Microstructure and microwave electromagnetic properties of Dy~(3+)-doped W-type hexaferrites

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Ba 1 x Dy x Co 2 Fe 16 O 27 (x = 0.00, 0.05, 0.10, 0.15, and 0.20) was prepared by the solid-state method. The phase structure was studied using powder X-ray diffraction (XRD), the electromagnetic properties were measured, and the reflection loss of Dy 3+ -doped ferrite material was calculated using electromagnetic parameters by the transmission line theory. All XRD patterns showed the single phase of the magnetoplumbite barium ferrite without other intermediate phase when x ≤ 0.15. The values of ε′ and ε″ increased slightly with Dy 3+ ions doping. The values of μ″ and μ′ were improved with Dy 3+ doping, exhibiting excellent microwave magnetic performance. The reasons have also been discussed using the electromagnetic theory. Dy substitution could increase microwave-absorbing performance and broaden frequency band (reflection loss (RL) < -10 dB), and the absorbing peak shifted to high-frequency position. When x = 0.2, ferrite layer exhibited the most excellent microwave-absorbing performance at a thin matching thickness of 1.5 mm. The peak value of RL was around -15 dB, and the frequency band (RL < -10 dB) was about 7 GHz (from 8 to 15 GHz). Ba 1 x Dy x Co 2 Fe 16 O 27 (x = 0.00, 0.05, 0.10, 0.15, and 0.20) was prepared by the solid-state method. The phase structure was studied using powder X-ray diffraction (XRD) electromagnetic properties were measured, and the reflection loss of Dy 3+ -doped ferrite material was calculated using electromagnetic parameters by the transmission line theory. All XRD patterns showed the single phase of the magnetoplumbite barium ferrite without other intermediate phase when x ≤ 0.15. The values ​​of ε ’and ε “increased slightly with Dy 3+ ions doping. The values ​​of μ” and μ’ were improved with Dy 3+ doping, exhibiting excellent microwave magnetic performance. The reasons have also been discussed using the electromagnetic theory. Dy substitution could increase microwave-absorbing performance and broaden frequency band (reflection loss (RL) <-10 dB), and the absorbing peak shifted to high-frequency position. When x = 0.2, bsorbing performance at a thin matching thickness of 1.5 mm. The peak value of RL was around -15 dB, and the frequency band (RL <-10 dB) was about 7 GHz (from 8 to 15 GHz).
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