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Dielectric Properties of Colossal Permittivity Materials: An Update

机译:介电常数材料的介电性能:更新

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摘要

During the last 10 years, a lot of interests have been devoted to the so-called CDC (colossal dielectric constant) materials. The first materials exhibiting this behavior were the perovskite-based ceramics on the CCTO (CaCu_3Ti_4O_(12)) composition. Relative dielectric permittivity can attain values up to (or even larger than) 10~5. Nevertheless, their dielectric losses are too high, the lower values ranging 10%, in a narrow frequency range, thus limiting their applications. The underlying physical mechanisms at the origin of the CDC are still under study. The analysis of broadband impedance spectroscopy measurements leads most of the authors to propose an interfacial polarization mechanism (at the electrodes or at internal barriers), there is a limited number of complementary electrical characterization techniques, which, up to now, comfort the proposed interfacial polarization mechanisms. In the present work, Ⅰ-Ⅴ and time-domain polarization are used to characterize these materials. One of the main results is the observation of a non-symmetrical response of these materials related to the direction of the polarization. These results are observed for both macroscopic level on bulk polycrystalline material and within individual grains of the same samples. These results do not fit current accepted models for polarization for CDC materials.
机译:在过去的十年中,人们对所谓的CDC(巨大介电常数)材料投入了很多兴趣。表现出这种行为的第一种材料是CCTO(CaCu_3Ti_4O_(12))成分上的钙钛矿基陶瓷。相对介电常数可以达到(甚至大于)10〜5。然而,它们的介电损耗太高,在狭窄的频率范围内的较低值在10%左右,从而限制了它们的应用。 CDC起源的潜在物理机制仍在研究中。宽带阻抗谱测量的分析导致大多数作者提出了一种界面极化机制(在电极或内部势垒处),而互补的电学表征技术数量有限,到现在为止,这些技术都使拟议的界面极化变得令人安心。机制。在目前的工作中,使用Ⅰ-Ⅴ和时域极化来表征这些材料。主要结果之一是观察到这些材料与偏振方向有关的非对称响应。在大块多晶材料上以及在同一样品的单个晶粒内的宏观水平上都观察到了这些结果。这些结果与当前接受的CDC材料极化模型不符。

著录项

  • 来源
    《Journal of energy and power engineering》 |2013年第4期|726-732|共7页
  • 作者单位

    LAPLACE (Laboratoire Plasma et Conversion d'Energie), Universite de Toulouse, Toulouse 9 F-31062, France,CNRS (Centre National de la Recherche Scientifique), LAPLACE, Toulouse F-31062, France;

    LAPLACE (Laboratoire Plasma et Conversion d'Energie), Universite de Toulouse, Toulouse 9 F-31062, France,CNRS (Centre National de la Recherche Scientifique), LAPLACE, Toulouse F-31062, France;

    Centre Universitaire Jean-Francois Champollion, Albi 81012, France;

    LAPLACE (Laboratoire Plasma et Conversion d'Energie), Universite de Toulouse, Toulouse 9 F-31062, France,CNRS (Centre National de la Recherche Scientifique), LAPLACE, Toulouse F-31062, France;

    LAPLACE (Laboratoire Plasma et Conversion d'Energie), Universite de Toulouse, Toulouse 9 F-31062, France,CNRS (Centre National de la Recherche Scientifique), LAPLACE, Toulouse F-31062, France;

    LAPLACE (Laboratoire Plasma et Conversion d'Energie), Universite de Toulouse, Toulouse 9 F-31062, France,CNRS (Centre National de la Recherche Scientifique), LAPLACE, Toulouse F-31062, France;

    Institut Carnot CIRIMAT (Centre Inter-universitaire de Recherche et d'Ingenierie des Materiaux), Universite Paul Sabatier,Toulouse 9 31062, France;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Colossal permittivity; CaCu_3Ti_4O_(12); CCTO dielectric properties;

    机译:介电常数CaCu_3Ti_4O_(12);CCTO介电性能;

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