3 research outputs found
Ferroelectricity, High Permittivity, and Tunability in Millimeter-Size Crack-Free Ba<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>TiO<sub>3</sub> Flexible Epitaxial Sheets
Flexible oxide sheets exhibiting
ferroelectricity and high permittivity
are crucial for the advancement of various emerging technologies.
However, achieving large-area crack-free flexible oxide sheets remains
difficult because oxides easily crack when their thicknesses are significantly
reduced. In this study, we focused on Ba1–xSrxTiO3 (BST), which
is an important material owing to its high permittivity and electric-field-induced
tunability. By employing an amorphous AlOx protective layer with a thickness greater than 10 nm, we successfully
fabricated millimeter-sized crack-free BST epitaxial sheets. In contrast,
the sheets fabricated without protective layers exhibited breakage.
In addition, we observed that a polycrystalline indium tin oxide layer
acted as a suitable bottom electrode. The BST sheet with a composition
of x = 0.25 exhibited excellent ferroelectric switching
behavior and minimal current leakage, even when used with electrodes
with a diameter of 100 μm. Furthermore, the BST sheet with a
composition of x = 0.5 simultaneously exhibited high
permittivity (εr ∼ 3500 at 10 kHz) and tunability
(56%), combining the desirable characteristics of both bulk and thin-film
materials. These improved dielectric properties are attributed to
the absence of substrate-induced strain, which is a characteristic
not observed in thin-film materials
Significant Suppression of Cracks in Freestanding Perovskite Oxide Flexible Sheets Using a Capping Oxide Layer
Flexible and functional perovskite oxide sheets with
high orientation
and crystallization are the next step in the development of next-generation
devices. One promising synthesis method is the lift-off and transfer
method using a water-soluble sacrificial layer. However, the suppression
of cracks during lift-off is a crucial problem that remains unsolved.
In this study, we demonstrated that this problem can be solved by
depositing amorphous Al2O3 capping layers on
oxide sheets. Using this simple method, over 20 mm2 of
crack-free, deep-ultraviolet transparent electrode La:SrSnO3 and ferroelectric Ba0.75Sr0.25TiO3 flexible sheets were obtained. By contrast, the sheets without any
capping layers broke. The obtained sheets showed considerable flexibility
and high functionality. The La:SrSnO3 sheet simultaneously
exhibited a wide bandgap (4.4 eV) and high electrical conductivity
(>103 S/cm). The Ba0.75Sr0.25TiO3 sheet exhibited clear room-temperature ferroelectricity with
a remnant polarization of 17 μC/cm2. Our findings
provide a simple transfer method for obtaining large, crack-free,
high-quality, single-crystalline sheets
Magnetic Phase Transition-Induced Modulation of Ferroelectric Properties in Hexagonal <i>R</i>FeO<sub>3</sub> (<i>R</i> = Tb and Ho)
Hexagonal rare-earth iron oxides (h-RFeO3) exhibit spontaneous magnetization and room-temperature
ferroelectricity
simultaneously. However, achieving a large magnetoelectric coupling
necessitates further exploration. Herein, we report the impact of
the magnetic phase transition on the ferroelectric properties of epitaxial h-RFeO3 (R = Tb and Ho) films
prepared by pulsed laser deposition. The metastable h-RFeO3 phase is successfully stabilized
with high crystallinity and low leakage current due to the ITO buffer
layer, making it possible to investigate the ferroelectric properties.
The h-TbFeO3 film exhibits a magnetic-field-induced
transition from antiferromagnetic (AFM) to weak ferromagnetic (wFM)
phases below 30 K, while also exhibiting ferroelectricity at 300 K.
The dielectric constants change with the magnetic phase transition,
demonstrating hysteresis in the magnetocapacitance. In contrast, the h-HoFeO3 film exhibits antiferroelectric-like
behavior and an AFM–wFM phase transition.
Notably, the h-HoFeO3 film shows a rapid
increase in the remnant polarization during the AFM–wFM phase
transition accompanied by an increase in the ferroelectric component.
Considering the strong connection between the antiferroelectric behavior
in the h-RFeO3 system and the ferroelectric
domain wall motion, this considerable modification of ferroelectric
properties during the magnetic phase transition is probably due to
the faster movement of the ferroelectric domain walls in the wFM phase
induced by the clamping effect. Our findings indicate the effectiveness
of magnetic phase transitions in enhancing the magnetoelectric coupling,
particularly when utilizing domain wall clamping properties
