7 research outputs found
Strain-Driven Nanoscale Phase Competition near the AntipolarāNonpolar Phase Boundary in Bi<sub>0.7</sub>La<sub>0.3</sub>FeO<sub>3</sub> Thin Films
Complex-oxide
materials tuned to be near phase boundaries via chemistry/composition,
temperature, pressure, etc. are known to exhibit large susceptibilities.
Here, we observe a strain-driven nanoscale phase competition in epitaxially
constrained Bi<sub>0.7</sub>La<sub>0.3</sub>FeO<sub>3</sub> thin films
near the antipolarānonpolar phase boundary and explore the
evolution of the structural, dielectric, (anti)Āferroelectric, and
magnetic properties with strain. We find that compressive and tensile
strains can stabilize an antipolar PbZrO<sub>3</sub>-like <i>Pbam</i> phase and a nonpolar <i>Pnma</i> orthorhombic
phase, respectively. Heterostructures grown with little to no strain
exhibit a self-assembled nanoscale mixture of the two orthorhombic
phases, wherein the relative fraction of each phase can be modified
with film thickness. Subsequent investigation of the dielectric and
(anti)Āferroelectric properties reveals an electric-field-driven phase
transformation from the nonpolar phase to the antipolar phase. X-ray
linear dichroism reveals that the antiferromagnetic-spin axes can
be effectively modified by the strain-induced phase transition. This
evolution of antiferromagnetic-spin axes can be leveraged in exchange
coupling between the antiferromagnetic Bi<sub>0.7</sub>La<sub>0.3</sub>FeO<sub>3</sub> and a ferromagnetic Co<sub>0.9</sub>Fe<sub>0.1</sub> layer to tune the ferromagnetic easy axis of the Co<sub>0.9</sub>Fe<sub>0.1</sub>. These results demonstrate that besides chemical
alloying, epitaxial strain is an alternative and effective way to
modify subtle phase relations and tune physical properties in rare
earth-alloyed BiFeO<sub>3</sub>. Furthermore, the observation of antiferroelectric-antiferromagnetic
properties in the <i>Pbam</i> Bi<sub>0.7</sub>La<sub>0.3</sub>FeO<sub>3</sub> phase could be of significant scientific interest
and great potential in magnetoelectric devices because of its dual
antiferroic nature
Microbial Reduction of Arsenic-Doped Schwertmannite by <i>Geobacter sulfurreducens</i>
The fate of AsĀ(V) during microbial reduction by <i>Geobacter
sulfurreducens</i> of FeĀ(III) in synthetic arsenic-bearing schwertmannites
has been investigated. During incubation at pH7, the rate of biological
FeĀ(III) reduction increased with increasing initial arsenic concentration.
From schwertmannites with a relatively low arsenic content (<0.3
wt %), only magnetite was formed as a result of dissimilatory iron
reduction. However, bioreduction of schwertmannites with higher initial
arsenic concentrations (>0.79 wt %) resulted in the formation of
goethite.
At no stage during the bioreduction process did the concentration
of arsenic in solution exceed 120 Ī¼gL<sup>1</sup>, even for
a schwertmannite with an initial arsenic content of 4.13 wt %. This
suggests that the majority of the arsenic is retained in the biominerals
or by sorption at the surfaces of newly formed nanoparticles.Subtle differences in the As <i>K</i>-edge XANES spectra
obtained from biotransformation products are clearly related to the
initial arsenic content of the schwertmannite starting materials.
