30 research outputs found
Molecular Insights into Early Nuclei and Interfacial Mismatch during Vapor Deposition of Hybrid Perovskites on Titanium Dioxide Substrate
Theoretical
understanding of the nucleus structures of hybrid perovskites,
such as those of the prototypical methylammonium lead triiodide (MAPbI<sub>3</sub>), can greatly improve the deposited thin film quality and
the resulting optoelectronic device performance. In this paper, we
report a systematic molecular dynamics simulation study on nucleation
and interfacial mismatch during the vapor deposition of MAPbI<sub>3</sub> on the TiO<sub>2</sub> substrate under different ionic precursor
(PbI<sub>2</sub> and MAI salts) compositions and temperatures. Despite
significant anisotropic lattice mismatches, small defects are observed
at the TiO<sub>2</sub>/[MAI]<sup>0</sup> interface due to intermediate
electrostatic attractions between I and Ti atoms, while very strong
electrostatic attractions between Pb and O atoms lead to significant
defects at the TiO<sub>2</sub>/[PbI<sub>2</sub>]<sup>0</sup> interface.
From the vapor deposition simulations, we identify PbI<sub>4</sub><sup>2â</sup> tetrahedra, PbI<sub>5</sub><sup>3â</sup> pyramids, and PbI<sub>6</sub><sup>4â</sup> octahedra as dominant
polyhedral building blocks of early MAPbI<sub>3</sub> nuclei. Specifically,
the PbI<sub>5</sub><sup>3â</sup> pyramids dominate over other
polyhedra and could be a good candidate for converting into PbI<sub>6</sub><sup>4â</sup> octahedra upon further crystallization.
We further identify early MAPbI<sub>3</sub> nuclei built upon well-connected
PbI<sub><i>x</i></sub> polyhedral clusters and finally locate
the efficient early MAPbI<sub>3</sub> nuclei based on sufficient amounts
of surrounding MA<sup>+</sup> cations. The populations of these early
nuclei increase rapidly with increasing the MAI composition, suggesting
that potential improvements in film quality could be introduced by
depositing more MAI salts or MA<sup>+</sup> cations, a finding consistent
with experiments. Although the impact from temperature is weaker than
that from composition, the optimal temperature for nucleation is found
to decrease with increasing the precursor composition PbI<sub>2</sub>/MAI. Finally, the TiO<sub>2</sub> substrate leads to layered structures
of ionic species close to its surface, but such ordering does not
seem to promote prenucleation, which poses a need for the new design
of substrates that are more compatible with PbI<sub>6</sub><sup>4â</sup>-based early nuclei
Reactive Molecular Dynamics Simulations of Biomass Pyrolysis and Combustion under Various Oxidative and Humidity Environments
Biomass,
as a renewable carbon neutral energy source with abundant
reserves, is a good candidate for future energy supplies. In this
paper, a simplified biomass model composed of cellulose, hemicellulose,
and lignin, described by a carefully selected reactive force field
(ReaxFF), is investigated using molecular dynamics (MD) simulations.
The pyrolysis and combustion processes of the biomass under different
temperatures and oxidative and humidity conditions, are studied. We
find that the individual products from the pyrolysis of the three
biomass components are similar, including H<sub>2</sub>O, H<sub>2</sub>, CO, CO<sub>2</sub>, and small organic molecules. The calculated
activation energies for CâC bond dissociation are 34.53, 26.08,
and 16.23 kJ mol<sup>â1</sup>, respectively, for cellulose,
hemicellulose, and lignin, consistent with the trend in experiments.
Interestingly, light tar (C5â13) production reaches a maximum
under intermediate temperatures, which could be further explored to
optimize the production of light tar as liquid fuels. Compared to
biomass pyrolysis in vacuum, hydrothermal treatment makes the CâC
bonds more difficult to dissociate, but CâO bonds more vulnerable
due to stronger attacks from ·H radicals. Higher H<sub>2</sub> concentration is produced under the H<sub>2</sub>O atmosphere, while
more CO is formed under the mixed H<sub>2</sub>O/O<sub>2</sub> atmosphere.
