28 research outputs found
Valence Electron Density-Dependent Pseudopermittivity for Nonlocal Effects in Optical Properties of Metallic Nanoparticles
The peak positions
of localized surface plasmonic resonance (LSPR)
are strongly dependent on the sizes of metallic nanoparticles. TDDFT
calculations have shown a remarkable size effect for metallic nanoparticles
smaller than 1 nm, because it could account for fully nonlocal effects.
Due to the high resource consumption of TDDFT, several semiquantum
approaches have been proposed to reduce the computation time while
addressing nonlocal effects, and it is still desirable to introduce
new ideas into this area since physical origins of related fields
are not completely known yet. In this work, we took account of both
spilling out of s-band electrons and the screening effect of d-band
electrons in the LSPR phenomena and developed a model using pseudopermittivity
to describe several quantum mechanical effects that contribute to
nonlocal effects in LSPR. With incorporation of machine learning,
this model is capable of calculating the optical response of large
nanostructures above the nanometer scale. Besides successful prediction
for different metallic nanoparticle monomers, the tunneling effect
occurring in dimers can also be well described by using the concept
of pseudopermittivity. The employing of pseudopermittivity and machine
learning is expected to achieve both high accuracy and high efficiency
in quantum plasmonics. It provides a new ideology in the simulation
of wave–matter interactions
Widening the Spectral Range of Ultrahigh Field Enhancement by Efficient Coupling of Localized to Extended Plasmons and Cavity Resonances in Grating Geometry
Excitation
of localized via extended plasmons was shown recently
to reveal ultrahigh electromagnetic field (EM) enhancement when optimum
coupling is obtained in the prism configuration. Using grating coupling,
one expects several advantages over the prism scheme such as being
planar, more compact, and most important the possibility of tuning
the spectral range over which the enhancement occurs. In this work
we show that via gratings coupling the EM field enhancement can be
up to 3 orders of magnitude higher than that obtained using free space
excitation of localized surface plasmons (LSPs). Furthermore, the
spectral range over which the ultrahigh enhancement achieved becomes
wider by tuning the grating parameters. The cavity resonances generated
by thick enough gratings couple to the LSPs producing ultrahigh local
enhancement and play an important role in widening the spectral range
to cover the range 400–2000 nm. This is important for solar
energy harvesting and improving the efficiency of infrared optoelectronic
devices. Having the periodic NPs arrangement on top of the grating
was found to be very significant not only under transverse magnetic
(TM) polarization but also under transverse electric (TE) polarization,
thus reducing the dependence on the polarization
Quantitative Prediction of Position and Orientation for Platonic Nanoparticles at Liquid/Liquid Interfaces
Because of their intrinsic geometric
structure of vertices, edges,
and facets, Platonic nanoparticles are promising materials in plasmonics
and biosensing. Their position and orientation often play a crucial
role in determining the resultant assembly structures at a liquid/liquid
interface. Here, we numerically explored all possible orientations
of three Platonic nanoparticles (tetrahedron, cube, and octahedron)
and found that a specific orientation (vertex-up, edge-up, or facet-up)
is more preferred than random orientations. We also demonstrated their
positions and orientations can be quantitatively predicted when the
surface tensions dominate their total interaction energies. The line
tensions may affect their positions and orientations only when total
interaction energies are close to each other for more than one orientation.
The molecular dynamics simulation results were in excellent agreement
with our theoretical predictions. Our theory will advance our ability
toward predicting the final structures of Platonic nanoparticle assemblies
at a liquid/liquid interface
Synergistic Effects of Water and Oxygen Molecule Co-adsorption on (001) Surfaces of Tetragonal CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>: A First-Principles Study
The poor environmental stability
of organometallic halide perovskite
solar cells presents a big challenge for its commercialization, which
is mainly due to the degradation of perovskite materials in humid
air. The role played by water molecules has been extensively studied
in the degradation processes, where strong interactions between water
molecules and perovskite surfaces are found. Using first-principles
simulations, we find that oxygen molecules also have strong interactions
with (001) surfaces of tetragonal CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> through the formation of a chemical Pb–O bond on the
PbI<sub>2</sub>-terminated surface and a hydrogen bond on the CH<sub>3</sub>NH<sub>3</sub>I-terminated surface. The adsorbed oxygen molecules
introduce empty states near the Fermi level of the surfaces, which
can facilitate charge transfer between the surface and oxygen molecules.
