7 research outputs found
Morphology-Tuned Phase Transitions of Horseshoe Shaped BaTiO<sub>3</sub> Nanomaterials under High Pressure
Exploring new physical
properties of nanomaterials with special
morphology have been important topics in nanoscience and nanotechnology.
Here we report a morphology-tuned structural phase transition under
high pressure in the horseshoe shaped BaTiO<sub>3</sub> nanomaterials
with an average diameter of 26 ± 4 nm. A direct structural phase
transition from the tetragonal to the cubic phase without local rhombohedral
distortion was observed at about 7.7 GPa by in situ high-pressure
X-ray diffraction and Raman spectroscopy, which is clearly different
from the phase transition processes of the BaTiO<sub>3</sub> bulks
and nanoparticles. Additionally, bulk modulus of the tetragonal and
cubic phases were determined to be 125.0 and 211.7 GPa, respectively,
obviously smaller than the estimated values for BaTiO<sub>3</sub> nanoparticles
with the same grain size. Further analysis shows that the unique phase
transition process and the enhanced structural stability of the tetragonal
horseshoe shaped BaTiO<sub>3</sub> nanomaterials, may be attributed
to the similar axes compressibility. Comparing with the high-pressure
study on BaTiO<sub>3</sub> nanoparticles, this study suggests that
the morphology plays an important role in the pressure-induced phase
transition of BaTiO<sub>3</sub> nanomaterials
Pressure-induced enhancement and retainability of optoelectronic properties of NiPS<sub>3</sub>
Here, we report significant pressure-modulate optoelectronic properties of NiPS3. Upon compression, NiPS3 exhibited a photocurrent increase of five orders of magnitude over the initial value. Interestingly, when NiPS3 was finally decompressed to ambient conditions, the photocurrent could maintain a two-order-of-magnitude enhancement. In addition, the spectral response range was extended to the near-infrared spectral range (up to 1650 nm) under high pressure. Raman and XRD measurements and theoretical calculations revealed significant enhancement in both interlayer and intralayer interactions during compression, leading to a remarkable modulation of the optoelectronic properties. By applying pressure, giant enhancement of photocurrent and tunable spectral response range were achieved in NiPS3, which provides a potential way to modify the optoelectronic properties for materials.</p
Significant Enhancement of Optoelectronic Properties in CuInP<sub>2</sub>S<sub>6</sub> via Pressure-Induced Structural Phase Transition
Quaternary layered transition metal thiophosphate CuInP2S6 (CIPS) has attracted extensive research interest
because
of its outstanding optical and ferroelectric properties. Pressure-tuned
phase transition is an efficient method to regulate the properties
of functional materials in situ, yet there is still much to explore.
Herein, we studied the pressure-regulated optoelectronic properties
of CIPS and found a four-stage evolution of photoresponsivity under
compression. The photoresponse of CIPS barely changes with pressure
initially but increases dramatically above 4.2 GPa. Under further
compression, the photoresponse first shows a decrease above 7.5 GPa
and then a significant increase up to 23.5 GPa. Remarkably, the photoresponse
at the highest pressure enhances by two orders of magnitude compared
with the starting value. To investigate the origin of these abnormal
variations in CIPS, high-pressure UV–vis absorption, Raman,
and XRD measurements were conducted and a phase transition from Cc
to P3Ì…1m symmetry was found at approximately 4.0 GPa. We suggest
that the pressure-modulated optoelectronic properties in CIPS are
closely related to the conductivity change of CIPS caused by its structural
phase transition. Our study spotlights the outstanding pressure regulation
of optoelectronic properties in CIPS, which paves the way for modifying
the behavior of other optoelectronic materials
The Multifunctionality of Lanthanum–Strontium Cobaltite Nanopowder: High-Pressure Magnetic Studies and Excellent Electrocatalytic Properties for OER
Simultaneous study of magnetic and electrocatalytic properties
of cobaltites under extreme conditions expands the understanding of
physical and chemical processes proceeding in them with the possibility
of their further practical application. Therefore, La0.6Sr0.4CoO3 (LSCO) nanopowders were synthesized
at different annealing temperatures tann = 850–900 °C, and their multifunctional properties were
studied comprehensively. As tann increases,
the rhombohedral perovskite structure of the LSCO becomes more single-phase,
whereas the average particle size and dispersion grow. Co3+ and Co4+ are the major components. It has been found
that LSCO-900 shows two main Curie temperatures, TC1 and TC2, associated with
a particle size distribution. As pressure P increases,
average ⟨TC1⟩ and ⟨TC2⟩ increase from 253 and 175 K under
ambient pressure to 268 and 180 K under P = 0.8 GPa,
respectively. The increment of ⟨dTC/dP⟩ for the smaller and bigger particles
is sufficiently high and equals 10 and 13 K/GPa, respectively. The
magnetocaloric effect in the LSCO-900 nanopowder demonstrates an extremely
wide peak δTfwhm > 50 K that
can
be used as one of the composite components, expanding its working
temperature window. Moreover, all LSCO samples showed excellent electrocatalytic
performance for the oxygen evolution reaction (OER) process (overpotentials
of only 265–285 mV at a current density of 10 mA cm–2) with minimal η10 for LSCO-900. Based on the experimental
data, it was concluded that the formation of a dense amorphous layer
on the surface of the particles ensures high stability as a catalyst
(at least 24 h) during electrolysis in 1 M KOH electrolyte
Tuning the Flat Band in Bi<sub>2</sub>O<sub>2</sub>Se by Pressure to Induce Superconductivity
The discovery of superconductivity in twisted bilayer
graphene
has reignited enthusiasm in the field of flat-band superconductivity.
