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Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics
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| Zeitschriftentitel: | Journal of the American Ceramic Society |
|---|---|
| Personen und Körperschaften: | , , , , |
| In: | Journal of the American Ceramic Society, 101, 2018, 1, S. 274-282 |
| Format: | E-Article |
| Sprache: | Englisch |
| veröffentlicht: |
Wiley
|
| Schlagwörter: |
| author_facet |
Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong |
|---|---|
| author |
Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong |
| spellingShingle |
Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong Journal of the American Ceramic Society Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics Materials Chemistry Ceramics and Composites |
| author_sort |
huang, xiang |
| spelling |
Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong 0002-7820 1551-2916 Wiley Materials Chemistry Ceramics and Composites http://dx.doi.org/10.1111/jace.15179 <jats:title>Abstract</jats:title><jats:p><jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>P</jats:styled-content>b(Zn<jats:sub>0.5</jats:sub>Te<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub>–(1−<jats:italic>x</jats:italic>)Pb(Zr<jats:sub>0.5</jats:sub>Ti<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub> (<jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content>) ceramics were prepared by the solid‐state reaction method. The phase structure, microstructure, ferroelectric and dielectric properties and thermal expansion properties were systematically investigated. X‐ray diffraction analysis showed the morphotropic phase boundary (<jats:styled-content style="fixed-case">MPB</jats:styled-content>) existed at the composition of <jats:italic>x</jats:italic> = 0.08, which was the coexistence of the rhombohedral phase and the tetragonal phase. The grain size of ceramics decreased rapidly from 10‐20 μm to 1‐3 μm when the <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe was added in. The <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics at the <jats:styled-content style="fixed-case">MPB</jats:styled-content> composition showed the largest high field effective piezoelectric coefficient <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/jace15179-math-0001.png" xlink:title="urn:x-wiley:00027820:media:jace15179:jace15179-math-0001" /> and the lowest strain hysteresis <jats:italic>H</jats:italic>. The dielectric permittivity and phase transition temperature exhibited strongly compositional dependence. A good linear relation was shown in <jats:italic>T</jats:italic><jats:sub>m</jats:sub> temperature vs <jats:italic>x</jats:italic> content and a <jats:styled-content style="fixed-case">DPT</jats:styled-content> behavior was found in <jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>PZnT</jats:styled-content>e–(1−<jats:italic>x</jats:italic>)<jats:styled-content style="fixed-case">PZT</jats:styled-content> (<jats:italic>x</jats:italic> = 0.02‐0.08). The thermal expansion properties showed a low thermal expansion coefficient in the low temperature while a high thermal expansion coefficient in the high temperature. Besides, the thermal expansion curve also showed the characteristic of <jats:styled-content style="fixed-case">DPT</jats:styled-content> in <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics.</jats:p> Structure, electrical, and thermal expansion properties of <scp>PZ</scp>nTe–<scp>PZT</scp> ternary system piezoelectric ceramics Journal of the American Ceramic Society |
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10.1111/jace.15179 |
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Online |
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Chemie und Pharmazie Technik |
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ElectronicArticle |
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DE-Pl11 DE-Rs1 DE-105 DE-14 DE-Ch1 DE-L229 DE-D275 DE-Bn3 DE-Brt1 DE-D161 DE-Gla1 DE-Zi4 DE-15 |
| imprint |
Wiley, 2018 |
| imprint_str_mv |
Wiley, 2018 |
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1551-2916 0002-7820 |
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1551-2916 0002-7820 |
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huang2018structureelectricalandthermalexpansionpropertiesofpzntepztternarysystempiezoelectricceramics |
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2018 |
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Wiley |
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Journal of the American Ceramic Society |
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49 |
