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Crystal structure, phonon characteristic, and intrinsic properties of Sm(Mg_(1/2)Sn_(1/2))O_3 double perovskite ceramic

机译:Sm(Mg_(1/2)Sn_(1/2))O_3双层钙钛矿陶瓷的晶体结构,声子特性和固有性质

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摘要

Sm(Mg_(1/2)Sn_(1/2))O_3(SMS) microwave dielectric ceramic was prepared by the traditional solid state synthesis method. The samples were tested by X-ray diffraction (XRD), vibrational spectra (Raman scattering and far-infrared reflectance spectroscopy). The Sm(Mg_(1/2)Sn_(1/2))O_3 perovskite is monoclinic with the space group P2_1 proved by XRD. Raman vibrational modes were fitted and assigned by Lorentz function. To calculate the intrinsic properties, far-infrared spectra with seven active modes were fitted using a four-parameter semi-quantitative (FPSQ) model. The dielectric constant calculated according to FPSQ is similar to that obtained from the molecular polarization and the Clausius equation. The intrinsic loss has been determined by the relationship between the damping factor and the spectral center frequency, which is slightly larger than the value obtained in the four-parameter fitting, and indicates that A_(1g)(Sm) Raman mode has a enormous effect on the dielectric loss. F_(3u) ~((3)) and F_(4u) ~((4)) have the greatest contribution to the dielectric constant and loss. Finally, the real and imaginary parts of permittivity were analyzed with Kramers-Krönig transformation.
机译:采用传统的固态合成方法制备了Sm(Mg_(1/2)Sn_(1/2))O_3(SMS)微波介电陶瓷。通过X射线衍射(XRD),振动光谱(拉曼散射和远红外反射光谱)测试样品。 Sm(Mg_(1/2)Sn_(1/2))O_3钙钛矿为单斜晶系,XRD证明其空间群为P2_1 / n。拉曼振动模式由Lorentz函数拟合并指定。为了计算固有特性,使用四参数半定量(FPSQ)模型拟合了具有七个活动模式的远红外光谱。根据FPSQ计算的介电常数类似于从分子极化和Clausius方程获得的介电常数。本征损耗是由阻尼因子与频谱中心频率之间的关系确定的,该关系略大于四参数拟合中获得的值,表明A_(1g)(Sm)拉曼模式具有巨大的影响介电损耗。 F_(3u)〜((3))和F_(4u)〜((4))对介电常数和损耗的贡献最大。最后,用Kramers-Krönig变换分析了介电常数的实部和虚部。

著录项

  • 来源
    《Journal of materials science》 |2017年第19期|14156-14162|共7页
  • 作者单位

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    Science and Technology on Electronic Test & Measurement Laboratory, North University of China, Taiyuan, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

    National Synchrotron Radiation Laboratory, China University of Science and Technology, Hefei, China;

    School of Material Science & Engineering, Shandong University of Science and Technology, Qingdao, China;

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