16 research outputs found
First-Principles Screening of All-Inorganic Lead-Free ABX<sub>3</sub> Perovskites
In
order to address an all-inorganic halide lead-free perovskite
for potential photovoltaic applications, we carried out first-principles
calculations of bandgaps of 260 all-inorganic halide perovskites belonging
to the class ABX<sub>3</sub>, with A = Li, Na, K, Rb, Cs, B = Pb,
Sn, and Ge, and X = F, Cl, Br, I. Three most common crystal symmetries
were chosen, including cubic, tetragonal, and two orthorhombic phases.
The bandgap exhibited increase with the decreasing of the anions radius
(I, Br, Cl, F) and lowering the symmetry of the structures. With consideration
of multiple factors forming perovskites, we reported three all-inorganic
lead-free halides perovskites including cubic-KSnCl<sub>3</sub>, cubic-RbSnCl<sub>3</sub>, and trigonal-NaGeBr<sub>3</sub> as candidates with desirable
bandgap (1.24–1.44 eV) for photovoltaic applications
Direct Visualization of the Formation about Inverse Catalyst CoO<sub>(<i>x</i>)</sub>/Pt(111)
In
nonhomogeneous catalysts, the catalyst formation process plays
a critical role in determining catalytic performance. However, there
is limited research on visualizing the synthesis process on the atomic
scale. In this study, we successfully grew cobaltocene films on Pt(111)
under ultrahigh vacuum (UHV) conditions using an ultralow temperature
atomic layer deposition technique. To simulate real-world conditions,
we investigated the effects of oxygen and temperature on cobaltocene
(CoCp2) thin films by introducing oxygen into an ultrahigh
vacuum chamber. The characterization of the formation process was
conducted in detail by scanning tunneling microscopy (STM). Additionally,
we elaborate on the entire process of treating Pt single crystals
by using the E-beam method. Given the significance of cobaltocene
adsorption in the overall process, we investigated its behavior at
different exposure times. At an exposure time of 30 s, cobaltocene
was observed to be dispersed on the surface as atomic clusters. With
longer exposure times, the surface of Pt(111) became fully covered
by cobaltocene molecules, reaching a height of about 70 pm. Subsequently,
through oxidation annealing in 1 × 10–7 mbar
O2 at 673 K, amorphous cobaltocene films were transformed
into CoO(x) islands with crystal structures.
To assess the stability of CoO(x) islands
on Pt(111) at different temperatures, ab initio molecular dynamics
(AIMD) and density functional theory (DFT) calculations were performed.
Molecular dynamics simulations were performed on the two heterostructures
at 623 and 673 K, respectively. After 2000 fs cycles, both the energy
and temperature gradually stabilized following a brief oscillation,
eventually reaching equilibrium
Boosting the Self-Trapped Exciton Emission in Cs<sub>2</sub>NaYCl<sub>6</sub> Double Perovskite Single Crystals and Nanocrystals
Halide double perovskites have aroused substantial research
interest
because of their unique optical properties and intriguing flexibility
for various compositional adjustments. Herein, we report the synthesis
and photophysics of rare-earth element yttrium (Y)-based double perovskite
single crystals (SCs) and nanocrystals (NCs). The pristine Cs2NaYCl6 bulk SCs exhibit a weak sky-blue emission
with a low photoluminescence quantum yield (PLQY) of 7.68% based on
the self-trapped exciton (STE), while no PL emission was observed
for NCs. Excitingly, the STE emission of SCs and NCs is greatly enhanced
via Sb3+ doping. The optimized Cs2NaYCl6:Sb3+ SCs and NCs exhibit high PLQYs up to 82.5%
and 51.8%, respectively. Theoretical calculations and charge-carrier
dynamic studies demonstrate that the giant emission enhancement after
Sb3+ doping is related with the enhancement of the sensitization
