In this work, novel medium-entropy Ca3(Co0.25Zn0.25Mg0.25Cu0.25)2SiV2O12 (CZMC) ceramics with garnet structure were designed and synthesized based on the entropy effect. A small average atomic size difference was proven to be advantageous for the formation of a garnet-structured solid solution, as evidenced via X-ray diffraction (XRD) and Rietveld refinement results. The sintering temperature was effectively reduced due to an increase in the configurational entropy (ΔSconfig). The dielectric constant (εr) of the CZMC ceramics showed the opposite trend to that of the Raman shift at approximately 838 cm−1, whereas the variation in the quality factor (Q×f) was identical to that of the relative density but opposite to that of the full width at half maximum (FWHM) of the Raman spectra. Alternating current (AC) impedance spectroscopy revealed that the conductivity of the CZMC ceramics was affected mainly by the diffusion of thermally activated oxygen vacancies. The high activation energy further indicated that the low defect concentration in the sample contributed to reducing the dielectric loss of the ceramics. The B‒O bond had the strongest contribution to the total bond energy, thus playing an important role in manipulating the temperature coefficient of the resonant frequency (τf) of the ceramics. Moreover, the V‒O bond significantly influenced the εr and the Q×f of the CZMC ceramics. Finally, superior microwave dielectric properties (εr = 10.89, Q×f = 59,200 GHz, and τf = –9.6 ppm/°C) together with a high relative density of 95.4% were achieved at 1010 °C. Therefore, extensive applications can be found in the field of millimeter wave communication for CZMC ceramics.
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Complex ion substitution is gaining more attention as an appealing method of modifying the structure and performance of microwave ceramics. In this work, Li2Zn[Ti1−x(Ni1/3Nb2/3)x]3O8 (LZTNNx, 0 ≤ x ≤ 0.3) ceramics were designed based on the complex ion substitution strategy, following the substitution rule of radius and valence to investigate the relationship among phase compositions (containing oxygen vacancies and Ti3+ ions), microstructures, and microwave dielectric characteristics of the LZTNNx ceramics. The samples maintained a single Li2ZnTi3O8 solid solution phase as x ≤ 0.2, whereas the sample of x = 0.3 produced a second phase with the LiNbO3 structure. The appropriate amount of (Ni1/3Nb2/3)4+ substitution could slightly improve the densification of the LZTNNx ceramics due to the formation of the Li2ZnTi3O8 solid solution accompanied by a decrease in the average grain size. The presence of a new A1g Raman active band at about 848 cm−1 indicated that local symmetry changed, affecting atomic interactions of the LZTNNx ceramics. The variation of the relative dielectric constant (εr) was closely related to the molar volume ionic polarizability (
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A rapid and facile approach was developed for the synthesis of ultrafine SmAlO3 powders through the combustion of stearic acid precursors. The obtained products were characterized by typical techniques including X-ray diffraction (XRD), Fourier Transform Infrared (FT-IR), thermogravimetric and differential thermal analysis (TG-DTA), scanning electron microscopy (SEM), and transmission electron microscopy (TEM) to analyze the phase composition and microstructure. The dielectric characteristics of SmAlO3 microwave ceramics, using the as-obtained products as original materials, were also studied. Compared with the conventional solid-state reaction method, the synthesis temperature was dramatically reduced to 750 ℃. The large-size sheet structure was composed of a number of micro/nano-scale crystallites, which were mostly irregular in shape due to the mutual growth and overlapping shapes of adjacent grains. The SmAlO3 ceramics with high density and uniform microstructure were obtained after sintering at 1500 ℃ for 4 h due to the favorable sintering activity of the as-synthesized powders. In addition, desired dielectric properties at microwave frequencies (dielectric constant εr = 20.22, quality factor Q·f = 74110 GHz, and a temperature coefficient of resonant frequency τf = -74.6 ppm/℃) were achieved.
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