Bias-field effect on the temperature anomalies of dielectric permittivity in PbMg1/3Nb2/3O3-PbTiO3 single crystals -: art. no. 184104

被引:72
作者
Raevski, IP [1 ]
Prosandeev, SA
Emelyanov, AS
Raevskaya, SI
Colla, EV
Viehland, D
Kleemann, W
Vakhrushev, SB
Dellis, JL
El Marssi, M
Jastrabik, L
机构
[1] Rostov State Univ, Inst Phys Res, Rostov Na Donu 344090, Russia
[2] Univ Illinois, Dept Phys, Urbana, IL 61801 USA
[3] Virginia Tech, Dept Mat Sci & Engn, Blacksburg, VA 24061 USA
[4] Univ Duisburg Gesamthsch, D-47048 Duisburg, Germany
[5] AF Ioffe Phys Tech Inst, St Petersburg 194021, Russia
[6] Univ Picardie, Phys Mat Condensee Lab, F-80039 Amiens, France
[7] AS CR, Inst Phys, Prague 18221, Czech Republic
关键词
D O I
10.1103/PhysRevB.72.184104
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In contrast to ordinary ferroelectrics where the temperature T-m of the permittivity maximum monotonically increases with bias field E in (1-x)PbMg1/3Nb2/3O3-(x)PbTiO3 (0 <= x <= 0.35) single crystals, T-m was found to remain constant or to decrease with E up to a certain threshold field E-t, above which T-m starts increasing. The threshold field E-t decreases with increasing x, tending toward zero at approximately x=0.4. We explain this dependence in the framework of models which take into account quenched random fields and random bonds. For crystals with 0.06 <= x <= 0.13, the E-T phase diagrams are constructed. In contrast to PMN, they exhibit an additional, nearly field-independent boundary, in the vicinity of the Vogel-Fulcher temperature. We believe this boundary to correspond to an additional phase transition and the appearing order parameter is likely to be nonpolar.
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