6 research outputs found
Low-Voltage Control of (Co/Pt)<sub><i>x</i></sub> Perpendicular Magnetic Anisotropy Heterostructure for Flexible Spintronics
The
trend of mobile Internet requires portable and wearable devices
as bio-device interfaces. Electric field control of magnetism is a
promising approach to achieve compact, light-weight, and energy-efficient
wearable devices. Within a flexible sandwich heterostructure, perpendicular
magnetic anisotropy switching was achieved <i>via</i> low-voltage
gating control of an ionic gel in mica/Ta/(Pt/Co)<sub><i>x</i></sub>/Pt/ionic gel/Pt, where (Pt/Co)<sub><i>x</i></sub> acted as a functional layer. By conducting <i>in situ</i> VSM, EPR, and MOKE measurements, a 1098 Oe magnetic anisotropy field
change was determined at the bending state with tensile strain, corresponding
to a magnetic anisotropy energy change of 3.16 × 10<sup>5</sup> J/m<sup>3</sup> and a giant voltage tunability coefficient of 0.79
× 10<sup>5</sup> J/m<sup>3</sup>·V. The low voltage and
strain dual control of magnetism on mica substrates enables tunable
flexible spintronic devices with an increased degree of manipulation
Low-Voltage Control of (Co/Pt)<sub><i>x</i></sub> Perpendicular Magnetic Anisotropy Heterostructure for Flexible Spintronics
The
trend of mobile Internet requires portable and wearable devices
as bio-device interfaces. Electric field control of magnetism is a
promising approach to achieve compact, light-weight, and energy-efficient
wearable devices. Within a flexible sandwich heterostructure, perpendicular
magnetic anisotropy switching was achieved <i>via</i> low-voltage
gating control of an ionic gel in mica/Ta/(Pt/Co)<sub><i>x</i></sub>/Pt/ionic gel/Pt, where (Pt/Co)<sub><i>x</i></sub> acted as a functional layer. By conducting <i>in situ</i> VSM, EPR, and MOKE measurements, a 1098 Oe magnetic anisotropy field
change was determined at the bending state with tensile strain, corresponding
to a magnetic anisotropy energy change of 3.16 × 10<sup>5</sup> J/m<sup>3</sup> and a giant voltage tunability coefficient of 0.79
× 10<sup>5</sup> J/m<sup>3</sup>·V. The low voltage and
strain dual control of magnetism on mica substrates enables tunable
flexible spintronic devices with an increased degree of manipulation
Low-Voltage Control of (Co/Pt)<sub><i>x</i></sub> Perpendicular Magnetic Anisotropy Heterostructure for Flexible Spintronics
The
trend of mobile Internet requires portable and wearable devices
as bio-device interfaces. Electric field control of magnetism is a
promising approach to achieve compact, light-weight, and energy-efficient
wearable devices. Within a flexible sandwich heterostructure, perpendicular
magnetic anisotropy switching was achieved <i>via</i> low-voltage
gating control of an ionic gel in mica/Ta/(Pt/Co)<sub><i>x</i></sub>/Pt/ionic gel/Pt, where (Pt/Co)<sub><i>x</i></sub> acted as a functional layer. By conducting <i>in situ</i> VSM, EPR, and MOKE measurements, a 1098 Oe magnetic anisotropy field
change was determined at the bending state with tensile strain, corresponding
to a magnetic anisotropy energy change of 3.16 × 10<sup>5</sup> J/m<sup>3</sup> and a giant voltage tunability coefficient of 0.79
× 10<sup>5</sup> J/m<sup>3</sup>·V. The low voltage and
strain dual control of magnetism on mica substrates enables tunable
flexible spintronic devices with an increased degree of manipulation
Ferroelectric Phase Transition Induced a Large FMR Tuning in Self-Assembled BaTiO<sub>3</sub>:Y<sub>3</sub>Fe<sub>5</sub>O<sub>12</sub> Multiferroic Composites
Yttrium
iron garnet (YIG) is of great importance in RF/microwave devices for
its low loss, low intrinsic damping, and high permeability. Nevertheless,
tuning of YIG-based multiferroics is still a challenge due to its
near-zero magnetostriction and the difficulty of building epitaxial
interface between ferromagnetic garnet and ferroelectric perovskite
phases. In this work, the vertically aligned heterostructure of YIG:BTO/STO(001)
with local epitaxial interface between BTO and YIG is well-constructed,
where the single crystal BTO pillars are embedded in YIG matrix. A
large magnetoelectric coupling effect that drives YIG’s FMR
shift up to 512 and 333 Oe (1–2 order greater than those of
all state-of-the-art progresses) is obtained through BTO ferroelectric
phase changes induced by temperature variation at 295 and 193 K, correspondingly.
This record high magnetoelectric tunability of YIG paves a way toward
thermal/electrical tunable YIG devices
Discovery of Enhanced Magnetoelectric Coupling through Electric Field Control of Two-Magnon Scattering within Distorted Nanostructures
Electric
field control of dynamic spin interactions is promising
to break through the limitation of the magnetostatic interaction based
magnetoelectric (ME) effect. In this work, electric field control
of the two-magnon scattering (TMS) effect excited by in-plane lattice
rotation has been demonstrated in a La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3</sub> (LSMO)/PbÂ(Mn<sub>2/3</sub>Nb<sub>1/3</sub>)-PbTiO<sub>3</sub> (PMN-PT) (011) multiferroic heterostructure. Compared with
the conventional strain-mediated ME effect, a giant enhancement of
ME effect up to 950% at the TMS critical angle is precisely determined
by angular resolution of the ferromagnetic resonance (FMR) measurement.
Particularly, a large electric field modulation of magnetic anisotropy
(464 Oe) and FMR line width (401 Oe) is achieved at 173 K. The electric-field-controllable
TMS effect and its correlated ME effect have been explained by electric
field modulation of the planar spin interactions triggered by spin–lattice
coupling. The enhancement of the ME effect at various temperatures
and spin dynamics control are promising paradigms for next-generation
voltage-tunable spintronic devices