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@ARTICLE{Jafari:886118,
author = {Jafari, Atefeh and Klobes, Benedikt and Sergueev, Ilya and
Moseley, Duncan H. and Manley, Michael E. and Dronskowski,
Richard and Deringer, Volker L. and Stoffel, Ralf P. and
Bessas, Dimitrios and Chumakov, Aleksandr I. and Rüffer,
Rudolf and Mahmoud, Abdelfattah and Bridges, Craig A. and
Daemen, Luke L. and Cheng, Yongqiang and Ramirez-Cuesta,
Anibal J. and Hermann, Raphael P.},
title = {{P}honon {S}pectroscopy in {A}ntimony and {T}ellurium
{O}xides},
journal = {The journal of physical chemistry / A},
volume = {124},
number = {39},
issn = {1520-5215},
address = {Washington, DC},
publisher = {Soc.},
reportid = {FZJ-2020-04281},
pages = {7869 - 7880},
year = {2020},
abstract = {α-Sb2O3 (senarmontite), β-Sb2O3 (valentinite), and
α-TeO2 (paratellurite) are compounds with pronounced
stereochemically active Sb and Te lone pairs. The
vibrational and lattice properties of each have been
previously studied but often lead to incomplete or
unreliable results due to modes being inactive in infrared
or Raman spectroscopy. Here, we present a study of the
relationship between bonding and lattice dynamics of these
compounds. Mössbauer spectroscopy is used to study the
structure of Sb in α-Sb2O3 and β-Sb2O3, whereas the
vibrational modes of Sb and Te for each oxide are
investigated using nuclear inelastic scattering, and further
information on O vibrational modes is obtained using
inelastic neutron scattering. Additionally, vibrational
frequencies obtained by density functional theory (DFT)
calculations are compared with experimental results in order
to assess the validity of the utilized functional. Good
agreement was found between DFT-calculated and experimental
density of phonon states with a $7\%$ scaling factor. The
Sb–O–Sb wagging mode of α-Sb2O3 whose frequency was not
clear in most previous studies is experimentally observed
for the first time at ∼340 cm–1. Softer lattice
vibrational modes occur in orthorhombic β-Sb2O3 compared to
cubic α-Sb2O3, indicating that the antimony bonds are
weakened upon transforming from the molecular α phase to
the layer-chained β structure. The resulting vibrational
entropy increase of 0.45 ± 0.1 kB/Sb2O3 at 880 K accounts
for about half of the α–β transition entropy. The
comparison of experimental and theoretical approaches
presented here provides a detailed picture of the lattice
dynamics in these oxides beyond the zone center and shows
that the accuracy of DFT is sufficient for future
calculations of similar material structures.},
cin = {JCNS-2 / PGI-4 / JARA-FIT},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {144 - Controlling Collective States (POF3-144) / 524 -
Controlling Collective States (POF3-524) / 6212 - Quantum
Condensed Matter: Magnetism, Superconductivity (POF3-621) /
6213 - Materials and Processes for Energy and Transport
Technologies (POF3-621) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-524 /
G:(DE-HGF)POF3-6212 / G:(DE-HGF)POF3-6213 /
G:(DE-HGF)POF3-6G4},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:32894948},
UT = {WOS:000577149400002},
doi = {10.1021/acs.jpca.0c05060},
url = {https://juser.fz-juelich.de/record/886118},
}