3 research outputs found
Coexistence of High Magnetization and Anisotropy with Non-monotonic Particle Size Effect in Ferromagnetic PrMnO<sub>3</sub> Nanoparticles
Instances
of the coexistence of high ferromagnetic magnetization
with large anisotropy are scarce in the rare-earth manganite family.
In manganites, high magnetizations are compromised with small coercivity
and vice versa. Using nonaqueous sol–gel techniques, the undoped
PrMnO<sub>3</sub> nanoparticles with oxygen nonstoichiometry were
rendered with exceptional ferromagnetic character. While ∼40
nm sized nanoparticles had magnetization of 84 emu/g and coercivity
of 885 Oe with 50 kOe sweeping field, the bulk 2 μm sized particles
showed a magnetization of 51 emu/g albeit with a higher coercivity
of 2000 Oe. These parameters are so far the highest among manganite
systems with similarly sized particles. The competition between the
ferromagnetic and antiferromagnetic phases both at the particle core
and at the grain boundaries resulted in a non-monotonous trend of
magnetic properties between 20, 40, and 2 μm particles. The
sudden increase of coercivity toward lower temperatures was a result
of the freezing of random spins at the surface of the strongly interacting
nanoparticles which also increased the magnetic anisotropy. These
results are of prime significance since the coexistence of such a
large magnetization with high coercivity was rarely observed in pristine
or doped manganites
Surfactant-Mediated Resistance to Surface Oxidation in MnO Nanostructures
The intrinsic physical properties
of nanostructures of metals and
their oxides are altered when they are prone to surface oxidation
in ambient atmosphere. To overcome this limitation, novel synthesis
methodologies are required. In this study, solid octahedral shapes
of MnO limit the inward oxygen diffusion compared to that of the MnO-nanoparticle-assembled
octahedra. In addition to morphology control, which restricts the
thickness of the Mn<sub>3</sub>O<sub>4</sub> surface layer, the binding
chemistry of the surfactants plays an essential role. For example,
the Mn<sub>3</sub>O<sub>4</sub> surface layer is 0.4 nm thinner with
trioctylphosphine oxide than with trioctylamine as the surfactant.
The nanostructures were prepared by varying the surfactants, surfactant-to-precursor
molar ratio, accelerating agent, and reaction heating rate. The surface
oxidation of MnO nano-octahedra was probed by Rietveld analysis of
X-ray diffraction patterns and X-ray photoelectron spectroscopy and
characterized by magnetic measurements, as the presence of ferrimagnetic
Mn<sub>3</sub>O<sub>4</sub> shell on the antiferromagnetic MnO core
provides an exchange coupling at the core–shell interface.
Thicker the Mn<sub>3</sub>O<sub>4</sub> shell, higher is the exchange-biased
hysteresis loop shift
Maneuvering the Physical Properties and Spin States To Enhance the Activity of La–Sr–Co–Fe–O Perovskite Oxide Nanoparticles in Electrochemical Water Oxidation
Perovskite
oxides have attracted considerable attention as durable electrocatalysts
for metal–air batteries and fuel cells due to their precedence
in oxygen electrocatalysis in spite of the complexities involved with
their crystal structure, spin states, and physical properties. Here
we report optimization of the activity of a model perovskite system
La<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>Co<sub>1–<i>y</i></sub>Fe<sub><i>y</i></sub>O<sub>3−δ</sub> (LSCF; <i>x</i> = 0.301, <i>y</i> = 0.298, and δ = 0.05–0.11) toward electrochemical
water oxidation (OER) by altering the calcination temperature of the
nonaqueous sol–gel synthesized nanoparticles (NPs). Our results
show that improved OER activity is the result of a synergism between
its morphology, surface area, electrical conductivity, and spin state
of the active transition metal site. With an e<sub>g</sub> orbital
occupancy of 1.26, the interconnected ∼90 nm LSCF NPs prepared
at 975 °C (LSCF-975) outperforms the other distinguishable LSCF
morphologies, requiring 440 mV overpotential to achieve 10 mA/cm<sup>2</sup>, a performance comparable to the best-performing perovskite
oxide electrocatalysts. While the interconnected NP morphology increases
the propensity of electronic conduction across crystalline grain boundaries,
the morphology-tuned high spin Co<sup>3+</sup> ions increases the
probability of binding reaction intermediates at the available surface
sites. Density functional theory based work function modeling further
demonstrates that LSCF-975 is the most favorable OER catalyst among
others in terms of a moderate work function and Fermi energy level
facilitating the adsorption and desorption of reaction intermediates