(1-x)CeO2-0.5xSm2O3 (x=0-0.9) microwave dielectric ceramics are synthesized by the conventional solid-phase reaction method, with the effects of phase transition on structure and microwave dielectric properties being investigated in detail. The phase transition process is analyzed using the ionicity and lattice energy of (1-x)CeO2-0.5xSm2O3 ceramics, which is related to the coordination number and effective valence electron charge. With the increase of Sm3+ content, there are three phase regions: the cubic fluorite phase (0 ≤ x ≤ 0.4), the rare-earth C-type phase (0.4 <x ≤ 0.8) and the mixed phase (0.8 <x < 1.0). With the phase transition, the microstructures of (1-x)CeO2-0.5xSm2O3 (x=0-0.9) ceramics show a quasi-periodic change, where x=0.4 and x=0.8 are the critical points with similar grain size and distribution. When the phase transition occurs, the polarization, Q׃ values and the resonant frequency temperature coefficients (τƒ) of (1-x)CeO2-0.5xSm2O3 (x=0-0.8) ceramics are all mutated, which is due to the change of bond ionicity and effective valence electron charge caused by the phase transition. The microwave dielectric properties in each pure phase region vary regularly with bond ionicity and valence. Compared with the cubic fluorite phase (0 ≤ x ≤ 0.4), (1-x)CeO2-0.5xSm2O3 ceramics with rare-earth C-type phase (0.4 <x ≤ 0.8) have lower dielectric constant, with better Q׃ values and τƒ values.
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