首页> 外文期刊>Journal of the Korean Physical Society >Electrical Response of Mixed Regions in the Pb(Mg_(1/3)Ta_(2/3))O_3 and the Pb(Mg_(1/3)Nb_(2/3))O_3 Complex Perovskites
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Electrical Response of Mixed Regions in the Pb(Mg_(1/3)Ta_(2/3))O_3 and the Pb(Mg_(1/3)Nb_(2/3))O_3 Complex Perovskites

机译:Pb(Mg_(1/3)Ta_(2/3))O_3和Pb(Mg_(1/3)Nb_(2/3))O_3复合钙钛矿中混合区的电响应

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The dielectric properties of the Pb(Mg_(1/3)Ta_(2/3))O_3-Pb(Mg_(1/3)Nb_(2/3))O_3-PbTiO_3 ternary systems were examined as a function of temperature. The split (002) or (200) X-ray diffraction patterns were in the 2θ range of 43.5 ~ 45.5? for xPb(Mg_(1/3)Ta_(2/3))O_3-(0.6-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.4PbTiO_3 indicating the formation of a tetragonal phase at room temperatures. The reciprocal dielectric constant spectra were analyzed further in terms of normal and relaxor ferroelectrics. The frequency dispersion of the dielectric constant maxima was decreased by PbTiO_3. From the dielectric data for xPb(Mg_(1/3)Ta_(2/3))O_3-(0.7-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.3PbTiO_3, two major anomalies corresponding to the rhombohedral → tetragonal → cubic phase transitions were observed. At a temperature of about 160 ~ 190?C, the dielectric constant deviates from the Curie-Weiss law and the deviation temperature for normal ferroelectrics. The maximum values of the dielectric constant increased from 21151 for 0.1Pb(Mg_(1/3)Ta_(2/3))O_3 to 29227 for 0.5Pb(Mg_(1/3)Ta_(2/3))O_3 for the xPb(Mg_(1/3)Ta_(2/3))O_3- (0.6-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.4PbTiO_3 systems. However, the dielectric constant maxima between 32626 at 0.1Pb(Mg_(1/3)Ta_(2/3))O_3 and 28757 at 0.3Pb(Mg_(1/3)Ta_(2/3))O_3 decreased with increasing mole fraction x for the xPb(Mg_(1/3)Ta_(2/3))O_3-(0.7-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.3PbTiO_3 systems. The value of the diffuseness component varied from 1.56 to 1.74 in Pb(Mg_(1/3)Ta_(2/3))O_3-Pb(Mg_(1/3)Nb_(2/3))O_3- PbTiO_3 ternary systems at different Pb(Mg_(1/3)Ta_(2/3))O_3 ratios.
机译:研究了Pb(Mg_(1/3)Ta_(2/3))O_3-Pb(Mg_(1/3)Nb_(2/3))O_3-PbTiO_3三元体系的介电性能随温度的变化。 (002)或(200)的X射线衍射图谱的2θ范围为43.5〜45.5?对于xPb(Mg_(1/3)Ta_(2/3))O_3-(0.6-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.4PbTiO_3表示在室温。根据正铁电体和弛豫铁电体进一步分析了相互的介电常数谱。 PbTiO_3降低了介电常数最大值的频率色散。从xPb(Mg_(1/3)Ta_(2/3))O_3-(0.7-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.3PbTiO_3的介电数据来看观察到对应于菱形→四方→立方相变。在约160〜190?C的温度下,介电常数会偏离居里-魏斯定律和正常铁电体的偏离温度。介电常数的最大值从0.1Pb(Mg_(1/3)Ta_(2/3))O_3的21151增加到0.5Pb(Mg_(1/3)Ta_(2/3))O_3的29227 xPb(Mg_(1/3)Ta_(2/3))O_3-(0.6-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.4PbTiO_3系统。但是,随着摩尔的增加,介电常数最大值在0.1Pb(Mg_(1/3)Ta_(2/3))O_3处的32626和0.3Pb(Mg_(1 / 3Gg_Ta_(2/3))O_3处的28757之间的介电常数最大值减小xPb(Mg_(1/3)Ta_(2/3))O_3-(0.7-x)Pb(Mg_(1/3)Nb_(2/3))O_3-0.3PbTiO_3系统的分数x。 Pb(Mg_(1/3)Ta_(2/3))O_3-Pb(Mg_(1/3)Nb_(2/3))O_3- PbTiO_3三元系中的扩散分量的值从1.56到1.74不等不同的Pb(Mg_(1/3)Ta_(2/3))O_3比。

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