Furthermore, when an oxygen molecule is located atop a Pb atom on
PbI<sub>2</sub>-terminated surface, the calculated adsorption energies
indicate that the surface is more attractive to water molecules, making
the surface even more sensitive to humidity. These findings reveal
that oxygen molecules also play an important role in the initial stage
of the degradation of perovskite materials
Structural Effects in the Electromagnetic Enhancement Mechanism of Surface-Enhanced Raman Scattering: Dipole Reradiation and Rectangular Symmetry Effects for Nanoparticle Arrays
Surface-enhanced Raman scattering (SERS) enhancement
factors for
Ag and Au sphere array structures are determined by rigorously including
dipole reradiation in a T-matrix formalism. Comparisons are made with
the more commonly used local field enhancement due to plane-wave excitation,
|<b>E</b>(<b>r</b><sub>0</sub>;ω)|<sup>2</sup>|<b>E</b>(<b>r</b><sub>0</sub>;ω<sub><i>s</i></sub>)|<sup>2</sup> which for zero Stokes shift is |<b>E</b>(<b>r</b><sub>0</sub>;ω)|<sup>4</sup> to determine the
errors associated with this approximation. Substantial errors (factors
of 10–100) are found for the peak enhancements at a scattering
angle well away from the incident direction, but for backscattering,
the errors are negligible. We also present |<b>E</b>|<sup>4</sup> enhancement factors using a periodic boundary discrete dipole approximation
method for several metal strip array structures, and we show that
a certain combination of rectangular array structure and strip properties
leads to electromagnetic enhancement factors for mixed photonic-plasmonic
resonances that are considerably higher than can be produced with
either square arrays or 1-D arrays based on the same particles and
spacings
Optimal Interparticle Gap for Ultrahigh Field Enhancement by LSP Excitation via ESPs and Confirmation Using SERS
We have predicted
extremely high electromagnetic hot spots using
the extended–localized coupled surface plasmon resonance configuration.
With this unique configuration, we found that an array of particles
shows the critical importance of the interparticle gap on the enhancement
factor, which was confirmed experimentally using surface-enhanced
Raman scattering (SERS). The extended plasmon wave excited in the
Kretschmann–Raether configuration propagates on the silver
film surface and couples with the gold nanoparticles dispersed on
top through excitation of the localized plasmons. A monomolecular
layer of 4-aminothiophenol sandwiched between the metal film and the
nanoparticles showed an SERS enhancement factor of the order of 10<sup>10</sup> per molecule in the hot spots. The configuration was optimized,
both by simulations and experiments, with respect to the size of the
nanoparticles and the interparticle distances. It is demonstrated
that the ultrahigh SERS enhancement does occur only when the extended
surface plasmon is coupled to the localized surface plasmon at an
optimized interparticle gap. Further, highly sensitive detection of
glycerol in ethanol is demonstrated using the optimum structure with
a detection limit on the order of 10<sup>–12</sup> to the weight
percentage of ethanol, which is equivalent to detection of a few molecules.
This ultrahigh enhancement is useful in realizing various highly sensitive
biosensors when strong enhancement is required as well as in highly
efficient optoelectronic and energy devices
Dependence of Plasmonic Properties on Electron Densities for Various Coupled Au Nanostructures
Noble metallic nanostructures have
great potential in optical sensing
application in visible and near-infrared frequencies. Their plasmonic
properties can be manipulated by <i>in situ</i> controlling
their electron densities for isolated nanostructures. However, the
effect of charging remains underexplored for coupled systems. In this
work, we theoretically investigated the dependence of their far-field
and near-field properties on their electron densities for various
coupled gold structures. With increasing electron densities, their
enhancement factors increase while their plasmonic resonance peaks
are blue-shifted. The resonance peak position of ellipsoid-ellipsoid
dimers shows the highest sensitivity in response to the charging effects
with the slope of −2.87. The surface-averaged electric field
of ellipsoid monomer shows largest enhancement ratio of 1.13 with
16% excess electrons. These results can be well explained by an effective
dipole moment model. In addition, we also studied the sphere-on-substrate
nanostructure which can be precisely fabricated. This system shows
low sensitivity to the charging effect with the slope of −1.46
but remarkable enhancement ratio of 1.13 on near field response with
16% excess electrons
Origins of Charge Mobility Decreasing from Stretching–Releasing Cycles in Polymer Semiconductors
Polymer semiconductors as a key component of electronic
skin need
to maintain the coexistence of stretchability and electrical functionalities.
