TY - JOUR
T1 - Features of the ferroelectric tetragonal state in the simple-perovskite mixed-oxide system (1-x)Pb(Sc1/2Nb1/2)O3-xPbTiO3
AU - Tsukasaki, Hirofumi
AU - Tateishi, Atsuhiro
AU - Koyama, Yasumasa
N1 - Publisher Copyright:
© 2018 The Ceramic Society of Japan. All rights reserved.
PY - 2018/3
Y1 - 2018/3
N2 - The crystallographic features of the ferroelectric tetragonal (FT) state in (1 - x)Pb(Sc1/2Nb1/2)O3-xPbTiO3 (PSN-xPT) were investigated between 300 and 700 K, primarily using transmission electron microscopy (TEM) with the help of the failure of Friedel's law in electron diffraction. The ferroelectric state for 0.60 ≤ × ≤ 1.0, which has been recognized as the normal FT state thus far, was found to have MC-type monoclinic symmetry with (201)C polarization vectors in the {100}C planes. Notably, the ferroelectric MC state (FMC) was characterized by pseudo 90 and 180° domain structures, in which the polarization rotates slightly from the (001)C direction of the FT state. In addition, in situ TEM observation during heating and permittivity measurement revealed that the (FMC → FT) transition occurred at below TC for 0.60 ≤ × < 1.0. The FT/FMC phase boundary, which is nearly perpendicular to the temperature axis, was therefore present at approximately 560 K.
AB - The crystallographic features of the ferroelectric tetragonal (FT) state in (1 - x)Pb(Sc1/2Nb1/2)O3-xPbTiO3 (PSN-xPT) were investigated between 300 and 700 K, primarily using transmission electron microscopy (TEM) with the help of the failure of Friedel's law in electron diffraction. The ferroelectric state for 0.60 ≤ × ≤ 1.0, which has been recognized as the normal FT state thus far, was found to have MC-type monoclinic symmetry with (201)C polarization vectors in the {100}C planes. Notably, the ferroelectric MC state (FMC) was characterized by pseudo 90 and 180° domain structures, in which the polarization rotates slightly from the (001)C direction of the FT state. In addition, in situ TEM observation during heating and permittivity measurement revealed that the (FMC → FT) transition occurred at below TC for 0.60 ≤ × < 1.0. The FT/FMC phase boundary, which is nearly perpendicular to the temperature axis, was therefore present at approximately 560 K.
KW - Domain structure
KW - Ferroelectrics
KW - Phase transition
KW - Transmission electron microscopy
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U2 - 10.2109/jcersj2.17241
DO - 10.2109/jcersj2.17241
M3 - Article
AN - SCOPUS:85042712408
SN - 1882-0743
VL - 126
SP - 170
EP - 177
JO - Nippon Seramikkusu Kyokai Gakujutsu Ronbunshi/Journal of the Ceramic Society of Japan
JF - Nippon Seramikkusu Kyokai Gakujutsu Ronbunshi/Journal of the Ceramic Society of Japan
IS - 3
ER -