During biomass combustion, CO<sub>2</sub> mainly comes from the cracking
and reforming of ·COOH and ·CHO radical groups or directly
from CO oxidation. We also observe that during biomass combustion,
the formation of CO is facilitated at higher temperatures, whereas
CO<sub>2</sub> production is favored at lower temperatures. More rapid
decomposition and oxidation of biomass during combustion occur under
fuel-lean conditions compared to fuel-rich conditions. Finally, more
H<sub>2</sub>O and fewer H<sub>2</sub> molecules are generated during
the combustion process under the O<sub>2</sub>/CO<sub>2</sub> atmosphere
when increasing the concentration of CO<sub>2</sub>. On the basis
of this theoretical study, a better understanding of the radicals,
intermediates, products, and reaction kinetics involved in biomass
pyrolysis and combustion could be achieved
Molecular Gibbs Surface Excess and CO<sub>2</sub>âHydrate Density Determine the Strong Temperature- and Pressure-Dependent Supercritical CO<sub>2</sub>âBrine Interfacial Tension
In
CO<sub>2</sub> geological storage, the interfacial tension (IFT) between
supercritical CO<sub>2</sub> and brine is critical for the storage
capacitance design to prevent CO<sub>2</sub> leakage. IFT relies not
only on the interfacial molecule properties but also on the environmental
conditions at different storage sites. In this paper, supercritical
CO<sub>2</sub>âNaCl solution systems are modeled at 343â373
K and 6â35 MPa under the salinity of 1.89 mol/L using molecular
dynamics simulations. After computing and comparing the molecular
density profile across the interface, the atomic radial distribution
function, the molecular orientation distribution, the molecular Gibbs
surface excess (derived from the molecular density profile), and the
CO<sub>2</sub>-hydrate number density under the above environmental
conditions, we confirm that only the molecular Gibbs surface excess
of CO<sub>2</sub> molecules and the CO<sub>2</sub>-hydrate number
density correlate strongly with the temperature- and pressure-dependent
IFTs. We also compute the populations of two distinct CO<sub>2</sub>-hydrate structures (T-type and H-type) and attribute the observed
dependence of IFTs to the dominance of the more stable, surfactant-like
T-type CO<sub>2</sub>-hydrates at the interface. On the basis of these
new molecular mechanisms behind IFT variations, this study could guide
the rational design of suitable injecting environmental pressure and
temperature conditions. We believe that the above two molecular-level
metrics (Gibbs surface excess and hydrate number density) are of great
fundamental importance for understanding the supercritical CO<sub>2</sub>âwater interface and engineering applications in geological
CO<sub>2</sub> storage
Ionic Effects on Supercritical CO<sub>2</sub>âBrine Interfacial Tensions: Molecular Dynamics Simulations and a Universal Correlation with Ionic Strength, Temperature, and Pressure
For
geological CO<sub>2</sub> storage in deep saline aquifers,
the interfacial tension (IFT) between supercritical CO<sub>2</sub> and brine is critical for the storage security and design of the
storage capacitance. However, currently, no predictive model exists
to determine the IFT of supercritical CO<sub>2</sub> against complex
electrolyte solutions involving various mixed salt species at different
concentrations and compositions. In this paper, we use molecular dynamics
(MD) simulations to investigate the effect of salt ions on the incremental
IFT at the supercritical CO<sub>2</sub>âbrine interface with
respect to that at the reference supercritical CO<sub>2</sub>âwater
interface. Supercritical CO<sub>2</sub>âNaCl solution, CO<sub>2</sub>âCaCl<sub>2</sub> solution and CO<sub>2</sub>-(NaCl+CaCl<sub>2</sub>) mixed solution systems are simulated at 343 K and 20 MPa
under different salinities and salt compositions. We find that the
valence of the cations is the primary contributor to the variation
in IFT, while the Lennard-Jones potentials for the cations pose a
smaller impact on the IFT. Interestingly, the incremental IFT exhibits
a general linear correlation with the ionic strength in the above
three electrolyte systems, and the slopes are almost identical and
independent of the solution types. Based on this finding, a universal
predictive formula for IFTs of CO<sub>2</sub>âcomplex electrolyte
solution systems is established, as a function of ionic strength,
temperature, and pressure. The predicted IFTs using the established
formula agree perfectly (with a high statistical confidence level
of âŒ96%) with a wide range of experimental data for CO<sub>2</sub> interfacing with different electrolyte solutions, such as
those involving MgCl<sub>2</sub> and Na<sub>2</sub>SO<sub>4</sub>.
