Phase equilibrium in the system Ln-Mn-O VI: Ln=Ho and Tb at 1100°C

Phase equilibria were established in Ho-Mn-O and Tb-Mn-O systems at 1100°C by varying the oxygen partial pressure from −log(P_O2/atm)=0-13.00, and phase diagrams for the corresponding Ln₂O₃-MnO-MnO₂ systems at 1100°C were presented. Stable Ln₂O₃, MnO, Mn₃O₄, LnMnO₃, and LnMn₂O₅ phases were found at 1100°C, whereas Ln₂Mn₂O₇, Ln₂MnO₄, Mn₂O₃, and MnO₂ were not found to be stable. Small nonstoichiometric ranges were found in the LnMnO₃ phase, with the composition of LnMnO₃ represented as functions of log(P_O2/atm), and . Activities of the components in the solid solution were calculated from these equations. The composition of LnMnO₃ may range from Ln₂O₃ rich to Ln₂O₃ poor, while MnO is slightly nonstoichiometric, being oxygen rich and LnMn₂O₅ seems to be nonstoichiometric. Lattice constants of LnMnO₃ quenched at different oxygen partial pressures and of LnMn₂O₅ quenched in air were determined. The standard Gibbs energy changes of the reactions appearing in the phase diagrams were also calculated. The relationship between the tolerance factor of LnMnO₃ and ΔG⁰of reaction, (1/2)Ln₂O₃+MnO+(1/4)O₂=LnMnO₃, is shown graphically.