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Single-phase Mn_(1-x)Zn_xFe_2O_4(x = 0.2, 0.5,0.8) hollow ceramic microspheres: One-step preparation and electromagnetic properties

机译:单相Mn_(1-x)Zn_xFe_2O_4(x = 0.2,0.5,0.8)空心陶瓷微球的一步制备及电磁性能

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摘要

Single-phase Mn_(1-x)Zn_xFe_2O_4 (x = 0.2, 0.5, 0.8) hollow ceramic microspheres (MnZn-HCMs) was one-step prepared using self-reactive quenching method. Material parameters of three MnZn-HCMs were studied by SEM and XRD, and electromagnetic properties were investigated by vibrating sample magnetometer and vector network analyzer. The results showed that the phase composition of three MnZn-HCMs presents single-phase, with particle size distribution of 20-60μm; when x was equal to 0.2 or 0.8, the surface of HCMs showed a large number of nano-lamellar crystal with crossing, connecting or laminating each other, and for 0.5, a large quantity of nano-isometric crystal was formed. Thanks to special surface structure and micron-particle size, three MnZn-HCMs exhibited superparamagnetic. With the content of Zn increases, the saturated magnetization (Ms) decreases first and then increases, meanwhile, the coercivity (Hc) decreases gradually. In the 0.1-18 GHz range, due to nano-lamellar structure could enhance the interfacial polarization and space charge polarization, Mn_(0.8)Zn_(0.2)Fe_2O_4 HCMs and Mn_(0.2)Zn_(0.8)Fe_2O_4 HCMs have higher real part of permittivity (ε') value than Mn_(0.5)Zn_(0.5)Fe_2O_4 HCMs. Owing to higher conductivity, the value of imaginary part of permittivity (ε") of Mn_(0.5)Zn_(0.5)Fe_2O_4 HCMs was the highest in 0.1-0.8 GHz range, however, with the frequency increases, the ε" of Mn_(0.8)Zn_(0.2)Fe_2O_4 HCMs and Mn_(0.2)Zn_(0.8)Fe_2O_4 HCMs increased significantly resulting from orientation polarization and interfacial polarization, which was greater than Mn_(0.5)Zn_(0.5)Fe_2O_4 HCMs. Due to the higher Ms, the value of imaginary part of permeability (μ") of Mn_(0.2)Zn_(0.8)Fe_2O_4 HCMs and Mn_(0.8)Zn_(0.2)Fe_2O_4 HCMs was greater than Mn_(0.5)Zn_(0.5)Fe_2O_4 HCMs. Moreover, the μ"-f curve reveals a broad resonance peak of Mn_(0.8)Zn_(0.2)Fe_2O_4 HCMs ranging from 0.1 to 8 GHz, which maybe relate to its thick nano-lamellar crystal.
机译:采用自反应猝灭法一步制备了单相Mn_(1-x)Zn_xFe_2O_4(x = 0.2,0.5,0.8)空心陶瓷微球(MnZn-HCMs)。通过SEM和XRD研究了三种MnZn-HCM的材料参数,并通过振动样品磁力计和矢量网络分析仪研究了电磁性能。结果表明,三种MnZn-HCMs的相组成呈单相,粒径分布为20-60μm。当x等于0.2或0.8时,HCM的表面显示出大量的纳米层晶体彼此交叉,连接或层压,并且对于0.5,形成了大量的纳米级等距晶体。由于特殊的表面结构和微米粒径,三种MnZn-HCM表现出超顺磁性。随着Zn含量的增加,饱和磁化强度(Ms)先减小然后增大,同时矫顽力(Hc)逐渐减小。在0.1-18 GHz范围内,由于纳米层状结构可增强界面极化和空间电荷极化,因此Mn_(0.8)Zn_(0.2)Fe_2O_4 HCM和Mn_(0.2)Zn_(0.8)Fe_2O_4 HCM具有较高的实部介电常数(ε')值要比Mn_(0.5)Zn_(0.5)Fe_2O_4 HCMs高。由于电导率较高,Mn_(0.5)Zn_(0.5)Fe_2O_4 HCM的介电常数的虚部(ε“)值在0.1-0.8 GHz范围内最高,但是随着频率的增加,Mn_( 0.8)Zn_(0.2)Fe_2O_4 HCMs和Mn_(0.2)Zn_(0.8)Fe_2O_4 HCMs由于取向极化和界面极化而显着增加,大于Mn_(0.5)Zn_(0.5)Fe_2O_4 HCM。由于较高的Ms,Mn_(0.2)Zn_(0.8)Fe_2O_4 HCM和Mn_(0.8)Zn_(0.2)Fe_2O_4 HCM的磁导率的虚部(μ“)大于Mn_(0.5)Zn_(0.5) Fe_2O_4 HCMs。此外,μ“ -f曲线揭示了Mn_(0.8)Zn_(0.2)Fe_2O_4 HCMs的宽共振峰,范围为0.1至8 GHz,这可能与其厚的纳米层状晶体有关。

著录项

  • 来源
    《Journal of Applied Physics》 |2014年第17期|174311.1-174311.7|共7页
  • 作者单位

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Military Representative Office in 743 Factory, Taiyuan 030000, China;

    Mechanical Engineering College, Shijiazhuang 050003, China;

    Mechanical Engineering College, Shijiazhuang 050003, 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);
  • 原文格式 PDF
  • 正文语种 eng
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