This work provides an efficient and accurate route to directly predict
IFTs in supercritical CO<sub>2</sub>âcomplex electrolyte solution
systems for practical engineering applications, such as geological
CO<sub>2</sub> sequestration in deep saline aquifers and other interfacial
systems involving complex electrolyte solutions
Non-Invasive <i>In Vivo</i> Imaging of Near Infrared-labeled Transferrin in Breast Cancer Cells and Tumors Using Fluorescence Lifetime FRET
<div><p>The conjugation of anti-cancer drugs to endogenous ligands has proven to be an effective strategy to enhance their pharmacological selectivity and delivery towards neoplasic tissues. Since cell proliferation has a strong requirement for iron, cancer cells express high levels of transferrin receptors (TfnR), making its ligand, transferrin (Tfn), of great interest as a delivery agent for therapeutics. However, a critical gap exists in the ability to non-invasively determine whether drugs conjugated to Tfn are internalized into target cells <i>in vivo</i>. Due to the enhanced permeability and retention (EPR) effect, it remains unknown whether these Tfn-conjugated drugs are specifically internalized into cancer cells or are localized non-specifically as a result of a generalized accumulation of macromolecules near tumors. By exploiting the dimeric nature of the TfnR that binds two molecules of Tfn in close proximity, we utilized a Förster Resonance Energy Transfer (FRET) based technique that can discriminate bound and internalized Tfn from free, soluble Tfn. In order to non-invasively visualize intracellular amounts of Tfn in tumors through live animal tissues, we developed a novel near infrared (NIR) fluorescence lifetime FRET imaging technique that uses an active wide-field time gated illumination platform. In summary, we report that the NIR fluorescence lifetime FRET technique is capable of non-invasively detecting bound and internalized forms of Tfn in cancer cells and tumors within a live small animal model, and that our results are quantitatively consistent when compared to well-established intensity-based FRET microscopy methods used in <i>in vitro</i> experiments.</p></div
DataSheet1_Comprehensive pan-cancer analysis and the regulatory mechanism of AURKA, a gene associated with prognosis of ferroptosis of adrenal cortical carcinoma in the tumor micro-environment.ZIP
Background: The only curative option for patients with locally or locally advanced adrenocortical carcinoma is primary tumor curative sexual resection (ACC). However, overall survival remains low, with most deaths occurring within the first 2Â years following surgery. The 5-year survival rate after surgery is less than 30%. As a result, more accurate prognosis-related predictive biomarkers must be investigated urgently to detect patientsâ disease status after surgery.Methods: Data from FerrDb were obtained to identify ferroptosis-related genes, and ACC gene expression profiles were collected from the GEO database to find differentially expressed ACC ferroptosis-related genes using differential expression analysis. The DEFGs were subjected to Gene Ontology gene enrichment analysis and KEGG signaling pathway enrichment analysis. PPI network building and predictive analysis were used to filter core genes. The expression of critical genes in ACC pathological stage and pan-cancer was then investigated. In recent years, immune-related factors, DNA repair genes, and methyltransferase genes have been employed in diagnosing and prognosis of different malignancies. Cancer cells are mutated due to DNA repair genes, and highly expressed DNA repair genes promote cancer. Dysregulation of methyltransferase genes and Immune-related factors, which are shown to be significantly expressed in numerous malignancies, also plays a crucial role in cancer. As a result, we investigated the relationship of AURKA with immunological checkpoints, DNA repair genes, and methyltransferases in pan-cancer.Result: The DEGs