40 research outputs found
Inverse Design of Nanoclusters for Light-Controlled CO<sub>2</sub>–HCOOH Interconversion
With
global push of hydrogen economy, efficient scenarios for hydrogen
storage, transportation, and generation are indispensable. Here we
devise a strategy for controllable hydrogen fuel storage and retrieval
via light-switched CO2-to-HCOOH interconversion. To realize
it, palladium sulfide nanocluster catalysts with multiple specific
functionalities are directly searched by our home-developed inverse
design approach based on genetic algorithm (IDOGA) and ab
initio calculations. Over 500 low-energy PdxSy (x + y ≤ 30) clusters are sieved through a multiobjective
function combining stability, activity, optical absorption, and reduction
capability of photocarriers. The structure–property relationships
and key factors governing the trade-off among these stringent criteria
are disclosed. Finally, 14 candidate PdxSy clusters with proper sulfidation degree
and high stability in an aqueous environment have been screened. Our
IDOGA program provides a general approach for inverse search of nanoclusters
with any designated elemental compositions and functionalities for
any device applications
Transition-Metal Interlink Neural Network: Machine Learning of 2D Metal–Organic Frameworks with High Magnetic Anisotropy
Two-dimensional (2D) metal–organic framework (MOF)
materials
with large perpendicular magnetic anisotropy energy (MAE) are important
candidates for high-density magnetic storage. The MAE-targeted high-throughput
screening of 2D MOFs is currently limited by the time-consuming electronic
structure calculations. In this study, a machine learning model, namely,
transition-metal interlink neural network (TMINN) based on a database
with 1440 2D MOF materials is developed to quickly and accurately
predict MAE. The well-trained TMINN model for MAE successfully captures
the general correlation between the geometrical configurations and
the MAEs. We explore the MAEs of 2583 other 2D MOFs using our trained
TMINN model. From these two databases, we obtain 11 unreported 2D
ferromagnetic MOFs with MAEs over 35 meV/atom, which are further demonstrated
by the high-level density functional theory calculations. Such results
show good performance of the extrapolation predictions of TMINN. We
also propose some simple design rules to acquire 2D MOFs with large
MAEs by building a Pearson correlation coefficient map between various
geometrical descriptors and MAE. Our developed TMINN model provides
a powerful tool for high-throughput screening and intentional design
of 2D magnetic MOFs with large MAE
Transition-Metal Interlink Neural Network: Machine Learning of 2D Metal–Organic Frameworks with High Magnetic Anisotropy
Two-dimensional (2D) metal–organic framework (MOF)
materials
with large perpendicular magnetic anisotropy energy (MAE) are important
candidates for high-density magnetic storage. The MAE-targeted high-throughput
screening of 2D MOFs is currently limited by the time-consuming electronic
structure calculations. In this study, a machine learning model, namely,
transition-metal interlink neural network (TMINN) based on a database
with 1440 2D MOF materials is developed to quickly and accurately
predict MAE. The well-trained TMINN model for MAE successfully captures
the general correlation between the geometrical configurations and
the MAEs. We explore the MAEs of 2583 other 2D MOFs using our trained
TMINN model. From these two databases, we obtain 11 unreported 2D
ferromagnetic MOFs with MAEs over 35 meV/atom, which are further demonstrated
by the high-level density functional theory calculations. Such results
show good performance of the extrapolation predictions of TMINN. We
also propose some simple design rules to acquire 2D MOFs with large
MAEs by building a Pearson correlation coefficient map between various
geometrical descriptors and MAE. Our developed TMINN model provides
a powerful tool for high-throughput screening and intentional design
of 2D magnetic MOFs with large MAE
Inverse Design of Nanoclusters for Light-Controlled CO<sub>2</sub>–HCOOH Interconversion
With
global push of hydrogen economy, efficient scenarios for hydrogen
storage, transportation, and generation are indispensable. Here we
devise a strategy for controllable hydrogen fuel storage and retrieval
via light-switched CO2-to-HCOOH interconversion. To realize
it, palladium sulfide nanocluster catalysts with multiple specific
functionalities are directly searched by our home-developed inverse
design approach based on genetic algorithm (IDOGA) and ab
initio calculations. Over 500 low-energy PdxSy (x + y ≤ 30) clusters are sieved through a multiobjective
