3 research outputs found
Synthesis of 4H-SrMnO<sub>3.0</sub> Nanoparticles from a Molecular Precursor and Their Topotactic Reduction Pathway Identified at Atomic Scale
Stoichiometric
4H-SrMnO<sub>3.0</sub> nanoparticles have been synthesized
from thermal decomposition of a new molecular heterometallic precursor
[SrMn(edta)(H<sub>2</sub>O)<sub>5</sub>]·<sup>3</sup>/<sub>2</sub>H<sub>2</sub>O whose crystal structure has been solved by single
crystal X-ray diffraction. From this precursor, highly homogeneous
4H-SrMnO<sub>3.0</sub> nanoparticles, with average particle size of
70 nm, are obtained. The agglomeration of these nanoparticles maintains
the sheet-assembling morphology of the metal–organic compound.
Local structural information, provided by atomically resolved microscopy
techniques, shows that 4H-SrMnO<sub>3.0</sub> nanoparticles exhibit
the same general structural features as the bulk material, although
structural disorder, due to edge dislocations, is observed. The nanometric
particle size enables a topotactic reduction process at low temperature
stabilizing a metastable 4H-SrMnO<sub>2.82</sub> phase. The oxygen
deficiency is accommodated through extra cubic layers breaking the
...chch... 4H-sequence. These defect areas are Mn<sup>3+</sup> rich,
as evidenced by high energy resolution EELS data. Magnetic characterization
of nano-SrMnO<sub>3.0</sub> shows significant variations with respect
to the bulk material. Besides the dominant antiferromagnetic interactions,
a weak ferromagnetic contribution as well as exchange bias and a glassy-like
component are present. After the reduction process, the stabilization
of Mn<sup>3+</sup> in the 4H-structure gives rise to magnetic anomalies
in the 40–60 K temperature range. The origin of such magnetic
features is discussed
SrMnO<sub>3</sub> Thermochromic Behavior Governed by Size-Dependent Structural Distortions
The influence of particle size in
both the structure and thermochromic
behavior of 4H-SrMnO<sub>3</sub> related perovskite is described.
Microsized SrMnO<sub>3</sub> suffers a structural transition from
hexagonal (<i>P</i>6<sub>3</sub>/<i>mmc</i>) to
orthorhombic (<i>C</i>222<sub>1</sub>) symmetry at temperature
close to 340 K. The orthorhombic distortion is due to the tilting
of the corner-sharing Mn<sub>2</sub>O<sub>9</sub> units building the
4H structural type. When temperature decreases, the distortion becomes
sharper reaching its maximal degree at ∼125 K. These structural
changes promote the modification of the electronic structure of orthorhombic
SrMnO<sub>3</sub> phase originating the observed color change. nano-SrMnO<sub>3</sub> adopts the ideal 4H hexagonal structure at room temperature,
the orthorhombic distortion being only detected at temperature below
170 K. A decrease in the orthorhombic distortion degree, compared
to that observed in the microsample, may be the reason why a color
change is not observed at low temperature (77 K)
Critical Influence of Redox Pretreatments on the CO Oxidation Activity of BaFeO<sub>3−δ</sub> Perovskites: An in-Depth Atomic-Scale Analysis by Aberration-Corrected and in Situ Diffraction Techniques
A BaFeO<sub>3−δ</sub> (δ ≈ 0.22) perovskite
was prepared by a sol–gel method and essayed as a catalyst
in the CO oxidation reaction. BaFeO<sub>3−δ</sub> (0.22
≤ δ ≤ 0.42) depicts a 6H perovskite hexagonal
structural type with Fe in both III and IV oxidation states and oxygen
stoichiometry accommodated by a random distribution of anionic vacancies.
The perovskite with the highest oxygen content, BaFeO<sub>2.78</sub>, proved to be more active than its lanthanide-based counterparts,
LnFeO<sub>3</sub> (Ln = La, Sm, Nd). Removal of the lattice oxygen
detected in both temperature-programmed oxidation (TPO) and reduction
(TPR) experiments at around 500 K and which leads to the complete
reduction of Fe<sup>4+</sup> to Fe<sup>3+</sup>, i.e. to BeFeO<sub>2.5</sub>, significantly decreases the catalytic activity, especially
in the low-temperature range. The analysis of thermogravimetric experiments
performed under oxygen and of TPR studies run under CO clearly support
the involvement of lattice oxygen in the CO oxidation on these Ba-Fe
perovskites, even at the lowest temperatures. Atomically resolved
images and chemical maps obtained using different aberration-corrected
scanning transmission electron microscopy techniques, as well as some
in situ type experiments, have provided a clear picture of the accommodation
of oxygen nonstoichiometry in these materials. This atomic-scale view
has revealed details of both the cation and anion sublattices of the
different perovskites that have allowed us to identify the structural
origin of the oxygen species most likely responsible for the low-temperature
CO oxidation activity