found in the GEO database were crossed with ferroptosis-related genes, yielding 42 differentially expressed ferroptosis-related genes. Six of these 42 genes, particularly AURKA, are linked to the prognosis of ACC. AURKA expression was significantly correlated with poor prognosis in patients with multiple cancers, and there was a significant positive correlation with Th2 cells. Furthermore, AURKA expression was positively associated with tumor immune infiltration in Lung adenocarcinoma (LUAD), Liver hepatocellular carcinoma (LIHC), Sarcoma (SARC), Esophageal carcinoma (ESCA), and Stomach adenocarcinoma (STAD), but negatively correlated with the immune score, matrix score, and calculated score in these tumors. Further investigation into the relationship between AURKA expression and immune examination gene expression revealed that AURKA could control the tumor-resistant pattern in most tumors by regulating the expression level of specific immune examination genes.Conclusion: AURKA may be an independent prognostic marker for predicting ACC patient prognosis. AURKA may play an essential role in the tumor microenvironment and tumor immunity, according to a pan-cancer analysis, and it has the potential to be a predictive biomarker for multiple cancers.</p
NIR fluorescence lifetime FRET of TfnR-Tfn complexes in normal vs. cancer cells using time-domain, wide-field macroscopic imaging <i>in vitro.</i>
<p>Fluorescence lifetime analysis of TfnR-Tfn complexes using NIR FRET pair AF700âAF750 and a time-domain, wide-field macroscopic imaging system. (A) T47D (left panels) and HMECs (right panels) were internalized with AF700-Tfn (donor) or AF750-Tfn (acceptor) in increasing A:D ratios of 0â¶1, 1â¶4, 1â¶3, 1â¶2, 1â¶1, 2â¶1, and 3â¶1 in a 96-well format. The first column on the left indicates the pixel intensity (PI) of donor fluorophores (AF700-Tfn) and the subsequent decrease in intensity as the ratio of acceptor molecules (AF750-Tfn) increase due to quenching. Short component lifetimes (SL) measured in picoseconds (ps) are shown in the second column, indicating a high sensitivity and uniform detection despite the heterogeneity of donor intensities in the sample (Table S3 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>). The columns on the left indicate the relative abundance of NFD populations and FD populations. Each image shows 20Ă20 pixels with 0.5 mm/pixel size. (B) Quantification of donors participating in FRET events are shown as %FD and show a positive relationship relative to increasing proportion of acceptor molecules in both T47D and HMECs (Table S4 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>). (C) The %FD in relation to acceptor levels show an independent relationship as seen in FRET results using visible FRET detected by confocal microscopy (Table S5 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>). (D) Sensitivity of FD% is consistent across 1Ă10<sup>5</sup> to 1Ă10<sup>4</sup> cells (Table S6 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>). PIâ=âpixel intensity, SLâ=âshort lifetime, NFD%â=ânon-FRET Donor%, FD%â=âFRET Donor%. Error bars indicate standard deviation.</p
Electrostatically Tuned Microdomain Morphology and Phase-Dependent Ion Transport Anisotropy in Single-Ion Conducting Block Copolyelectrolytes
Block
copolyelectrolytes are solid-state single-ion conductors
which phase separate into ubiquitous microdomains to enable both high
ion transference number and structural integrity. Ion transport in
these charged block copolymers highly depends on the nanoscale microdomain
morphology; however, the influence of electrostatic interactions on
morphology and ion diffusion pathways in block copolyelectrolytes
remains an obscure feature. In this paper, we systematically predict
the phase diagram and morphology of diblock copolyelectrolytes using
a modified dissipative particle dynamics simulation framework, considering
both explicit electrostatic interactions and ion diffusion dynamics.