However, repeated stretching–compressing cycles inevitably
lead to the charge mobilities decreasing and poor working performance
of polymer semiconductors. Here, a method combining molecular dynamics
(MD) simulations and charge transport theory was developed to obtain
the morphology–mobility relationship of amorphous poly(3-hexylthiophene)
(P3HT). The simulation results show that the hole mobility decreases
by 6% along the strain direction after three stretching–compressing
cycles with 80% strain. These results are due to the chain alignment
change caused by the mechanical operations. The stretched P3HT material
presents higher charge mobility due to its better chain alignment,
while the compressed P3HT shows lower charge mobility because of the
poor chain alignment. Repeated stretching–compressing cycles
lead to the chain alignment parameters decreasing along the deformation
direction with accumulation and saturation effects. The repeated cycles
also result in the primitive path length decreasing, which indicates
polymer chain spatial distribution is more localized after repeated
deformations. Our findings provide microscale knowledge about the
dependence of molecular morphology and charge mobility on stretching–compressing
cycles, which can help to guide the design of polymer semiconductors
with higher charge mobility under repeated stretching–compressing
cycles
Origins of Charge Mobility Decreasing from Stretching–Releasing Cycles in Polymer Semiconductors
Polymer semiconductors as a key component of electronic
skin need
to maintain the coexistence of stretchability and electrical functionalities.
However, repeated stretching–compressing cycles inevitably
lead to the charge mobilities decreasing and poor working performance
of polymer semiconductors. Here, a method combining molecular dynamics
(MD) simulations and charge transport theory was developed to obtain
the morphology–mobility relationship of amorphous poly(3-hexylthiophene)
(P3HT). The simulation results show that the hole mobility decreases
by 6% along the strain direction after three stretching–compressing
cycles with 80% strain. These results are due to the chain alignment
change caused by the mechanical operations. The stretched P3HT material
presents higher charge mobility due to its better chain alignment,
while the compressed P3HT shows lower charge mobility because of the
poor chain alignment. Repeated stretching–compressing cycles
lead to the chain alignment parameters decreasing along the deformation
direction with accumulation and saturation effects. The repeated cycles
also result in the primitive path length decreasing, which indicates
polymer chain spatial distribution is more localized after repeated
deformations. Our findings provide microscale knowledge about the
dependence of molecular morphology and charge mobility on stretching–compressing
cycles, which can help to guide the design of polymer semiconductors
with higher charge mobility under repeated stretching–compressing
cycles
Synthesis of Spiky Ag–Au Octahedral Nanoparticles and Their Tunable Optical Properties
Spiky nanoparticles
exhibit higher overall plasmonic excitation
cross sections than their nonspiky peers. In this work, we demonstrate
a two-step seed-mediated growth method to synthesize a new class of
spiky Ag–Au octahedral nanoparticles with the aid of a high
molecular weight polyÂ(vinylpyrrolidone) polymer. The length of the
nanospikes can be controlled from 10 to 130 nm with sharp tips by
varying the amount of gold precursor added and the injection rates.
Spatially resolved electron energy-loss spectroscopy (EELS) study
and finite-difference time-domain (FDTD) simulations on individual
spiky Ag–Au nanoparticles illustrate multipolar plasmonic responses.
While the octahedral core retains its intrinsic plasmon response,
the spike exhibits a hybridized dipolar surface plasmon resonance
at lower energy. With increasing spike length from 50 to 130 nm, the
surface plasmon of the spike can be tuned from 1.16 to 0.78 eV. The
electric field at the spike region increases rapidly with increasing
spike length, with a 10<sup>4</sup> field enhancement achieved at
the tips of 130-nm spike. The results highlight that it is important
to synthesize long spikes (>50 nm) on nanoparticles to achieve
strong
electric field enhancement. A hypothesis for the formation of sharp
spikes is proposed based on our studies using X-ray photoelectron
spectroscopy (XPS), scanning electron microscopy (SEM), and high resolution
transmission electron microscopy (TEM)