For products obtained from schwertmannites with higher initial As
concentrations, one dominant population of AsĀ(V) species bonded to
only two Fe atoms was evident. By contrast, schwertmannites with relatively
low arsenic concentrations gave biotransformation products in which
two distinctly different populations of AsĀ(V) persisted. The first
is the dominant population described above, the second is a minority
population characterized by AsĀ(V) bonded to four Fe atoms. Both XAS
and XMCD evidence suggest that the latter form of arsenic is that
taken into the tetrahedral sites of the magnetite.We conclude
that the majority population of AsĀ(V) is sorbed to
the surface of the biotransformation products, whereas the minority
population comprises AsĀ(V) incorporated into the tetrahedral sites
of the biomagnetite. This suggests that microbial reduction of highly
bioavailable AsĀ(V)-bearing FeĀ(III) mineral does not necessarily result
in the mobilization of the arsenic
A One-Pot Synthesis of Monodispersed Iron Cobalt Oxide and Iron Manganese Oxide Nanoparticles from Bimetallic Pivalate Clusters
Monodispersed iron cobalt oxide (Fe<sub>2</sub>CoO<sub>4</sub>)
and iron manganese oxide (Mn<sub>0.43</sub>Fe<sub>2.57</sub>O<sub>4</sub>) nanoparticles have been synthesized using bimetallic pivalate
clusters of [Fe<sub>2</sub>CoOĀ(O<sub>2</sub>C<sup>t</sup>Bu)<sub>6</sub>(HO<sub>2</sub>C<sup>t</sup>Bu)<sub>3</sub>] (<b>1</b>), Co<sub>4</sub>Fe<sub>2</sub>O<sub>2</sub>(O<sub>2</sub>C<sup>t</sup>Bu)<sub>10</sub>(MeCN)<sub>2</sub>] (<b>2</b>), and [Fe<sub>2</sub>MnOĀ(O<sub>2</sub>C<sup>t</sup>Bu)<sub>6</sub>(HO<sub>2</sub>C<sup>t</sup>Bu)<sub>3</sub>] (<b>3</b>) respectively as single source
precursors. The precursors were thermolyzed in a mixture of oleylamine
and oleic acid with either diphenyl ether or benzyl ether as solvent
at their respective boiling points of 260 or 300 Ā°C. The effect
of reaction time, temperature and precursor concentration (0.25 or
0.50 mmol) on the stoichiometry, phases or morphology of the nanoparticles
were studied. TEM showed that highly monodispersed spherical nanoparticles
of Fe<sub>2</sub>CoO<sub>4</sub> (3.6 Ā± 0.2 nm) and Mn<sub>0.43</sub>Fe<sub>2.57</sub>O<sub>4</sub> (3.5 Ā± 0.2 nm) were obtained
from 0.50 mmol of <b>1</b> or <b>3</b>, respectively at
260 Ā°C. The decomposition of the precursors at 0.25 mmol and
300 Ā°C revealed that larger iron cobalt oxide or iron manganese
oxide nanoparticles were obtained from <b>1</b> and <b>3</b>, respectively, whereas the opposite was observed for iron cobalt
oxide from <b>2</b> as smaller nanoparticles appeared. The reaction
time was investigated for the three precursors at 0.25 mmol by withdrawing
aliquots at 5 min, 15 min, 30 min, 1 h, and 2 h. The results obtained
showed that aliquots withdrawn at reaction times of less than 1 h
contain traces of iron oxide, whereas only pure cubic iron cobalt
oxide or iron manganese oxide was obtained after 1 h. Magnetic measurements
revealed that all the nanoparticles are superparamagnetic at room
temperature with high saturation magnetization values. XMCD confirmed
that in iron cobalt oxide nanoparticles, most of the Co<sup>2+</sup> cations are in the octahedral site. There is also evidence in the
magnetic measurements for considerable hysteresis (>1T) observed
at
5 K. EPMA analysis and ICP-OES measurements performed on iron cobalt
oxide nanoparticles obtained from [Fe<sub>2</sub>CoOĀ(O<sub>2</sub>C<sup>t</sup>Bu)<sub>6</sub>(HO<sub>2</sub>C<sup>t</sup>Bu)<sub>3</sub>] <b>(1)</b> revealed that stoichiometric Fe<sub>2</sub>CoO<sub>4</sub> was obtained only for 0.50 mmol precursor concentration.