Various experimentally controllable conditions are considered here,
including block volume fraction, FloryâHuggins parameter, block
charge fraction or ion concentration, and dielectric constant. Boundaries
for microphase transitions are identified based on the computed structure
factors, mimicking small-angle X-ray scattering patterns. Furthermore,
we develop a novel âdiffusivity tensorâ approach to
predict the degree of anisotropy in ion diffusivity along the principal
microdomain orientations, which leads to high-throughput mapping of
phase-dependent ion transport properties. Inclusion of ions leads
to a significant leftward and upward shift of the phase diagram due
to ion-induced excluded volume, increased entropy of mixing, and reduced
interfacial tension between dissimilar blocks. Interestingly, we discover
that the inverse topology gyroid and cylindrical phases are ideal
candidates for solid-state electrolytes in metal-ion batteries. These
inverse phases exhibit an optimal combination of high ion conductivity,
well-percolated diffusion pathways, and mechanical robustness. Finally,
we find that higher dielectric constants can lead to higher ion diffusivity
by reducing electrostatic cohesions between the charged block and
counterions to facilitate ion diffusion across block microdomain interfaces.
This work significantly expands the design space for emerging block
copolyelectrolytes and motivates future efforts to explore inverse
phases to avoid engineering hurdles of aligning microdomains or removing
grain boundaries
Accuracy of fluorescence lifetime FRET using NIR fluorophores <i>in vivo.</i>
<p>Decreased fluorescence lifetime due to FRET is detectable through living mice. (A) Mice are injected with matrigel resuspended âŒ1Ă10<sup>6</sup> cells pre-internalized with Tfn conjugated with NIR dyes at A:D ratios of donor only, 1â¶2, 1â¶1, and 2â¶1 and imaged. Images show donor intensities on the left column followed by measurements of the short lifetime component (Table S11 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>), which also shows uniformity. The NFD and FD species are shown on the following columns to the right. Each image shows 60Ă60 pixels with 0.5 mm/pixel size. (B) Quantification of the FD% shows a robust linear increase in proportion to an increasing amount of AF750-Tfn (acceptor). These results indicate that the macroscopic imaging system employed is capable of determining FRET-mediated lifetime changes of donor fluorophores in cells through living animal tissues. Error bars indicate standard deviation.</p
NIR fluorescence lifetime FRET of TfnR-Tfn complexes in normal vs. cancer cells using wide-field macroscopic imaging <i>in vivo.</i>
<p>Fluorescence lifetime FRET is detected between AF700-Tfn (donor) and AF750-Tfn (acceptor) in T47D cells within a live mouse. (A) Mice injected with âŒ1.5Ă10<sup>6</sup> T47D cells internalized with various ratios of NIR dyes conjugated to Tfn are shown. In the top two rows, donor AF700-Tfn is held constant at 40 ”g/ml and imaged. Pixel intensity (PI) is shown on the first column on the left of the donor fluorophore. Short component lifetime (SL) of the donor dye (Table S7 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>) is uniform among a varied intensity of donor dye. The next two columns on the right show the population of non-FRET donor (NFD) and FRET-donor (FD), respectively, showing an increase upon introduction of the AF750-Tfn (acceptor). Similar results are shown with Tfn-AF700 (donor) at 20 ”g/ml. Each image shows 60Ă60 pixels with 0.5 mm/pixel size. (B) Results of the FD% show similar results between the two amounts, and also showing similar increases in FD in relation to the addition of AF750-Tfn acceptor (Tables S8âS10 in <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0080269#pone.0080269.s001" target="_blank">File S1</a>). Error bars indicate standard deviation. PIâ=âpixel intensity, SLâ=âshort lifetime, NFD%â=ânon-FRET Donor%, FD%â=âFRET Donor%.</p