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@ARTICLE{Shiratori:61312,
author = {Shiratori, Y. and Magrez, A. and Fischer, W. and Pithan, C.
and Waser, R.},
title = {{T}emperature-induced phase transitions in micro- submicro-
and nanocrystalline {N}a{N}b{O}3},
journal = {The journal of physical chemistry / C},
volume = {111},
issn = {1932-7447},
address = {Washington, DC},
publisher = {Soc.},
reportid = {PreJuSER-61312},
pages = {18493},
year = {2007},
note = {Record converted from VDB: 12.11.2012},
abstract = {Phase transitions in micro-, submicro-, and nanocrystalline
NaNbO3 were investigated by temperature-tuning Raman
spectroscopy and X-ray powder diffraction method. Three
powders with different average particle size showed
successive phase transitions within the measured temperature
range from -150 to 450 degrees C. The temperature
characteristics of Raman active phonons in
n-ticrocrystalline NaNbO3 corresponded the one reported for
bulk NaNbO3, which transforms with increasing temperature
from the ferroelectric N into the antiferroelectric P phase
and finally above 373 degrees C (T-s3) into the
antiferroeletric R phase. Submicrocrystalline NaNbO3, which
takes the noncentrosymmetric orthorhombic Pmc2(1) structure
at room temperature, transformed into a pseudocubic
structure at 333 degrees C (TO). Nanocrystalline NaNbO3
showed a diffused phase transition from an orthorhombic Pmma
structure to a high-temperature phase at around 180 degrees
C (T-s2). For micro- and submicrocrystalline NaNbO3,
hysteretic phase transition behavior was found for the
temperature characteristics of specific phonons. On the
other hand, the characteristics obtained for nanocrystalline
NaNbO3 were much more diffused and did not show any
hysteretic effect. Crystal structure refinements of the
X-ray powder diffraction patterns using the Rietveld method
demonstrated a hysteretic deformation of the a-b plane for
microcrystalline NaNbO3 around T-3 and of the b-c plane for
submicrocrystalline NaNbO3 around T-s3. The temperature
dependence of the primitive perovskite volumes showed a very
small hysteresis for microcrystalline NaNbO3 but a clear one
for submicrocrystalline NaNbO3. Lattice distortion of the
submicrocrystalline Pmc2(1) structure from a cubic
perovskite lattice induced a particularly large contraction
of parameter c around T-s3 with increasing temperature,
which resulted in a decrease of the primitive cell volume.
This transition showed a first-order type character, which
may relate to a ferroelectric-antiferroelectric transition.
Rearrangement of the NbO6 octahedra induces a transition
from an orthorhombic into a pseudocubic structure.},
keywords = {J (WoSType)},
cin = {IFF-6 / JARA-FIT},
ddc = {540},
cid = {I:(DE-Juel1)VDB786 / $I:(DE-82)080009_20140620$},
pnm = {Kondensierte Materie},
pid = {G:(DE-Juel1)FUEK414},
shelfmark = {Chemistry, Physical / Nanoscience $\&$ Nanotechnology /
Materials Science, Multidisciplinary},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000251615500008},
doi = {10.1021/jp0738053},
url = {https://juser.fz-juelich.de/record/61312},
}