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Intermediate phases in rhombohedral Pb(Mg1∕3Nb2∕3)1−xTixO3 crystal
Author(s) -
ChiShun Tu,
Hsiu-Mei Chuang,
S.-C. Lee,
R. R. Chien,
V. Hugo Schmidt,
Hui Luo
Publication year - 2008
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.2956611
Subject(s) - poling , tetragonal crystal system , dielectric , curie temperature , materials science , condensed matter physics , monoclinic crystal system , permittivity , polarization (electrochemistry) , phase transition , electric field , ferroelectricity , crystallography , crystal structure , chemistry , physics , ferromagnetism , optoelectronics , quantum mechanics
Phase transformations of (111)-cut Pb(Mg1∕3Nb2∕3)1−xTixO3 (x=0.30) single crystals before and after an electric (E)–field poling have been investigated by means of dielectric permittivity, hysteresis loop, polarization current, and in situ x-ray diffraction as a function of temperature. An R-T-C transition sequence was observed in the unpoled sample upon zero-field heating. R, T, and C are rhombohedral, tetragonal, and cubic phases, respectively. After a prior E-field poling, an extra intermediate monoclinic (possible MA) phase was induced and the crystal underwent an R-MA-T-C phase sequence with significant responses in polarization current. The dielectric dispersion was diminished after poling and reappeared in the cubic state. The dielectric permittivities with and without a prior poling were found to follow the Curie–Weiss equation, e′=C∕(T−T0), above the Burns temperature 505K with the same constants C=1.9×105 K and T0=460K.

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