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首页> 外文期刊>Journal of materials science >Dielectric response of 0.85 Ba(Ti0.96Zr0.04)O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3 relaxor ferroelectrics under electric field: evolution of PNRs
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Dielectric response of 0.85 Ba(Ti0.96Zr0.04)O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3 relaxor ferroelectrics under electric field: evolution of PNRs

机译:电场下0.85 Ba(Ti0.96Zr0.04)O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3弛豫铁电的介电响应:PNR的演化

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摘要

0.85 Ba(Ti_(0.96)Zr_(0.04))O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3 relaxor ferroelectric ceramic samples were synthesized through traditional solid state reaction method. The asymmetric single peak of (200) at 45° was revealed by XRD measurement, combined with diffuse phase transition peaks in dielectric-temperature spectrum and a slim but discernible hysteresis loop, which proved the existence of the polar nano-regions (PNRs) in paraelectric matrix of the sample. The investigation of dielectric response of the ceramic samples under electric field (changing field magnitude and field history) was employed to analysize the evolution of PNRs. Electric field dependence of dielectric constant was obtained both by small signal bias electric field measurement and differential calculation from P-E curves, they all reached the maximum value firstly at the critical electric field and then decreased with the continuous increasing of electric field, instead of decreasing directly. However, the value of dielectric constant and critical field of bias electric field measurement was hys-teretic electrically to those of differential calculation from P-E curves. Both the glassy model and macro-micro theory model were employed to explain and explore the evolution of PNRs, though from different perspective.
机译:通过传统的固态反应方法合成了0.85 Ba(Ti_(0.96)Zr_(0.04)O_3-0.15 Bi(Mg_(0.5)Ti_(0.5))O_3弛豫铁电陶瓷样品。通过X射线衍射(XRD)测量揭示了(200)在45°处的不对称单峰,并结合了介电温度谱中的弥散相变峰和纤细但可辨认的磁滞回线,证明了存在极性纳米区(PNR)。样品的顺电矩阵。通过研究陶瓷样品在电场(变化的场强和场历史)下的介电响应来分析PNR的演化。通过小信号偏置电场测量和PE曲线的微分计算获得了介电常数的电场依赖性,它们都在临界电场处先达到最大值,然后随着电场的不断增加而减小,而不是直接减小。然而,介电常数和偏置电场测量的临界场的值在电学上与从P-E曲线进行差分计算的值相比具有滞后性。尽管从不同的角度来看,玻璃模型和宏观微观理论模型都被用来解释和探索PNR的演变。

著录项

  • 来源
    《Journal of materials science》 |2015年第11期|9146-9151|共6页
  • 作者单位

    State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, Wuhan University of Technology, Luoshi Road 122, Wuhan 430070, China;

    State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, Wuhan University of Technology, Luoshi Road 122, Wuhan 430070, China;

    State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, Wuhan University of Technology, Luoshi Road 122, Wuhan 430070, China;

    State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, Wuhan University of Technology, Luoshi Road 122, Wuhan 430070, China;

    State Key Laboratory of Advanced Technology for Materials Synthesis and Processing, School of Material Science and Engineering, Wuhan University of Technology, Luoshi Road 122, Wuhan 430070, China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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