Abstract

As new oxide ion conducting ceramics, binary rare earth metal fluoride oxides (BMFO, LnLn′F xO y, Ln,Ln′; rare earth) were obtained by firing the powdered mixture of rare earth fluoeide (LnF 3) and oxide (Ln′ 2O 3) at a temperature of 1100–1400 °C in an argon atmosphere. In the solid phase reaction, the anion exchange reaction between LnF 3 and Ln′ 2O 3 took place in the temperature range from 200 to 600 °C to give two simple metal fluoride oxides (SMFO) of LnF xO y and Ln′F xO y, and then above 900 °C, both SMFOs began to react with each other to produce BMFO. Two homogeneous phases were identified to be the rhombohedral and the tetragonal. The rhombohedral phase was formed as a stoichiometric compound (LnLn′ 2F 3O 3) from an equimolar mixture of LnF 3 and Ln′ 2O 3. The tetragonal one was found to have a wide homogeneity composition of Ln xLn′ 2(1−x)F 3xO 3(1−x) where x-value was 0.58–0.78. The electrical conductivity of the tetragonal was at least 100 times higher than for the rhombohedral. All of 210 tetragonal Ln 2Ln′ 2F 6O 3 samples involving reciprocal systems have been investigated. The samples containing Pr or Nd or both gave a high electrical conductivity more than 10 −2 Scm −1 at 650 °C under around 10 −7atm oxygen and their crystal structures closely resembled the cubic. The charge carring species of these BMFOs except Ce and Tb-compounds was assumed to be oxide ion. The electrical conductivity of the sintered Y 2Nd 2F 6O 3 sample obtained by hot-pressing at 1250 °C under 300 kgcm −2 was measured to be 8.0 x 10 −2 Scm −1 at 750 °C, and its oxide ion transport number was calculated to be over 0.93.

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