of the emissive STE states, the passivating of the nonradiative carrier
trapping processes, and the regulation of carrier–phonon coupling
Computational Design and Experimental Validation of Enzyme Mimicking Cu-Based Metal–Organic Frameworks for the Reduction of CO<sub>2</sub> into C<sub>2</sub> Products: C–C Coupling Promoted by Ligand Modulation and the Optimal Cu–Cu Distance
While
extensive research has been conducted on the conversion of
CO2 to C1 products, the synthesis of C2 products still strongly depends on the Cu electrode. One main issue
hindering the C2 production on Cu-based catalysts is the
lack of an appropriate Cu–Cu distance to provide the ideal
platform for the C–C coupling process. Herein, we identify
a lab-synthesized artificial enzyme with an optimal Cu–Cu distance,
named MIL-53 (Cu) (MIL= Materials of Institute Lavoisier), for CO2 conversion by using a density functional theory method. By
substituting the ligands in the porous MIL-53 (Cu) nanozyme with functional
groups from electron-donating NH2 to electron-withdrawing
NO2, the Cu–Cu distance and charge of Cu can be
significantly tuned, thus modulating the adsorption strength of CO2 that impacts the catalytic activity. MIL-53 (Cu) decorated
with a COOH-ligand is found to be located at the top of a volcano-shaped
plot and exhibits the highest activity and selectivity to reduce CO2 to CH3CH2OH with a limiting potential
of only 0.47 eV. In addition, experiments were carried out to successfully
synthesize COOH-decorated MIL-53(Cu) to prove its high catalytic performance
for C2 production, which resulted in a −55.5% faradic
efficiency at −1.19 V vs RHE, which is much higher than the
faradic efficiency of the benchmark Cu electrode of 35.7% at −1.05
V vs RHE. Our results demonstrate that the biologically inspired enzyme
engineering approach can redefine the structure–activity relationships
of nanozyme catalysts and can also provide a new understanding of
the catalytic mechanisms in natural enzymes toward the development
of highly active and selective artificial nanozymes
Low Threshold Two-Photon-Pumped Amplified Spontaneous Emission in CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> Microdisks
Two-photon-pumped amplified spontaneous
emission (ASE) of CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> microdisks
(MDs) were investigated by using femtosecond laser system. Low threshold
at 2.2 mJ cm<sup>–2</sup> was obtained. Also, emission spectral
tunability from 500 to 570 nm was demonstrated by synthesis the mixed
halide perovskite MDs. The spatial effect of photoluminescence (PL)
properties under one-photon and two-photon excitation were also studied
by means of two-photon laser scanning microscope (TPLSM) and time-resolved
PL spectroscopy. It was found that the band to band emission of near-surface
regions and photocarriers’ diffusion from near-surface regions
to interior regions is significant for one-photon excitation. By contrast,
reabsorption of emission under two-photon excitation plays a major
role in the emission properties of the MDs. These results will give
a more comprehensive understanding of the nonlinear effect of CH<sub>3</sub>NH<sub>3</sub>PbBr<sub>3</sub> single crystals
Paper-Fiber-Activated Triplet Excitons of Carbon Nanodots for Time-Resolved Anti-counterfeiting Signature with Artificial Intelligence Authentication
The easy-to-imitate character of a personal signature
may cause
significant economy loss due to the lack of speed and strength information.
In this work, we report a time-resolved anti-counterfeiting signature
strategy with artificial intelligence (AI) authentication based on
the designed luminescent carbon nanodot (CND) ink, whose triplet excitons
can be activated by the bonding between the paper fibers and the CNDs.
