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首页> 外文期刊>Journal of Applied Physics >Electrostrictive and relaxor ferroelectric behavior in BiAlO_3-modified BaTiO_3 lead-free ceramics
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Electrostrictive and relaxor ferroelectric behavior in BiAlO_3-modified BaTiO_3 lead-free ceramics

机译:BiAlO_3改性的BaTiO_3无铅陶瓷的电致伸缩和弛豫铁电行为

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摘要

The crystal structure of (1-x)BaTiO_(3-x)BiAlO_3 (x = 0, 0.02, 0.05, 0.08, and 0.1) ceramics was determined using X-ray diffraction and Raman spectroscopy at room temperature, which revealed a phase transition from tetragonal to rhombohedral with increasing x. The dielectric properties were studied as a function of temperature at different frequencies, which indicated that the phase transition temperature (T_m) decreased with increasing x. The relaxor behavior was observed by frequency and temperature dependent dielectric permittivity. The Lorenz-type quadratic law was used to characterize the dielectric permittivity peaks near T_m of high-temperature slopes at 1 MHz. The temperatures T_m of dielectric permittivity peaks fit very well with the Vogel-Fulcher law in x = 0.05 and x = 0.1. The polarization hysteresis loops and electrostrictive were displayed at room temperature. The sample for x = 0.1 exhibits a slim loop with negligible hysteresis and a subtle linear feature, which is a promising transducer material for use as an active element.
机译:在室温下使用X射线衍射和拉曼光谱法确定了(1-x)BaTiO_(3-x)BiAlO_3(x = 0、0.02、0.05、0.08和0.1)陶瓷的晶体结构,揭示了相变从四边形到菱形,随x的增加而增加。研究了介电特性随温度在不同频率下的变化,表明相变温度(T_m)随着x的增加而降低。通过频率和温度相关的介电常数观察到弛豫行为。使用Lorenz型二次定律来表征1 MHz处高温斜率T_m附近的介电常数峰值。介电常数峰值的温度T_m与Vogel-Fulcher定律非常吻合,x = 0.05和x = 0.1。在室温下显示极化磁滞回线和电致伸缩。 x = 0.1的样品表现出纤细的回线,具有可忽略的磁滞和微妙的线性特征,这是用作有源元件的有前途的换能器材料。

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  • 来源
    《Journal of Applied Physics》 |2013年第9期|094102.1-094102.5|共5页
  • 作者单位

    State Key Laboratory Breeding Base of Non-Ferrous Metal and Characteristic Materials Processing,College of Materials Science and Engineering, Guilin University of Technology, Guilin 541004,People's Republic of China;

    Laboratory of Chemical Analysis Elaboration and Materials, Engineering (LEACIM), Universite de La Rochelle, Avenue Michel Crepeau, 17042 La Rochelle, Cedex 01, France;

    State Key Laboratory Breeding Base of Non-Ferrous Metal and Characteristic Materials Processing,College of Materials Science and Engineering, Guilin University of Technology, Guilin 541004,People's Republic of China;

    State Key Laboratory Breeding Base of Non-Ferrous Metal and Characteristic Materials Processing,College of Materials Science and Engineering, Guilin University of Technology, Guilin 541004,People's Republic of China;

    State Key Laboratory Breeding Base of Non-Ferrous Metal and Characteristic Materials Processing,College of Materials Science and Engineering, Guilin University of Technology, Guilin 541004,People's Republic of China;

    Department of Physical Chemistry, University of Science and Technology Beijing, Beijing 100083, China;

    Department of Physical Chemistry, University of Science and Technology Beijing, Beijing 100083, China;

    State Key Laboratory Breeding Base of Non-Ferrous Metal and Characteristic Materials Processing,College of Materials Science and Engineering, Guilin University of Technology, Guilin 541004,People's Republic of China;

    Laboratory of Chemical Analysis Elaboration and Materials, Engineering (LEACIM), Universite de La Rochelle, Avenue Michel Crepeau, 17042 La Rochelle, Cedex 01, France;

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