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024 7 _ |2 DOI
|a 10.1016/j.ssi.2011.06.010
024 7 _ |2 WOS
|a WOS:000295572000004
037 _ _ |a PreJuSER-16240
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Chemistry, Physical
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |0 P:(DE-HGF)0
|a Niedrig, C.
|b 0
245 _ _ |a Thermal Stability of the Cubic Phase in Ba0.5Sr0.5Co0.8Fe0.2O3- (BSCF)
260 _ _ |a Amsterdam [u.a.]
|b Elsevier Science
|c 2011
300 _ _ |a 25 - 31
336 7 _ |a Journal Article
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336 7 _ |a Journal Article
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336 7 _ |a ARTICLE
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336 7 _ |a JOURNAL_ARTICLE
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336 7 _ |a article
|2 DRIVER
440 _ 0 |0 5565
|a Solid State Ionics
|v 197
|x 0167-2738
|y 1
500 _ _ |a Financial support from the Helmholtz Association of German Research Centres (Initiative and Networking Fund) through the MEM-BRAIN Helmholtz Alliance (www.mem-brain-allianz.eu) is gratefully acknowledged. The authors also thank the German Federal Ministry of Economics and Technology (BMWi grant no. 0327803F) and the DFG-Research Center for Functional Nanostructures (CFN, project F2.1) for funding.
520 _ _ |a Ba0.5Sr0.5Co0.8Fe0.2O0-delta (BSCF) is a material with excellent oxygen ionic and electronic transport properties reported by many research groups. In its cubic phase, this mixed ionic-electronic conducting (MIEC) perovskite is a promising candidate for oxygen permeation membranes. For this application, its long-term stability under operating conditions (especially temperature and oxygen partial pressure) is of crucial importance.The present work is focused on the thermal stability of the BSCF cubic phase in the targeted temperature range for applications (700 ... 900 degrees C) in light of previous studies in literature reporting a reversible transition to a hexagonal phase somewhere below 900 degrees C.To this end, single phase cubic BSCF powders were annealed at different temperatures over varying periods of time. Phase composition was subsequently analysed by X-ray diffractometry (XRD) in order to determine both the temperature limit and the time-scale for the formation of the hexagonal phase. Additionally, the long-term behaviour of the electrical conductivity was examined on bulk samples at 700 degrees C, 800 degrees C and 900 degrees C over several hundreds of hours, showing a prolonged decrease at 800 degrees C. The decrease in electrical conductivity at this temperature was also examined on bulk samples with different grain sizes, showing a more pronounced decrease the smaller the average grain size. Coexistence of both phases (cubic and hexagonal) could also be shown for 700 degrees C, however with a different phase equilibrium than at 800 degrees C. (C) 2011 Elsevier B.V. All rights reserved.
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653 2 0 |2 Author
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653 2 0 |2 Author
|a Electrical conductivity
653 2 0 |2 Author
|a Phase stability
653 2 0 |2 Author
|a Hexagonal phase
700 1 _ |0 P:(DE-HGF)0
|a Taufall, S.
|b 1
700 1 _ |0 P:(DE-HGF)0
|a Burriel, M.
|b 2
700 1 _ |0 P:(DE-HGF)0
|a Menesklou, W.
|b 3
700 1 _ |0 P:(DE-Juel1)VDB92808
|a Wagner, S.F.
|b 4
|u FZJ
700 1 _ |0 P:(DE-HGF)0
|a Baumann, S.
|b 5
700 1 _ |0 P:(DE-HGF)0
|a Ivers-Tiffée, E.
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773 _ _ |0 PERI:(DE-600)1500750-9
|a 10.1016/j.ssi.2011.06.010
|g Vol. 197, p. 25 - 31
|p 25 - 31
|q 197<25 - 31
|t Solid state ionics
|v 197
|x 0167-2738
|y 2011
856 7 _ |u http://dx.doi.org/10.1016/j.ssi.2011.06.010
909 C O |o oai:juser.fz-juelich.de:16240
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