are not stable. Wide ranges of nonstoichiometry were found is the LaMnO 3 phase. x ranges from ؊0.050 at log P O2 ؍ ؊13.05 to 0.18 at log P O2 ؍ 0 in the form of LaMnO 3؉x . The nonstoichiometry is represented with the equation, N O /N LaMnO3 ؍ 1.94؋10 ؊4 (log P O2 ) 3 ؉ 5.24؋10 ؊3 (log P O2
✦ LIBER ✦
Phase Equilibrium in the System Ln–Mn–O IV. Ln=Sm at 1100°C
✍ Scribed by Kenzo Kitayama; Minehito Kobayashi; Takashi Kimoto
- Publisher
- Elsevier Science
- Year
- 2002
- Tongue
- English
- Weight
- 197 KB
- Volume
- 167
- Category
- Article
- ISSN
- 0022-4596
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📜 SIMILAR VOLUMES
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2000
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⚖ 117 KB
Phase equilibria in the system Pr+Co+O at 1100 and 11503C are established by changing the oxygen partial pressure from 0 to 12.00 in ؊log (P O 2 /atm), and a representative phase diagram at 11003C is presented for the Pr 2 O 3 +Co+CO 2 O 3 system. Under experimental conditions, the PrO 1.63؉ ( ), Pr
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⚖ 601 KB
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L. Ya. Gavrilova; T. V. Aksenova; N. E. Volkova; A. S. Podzorova; V. A. Cherepan
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## Abstract Phase equilibria in the title systems at 1100 °C in air and the crystal structure of intermediate phases are investigated by powder XRD.