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@ARTICLE{Niedrig:16240,
author = {Niedrig, C. and Taufall, S. and Burriel, M. and Menesklou,
W. and Wagner, S.F. and Baumann, S. and Ivers-Tiffée, E.},
title = {{T}hermal {S}tability of the {C}ubic {P}hase in
{B}a0.5{S}r0.5{C}o0.8{F}e0.2{O}3- ({BSCF})},
journal = {Solid state ionics},
volume = {197},
issn = {0167-2738},
address = {Amsterdam [u.a.]},
publisher = {Elsevier Science},
reportid = {PreJuSER-16240},
pages = {25 - 31},
year = {2011},
note = {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.},
abstract = {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.},
keywords = {J (WoSType)},
cin = {IEK-1},
ddc = {530},
cid = {I:(DE-Juel1)IEK-1-20101013},
pnm = {Rationelle Energieumwandlung},
pid = {G:(DE-Juel1)FUEK402},
shelfmark = {Chemistry, Physical / Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000295572000004},
doi = {10.1016/j.ssi.2011.06.010},
url = {https://juser.fz-juelich.de/record/16240},
}