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Dielectric relaxation and polar phonon softening in relaxor ferroelectric PbMg_(1/3)Ta_(2/3)O_3

机译:弛豫中的介电弛豫和极化声子软化   铁电pbmg_(1/3)Ta_(2/3)O_3

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摘要

Relaxor ferroelectric PbMg_1/3Ta_2/3O_3 ceramics and thin films wereinvestigated by means of broad-band dielectric, time-domain terahertz (THz) andFourier-transform infrared (IR) spectroscopy in the frequency range 100 Hz - 90THz at temperatures 100 - 490 K, the THz and IR spectra were studied from 20 to900K. Diffused and strongly temperature dependent peak in the complexpermittivity is caused by a dielectric relaxation due to the dynamics of polarclusters. The relaxation appears below Burns temperature T_d in the THz range,slows down on cooling through the microwave and MHz range and anomalouslybroadens. The shortest and longest relaxation times of the distribution ofrelaxation times follow Arrhenius and Vogel-Fulcher law, respectively. Thedegree of B-site order has only a small influence on the parameters of thedielectric relaxation and almost no influence on the phonon parameters. BelowT_m ~ 180K, the distribution of relaxation frequencies becomes broader than ourexperimental spectral range and frequency independent dielectric losses developbelow 100 GHz in the spectra. Although the macroscopic crystal structure iscubic, IR spectra give evidence about the lower local symmetry which can beassigned to the presence of polar clusters below T_d. Infrared spectra aboveT_d still reveal more modes than predicted by selection rules in theparaelectric phase of the Fm-3m space group so that we suggest selection ruleswhich take into account chemical inhomogeneity in the beta''-perovskitesublattice.
机译:利用宽带介电,时域太赫兹(THz)和傅里叶变换红外(IR)光谱研究了频率为100 Hz-90THz,温度为100-490 K的弛豫铁电PbMg_1 / 3Ta_2 / 3O_3陶瓷和薄膜,在20至900K范围内研究了THz和IR光谱。复电容率的扩散且强烈依赖温度的峰是由于极性团簇的动力学引起的介电弛豫而引起的。弛豫出现在THz范围内的Burns温度T_d以下,通过微波和MHz范围的冷却以及异常扩展会减慢速度。松弛时间分布的最短和最长弛豫时间分别遵循Arrhenius和Vogel-Fulcher定律。 B位有序度对介电弛豫参数影响很小,对声子参数几乎没有影响。在T_m〜180K以下,弛豫频率的分布变得比我们的实验光谱范围更宽,并且在100 GHz以下的光谱中,频率无关的介电损耗逐渐增大。尽管宏观晶体结构是立方的,但红外光谱提供了较低的局部对称性的证据,这可能归因于T_d以下极性簇的存在。 T_d以上的红外光谱仍然显示出比Fm-3m空间群顺电相中选择规则所预测的模式更多的模态,因此我们建议选择规则考虑到β''-钙钛矿亚晶格中的化学不均匀性。

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