function combining stability, activity, optical absorption, and reduction
capability of photocarriers. The structure–property relationships
and key factors governing the trade-off among these stringent criteria
are disclosed. Finally, 14 candidate PdxSy clusters with proper sulfidation degree
and high stability in an aqueous environment have been screened. Our
IDOGA program provides a general approach for inverse search of nanoclusters
with any designated elemental compositions and functionalities for
any device applications
Table_1_Hydrated Sodium Ion Clusters [Na+(H2O)n (n = 1–6)]: An ab initio Study on Structures and Non-covalent Interaction.DOCX
Structural, thermodynamic, and vibrational characteristics of water clusters up to six water molecules incorporating a single sodium ion [Na+(H2O)n (n = 1–6)] are calculated using a comprehensive genetic algorithm combined with density functional theory on global search, followed by high-level ab initio calculation. For n ≥ 4, the coordinated water molecules number for the global minimum of clusters is 4 and the outer water molecules connecting with coordinated water molecules by hydrogen bonds. The charge analysis reveals the electron transfer between sodium ions and water molecules, providing an insight into the variations of properties of O–H bonds in clusters. Moreover, the simulated infrared (IR) spectra with anharmonic correction are in good agreement with the experimental results. The O–H stretching vibration frequencies show redshifts comparing with a free water molecule, which is attributed to the non-covalent interactions, including the ion–water interaction, and hydrogen bonds. Our results exhibit the comprehensive geometries, energies, charge, and anharmonic vibrational properties of Na+(H2O)n (n = 1–6), and reveal a deeper insight of non-covalent interactions.</p
Structures and Spectroscopic Properties of F<sup>–</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> with <i>n</i> = 1–10 Clusters from a Global Search Based On Density Functional Theory
Using a genetic algorithm
incorporated in density functional theory,
we explore the ground state structures of fluoride anion–water
clusters F<sup>–</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> with <i>n</i> = 1–10. The F<sup>–</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> clusters prefer structures
in which the F<sup>–</sup> anion remains at the surface of
the structure and coordinates with four water molecules, as the F<sup>–</sup>(H<sub>2</sub>O)<sub><i>n</i></sub> clusters
have strong F<sup>–</sup>–H<sub>2</sub>O interactions
as well as strong hydrogen bonds between H<sub>2</sub>O molecules.
The strong interaction between the F<sup>–</sup> anion and
adjacent H<sub>2</sub>O molecule leads to a longer O–H distance
in the adjacent molecule than in an individual water molecule. The
simulated infrared (IR) spectra of the F<sup>–</sup>(H<sub>2</sub>O)<sub>1–5</sub> clusters obtained via second-order
vibrational perturbation theory (VPT2) and including anharmonic effects
reproduce the experimental results quite well. The strong interaction
between the F<sup>–</sup> anion and water molecules results
in a large redshift (600–2300 cm<sup>–1</sup>) of the
adjacent O–H stretching mode. Natural bond orbital (NBO) analysis
of the lowest-energy structures of the F<sup>–</sup>(H<sub>2</sub>O)<sub>1–10</sub> clusters illustrates that charge
transfer from the lone pair electron orbital of F<sup>–</sup> to the antibonding orbital of the adjacent O–H is mainly
responsible for the strong interaction between the F<sup>–</sup> anion and water molecules, which leads to distinctly different geometric
and vibrational properties compared with neutral water clusters
Rational Design of Full-Color Fluorescent C<sub>3</sub>N Quantum Dots
Carbon-based
quantum dots (QDs) exhibit unique photoluminescence
due to size-dependent quantum confinement, giving rise to fascinating
full-color emission properties. Accurate emission calculations using
time-dependent density functional theory are a time-costing and expensive
process. Herein, we employed an artificial neural network (ANN) combined
with statistical learning to establish the relationship between geometrical/electronic
structures of ground states and emission wavelength for C3N QDs. The emission energy of these QDs can be doubly modulated by
size and edge effects, which are governed by the number of C4N2 rings and the CH group, respectively. Moreover, these
two structural characteristics also determine the phonon vibration
mode of C3N QDs to harmonize the emission intensity and
lifetime of hot electrons in the electron–hole recombination
process, as indicated by nonadiabatic molecular dynamics simulation.
