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Broadband inelastic light scattering study on relaxor ferroelectric Pb(In1/2Nb1/2)-Pb(Mg1/3Nb2/3)O3-PbTiO3 single crystals
Author(s) -
Tae Hyun Kim,
Seiji Kojima,
JaeHyeon Ko
Publication year - 2014
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 - 10.1063/1.4878855
Subject(s) - materials science , raman spectroscopy , poling , tetragonal crystal system , raman scattering , condensed matter physics , phase transition , ferroelectricity , x ray raman scattering , phase (matter) , optics , crystallography , crystal structure , dielectric , chemistry , optoelectronics , physics , organic chemistry
The broadband inelastic light scattering spectra of ternary Pb(In1/2 Nb 1/2)-Pb(Mg1/3 Nb 2/3)O3-PbTiO3 single crystals were investigated as a function of temperature and crystal orientation by combining Raman and Brillouin spectroscopies. The angular dependence of the strong Raman peak located at ∼50 cm−1 was investigated at 300 °C. The intensity variation of this mode with rotation angle was compatible with the mode of symmetry, suggesting that this mode arises from the 1:1 chemical order at the B-site in this perovskite structure. The temperature evolution of the polar nanoregions was associated with the growth of two central peaks and the change in the intensity of some Raman peaks, which were known to be sensitive to the rhombohedral symmetry. Both relaxation processes exhibited partial slowing-down behaviors with a common critical temperature of ∼160 °C. Poling the crystal along the [001] direction induced abrupt changes in some of the Raman bands at the rhombohedral–tetragonal phase transition. On the other hand, the diffuse tetragonal–cubic phase transition was not affected by the poling process. This high-temperature phase transformation seems to be smeared out by the inherent disorder and strong random fields enhanced by the addition of Pb(In1/2 Nb 1/2) into Pb(Mg1/3 Nb 2/3)O3-PbTiO3.F2gFm3¯

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