However, important challenges remain, such as constructing a flat-band
structure and inducing a superconducting state in materials. Here,
we successfully achieved superconductivity in Bi2O2Se by pressure-tuning the flat-band electronic structure.
Experimental measurements combined with theoretical calculations reveal
that the occurrence of pressure-induced superconductivity at 30 GPa
is associated with a flat-band electronic structure near the Fermi
level. Moreover, in Bi2O2Se, a van Hove singularity
is observed at the Fermi level alongside pronounced Fermi surface
nesting. These remarkable features play a crucial role in promoting
strong electron–phonon interactions, thus potentially enhancing
the superconducting properties of the material. These findings demonstrate
that pressure offers a potential experimental strategy for precisely
tuning the flat band and achieving superconductivity
Linear Tunability of the Band Gap and Two-Dimensional (2D) to Three-Dimensional (3D) Isostructural Transition in WSe<sub>2</sub> under High Pressure
Transition metal
dichalcogenides (TMDs) have recently gained tremendous interest for
use in electronic and optoelectronic applications. Unfortunately,
the electronic structure or band gap of most TMDs shows noncontinuously
tunable characteristics, which limits their application to energy-variable
optoelectronics. Thus, layered materials with better tunability in
their electronic structures and band gaps are desired. Herein, we
experimentally demonstrated that layered WSe<sub>2</sub> possessed
highly tunable transport properties under various pressures, with
a linearly decreasing band gap that culminates in metallization. Pressure
tuned the band gap of WSe<sub>2</sub> linearly, at a rate of 25 meV/GPa.
The high tunability of WSe<sub>2</sub> was attributed to the larger
electron orbitals of W<sup>2+</sup> and Se<sup>2–</sup> in
WSe<sub>2</sub> compared to the Mo<sup>2+</sup> and S<sup>2–</sup> in MoS<sub>2</sub>. WSe<sub>2</sub> underwent an isostructural phase
transition from a 2D layered structure to a 3D structure at approximately
51.7 GPa, where a conversion from van der Waals (vdW) to covalent-like
bonding was observed in the valence electron localization function
(ELF). Our results present an important advance toward controlling
the band structure of layered materials and suggest significant implications
for energy-variable optoelectronic devices via pressure engineering
Structural Phase Transition and Photoluminescence Properties of YF<sub>3</sub>:Eu<sup>3+</sup> Nanocrystals under High Pressure
High-pressure behaviors of YF<sub>3</sub>:Eu<sup>3+</sup> nanocrystals
with an average grain size of 40 nm were investigated by in situ high-pressure
synchrotron radiation X-ray diffraction measurements up to 31.1 GPa
at ambient temperature. The pressure-induced structural phase transition
starts at 11.8 GPa and completes at 23.3 GPa. YF<sub>3</sub>:Eu<sup>3+</sup> nanocrystals with a starting phase of orthorhombic structure
transform into a high-pressure phase, which is inferred to be hexagonal
structure. The high-pressure structure returned to the orthorhombic
phase after release of pressure. The transition pressure is enhanced
in nanosized YF<sub>3</sub>:Eu<sup>3+</sup> as compared to submicrometer
size samples, which is due to the surface energy differences between
submicrometer size and nanosized materials. The nanosized samples
of high-pressure phase were easier to compress with smaller bulk modulus
than the submicrometer size samples. The photoluminescence properties
of YF<sub>3</sub>:Eu<sup>3+</sup> have also been studied in the pressure
range from ambient pressure to 25.0 GPa at room temperature. Accompanied
by the structure transformation, the Eu<sup>3+</sup> ion luminescence
from <sup>5</sup>D<sub>0</sub> → <sup>7</sup>F<sub>1,2,3,4</sub> transition in YF<sub>3</sub>:Eu<sup>3+</sup> nanocrystals emerges
obvious changes, which indicate the variation of the local symmetry
of Eu<sup>3+</sup> ions