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DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2)
The origins of dielectric responses in Ni(2+) and Nb(5+) co-doped TiO(2) were explored considering intrinsic and extrinsic effects. DFT calculations demonstrated that Ni(2+) doping induced oxygen vacancies, while Nb(5+) doping generated free electrons. Theoretical predictions indicated complex defec...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10619632/ https://www.ncbi.nlm.nih.gov/pubmed/37920200 http://dx.doi.org/10.1039/d3ra06541c |
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author | Thongyong, Nateeporn Thongbai, Prasit Srepusharawoot, Pornjuk |
author_facet | Thongyong, Nateeporn Thongbai, Prasit Srepusharawoot, Pornjuk |
author_sort | Thongyong, Nateeporn |
collection | PubMed |
description | The origins of dielectric responses in Ni(2+) and Nb(5+) co-doped TiO(2) were explored considering intrinsic and extrinsic effects. DFT calculations demonstrated that Ni(2+) doping induced oxygen vacancies, while Nb(5+) doping generated free electrons. Theoretical predictions indicated complex defect dipoles forming in the rutile structure, contributing to overall dielectric responses. Theoretical calculations also showed a possible linear alignment of Ni(2+)–2Nb(5+) without oxygen vacancies, especially in high doping concentrations. Experimentally, (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) ceramics (x = 1%, 2.5%, and 10%) were synthesized. The substantial dielectric response at room temperature, attributed to factors like defect dipoles and grain boundary/surface barrier layer capacitor (GBLC/SBLC) effects, increased with higher doping levels. However, in a temperature range where GBLC/SBLC effects were suppressed, the dielectric response decreased with increased doping, likely due to self-charge compensation between Ni(2+)–2N(b5+). Notably, (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) with x = 2.5% exhibited a high dielectric permittivity of 10(4) and a low loss tangent of 0.029 at 1 kHz. Moreover, the dielectric permittivity changed by less than ±15% (compared to 25 °C) at 150 °C. This work provides an understanding of the origins of dielectric responses in co-doped TiO(2) and optimizes the doping concentration to achieve the best dielectric performance. |
format | Online Article Text |
id | pubmed-10619632 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | The Royal Society of Chemistry |
record_format | MEDLINE/PubMed |
spelling | pubmed-106196322023-11-02 DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) Thongyong, Nateeporn Thongbai, Prasit Srepusharawoot, Pornjuk RSC Adv Chemistry The origins of dielectric responses in Ni(2+) and Nb(5+) co-doped TiO(2) were explored considering intrinsic and extrinsic effects. DFT calculations demonstrated that Ni(2+) doping induced oxygen vacancies, while Nb(5+) doping generated free electrons. Theoretical predictions indicated complex defect dipoles forming in the rutile structure, contributing to overall dielectric responses. Theoretical calculations also showed a possible linear alignment of Ni(2+)–2Nb(5+) without oxygen vacancies, especially in high doping concentrations. Experimentally, (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) ceramics (x = 1%, 2.5%, and 10%) were synthesized. The substantial dielectric response at room temperature, attributed to factors like defect dipoles and grain boundary/surface barrier layer capacitor (GBLC/SBLC) effects, increased with higher doping levels. However, in a temperature range where GBLC/SBLC effects were suppressed, the dielectric response decreased with increased doping, likely due to self-charge compensation between Ni(2+)–2N(b5+). Notably, (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) with x = 2.5% exhibited a high dielectric permittivity of 10(4) and a low loss tangent of 0.029 at 1 kHz. Moreover, the dielectric permittivity changed by less than ±15% (compared to 25 °C) at 150 °C. This work provides an understanding of the origins of dielectric responses in co-doped TiO(2) and optimizes the doping concentration to achieve the best dielectric performance. The Royal Society of Chemistry 2023-11-01 /pmc/articles/PMC10619632/ /pubmed/37920200 http://dx.doi.org/10.1039/d3ra06541c Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by-nc/3.0/ |
spellingShingle | Chemistry Thongyong, Nateeporn Thongbai, Prasit Srepusharawoot, Pornjuk DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title | DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title_full | DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title_fullStr | DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title_full_unstemmed | DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title_short | DFT calculations and giant dielectric responses in (Ni(1/3)Nb(2/3))(x)Ti(1−x)O(2) |
title_sort | dft calculations and giant dielectric responses in (ni(1/3)nb(2/3))(x)ti(1−x)o(2) |
topic | Chemistry |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10619632/ https://www.ncbi.nlm.nih.gov/pubmed/37920200 http://dx.doi.org/10.1039/d3ra06541c |
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