Abstract. Perovskite oxides with higher phase transition temperature receive much attention as promising candidates which possess excellent and stable dielectric properties over wide temperature range. In the present research, dense ceramics of Ba-based perovskite oxides of Ba(Cu 1/3 Nb 2/3 )O 3 (BCN) were fabricated by powder sintering. Mn-substituted BCN (Mn-BCN) ceramics were also fabricated for improving the insulating property of the BCN ceramics. Mn-BCN ceramics were fabricated by powder sintering using fine precursor powders derived from sol-gel solutions. The chemical composition of the precursors were Ba[(Cu 1/3 Nb 2/3 ) 1-y Mn y ]O 3 with Mn content of y = 0-0.05. The cylindrical compacts of the powders were heat-treated at 1200-1350 o C for 1-6 h for sintering. All of Mn-BCN ceramics consisted of perovskite-type crystal structure in tetragonal system at room temperature. The relative density of the pure and Mn-BCN ceramics sintered at 1300 o C for 1 h were higher than 90%. The densities were degraded by firing at higher temperature and/or for longer time, owing to the thermal decomposition of the BCN crystalline phase. The Mn-substitution for BCN ceramics resulted in disappearing the dielectric relaxation and suppressing the leakage current conduction.
IntroductionRecently, aggressive researches on alternate materials of Pb(Zr,Ti)O 3 [PZT] have been progressed because Pb element in PZT is hazardous for human body and environment. Bi-base ferroelectric and piezoelectric materials, including BiFeO 3 [BFO] and (Bi,Na)TiO 3 [BNT], are dominant candidates, for Pb-based materials as large spontaneous polarization and piezoelectric constant are reported for these materials. However, most of Bi-based materials exhibit poor insulating property essentially due to volatile Bi element that degrade the performance of these materials [1-2]. New candidates, i.e. Pb-/Bifree ferroelectric materials, would be therefore required in near future.Among several alternative materials for PZT, we focus on the solid-solution system of Ba(Cu 1/3 Nb 2/3 )O 3 (BCN, tetragonal)-Ba(Mg 1/3 Nb 2/3 )O 3 (BMN,) because it possesses similar structure to PbTiO 3 -PbZrO 3 . BCN had tetragonal crystal system with its lattice parameters of a = 0.40464(4) and c = 0.41807(4) nm (c/a = 1.033). High-temperature XRD determined the phase transition temperature from tetragonal-to-cubic phase in the temperature range of 500-600 o C. The P-E and S-E hysteresis loops were measured at room temperature and the apparent maximum in the