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([Formula: see text])LiCuNb 3 O 9 -[Formula: see text]Bi(Mg[Formula: see text]Zr[Formula: see text])O 3  ceramics (([Formula: see text])LCN-[Formula: see text]BMZ) with [Formula: see text] were synthesized by a solid-state reaction method. The phase structure of ([Formula: see text])LCN-[Formula: see text]BMZ ceramics was characterized by X-ray diffraction (XRD), which revealed that the ceramics were distorted cubic perovskite structures. Apparent giant permittivity of [Formula: see text]–[Formula: see text] at 100[Formula: see text]kHz over the measured temperature range (25[Formula: see text]C–250[Formula: see text]C) was observed in the sintered ([Formula: see text])LCN-[Formula: see text]BMZ ([Formula: see text]) ceramics. Especially for the sample of [Formula: see text]0.04, the temperature stability of permittivity was markedly increased ([Formula: see text]/[Formula: see text]%), and high relative permittivity ([Formula: see text]) were obtained over a wide temperature range from 100[Formula: see text]C to 250[Formula: see text]C at 100[Formula: see text]kHz, which indicates that this ceramic is a promising dielectric material for elevated temperature dielectrics. The giant dielectric property of ([Formula: see text])LCN-[Formula: see text]BMZ ceramics are profoundly concerned with the Maxwell–Wagner effect.

Giant permittivity and good thermal stability of LiCuNb3O9-Bi(Mg0.5Zr0.5)O3 solid solutions

Giant permittivity and good thermal stability of LiCuNb₃O₉-Bi(Mg0.5Zr0.5)O₃ solid solutions