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Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals
A series of high-quality, large-sized (maximum size of 16 × 16 × 32 mm(3)) K(1−x)Na(x)Ta(1−y)Nb(y)O(3) (x = 0.61, 0.64, and 0.70 and corresponding y = 0.58, 0.60, and 0.63) single crystals were grown using the top-seed solution growth method. The segregation of the crystals, which allowed for precis...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4861918/ https://www.ncbi.nlm.nih.gov/pubmed/27160075 http://dx.doi.org/10.1038/srep25637 |
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author | Tian, Hao Meng, Xiangda Hu, Chengpeng Tan, Peng Cao, Xilong Shi, Guang Zhou, Zhongxiang Zhang, Rui |
author_facet | Tian, Hao Meng, Xiangda Hu, Chengpeng Tan, Peng Cao, Xilong Shi, Guang Zhou, Zhongxiang Zhang, Rui |
author_sort | Tian, Hao |
collection | PubMed |
description | A series of high-quality, large-sized (maximum size of 16 × 16 × 32 mm(3)) K(1−x)Na(x)Ta(1−y)Nb(y)O(3) (x = 0.61, 0.64, and 0.70 and corresponding y = 0.58, 0.60, and 0.63) single crystals were grown using the top-seed solution growth method. The segregation of the crystals, which allowed for precise control of the individual components of the crystals during growth, was investigated. The obtained crystals exhibited excellent properties without being annealed, including a low dielectric loss (0.006), a saturated hysteresis loop, a giant piezoelectric coefficient d(33) (d(33) = 416 pC/N, determined by the resonance method and d(33)(*) = 480 pC/N, measured using a piezo-d(33) meter), and a large electromechanical coupling factor, k(33) (k(33) = 83.6%), which was comparable to that of lead zirconate titanate. The reason the piezoelectric coefficient d(33) of K(0.39)Na(0.61)Ta(0.42)Nb(0.58)O(3) was larger than those of the other two crystals grown was elucidated through first-principles calculations. The obtained results indicated that K(1−x)Na(x)Ta(1−y)Nb(y)O(3) crystals can be used as a high-quality, lead-free piezoelectric material. |
format | Online Article Text |
id | pubmed-4861918 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-48619182016-05-20 Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals Tian, Hao Meng, Xiangda Hu, Chengpeng Tan, Peng Cao, Xilong Shi, Guang Zhou, Zhongxiang Zhang, Rui Sci Rep Article A series of high-quality, large-sized (maximum size of 16 × 16 × 32 mm(3)) K(1−x)Na(x)Ta(1−y)Nb(y)O(3) (x = 0.61, 0.64, and 0.70 and corresponding y = 0.58, 0.60, and 0.63) single crystals were grown using the top-seed solution growth method. The segregation of the crystals, which allowed for precise control of the individual components of the crystals during growth, was investigated. The obtained crystals exhibited excellent properties without being annealed, including a low dielectric loss (0.006), a saturated hysteresis loop, a giant piezoelectric coefficient d(33) (d(33) = 416 pC/N, determined by the resonance method and d(33)(*) = 480 pC/N, measured using a piezo-d(33) meter), and a large electromechanical coupling factor, k(33) (k(33) = 83.6%), which was comparable to that of lead zirconate titanate. The reason the piezoelectric coefficient d(33) of K(0.39)Na(0.61)Ta(0.42)Nb(0.58)O(3) was larger than those of the other two crystals grown was elucidated through first-principles calculations. The obtained results indicated that K(1−x)Na(x)Ta(1−y)Nb(y)O(3) crystals can be used as a high-quality, lead-free piezoelectric material. Nature Publishing Group 2016-05-10 /pmc/articles/PMC4861918/ /pubmed/27160075 http://dx.doi.org/10.1038/srep25637 Text en Copyright © 2016, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Tian, Hao Meng, Xiangda Hu, Chengpeng Tan, Peng Cao, Xilong Shi, Guang Zhou, Zhongxiang Zhang, Rui Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title | Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title_full | Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title_fullStr | Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title_full_unstemmed | Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title_short | Origin of giant piezoelectric effect in lead-free K(1−x)Na(x)Ta(1−y)Nb(y)O(3) single crystals |
title_sort | origin of giant piezoelectric effect in lead-free k(1−x)na(x)ta(1−y)nb(y)o(3) single crystals |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4861918/ https://www.ncbi.nlm.nih.gov/pubmed/27160075 http://dx.doi.org/10.1038/srep25637 |
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