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@INPROCEEDINGS{Sohn:850086,
author = {Sohn, Yoo Jung and Mauer, Georg and Roth, Georg and
Guillon, Olivier and Vassen, Robert},
title = {{B}-site ordered double perovskite,
{L}a2({A}l0.5{M}g{T}a0.5){O}6 for thermal barrier
applications and its high-temperature phase transition},
reportid = {FZJ-2018-04167},
year = {2018},
abstract = {An improvement of gas turbine engines can be obtained by
increase of the inlet temperatures. The standard thermal
barrier coating (TBC) material yttria partially stabilized
zirconia (YSZ) decomposes at elevated temperatures into
high-yttria and low-yttria phases. The latter transforms
upon cooling into the monoclinic phase with an associated
large volume increase, which may result in failure of the
TBC [1]. Thus, new TBC materials are widely searched to
further improve the gas turbine engine efficiency at
long-term operation temperatures above 1200 °C. Over the
last decades a large amount of candidates have been
investigated to identify alternative TBC materials. Among
them, the complex rare-earth perovskites gained interest due
to their high melting point and possible tailoring
properties with B-site cation ordering effect [2,3].
Recently, plasma sprayed La2(Al0.5MgTa0.5)O6 (LAMT) coatings
showed significantly improved thermal cycling lifetime
results, and were suggested to be a promising candidate
[4,5]. Up to now, synthesized LAMT-powder was identified to
be an orthorhombic phase with the space group symmetry,
Pnma, which is isostructural to orthorhombic LaFeO3. The
Pawley refinement on the measured powder X-ray diffraction
(XRD) data revealed no oddity. However, a strong mismatch of
the peak intensities was detected during the Rietveld
analysis. A possible texture effect was excluded because of
the powder morphology, as well as, by trying out the
different sample preparation methods. To clarify the correct
crystal structure of LAMT and to check the phase stability,
in-situ high-temperature XRD was carried out in the
temperature range of 25-1200 °C. Unlike reported earlier
[4], a structural phase transition was observed at ~ 855 °C
upon heating, and this phase transition was completely
reversible. The crystal structure of LAMT was then refined
by Rietveld analysis in the monoclinic space group symmetry,
P21/n [6] at room temperature, with β = ~ 90°. In the
monoclinic crystal structure, the B-site cations are
ordering in a rock-salt type arrangement. The Mg2+-ions take
the fully occupied 2c-Wyckoff position whereas the Al3+- and
Ta5+-ions occupy each half of the 2d-Wyckoff position. The
crystal structure of LAMT becomes rhombohedral with the
space group, R-3 above ~ 855°C. The unit cell volume
changes gradually as a function of temperature without any
abrupt jump. [1] Vaßen R., Jarligo M.O., Steinke T., Mack
D.E. and Stöver D. Surf. Coat. Technol., 2010, 205, 938.
[2] Guo R., Bhalla A.S. and Cross L.E. J. Appl. Phys., 1994,
75, 4704. [3] Tarvin R. and Davies P.K. J. Am. Ceram. Soc.,
2004, 87, 859. [4] Jarligo M.O., Mack D.E., Vaßen R. and
Stöver D. J. Therm. Spray Technol., 2009, 18, 187.[5]
Schlegel N., Sebold D., Sohn Y.J., Mauer G. and Vaßen R. J.
Therm. Spray Technol., 2015, 24, 1205.[6] Kim Y.I. and
Woodward P.M. Solid State Chem., 2007, 180, 2798.Keywords:
thermal barrier coatings, ordered double perovskite, in-situ
high-temperature XRD},
month = {Jul},
date = {2018-07-01},
organization = {The 16th European Powder Diffraction
Conference, Edinburgh (U.K.), 1 Jul
2018 - 4 Jul 2018},
subtyp = {Other},
cin = {IEK-1 / JARA-ENERGY},
cid = {I:(DE-Juel1)IEK-1-20101013 / $I:(DE-82)080011_20140620$},
pnm = {113 - Methods and Concepts for Material Development
(POF3-113)},
pid = {G:(DE-HGF)POF3-113},
typ = {PUB:(DE-HGF)24},
url = {https://juser.fz-juelich.de/record/850086},
}