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Kinetics of electric-field-induced ferroelectric phase transitions in relaxor ferroelectrics - art. no. 024111

机译:弛豫铁电体中电场感应铁电相变的动力学-艺术。没有。 024111

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摘要

The kinetics of electric-field-induced ferroelectric phase transitions in relaxor ferroelectrics observed recently [S. B. Vakhrushev, J. M. Kiat, and B. Dkhil, Solid State Commun. 103, 477 (1997): B. Dkhil and J. M. Kiat, J. Appl. Phys. 90, 4676 (2001)] is analyzed in the framework of a dynamical model of relaxors which incorporates features of nonequilibrium glassy dynamics resembling that in dipole glasses, with the high polarizabity of the system being in the vicinity of the ferroelectric threshold. We show that the dynamical equations may be reduced to a Landau-type phenomenological polynomial in which the linear coefficient-zero-field-cooled permittivity-is a function of time. The theory adequately reproduces the features of electric-field induced polarization growth observed in the experiment. [References: 22]
机译:最近观察到的弛豫铁电中电场引起的铁电相变的动力学[S. B. Vakhrushev,J。M. Kiat和B. Dkhil,固态社区。 103、477(1997):B。Dkhil和J.M. Kiat,J。Appl。物理90,4676(2001)]是在弛豫器动力学模型的框架内进行分析的,该模型具有类似于偶极玻璃的非平衡玻璃态动力学特征,系统的高极化率在铁电阈值附近。我们表明,动力学方程可以简化为Landau型现象学多项式,其中线性系数零场冷却介电常数是时间的函数。该理论充分再现了实验中观察到的电场感应极化增长的特征。 [参考:22]

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