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The effect of cation-size variance on the relaxor nature and insulating character of the lead free Rb substituted Na_(0.5)Bi_(0.5)TiO_3

机译:阳离子尺寸方差对无铅RB取代Na_(0.5)Bi_(0.5)TiO_3的弛豫性质和绝缘特性的影响

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Relaxation property is always matter of interest for the frequency dependent study of the ferroelectric materials. The Nyquist plot of the impedance data provides the information about the relaxation phenomena. Often, in solids, instead of a single relaxation time a distribution of the relaxation times is found, which arises from the different mechanisms. Usually, the relaxation times is varied by substitution and its influence is studied on the basis of the compositional effects, but the impact of the size of the substituent is rarely analyzed. Fundamentally, the substituted cations modulatethe crystal structure of the parent material, which attunes the relaxation phenomenon. In the current study, the Rb substituted lead free Na_(0.5)Bi_(0.5)TiO_3 (perovskite structure, ABO_3 type) is chosen as its A-site is compositionally disorder due to the presence of the different cations with dissimilar radii. The samples are prepared through the solid state sintering method. The imaginary part of the complex impedance (Z) vs its real part (Z) are plotted for all samples to verify the response of the grain and grain boundaries. At the higher temperatures (≥500°C) single semi-circular arcs are formed by the materials for all the compositions. Interestingly, two semi-circular arcs are observed for the material for the higher cation-site disordered system at lower temperature (below 300°C). The second circle is associated with the different relaxation time of the dipolar entity, which may be generated due to the substitution of the Rb~(1+). This observation prove that the cation size mismatch creates the variation in the relaxation times at the lower temperatures. The cation size mismatch also modulates the contribution of the grain boundary to the impedance property. The real part of impedance of the 4 mol %. substituted Na_(0.5)Bi_(0.5)TiO_3 is enhanced than parent Na_(0.5)Bi_(0.5)TiO_3, which fortifies its performance as a capacitor and energy storage device.
机译:放宽属性对于铁电材料的频率依赖性研究始终感兴趣。阻抗数据的奈奎斯特图提供了有关松弛现象的信息。通常,在固体中,不是单一的弛豫时间,发现松弛时间的分布,其出现来自不同的机制。通常,弛豫时间通过取代而变化,并且在组成效果的基础上进行了影响,但很少分析取代基的尺寸的影响。从根本上说,母体材料的替代阳离子模晶结构,其调节松弛现象。在目前的研究中,选择RB取代的无铅Na_(0.5)Bi_(0.5)TiO_3(钙钛矿结构,ABO_3型),因为其A现场是由于不同阳离子的不同阳离子具有不同的半径的组成紊乱。样品通过固态烧结方法制备。复杂阻抗(Z)VS的虚部绘制其真实部分(Z),用于所有样品以验证晶粒和晶界的响应。在较高的温度下(≥500°C),单个半圆形弧由所有组合物的材料形成。有趣的是,在较低温度(低于300℃以下的较高阳离子位点无序系统的材料中,观察到两个半圆形弧。第二圆与双极实体的不同弛豫时间相关联,这可能由于RB〜(1+)的取代而产生。该观察结果证明,阳离子尺寸不匹配在较低温度下产生松弛时间的变化。阳离子尺寸不匹配还调制晶界对阻抗性的贡献。 4摩尔%的阻抗的真实部分。取代的NA_(0.5)Bi_(0.5)TiO_3比父NA_(0.5)Bi_(0.5)TiO_3增强,这将其作为电容器和能量存储设备的性能强化。

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