These computational results provide a general approach to atomically
precise design the full-color fluorescent carbon-based QDs with targeted
functions and high performance
Rational Design of Full-Color Fluorescent C<sub>3</sub>N Quantum Dots
Carbon-based
quantum dots (QDs) exhibit unique photoluminescence
due to size-dependent quantum confinement, giving rise to fascinating
full-color emission properties. Accurate emission calculations using
time-dependent density functional theory are a time-costing and expensive
process. Herein, we employed an artificial neural network (ANN) combined
with statistical learning to establish the relationship between geometrical/electronic
structures of ground states and emission wavelength for C3N QDs. The emission energy of these QDs can be doubly modulated by
size and edge effects, which are governed by the number of C4N2 rings and the CH group, respectively. Moreover, these
two structural characteristics also determine the phonon vibration
mode of C3N QDs to harmonize the emission intensity and
lifetime of hot electrons in the electron–hole recombination
process, as indicated by nonadiabatic molecular dynamics simulation.
These computational results provide a general approach to atomically
precise design the full-color fluorescent carbon-based QDs with targeted
functions and high performance
Structure Evolution of Transition Metal-doped Gold Clusters M@Au<sub>12</sub> (M = 3d–5d): Across the Periodic Table
The
comprehensive genetic algorithm (CGA) incorporated with density
functional theory (DFT) calculations were used for a global search
of the potential energy surfaces of M@Au12 (M = 3d–5d)
clusters. The feasibility of the revTPSS functional was confirmed
by comparison between experimental and calculated data such as bond
lengths and vibrational frequencies of transition metal dimers. We
found the ground state structures of Mo/W@Au12 clusters
to be the perfect icosahedron cage. The V/Nb/Ta/Tc/Re@Au12 clusters were found to have the distorted icosahedron cages owing
to Jahn–Teller effects. The lowest energy structures of Sc/Ti/Cr/Mn/Fe/Co/Ru/Rh/Ir@Au12 have the perfect or distorted magnetic cuboctahedron cages,
which can be explained by a 14-electron rule in a cuboctahedral ligand
field (M2+@Au122–). Y/Zr/La/Hf@Au12 clusters have the half-cage ground states, while Ni/Cu/Zn/Pt/Ag/Cd/Pd/Au/HgAu12 clusters have oblate ground states. The scalar relativistic
X2C method combined with revTPSS/TZP were used to calculate the energy
difference between the magnetic cuboctahedron ground state and the
icosahedron isomers of Cr@Au12 using energy decomposition
analysis-natural orbitals for chemical valence. The magnetic M2+@Au122– model was found to significantly
enhance the d orbital interactions of transition metal atoms and reduce
Pauli repulsion, resulting in magnetic cuboctahedra as the more stable
structures
Typing versus texting and manual versus cell phone calculator wrist motion.
Maximum medial extension and range of motion (ROM) and minimum medial extension (A) and female maximum lateral extension and ROM (B) while texting or typing, and maximum medial extension, maximum lateral extension, and lateral extension ROM while using a cell phone or manual calculator (C, least squares mean ± SEM). Columns with different letters within each comparison are significantly different (p<0.05).</p