| title |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_unstemmed |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_full |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_fullStr |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_full_unstemmed |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_short |
Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_sort |
structure, electrical, and thermal expansion properties of <scp>pz</scp>nte–<scp>pzt</scp> ternary system piezoelectric ceramics |
| topic |
Materials Chemistry Ceramics and Composites |
| url |
http://dx.doi.org/10.1111/jace.15179 |
| publishDate |
2018 |
| physical |
274-282 |
| description |
<jats:title>Abstract</jats:title><jats:p><jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>P</jats:styled-content>b(Zn<jats:sub>0.5</jats:sub>Te<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub>–(1−<jats:italic>x</jats:italic>)Pb(Zr<jats:sub>0.5</jats:sub>Ti<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub> (<jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content>) ceramics were prepared by the solid‐state reaction method. The phase structure, microstructure, ferroelectric and dielectric properties and thermal expansion properties were systematically investigated. X‐ray diffraction analysis showed the morphotropic phase boundary (<jats:styled-content style="fixed-case">MPB</jats:styled-content>) existed at the composition of <jats:italic>x</jats:italic> = 0.08, which was the coexistence of the rhombohedral phase and the tetragonal phase. The grain size of ceramics decreased rapidly from 10‐20 μm to 1‐3 μm when the <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe was added in. The <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics at the <jats:styled-content style="fixed-case">MPB</jats:styled-content> composition showed the largest high field effective piezoelectric coefficient <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/jace15179-math-0001.png" xlink:title="urn:x-wiley:00027820:media:jace15179:jace15179-math-0001" /> and the lowest strain hysteresis <jats:italic>H</jats:italic>. The dielectric permittivity and phase transition temperature exhibited strongly compositional dependence. A good linear relation was shown in <jats:italic>T</jats:italic><jats:sub>m</jats:sub> temperature vs <jats:italic>x</jats:italic> content and a <jats:styled-content style="fixed-case">DPT</jats:styled-content> behavior was found in <jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>PZnT</jats:styled-content>e–(1−<jats:italic>x</jats:italic>)<jats:styled-content style="fixed-case">PZT</jats:styled-content> (<jats:italic>x</jats:italic> = 0.02‐0.08). The thermal expansion properties showed a low thermal expansion coefficient in the low temperature while a high thermal expansion coefficient in the high temperature. Besides, the thermal expansion curve also showed the characteristic of <jats:styled-content style="fixed-case">DPT</jats:styled-content> in <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics.</jats:p> |
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| author | Huang, Xiang, Zeng, Jiangtao, Ruan, Xuezheng, Zheng, Liaoying, Li, Guorong |
| author_facet | Huang, Xiang, Zeng, Jiangtao, Ruan, Xuezheng, Zheng, Liaoying, Li, Guorong, Huang, Xiang, Zeng, Jiangtao, Ruan, Xuezheng, Zheng, Liaoying, Li, Guorong |
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| description | <jats:title>Abstract</jats:title><jats:p><jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>P</jats:styled-content>b(Zn<jats:sub>0.5</jats:sub>Te<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub>–(1−<jats:italic>x</jats:italic>)Pb(Zr<jats:sub>0.5</jats:sub>Ti<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub> (<jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content>) ceramics were prepared by the solid‐state reaction method. The phase structure, microstructure, ferroelectric and dielectric properties and thermal expansion properties were systematically investigated. X‐ray diffraction analysis showed the morphotropic phase boundary (<jats:styled-content style="fixed-case">MPB</jats:styled-content>) existed at the composition of <jats:italic>x</jats:italic> = 0.08, which was the coexistence of the rhombohedral phase and the tetragonal phase. The grain size of ceramics decreased rapidly from 10‐20 μm to 1‐3 μm when the <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe was added in. The <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics at the <jats:styled-content style="fixed-case">MPB</jats:styled-content> composition showed the largest high field effective piezoelectric coefficient <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/jace15179-math-0001.png" xlink:title="urn:x-wiley:00027820:media:jace15179:jace15179-math-0001" /> and the lowest strain hysteresis <jats:italic>H</jats:italic>. The dielectric permittivity and phase transition temperature exhibited strongly compositional dependence. A good linear relation was shown in <jats:italic>T</jats:italic><jats:sub>m</jats:sub> temperature vs <jats:italic>x</jats:italic> content and a <jats:styled-content style="fixed-case">DPT</jats:styled-content> behavior was found in <jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>PZnT</jats:styled-content>e–(1−<jats:italic>x</jats:italic>)<jats:styled-content style="fixed-case">PZT</jats:styled-content> (<jats:italic>x</jats:italic> = 0.02‐0.08). The thermal expansion properties showed a low thermal expansion coefficient in the low temperature while a high thermal expansion coefficient in the high temperature. Besides, the thermal expansion curve also showed the characteristic of <jats:styled-content style="fixed-case">DPT</jats:styled-content> in <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics.</jats:p> |
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| spelling | Huang, Xiang Zeng, Jiangtao Ruan, Xuezheng Zheng, Liaoying Li, Guorong 0002-7820 1551-2916 Wiley Materials Chemistry Ceramics and Composites http://dx.doi.org/10.1111/jace.15179 <jats:title>Abstract</jats:title><jats:p><jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>P</jats:styled-content>b(Zn<jats:sub>0.5</jats:sub>Te<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub>–(1−<jats:italic>x</jats:italic>)Pb(Zr<jats:sub>0.5</jats:sub>Ti<jats:sub>0.5</jats:sub>)O<jats:sub>3</jats:sub> (<jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content>) ceramics were prepared by the solid‐state reaction method. The phase structure, microstructure, ferroelectric and dielectric properties and thermal expansion properties were systematically investigated. X‐ray diffraction analysis showed the morphotropic phase boundary (<jats:styled-content style="fixed-case">MPB</jats:styled-content>) existed at the composition of <jats:italic>x</jats:italic> = 0.08, which was the coexistence of the rhombohedral phase and the tetragonal phase. The grain size of ceramics decreased rapidly from 10‐20 μm to 1‐3 μm when the <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe was added in. The <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics at the <jats:styled-content style="fixed-case">MPB</jats:styled-content> composition showed the largest high field effective piezoelectric coefficient <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/jace15179-math-0001.png" xlink:title="urn:x-wiley:00027820:media:jace15179:jace15179-math-0001" /> and the lowest strain hysteresis <jats:italic>H</jats:italic>. The dielectric permittivity and phase transition temperature exhibited strongly compositional dependence. A good linear relation was shown in <jats:italic>T</jats:italic><jats:sub>m</jats:sub> temperature vs <jats:italic>x</jats:italic> content and a <jats:styled-content style="fixed-case">DPT</jats:styled-content> behavior was found in <jats:styled-content style="fixed-case"><jats:italic>x</jats:italic>PZnT</jats:styled-content>e–(1−<jats:italic>x</jats:italic>)<jats:styled-content style="fixed-case">PZT</jats:styled-content> (<jats:italic>x</jats:italic> = 0.02‐0.08). The thermal expansion properties showed a low thermal expansion coefficient in the low temperature while a high thermal expansion coefficient in the high temperature. Besides, the thermal expansion curve also showed the characteristic of <jats:styled-content style="fixed-case">DPT</jats:styled-content> in <jats:styled-content style="fixed-case">PZ</jats:styled-content>nTe–<jats:styled-content style="fixed-case">PZT</jats:styled-content> ceramics.</jats:p> Structure, electrical, and thermal expansion properties of <scp>PZ</scp>nTe–<scp>PZT</scp> ternary system piezoelectric ceramics Journal of the American Ceramic Society |
| spellingShingle | Huang, Xiang, Zeng, Jiangtao, Ruan, Xuezheng, Zheng, Liaoying, Li, Guorong, Journal of the American Ceramic Society, Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics, Materials Chemistry, Ceramics and Composites |
| title | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_full | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_fullStr | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_full_unstemmed | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_short | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| title_sort | structure, electrical, and thermal expansion properties of <scp>pz</scp>nte–<scp>pzt</scp> ternary system piezoelectric ceramics |
| title_unstemmed | Structure, electrical, and thermal expansion properties of PZnTe–PZT ternary system piezoelectric ceramics |
| topic | Materials Chemistry, Ceramics and Composites |
| url | http://dx.doi.org/10.1111/jace.15179 |