3 research outputs found
Stabilization of Monodisperse, Phase-Pure MgFe<sub>2</sub>O<sub>4</sub> Nanoparticles in Aqueous and Nonaqueous Media and Their Photocatalytic Behavior
Monodisperse,
monocrystalline magnesium ferrite (MgFe<sub>2</sub>O<sub>4</sub>)
nanoparticles were synthesized phase purely by fast
nonaqueous microwave-assisted solution-phase synthesis. Colloidal
stabilization of the nanocrystals in nonaqueous media was realized
either in-situ during synthesis or postsynthetically by surface capping
with oleylamine and oleic acid. Phase transfer to aqueous media was
performed employing citric acid and betaine hydrochloride, resulting
in agglomerate-free dispersions of citrate- or betaine-functionalized
MgFe<sub>2</sub>O<sub>4</sub> nanocrystals. Furthermore, a one-step
synthesis of highly stable, water-dispersible colloids of MgFe<sub>2</sub>O<sub>4</sub> was achieved using polyvinylpyrrolidone as stabilizer.
Characterization of the as-synthesized and functionalized nanoparticles
was performed employing X-ray diffraction, UV–vis and infrared
spectroscopy, thermogravimetry, dynamic light scattering, and transmission
electron microscopy. Special focus was laid on phase purity, which
was thoroughly monitored using Raman microscopy/spectroscopy. Photocatalytic
reactions were performed to evaluate the use of such highly stable
ferrite colloids for solar energy conversion
Shape-Controlled CeO<sub>2</sub> Nanoparticles: Stability and Activity in the Catalyzed HCl Oxidation Reaction
CeO<sub>2</sub> is a promising catalyst for the HCl oxidation (Deacon
process) in order to recover Cl<sub>2</sub>. Employing shape-controlled
CeO<sub>2</sub> nanoparticles (cubes, octahedrons, rods) with facets
of preferential orientations ((100), (111), (110)), we studied the
activity and stability under two reaction conditions (harsh: Ar:HCl:O<sub>2</sub> = 6:2:2 and mild: Ar:HCl:O<sub>2</sub> = 7:1:2). It turns
out that both activity and stability are structure-sensitive. In terms
of space time yield (STY), the rods are the most active particles,
followed by the cubes and finally the octahedrons. This very same
trend is reconciled with the complete oxygen storage capacity (OSCc),
indicating a correlation between the observed activity STY and the
OSCc. The apparent activation energies are about 50 kJ/mol for cubes
and rods, while the octahedrons reveal an apparent activation energy
of 65 kJ/mol. The reaction order in O<sub>2</sub> is positive (0.26–0.32).
Under mild reaction conditions, all three morphologies are stable,
consistent with corresponding studies of CeO<sub>2</sub> powders and
CeO<sub>2</sub> nanofibers. Under harsh reaction conditions, however,
cubes and octahedrons are both instable, forming hydrated CeCl<sub>3</sub>, while rods are still stable. The present stability and activity
experiments in the catalytic HCl oxidation reaction over shape-controlled
CeO<sub>2</sub> nanoparticles may serve as benchmarks for future ab
initio studies of the catalyzed HCl oxidation reaction over well-defined
CeO<sub>2</sub> surfaces
Aqueous Sol–Gel Route toward Selected Quaternary Metal Oxides with Single and Double Perovskite-Type Structure Containing Tellurium
Highly crystalline SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub>, Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub>, and Ba<sub>2</sub>NiTeO<sub>6</sub> have been synthesized
by using a specially developed
sol–gel route methodology, reducing the time needed employing
solid-state routes and resulting in high reaction yield up to 75%.
These materials have been studied by X-ray powder diffraction (XRPD),
scanning and transmission electron microscopy, Raman spectroscopy,
and dielectric and magnetic measurements. At room temperature, the
crystal structure of SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub> is cubic, space group <i>Pm</i>3̅<i>m</i>, with <i>a</i> = 3.9373(2) Å, whereas Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub> crystallizes in the hexagonal crystal
system, space group <i>P</i>6<sub>3</sub>/<i>mmc</i>, <i>a</i> = 5.7691(4) Å, and <i>c</i> =
14.208(1) Å. The third studied perovskite Ba<sub>2</sub>NiTeO<sub>6</sub> crystallizes in the trigonal <i>R</i>3̅<i>m</i> space group with <i>a</i> = 5.7974(4) Å
and <i>c</i> = 28.599(2) Å. Based on structural characterization
results, the obtained single and double perovskite crystallites are
nearly in nanometer regime, ranging from 45 to 164 nm, building micrometer-sized
particles with visible well-faceted hexagonal morphology. Magnetic
measurements show the onset of ferrimagnetic ordering at relatively
high temperature of 667 K for the SrFe<sub>2/3</sub>Te<sub>1/3</sub>O<sub>3</sub>, whereas Ba<sub>3</sub>Fe<sub>2</sub>TeO<sub>9</sub> and Ba<sub>2</sub>NiTeO<sub>6</sub> show antiferromagnetic ordering
below 80 and 8.6 K, respectively. The measured room temperature dielectric
constants are in the range between 15 and 77