TY - JOUR
T1 - Ferroelectric domain structures near the MPB in (1-x)Pb(Zn 1/3Nb2/3)O3-xPbTiO3
AU - Asada, T.
AU - Shibata, T.
AU - Koyama, Y.
N1 - Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2007
Y1 - 2007
N2 - In (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 (PZN-xPT), there exists the morphotropic phase boundary (MPB) as an almost temperature-independent boundary around x = 0.10. In order to understand an origin of the excellent piezoelectric response found near the MPB in PZN-xPT, the features of ferroelectric domain structures in the tetragonal side of the MPB have been examined mainly by transmission electron microscopy. The ferroelectric domain structure in x = 0.12 specimens prepared from single crystals as bulk samples was found to be the superposition of the tetragonal domain structure with the [001] polarization and the curved-boundary regions with the [100] or [010] one. On the other hand, the cooling from the paraelectric phase in thin specimens used for transmission-electron-microscopy observation resulted in two types of ferroelectric domain structures. One was the fine {110} banded structure in the fast cooling rate and the other was the maze-pattern structure in the slow rate. These two structures usually coexisted and the volume fraction between them was cooling-rate dependent. In order to understand these curious features, we proposed the domain-structure model based on the aggregation consisting of nano-scale ferroelectric domains.
AB - In (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 (PZN-xPT), there exists the morphotropic phase boundary (MPB) as an almost temperature-independent boundary around x = 0.10. In order to understand an origin of the excellent piezoelectric response found near the MPB in PZN-xPT, the features of ferroelectric domain structures in the tetragonal side of the MPB have been examined mainly by transmission electron microscopy. The ferroelectric domain structure in x = 0.12 specimens prepared from single crystals as bulk samples was found to be the superposition of the tetragonal domain structure with the [001] polarization and the curved-boundary regions with the [100] or [010] one. On the other hand, the cooling from the paraelectric phase in thin specimens used for transmission-electron-microscopy observation resulted in two types of ferroelectric domain structures. One was the fine {110} banded structure in the fast cooling rate and the other was the maze-pattern structure in the slow rate. These two structures usually coexisted and the volume fraction between them was cooling-rate dependent. In order to understand these curious features, we proposed the domain-structure model based on the aggregation consisting of nano-scale ferroelectric domains.
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U2 - 10.1080/00150190601186890
DO - 10.1080/00150190601186890
M3 - Conference article
AN - SCOPUS:34547251715
SN - 0015-0193
VL - 347
SP - 17
EP - 24
JO - Ferroelectrics
JF - Ferroelectrics
T2 - 8th Russia/CIS/Baltic/Japan Symposium on Ferroelectricity, RCBJSF-8
Y2 - 15 May 2006 through 19 May 2006
ER -