Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam

(1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 ((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this work, we extensively investigated (1-x)PZN-xPT (x = 0.07–0.11) ferroelectric single crystals using in-situ synchrotron μXRD, complemented by TEM and PFM, to correlate microstructures w...

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Main Authors: Li, Tao, Du, Zehui, Tamura, Nobumichi, Ye, Mao, Inguva, Saikumar, Lu, Wei, Zeng, Xierong, Ke, Shanming, Huang, Haitao
Other Authors: Temasek Laboratories
Format: Article
Language:English
Published: 2020
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Online Access:https://hdl.handle.net/10356/139727
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Institution: Nanyang Technological University
Language: English
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spelling sg-ntu-dr.10356-1397272020-05-21T05:33:04Z Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam Li, Tao Du, Zehui Tamura, Nobumichi Ye, Mao Inguva, Saikumar Lu, Wei Zeng, Xierong Ke, Shanming Huang, Haitao Temasek Laboratories Science::Physics Ferroelastic Domain Phase Transition (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 ((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this work, we extensively investigated (1-x)PZN-xPT (x = 0.07–0.11) ferroelectric single crystals using in-situ synchrotron μXRD, complemented by TEM and PFM, to correlate microstructures with phase transitions. The results reveal that (i) at 25 °C, the equilibrium state of (1-x)PZN-xPT is a metastable orthorhombic phase for x = 0.07 and 0.08, while it shows coexistence of orthorhombic and tetragonal phases for x = 0.09 and x = 0.11, with all ferroelectric phases accompanied by ferroelastic domains; (ii) upon heating, the phase transformation in x = 0.07 is Orthorhombic → Monoclinic → Tetragonal → Cubic. The coexistence of ferroelectric tetragonal and paraelectric cubic phases was in-situ observed in x = 0.08 above Curie temperature (TC), and (iii) phase transition can be explained by the evolution of the ferroelectric and ferroelastic domains. These results disclose that (1-x)PZN-xPT are in an unstable regime, which is possible factor for its anomalous dielectric response and high piezoelectric coefficient. 2020-05-21T05:33:04Z 2020-05-21T05:33:04Z 2017 Journal Article Li, T., Du, Z., Tamura, N., Ye, M., Inguva, S., Lu, W., . . . Huang, H. (2018). Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ X-ray microbeam. Journal of the European Ceramic Society, 38(4), 1488-1497. doi:10.1016/j.jeurceramsoc.2017.11.021 0955-2219 https://hdl.handle.net/10356/139727 10.1016/j.jeurceramsoc.2017.11.021 2-s2.0-85034826602 4 38 1488 1497 en Journal of the European Ceramic Society © 2017 Elsevier Ltd. All rights reserved.
institution Nanyang Technological University
building NTU Library
country Singapore
collection DR-NTU
language English
topic Science::Physics
Ferroelastic Domain
Phase Transition
spellingShingle Science::Physics
Ferroelastic Domain
Phase Transition
Li, Tao
Du, Zehui
Tamura, Nobumichi
Ye, Mao
Inguva, Saikumar
Lu, Wei
Zeng, Xierong
Ke, Shanming
Huang, Haitao
Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
description (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 ((1-x)PZN-xPT in short) is one of the most important piezoelectric materials. In this work, we extensively investigated (1-x)PZN-xPT (x = 0.07–0.11) ferroelectric single crystals using in-situ synchrotron μXRD, complemented by TEM and PFM, to correlate microstructures with phase transitions. The results reveal that (i) at 25 °C, the equilibrium state of (1-x)PZN-xPT is a metastable orthorhombic phase for x = 0.07 and 0.08, while it shows coexistence of orthorhombic and tetragonal phases for x = 0.09 and x = 0.11, with all ferroelectric phases accompanied by ferroelastic domains; (ii) upon heating, the phase transformation in x = 0.07 is Orthorhombic → Monoclinic → Tetragonal → Cubic. The coexistence of ferroelectric tetragonal and paraelectric cubic phases was in-situ observed in x = 0.08 above Curie temperature (TC), and (iii) phase transition can be explained by the evolution of the ferroelectric and ferroelastic domains. These results disclose that (1-x)PZN-xPT are in an unstable regime, which is possible factor for its anomalous dielectric response and high piezoelectric coefficient.
author2 Temasek Laboratories
author_facet Temasek Laboratories
Li, Tao
Du, Zehui
Tamura, Nobumichi
Ye, Mao
Inguva, Saikumar
Lu, Wei
Zeng, Xierong
Ke, Shanming
Huang, Haitao
format Article
author Li, Tao
Du, Zehui
Tamura, Nobumichi
Ye, Mao
Inguva, Saikumar
Lu, Wei
Zeng, Xierong
Ke, Shanming
Huang, Haitao
author_sort Li, Tao
title Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
title_short Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
title_full Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
title_fullStr Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
title_full_unstemmed Ferroelastic domain structure and phase transition in single-crystalline [PbZn1/3Nb2/3O3]1-x[PbTiO3]x observed via in situ x-ray microbeam
title_sort ferroelastic domain structure and phase transition in single-crystalline [pbzn1/3nb2/3o3]1-x[pbtio3]x observed via in situ x-ray microbeam
publishDate 2020
url https://hdl.handle.net/10356/139727
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