All the nanoparticles were characterized by powder X-ray diffraction
(p-XRD), transmission electron microscopy (TEM), inductively coupled
plasma-optical emission spectroscopy (ICP-OES), electron probe microanalysis
(EPMA), X-ray magnetic circular dichroism (XMCD), and superconducting
quantum interference device (SQUID) magnetometry
Tc(VII) and Cr(VI) Interaction with Naturally Reduced Ferruginous Smectite from a Redox Transition Zone
FeĀ(II)-rich clay minerals found in
subsurface redox transition
zones (RTZs) can serve as important sources of electron equivalents
limiting the transport of redox-active contaminants. While most laboratory
reactivity studies are based on reduced model clays, the reactivity
of naturally reduced field samples remains poorly explored. Characterization
of the clay size fraction of a fine-grained unit from the RTZ interface
at the Hanford site, Washington, including mineralogy, crystal chemistry,
and FeĀ(II)/(III) content, indicates that ferruginous montmorillonite
is the dominant mineralogical component. Oxic and anoxic fractions
differ significantly in FeĀ(II) natural content, but Fe<sub>TOTAL</sub> remains constant, demonstrating no Fe loss during its reductionāoxidation
cyclings. At native pH of 8.6, the anoxic fraction, despite its significant
FeĀ(II), ā¼23% of Fe<sub>TOTAL</sub>, exhibits minimal reactivity
with TcO<sub>4</sub><sup>ā</sup> and CrO<sub>4</sub><sup>2ā</sup> and much slower reaction kinetics than those measured in studies
with biologically/chemically reduced model clays. Reduction capacity
is enhanced by added/sorbed FeĀ(II) (if FeĀ(II)<sub>SORBED</sub> >
8%
clay FeĀ(II)<sub>LABILE</sub>); however, the kinetics of this conceptually
surface-mediated reaction remain sluggish. Surface-sensitive Fe L-edge
X-ray absorption spectroscopy shows that FeĀ(II)<sub>SORBED</sub> and
the resulting reducing equivalents are not available in the outermost
few nanometers of clay surfaces. Slow kinetics thus appear related
to diffusion-limited access to electron equivalents retained within
the clay mineral structure
Ultralow Damping in Nanometer-Thick Epitaxial Spinel Ferrite Thin Films
Pure
spin currents, unaccompanied by dissipative charge flow, are
essential for realizing energy-efficient nanomagnetic information
and communications devices. Thin-film magnetic insulators have been
identified as promising materials for spin-current technology because
they are thought to exhibit lower damping compared with their metallic
counterparts. However, insulating behavior is not a sufficient requirement
for low damping, as evidenced by the very limited options for low-damping
insulators. Here, we demonstrate a new class of nanometer-thick ultralow-damping
insulating thin films based on design criteria that minimize orbital
angular momentum and structural disorder. Specifically, we show ultralow
damping in <20 nm thick spinel-structure magnesium aluminum ferrite
(MAFO), in which magnetization arises from Fe<sup>3+</sup> ions with
zero orbital angular momentum. These epitaxial MAFO thin films exhibit
a Gilbert damping parameter of ā¼0.0015 and negligible inhomogeneous
linewidth broadening, resulting in narrow half width at half-maximum
linewidths of ā¼0.6 mT around 10 GHz. Our findings offer an
attractive thin-film platform for enabling integrated insulating spintronics
Strain-Engineered Oxygen Vacancies in CaMnO<sub>3</sub> Thin Films
We
demonstrate a novel pathway to control and stabilize oxygen vacancies
in complex transition-metal oxide thin films. Using atomic layer-by-layer
pulsed laser deposition (PLD) from two separate targets, we synthesize
high-quality single-crystalline CaMnO<sub>3</sub> films with systematically
varying oxygen vacancy defect formation energies as controlled by
coherent tensile strain. The systematic increase of the oxygen vacancy
content in CaMnO<sub>3</sub> as a function of applied in-plane strain
is observed and confirmed experimentally using high-resolution soft
X-ray absorption spectroscopy (XAS) in conjunction with bulk-sensitive
hard X-ray photoemission spectroscopy (HAXPES). The relevant defect
states in the densities of states are identified and the vacancy content
in the films quantified using the combination of first-principles
theory and coreāhole multiplet calculations with holistic fitting.
Our findings open up a promising avenue for designing and controlling
new ionically active properties and functionalities of complex transition-metal
oxides via strain-induced oxygen-vacancy formation and ordering
Magnetic Mesocrystal-Assisted Magnetoresistance in Manganite
Mesocrystal, a new class of crystals
as compared to conventional
and well-known single crystals and polycrystalline systems, has captured
significant attention in the past decade. Recent studies have been
focused on the advance of synthesis mechanisms as well as the potential
on device applications. In order to create further opportunities upon
functional mesocrystals, we fabricated a self-assembled nanocomposite
composed of magnetic CoFe<sub>2</sub>O<sub>4</sub> mesocrystal in
Sr-doped manganites. This combination exhibits intriguing structural
and magnetic tunabilities. Furthermore, the antiferromagnetic coupling
of the mesocrystal and matrix has induced an additional magnetic perturbation
to spin-polarized electrons, resulting in a significantly enhanced
magnetoresistance in the nanocomposite. Our work demonstrates a new
thought toward the enhancement of intrinsic functionalities assisted
by mesocrystals and advanced design of novel mesocrystal-embedded
nanocomposites