Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics
| Autor(a) principal: | |
|---|---|
| Data de Publicação: | 2013 |
| Outros Autores: | , , , |
| Tipo de documento: | Artigo |
| Idioma: | eng |
| Título da fonte: | Repositórios Científicos de Acesso Aberto de Portugal (RCAAP) |
| Texto Completo: | http://hdl.handle.net/10773/19776 |
Resumo: | Lead-free tetragonal tungsten bronze Sr5LaTi3Nb7O30 ceramics were prepared and the correlation of the relaxor nature and crystal structure was studied using dielectric spectroscopy and powder X-ray diffraction. Three dielectric relaxations were observed below the deviation temperature T-D similar to 330 K. Relaxation I and II followed the Vogel-Fulcher law with the freezing temperatures of 189 K and similar to 90 K. Low temperature relaxation III, which was first observed in filled tungsten bronze, followed well the Arrhenius law. Dielectric response becomes static below 50 K. Polarization-field (P-E) hysteresis loops were evaluated from 183 K to 298 K. P-r value of 0.41 mu C/cm(2) was observed at 183 K. Deviation of lattice parameter c from the linear contraction and increasing of tetragonality (c/a ratio) were observed below T-D, reflecting the structure change during the formation of polar nanoregions and the following freezing process. Opposite tendency was observed below 100 K for all the lattice parameters, corresponding to relaxation III. Generally, the main dielectric relaxation I and II were attributed to flipping and breathing of polar nanoregions along c axis, while the concerted rotations of the oxygen octahedra in the ab plane were suggested as the origin of relaxation III. (C) 2013 AIP Publishing LLC. |
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Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramicsPHASE-TRANSITIONSINGLE-CRYSTALSFERROELECTRIC PROPERTIESBEHAVIORLead-free tetragonal tungsten bronze Sr5LaTi3Nb7O30 ceramics were prepared and the correlation of the relaxor nature and crystal structure was studied using dielectric spectroscopy and powder X-ray diffraction. Three dielectric relaxations were observed below the deviation temperature T-D similar to 330 K. Relaxation I and II followed the Vogel-Fulcher law with the freezing temperatures of 189 K and similar to 90 K. Low temperature relaxation III, which was first observed in filled tungsten bronze, followed well the Arrhenius law. Dielectric response becomes static below 50 K. Polarization-field (P-E) hysteresis loops were evaluated from 183 K to 298 K. P-r value of 0.41 mu C/cm(2) was observed at 183 K. Deviation of lattice parameter c from the linear contraction and increasing of tetragonality (c/a ratio) were observed below T-D, reflecting the structure change during the formation of polar nanoregions and the following freezing process. Opposite tendency was observed below 100 K for all the lattice parameters, corresponding to relaxation III. Generally, the main dielectric relaxation I and II were attributed to flipping and breathing of polar nanoregions along c axis, while the concerted rotations of the oxygen octahedra in the ab plane were suggested as the origin of relaxation III. (C) 2013 AIP Publishing LLC.AMER INST PHYSICS2017-12-07T19:24:27Z2013-01-01T00:00:00Z2013info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleapplication/pdfhttp://hdl.handle.net/10773/19776eng0021-897910.1063/1.4822025Zhu, Xiao LiLi, KunRafiq, Muhammad AsifLiu, Xiao QiangChen, Xiang Minginfo:eu-repo/semantics/openAccessreponame:Repositórios Científicos de Acesso Aberto de Portugal (RCAAP)instname:FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiainstacron:RCAAP2024-05-06T04:07:11Zoai:ria.ua.pt:10773/19776Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireinfo@rcaap.ptopendoar:https://opendoar.ac.uk/repository/71602025-05-28T13:57:46.642571Repositórios Científicos de Acesso Aberto de Portugal (RCAAP) - FCCN, serviços digitais da FCT – Fundação para a Ciência e a Tecnologiafalse |
| dc.title.none.fl_str_mv |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| title |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| spellingShingle |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics Zhu, Xiao Li PHASE-TRANSITION SINGLE-CRYSTALS FERROELECTRIC PROPERTIES BEHAVIOR |
| title_short |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| title_full |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| title_fullStr |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| title_full_unstemmed |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| title_sort |
Relaxor nature in lead-free Sr5LaTi3Nb7O30 tetragonal tungsten bronze ceramics |
| author |
Zhu, Xiao Li |
| author_facet |
Zhu, Xiao Li Li, Kun Rafiq, Muhammad Asif Liu, Xiao Qiang Chen, Xiang Ming |
| author_role |
author |
| author2 |
Li, Kun Rafiq, Muhammad Asif Liu, Xiao Qiang Chen, Xiang Ming |
| author2_role |
author author author author |
| dc.contributor.author.fl_str_mv |
Zhu, Xiao Li Li, Kun Rafiq, Muhammad Asif Liu, Xiao Qiang Chen, Xiang Ming |
| dc.subject.por.fl_str_mv |
PHASE-TRANSITION SINGLE-CRYSTALS FERROELECTRIC PROPERTIES BEHAVIOR |
| topic |
PHASE-TRANSITION SINGLE-CRYSTALS FERROELECTRIC PROPERTIES BEHAVIOR |
| description |
Lead-free tetragonal tungsten bronze Sr5LaTi3Nb7O30 ceramics were prepared and the correlation of the relaxor nature and crystal structure was studied using dielectric spectroscopy and powder X-ray diffraction. Three dielectric relaxations were observed below the deviation temperature T-D similar to 330 K. Relaxation I and II followed the Vogel-Fulcher law with the freezing temperatures of 189 K and similar to 90 K. Low temperature relaxation III, which was first observed in filled tungsten bronze, followed well the Arrhenius law. Dielectric response becomes static below 50 K. Polarization-field (P-E) hysteresis loops were evaluated from 183 K to 298 K. P-r value of 0.41 mu C/cm(2) was observed at 183 K. Deviation of lattice parameter c from the linear contraction and increasing of tetragonality (c/a ratio) were observed below T-D, reflecting the structure change during the formation of polar nanoregions and the following freezing process. Opposite tendency was observed below 100 K for all the lattice parameters, corresponding to relaxation III. Generally, the main dielectric relaxation I and II were attributed to flipping and breathing of polar nanoregions along c axis, while the concerted rotations of the oxygen octahedra in the ab plane were suggested as the origin of relaxation III. (C) 2013 AIP Publishing LLC. |
| publishDate |
2013 |
| dc.date.none.fl_str_mv |
2013-01-01T00:00:00Z 2013 2017-12-07T19:24:27Z |
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info:eu-repo/semantics/publishedVersion |
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info:eu-repo/semantics/article |
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article |
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publishedVersion |
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http://hdl.handle.net/10773/19776 |
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http://hdl.handle.net/10773/19776 |
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eng |
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eng |
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0021-8979 10.1063/1.4822025 |
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info:eu-repo/semantics/openAccess |
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openAccess |
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application/pdf |
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AMER INST PHYSICS |
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AMER INST PHYSICS |
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