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<p>The sol–gel method was used in our work to develop Ca<sub>1-x</sub>Cu<sub>x</sub>Fe<sub>12-x</sub>Al<sub>x</sub>O<sub>19</sub> (x = 0.0, 0.05, 0.10, 0.15, 0.20) hexaferrites nanoparticles. The microstructure, phase, and magnetic characteristics of the samples were examined relative to different doping concentrations using SEM, XRD, and VSM techniques. The analysis indicates the presence of Fe<sub>2</sub>O<sub>3</sub> phases in all samples. The lattice parameters ‘a’ and ‘c’ were initially reduced and then enhanced with doping level. Similarly, the average crystallite size showed a decline continuously. The remanence as well as saturation magnetization both decline first with the doping level and then rise after reaching their minimum values at x = 0.15. Analogously, as the doping level is raised, the coercivity as well as magneto-crystalline anisotropy field first declines and then increases. The sample with the best magnetic properties is Ca<sub>0.85</sub>Cu<sub>0.15</sub>Fe<sub>11.85</sub>Al<sub>0.15</sub>O<sub>19</sub> with M<sub>s</sub> = 27.954&#xa0;emu/g, m<sub>B</sub>(µ<sub>B</sub>) = 5.117B, M<sub>r</sub> = 15.676&#xa0;emu/g, M<sub>r</sub>/M<sub>s</sub> = 0.577, H<sub>c</sub> = 2.726 kOe, and H<sub>a</sub> = 0.852 kOe. Dielectric properties suggested the decrease in loss and enhancement in the dielectric constant. Results recommend that M-type hexagonal ferrites could be well adjusted for numerous magnetic usages such as magnetic filters, storage devices and high-performance self-biased circulators and energy applications.</p>

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Structural, magnetic and dielectric features of Cu, Al substituted Ca-hexaferrites for magnetic and energy applications

  • 期刊论文

  • 发表日期：

    2025年2月7日

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  • M. M. Moharam,
  • I. Ahmad,
  • G. F. B. Solre,
  • S. U. Asif,
  • E. A. M. Saleh

摘要

The sol–gel method was used in our work to develop Ca1-xCuxFe12-xAlxO19 (x = 0.0, 0.05, 0.10, 0.15, 0.20) hexaferrites nanoparticles. The microstructure, phase, and magnetic characteristics of the samples were examined relative to different doping concentrations using SEM, XRD, and VSM techniques. The analysis indicates the presence of Fe2O3 phases in all samples. The lattice parameters ‘a’ and ‘c’ were initially reduced and then enhanced with doping level. Similarly, the average crystallite size showed a decline continuously. The remanence as well as saturation magnetization both decline first with the doping level and then rise after reaching their minimum values at x = 0.15. Analogously, as the doping level is raised, the coercivity as well as magneto-crystalline anisotropy field first declines and then increases. The sample with the best magnetic properties is Ca0.85Cu0.15Fe11.85Al0.15O19 with Ms = 27.954 emu/g, mB(µB) = 5.117B, Mr = 15.676 emu/g, Mr/Ms = 0.577, Hc = 2.726 kOe, and Ha = 0.852 kOe. Dielectric properties suggested the decrease in loss and enhancement in the dielectric constant. Results recommend that M-type hexagonal ferrites could be well adjusted for numerous magnetic usages such as magnetic filters, storage devices and high-performance self-biased circulators and energy applications.