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Phase Equilibria in the ZrO2–La2O3–Sm2O3 System at 1100°C

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Phase equilibria and structural transformations in the ternary ZrO2–La2O3–Sm2O3 system at 1100°C were studied by X-ray diffraction over the entire composition range. Fields of solid solutions based on the hexagonal (A) modification of La2O3, cubic (F) modification with fluorite-type structure and tetragonal (T) and monoclinic (M) modifications of ZrO2, monoclinic (B) modification of Sm2O3, and an ordered intermediate phase with pyrochlore-type structure, Ln2Zr2O7 (Py), were established to exist in the system. The boundaries of phase fields and lattice parameters of the phases were determined. In the zirconia-rich corner, solid solutions based on the tetragonal modification of ZrO2 are formed. The solubility of La2O3 in T-ZrO2 is low and amounts to ~0.5 mol.%, which is evidenced by X-ray diffraction and microstructural analyses. The solid solutions based on the tetragonal modification of ZrO2 cannot be quenched from high temperatures in the cooling conditions. The X-ray diffraction patterns recorded at room temperature show peaks of the M-ZrO2 monoclinic phase. The ordered pyrochlore-type phase, Ln2Zr2O7 (Py), is in equilibrium with all phases that exist in the ternary ZrO2–La2O3–Sm2O3 system at 1100°C and forms substitutional solid solutions with phases of the binary systems. In the system, an infinite series of solid solutions form from the Ln2Zr2O7 (Py) phase. The isothermal section of the ZrO2–La2O3–Sm2O3 phase diagram at 1100°C contains three three-phase regions (T + M + Py, T + F + Py, A + B + Py) and eight two-phase regions (A + B, A + Py, B + Py, F + Py, F + T, T + M, T + Py, Py + M). New phases were not found to form at 1100°C.

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Correspondence to O. A. Korniienko.

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E. R. Andrievskaya is deceased

Translated from Poroshkova Metallurgiya, Vol. 59, Nos. 3–4 (532), pp. 138–148, 2020.

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Korniienko, O.A., Bykov, A.I. & Andrievskaya, E.R. Phase Equilibria in the ZrO2–La2O3–Sm2O3 System at 1100°C. Powder Metall Met Ceram 59, 224–231 (2020). https://doi.org/10.1007/s11106-020-00154-5

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