@article{oai:niit.repo.nii.ac.jp:00000155,
 author = {Kitayama, Kenzo and Shioya, Natsuko and Iura, Motohiro and Ikeda, Syunsuke and Saeki, Naoki and Ishizawa, Yuzuru},
 journal = {新潟工科大学研究紀要},
 month = {Dec},
 note = {Phase equilibrium was established in a Ln-Mn-O (Ln=Er and Tm) system at 1100℃ with the oxygen partial pressure ranging from ?log (P_o2/atm) =  to 12.00, and phase diagrams for the corresponding Ln_2O_3-MnO-MnO_2 system at 1100℃ were constructed. Stable Er_2O_3, MnO, Mn_3O_4, and ErMnO_3 phased were found in the Er-Mn-O system, and stable Tm_2O_3, MnO, Mn_3O_4, and TmMnO_3 phases were found in the Tm-Mn-O system. LnMn_2O_5, Ln_2Mn_2Mn_O_7, Ln_2MnO_4, Mn_2O_3, and MnO_2 were not found in either system. Nonstoichiometric ranges were found in both LnMnO_3 phases, with the composition of LnMnO_3 represented as functions of log (Po_2/atm), No/N_ErMnO3= 2.68×10^-3 (log Po_2)-0.008 and No/N_TmMnO3 =2.53×10^-3 log(Po_2)-0.005 The activities of the components in a solid solution were calculated from the both equations. The lattice constants of ErMnO_3 and TmMnO_3 quenched in air were determined. The standard Gibbs energy changes of the reaction, 1/2 Ln_2O_3 + MnO + 1/4 O_2 = LnMnO_3, appearing in the phase diagrams were also calculated. The relationship between the tolerance factors (t) of ErMnO_3, TmMnO_3 andΔG^0 (hexa) = -6.426×10^2t + 5.406×10^2, which was previously obtained.},
 pages = {1--12},
 title = {Phase Equilibrium in the System Ln-Mn-O at 1100℃ : IX.Ln=Er and Tm},
 volume = {12},
 year = {2007}
}