6 research outputs found
Flexible Heteroepitaxy of CoFe<sub>2</sub>O<sub>4</sub>/Muscovite Bimorph with Large Magnetostriction
A bimorph
composed of ferrimagnetic cobalt ferrite (CoFe<sub>2</sub>O<sub>4</sub>, CFO) and flexible muscovite was fabricated via van der Waals epitaxy.
The combination of X-ray diffraction and transmission electron microscopy
was conducted to reveal the heteroepitaxy of the CFO/muscovite system.
The robust magnetic behaviors against mechanical bending were characterized
by hysteresis measurements and magnetic force microscopy, which maintain
a saturation magnetization (<i>M</i><sub>s</sub>) of ∼120–150
emu/cm<sup>3</sup> under different bending states. The large magnetostrictive
response of the CFO film was then determined by digital holographic
microscopy, where the difference of magnetostrction coefficient (Δλ)
is −104 ppm. The superior performance of this bimorph is attributed
to the nature of weak interaction between film and substrate. Such
a flexible CFO/muscovite bimorph provides a new platform to develop
next-generation flexible magnetic devices
A Strain-Driven Antiferroelectric-to-Ferroelectric Phase Transition in La-Doped BiFeO<sub>3</sub> Thin Films on Si
A strain-driven
orthorhombic (O) to rhombohedral (R) phase transition
is reported in La-doped BiFeO<sub>3</sub> thin films on silicon substrates.
Biaxial compressive epitaxial strain is found to stabilize the rhombohedral
phase at La concentrations beyond the morphotropic phase boundary
(MPB). By tailoring the residual strain with film thickness, we demonstrate
a mixed O/R phase structure consisting of O phase domains measuring
tens of nanometers wide within a predominant R phase matrix. A combination
of piezoresponse force microscopy (PFM), transmission electron microscopy
(TEM), polarization–electric field hysteresis loop (P–E
loop), and polarization maps reveal that the O-R structural change
is an antiferroelectric to ferroelectric (AFE-FE) phase transition.
Using scanning transmission electron microscopy (STEM), an atomically
sharp O/R MPB is observed. Moreover, X-ray absorption spectra (XAS)
and X-ray linear dichroism (XLD) measurements reveal a change in the
antiferromagnetic
axis orientation from out of plane (R-phase) to in plane (O-phase).
These findings provide direct evidence of spin-charge-lattice coupling
in La-doped BiFeO<sub>3</sub> thin films. Furthermore, this study
opens a new pathway to drive the AFE-FE O-R phase transition and provides
a route to study the O/R MPB in these films
Tuning Electronic Transport in a Self-Assembled Nanocomposite
Self-assembled nanocomposites with a high interface-to-volume ratio offer an opportunity to overcome limitations in current technology, where intriguing transport behaviors can be tailored by the choice of proper interactions of constituents. Here we integrated metallic perovskite oxide SrRuO<sub>3</sub>–wurzite semiconductor ZnO nanocomposites to investigate the room-temperature metal–insulator transition and its effect on photoresponse. We demonstrate that the band structure at the interface can be tuned by controlling the interface-to-volume ratio of the nanocomposites. Photoinduced carrier injection driven by visible light was detected across the nanocomposites. This work shows the charge interaction of the vertically integrated multiheterostructures by incorporating a controllable interface-to-volume ratio, which is essential for optimization of the design and functionality of electronic devices
Flexible Multiferroic Bulk Heterojunction with Giant Magnetoelectric Coupling <i>via</i> van der Waals Epitaxy
Magnetoelectric nanocomposites have
been a topic of intense research due to their profound potential in
the applications of electronic devices based on spintronic technology.
Nevertheless, in spite of significant progress made in the growth
of high-quality nanocomposite thin films, the substrate clamping effect
still remains a major hurdle in realizing the ultimate magnetoelectric
coupling. To overcome this obstacle, an alternative strategy of fabricating
a self-assembled ferroelectric–ferrimagnetic bulk heterojunction
on a flexible muscovite <i>via</i> van der Waals epitaxy is
adopted. In this study, we investigated the magnetoelectric coupling
in a self-assembled BiFeO<sub>3</sub> (BFO)–CoFe<sub>2</sub>O<sub>4</sub> (CFO) bulk heterojunction epitaxially grown on a flexible
muscovite substrate. The obtained heterojunction is composed of vertically
aligned multiferroic BFO nanopillars embedded in a ferrimagnetic CFO
matrix. Moreover, due to the weak interaction between the flexible
substrate and bulk heterojunction, the interface is incoherent and,
hence, the substrate clamping effect is greatly reduced. The phase-field
simulation model also complements our results. The magnetic and electrical
characterizations highlight the improvement in magnetoelectric coupling
of the BFO–CFO bulk heterojunction. A magnetoelectric coupling
coefficient of 74 mV/cm·Oe of this bulk heterojunction is larger
than the magnetoelectric coefficient reported earlier on flexible
substrates. Therefore, this study delivers a viable route of fabricating
a remarkable magnetoelectric heterojunction and yet flexible electronic devices
that are robust against extreme conditions with optimized performance
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
Giant Photoresponse in Quantized SrRuO<sub>3</sub> Monolayer at Oxide Interfaces
The
photoelectric effect in semiconductors is the main mechanism
for most modern optoelectronic devices, in which the adequate bandgap
plays the key role for acquiring high photoresponse. Among numerous
material categories applied in this field, the complex oxides exhibit
great possibilities because they present a wide distribution of band
gaps for absorbing light with any wavelength. Their physical properties
and lattice structures are always strongly coupled and sensitive to
light illumination. Moreover, the confinement of dimensionality of
the complex oxides in the heterostructures can provide more diversities
in designing and modulating the band structures. On the basis of this
perspective, we have chosen itinerary ferromagnetic SrRuO<sub>3</sub> as the model material, and fabricated it in one-unit-cell thickness
in order to open a small band gap for effective utilization of visible
light. By inserting this SrRuO<sub>3</sub> monolayer at the interface
of the well-developed two-dimensional electron gas system (LaAlO<sub>3</sub>/SrTiO<sub>3</sub>), the resistance of the monolayer can be
further revealed. In addition, a giant enhancement (>300%) of photoresponse
under illumination of visible light with power density of 500 mW/cm<sup>2</sup> is also observed. Such can be ascribed to the further modulation
of band structure of the SrRuO<sub>3</sub> monolayer under the illumination,
confirmed by cross-section scanning tunneling microscopy (XSTM). Therefore,
this study demonstrates a simple route to design and explore the potential
low dimensional oxide materials for future optoelectronic devices