur, Behera, Banarji, Kumar, Ashok, Thomas, Reji, Rack, Philip D., Pradhan, Dillip K.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10625606/
https://www.ncbi.nlm.nih.gov/pubmed/37925566
http://dx.doi.org/10.1038/s41598-023-45713-z
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author Sahoo, Satyaranjan
Pradhan, Dhiren K.
Kumari, Shalini
Samantaray, Koyal Suman
Singh, Charanjeet
Mishra, Anupam
Rahaman, Md. Mijanur
Behera, Banarji
Kumar, Ashok
Thomas, Reji
Rack, Philip D.
Pradhan, Dillip K.
author_facet Sahoo, Satyaranjan
Pradhan, Dhiren K.
Kumari, Shalini
Samantaray, Koyal Suman
Singh, Charanjeet
Mishra, Anupam
Rahaman, Md. Mijanur
Behera, Banarji
Kumar, Ashok
Thomas, Reji
Rack, Philip D.
Pradhan, Dillip K.
author_sort Sahoo, Satyaranjan
collection PubMed
description Ferroelectric materials exhibiting switchable and spontaneous polarization have strong potential to be utilized in various novel electronic devices. Solid solutions of different perovskite structures induce the coexistence of various phases and enhance the physical functionalities around the phase coexistence region. The construction of phase diagrams is important as they describe the material properties, which are linked to the underpinning physics determining the system. Here we present the phase diagram of (K(0.5)Na(0.5)NbO(3))–(Ba(0.5)Sr(0.5)TiO(3)) (KNN-BST) system as a function of composition and their associated physical properties. Lead-free (1 − x)KNN–xBST (0 ≤ x ≤ 0.3) solid solution ceramics were synthesized by conventional solid-state reaction technique. The X-ray diffraction and Raman spectroscopic studies indicate composition-dependent structural phase transitions from an orthorhombic phase for x = 0 to orthorhombic + tetragonal dual-phase (for 0.025 ≤ x ≤ 0.15), then a tetragonal + cubic dual-phase (x = 0.2) and finally a cubic single phase for x ≥ 0.25 at room temperature (RT). Among these, the orthorhombic + tetragonal dual-phase system shows an enhanced value of the dielectric constant at room temperature. The phase transition temperatures, orthorhombic to tetragonal (T(O-T)) and tetragonal to cubic (T(C)), decrease with the increase in BST concentrations. The ferroelectric studies show a decrease of both 2P(r) and E(C) values with a rise in BST concentration and x = 0.025 showed a maximum piezoelectric coefficient.
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spelling pubmed-106256062023-11-06 Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions Sahoo, Satyaranjan Pradhan, Dhiren K. Kumari, Shalini Samantaray, Koyal Suman Singh, Charanjeet Mishra, Anupam Rahaman, Md. Mijanur Behera, Banarji Kumar, Ashok Thomas, Reji Rack, Philip D. Pradhan, Dillip K. Sci Rep Article Ferroelectric materials exhibiting switchable and spontaneous polarization have strong potential to be utilized in various novel electronic devices. Solid solutions of different perovskite structures induce the coexistence of various phases and enhance the physical functionalities around the phase coexistence region. The construction of phase diagrams is important as they describe the material properties, which are linked to the underpinning physics determining the system. Here we present the phase diagram of (K(0.5)Na(0.5)NbO(3))–(Ba(0.5)Sr(0.5)TiO(3)) (KNN-BST) system as a function of composition and their associated physical properties. Lead-free (1 − x)KNN–xBST (0 ≤ x ≤ 0.3) solid solution ceramics were synthesized by conventional solid-state reaction technique. The X-ray diffraction and Raman spectroscopic studies indicate composition-dependent structural phase transitions from an orthorhombic phase for x = 0 to orthorhombic + tetragonal dual-phase (for 0.025 ≤ x ≤ 0.15), then a tetragonal + cubic dual-phase (x = 0.2) and finally a cubic single phase for x ≥ 0.25 at room temperature (RT). Among these, the orthorhombic + tetragonal dual-phase system shows an enhanced value of the dielectric constant at room temperature. The phase transition temperatures, orthorhombic to tetragonal (T(O-T)) and tetragonal to cubic (T(C)), decrease with the increase in BST concentrations. The ferroelectric studies show a decrease of both 2P(r) and E(C) values with a rise in BST concentration and x = 0.025 showed a maximum piezoelectric coefficient. Nature Publishing Group UK 2023-11-04 /pmc/articles/PMC10625606/ /pubmed/37925566 http://dx.doi.org/10.1038/s41598-023-45713-z Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Sahoo, Satyaranjan
Pradhan, Dhiren K.
Kumari, Shalini
Samantaray, Koyal Suman
Singh, Charanjeet
Mishra, Anupam
Rahaman, Md. Mijanur
Behera, Banarji
Kumar, Ashok
Thomas, Reji
Rack, Philip D.
Pradhan, Dillip K.
Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title_full Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title_fullStr Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title_full_unstemmed Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title_short Compositional induced structural phase transitions in (1 − x)(K(0.5)Na(0.5))NbO(3)–x(Ba(0.5)Sr(0.5))TiO(3) ferroelectric solid solutions
title_sort compositional induced structural phase transitions in (1 − x)(k(0.5)na(0.5))nbo(3)–x(ba(0.5)sr(0.5))tio(3) ferroelectric solid solutions
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10625606/
https://www.ncbi.nlm.nih.gov/pubmed/37925566
http://dx.doi.org/10.1038/s41598-023-45713-z
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