Paper fibers can bond with the CNDs through multiple hydrogen bonds,
and the activated triplet excitons release photons for about 13 s;
thus, the speed and strength of the signature are recorded through
recording the changes in luminescence intensity over time. The background
noise from commercial paper fluorescence is completely suppressed,
benefiting from the long phosphorescence lifetime of the CNDs. In
addition, a reliable AI authentication method with quick response
based on a convolutional neural network is developed, and 100% identification
accuracy of the signature based on the CND ink is achieved, which
is higher than that of the signature with commercial ink (78%). This
strategy can also be expanded for painting, calligraphy identification
Additional file 1 of Mechanisms of Bushen Tiaoxue Granules against controlled ovarian hyperstimulation-induced abnormal morphology of endometrium based on network pharmacology
Additional file 1: Table S1. Composition of the BTG. Table S2. Identification of chemical components in BTG. Table S3. Affinity of ingredients with potential targets. Figure S1. The blood drug concentration of kaempferol following BTG administration. Kaempferol standard was obtained from MedChemExpress (USA) with a purity of 99.86% (HY-14590). An appropriate amount of kaempferol was added to 75% methanol to prepare a stock solution of 200 μg/mL for the mixed control solution. Upon usage, it was sequentially diluted to obtain concentration gradient solutions. Utilizing the same 50 female SD rats as employed in the in vivo experiment, two rats constituted the blank control group, while the remaining 48 rats were divided into treatment groups, each consisting of 6 rats. The treatment groups received oral gavage of BTG at 3.27 g/kg for 3 consecutive days, while the blank control group received an equivalent volume of physiological saline using the same procedure. Prior to the final dosing, the rats were fasted for 12 hours but allowed access to water. Blood samples were collected from the abdominal aorta of the rats at 8 time intervals post administration (10 min, 20 min, 30 min, 1 h, 2 h, 4 h, 8 h, 12 h) after anesthetizing the rats using 1% pentobarbital sodium. The blood samples were centrifuged at 4°C, 3500 rpm for 10 min, and the supernatant was analyzed. Following the UPLC-MS analysis method described earlier, the peak areas of the analyte and internal standard were recorded to calculate the blood drug concentrations at each time point. Figure S2. The impact of BTG administration on rat liver and kidney function. The serum levels of (A) ALT, (B) AST, (C) CREA, (D) UA, and (E) UREA in each group of rats were measured using microplate assays. The assay kits were obtained from Nanjing Jiancheng Bioengineering Institute (China)
Constructing Sensitive and Fast Lead-Free Single-Crystalline Perovskite Photodetectors
We developed a high-performance
photodetector based on (CH<sub>3</sub>NH<sub>3</sub>)<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> (MA<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub>)
microsingle crystals (MSCs).
The MA<sub>3</sub>Sb<sub>2</sub>I<sub>9</sub> single crystals exhibit
a low-trap state density of ∼10<sup>10</sup> cm<sup>–3</sup> and a long carrier diffusion length reaching 3.0 μm, suggesting
its great potential for optoelectronic applications. However, the
centimeter single crystal (CSC)-based photodetector exhibits low responsivity
(10<sup>–6</sup> A/W under 1 sun illumination) due to low charge-carrier
collection efficiency. By constructing the MSC photodetector with
efficient charge-carrier collection, the responsivity can be improved
by three orders of magnitude (under 1 sun illumination) and reach
40 A/W with monochromatic light (460 nm). Furthermore, the MSC photodetectors
exhibit fast response speed of <1 ms, resulting in a high gain
of 108 and a gain-bandwidth product of 10<sup>5</sup> Hz. These numbers
are comparable to the lead-perovskite single-crystal-based photodetectors
(C<sub>6</sub>H<sub>5</sub>C<sub>2</sub>H<sub>4</sub>NH<sub>3</sub>)<sub>2</sub>GeI<sub>4</sub>: A Layered Two-Dimensional Perovskite with Potential for Photovoltaic Applications
Recently,
two-dimensional organic–inorganic perovskites
have attracted increasing attention due to their unique photophysical
properties and high stability. Here we report a lead-free, two-dimensional
perovskite, (PEA)<sub>2</sub>GeI<sub>4</sub> (PEA = C<sub>6</sub>H<sub>5</sub>(CH<sub>2</sub>)<sub>2</sub>NH<sub>3</sub><sup>+</sup>). Structural
characterization demonstrated that this 2D perovskite structure is
formed with inorganic germanium iodide planes separated by organic
PEAI layers. (PEA)<sub>2</sub>GeI<sub>4</sub> has a direct band gap
of 2.12 eV, in agreement with 2.17 eV obtained by density functional
theory (DFT) calculations, implying that it is suitable for a tandem
solar cell. (PEA)<sub>2</sub>GeI<sub>4</sub> luminesces at room-temperature
with a moderate lifetime, exhibiting good potential for photovoltaic
applications. In addition, 2D (PEA)<sub>2</sub>GeI<sub>4</sub> is
more stable than 3D CH<sub>3</sub>NH<sub>3</sub>GeI<sub>3</sub> in
air, owing to the presence of a hydrophobic organic long chain. This
work provides a direction for the development of 2D Ge-based perovskites
with potential for photovoltaic applications