13 research outputs found
Light Management in Upconverting Nanoparticles: Ultrasmall Core/Shell Architectures to Tune the Emission Color
Ultrasmall
NaGdF<sub>4</sub> nanoparticles with core/shell and
core/shell/shell architectures have been synthesized following a microwave-based
thermolysis procedure, allowing us to rapidly obtain homogeneous nanoparticles
compared to conventional heating. To analyze the possibilities of
the proposed structure in terms of tuning the emission color, core
and shells have been doped with different lanthanide ion pairs (either
Er<sup>3+</sup>/Yb<sup>3+</sup> and/or Tm<sup>3+</sup>/Yb<sup>3+</sup>), keeping them therefore spatially separated inside the different
layers of the nanoparticles. Here, we demonstrate that the position
of the dopants inside the nanoparticles affects the intensity of the
different emission bands of the luminescing Tm<sup>3+</sup> and Er<sup>3+</sup> ions and show how it has a relevant effect on the overall
emission color of the luminescence obtained after 975 nm excitation
Effect of Surface Oxidation on the Interaction of 1-Methylaminopyrene with Gold Nanoparticles
The effect of the surface chemistry of gold nanoparticles
(GNPs)
on the GNPâamine (âNH<sub>2</sub>) interaction was investigated
via conjugating an amine probeî¸1-methylaminopyrene (MAP) chromophoreî¸with
three Au colloidal samples of the same particle size yet different
surface chemistry. The surface of laser-irradiated and ligand-exchanged-irradiated
GNPs is covered with acetonedicarboxylic ligands (due to laser-introduced
citrate oxidization) and citrate ligands, respectively, and both surfaces
contain oxidized Au species which are essentially lacking for the
citrate-capped GNPs prepared by the pure chemical approach. Both laser-irradiated
samples show inferior adsorption capacity of MAP as compared with
the purely chemically prepared GNPs. Detailed investigations indicate
that MAP molecules mainly complex directly with Au atoms via forming
Au-NH<sub>2</sub>R bonds, and the oxidization of the GNP surface strongly
influences the ratio of this direct bonding to the indirect bonding
originating from the electrostatic interaction between protonated
amine (âNH<sub>3</sub><sup>+</sup>) and negatively charged
surface ligands. The impact of the oxidized GNP surface associated
with the laser treatment is further confirmed by aging experiment
on GNPâMAP conjugation systems, which straightforwardly verifies
that the surface oxidation leads to the decrease in the MAP adsorption
on GNPs
YolkâShell Nanoparticles with CO<sub>2</sub>âResponsive Outer Shells for Gas-Controlled Catalysis
Yolkâshell nanoparticles (YSNPs) consisting of
a gold nanoparticle
core, a CO2-responsive crosslinked polyÂ(N,N-diethylaminoethyl methacrylate) shell, and a
void in between, denoted as Au@void@PDEAEMA, were synthesized, characterized,
and utilized as a catalyst for the gas-controllable reduction of 4-nitrophenol
(4-NP) and nitrobenzene (NB). We show that the rate of the catalytic
reaction can be regulated by controlling the diffusion of reactant
molecules through the polymer shell by switching the latter between
a hydrophilic state upon CO2 bubbling and a hydrophobic
state by bubbling N2 to remove CO2. While for
the reduction of 4-NP, it is possible to turn on and turn off the
reaction through alternating bubbling of the two gases, with a mixture
of 4-NP and NB, the respective reactions of either reactant can be
selectively favored using the gases (CO2 for the relatively
faster reaction of 4-NP and N2 for the faster reaction
of NB). Moreover, the gas-controlled reversible dispersion and the
agglomeration state of Au@void@PDEAEMA were explored for in situ recovery
of the nanoparticle catalyst and their reuse for catalytic reactions
without using ultracentrifugation. Finally, the effect of structural
parameters of such YSNPs on the catalytic activity was investigated
by either varying the thickness of the polymer shell at the same void
space or changing the void while keeping the same polymer shell thickness
High-Efficiency Broadband C<sub>3</sub>N<sub>4</sub> Photocatalysts: Synergistic Effects from Upconversion and Plasmons
A plasmon and upconversion
enhanced broadband photocatalyst based
on Au nanoparticle (NP) and NaYF<sub>4</sub>:Yb<sup>3+</sup>, Er<sup>3+</sup>, Tm<sup>3+</sup> (NYF) microsphere loaded graphitic C<sub>3</sub>N<sub>4</sub> (g-C<sub>3</sub>N<sub>4</sub>) nanosheets (Au-NYF/g-C<sub>3</sub>N<sub>4</sub>) was subtly designed and synthesized. The simple
one-step synthesis of NYF in the presence of g-C<sub>3</sub>N<sub>4</sub>, which has not been reported in the literature either, leads
to both high NYF yield and high coupling efficiency between NYF and
g-C<sub>3</sub>N<sub>4</sub>. The Au-NYF/g-C<sub>3</sub>N<sub>4</sub> structure exhibits high stability, wide photoresponse from the ultraviolet
(UV), to visible and near-infrared regions, and prominently enhanced
photocatalytic activities compared with the plain g-C<sub>3</sub>N<sub>4</sub> sample in the degradation of methyl orange (MO). In particular,
with the optimization of Au loading, the rate constant normalized
with the catalysts mass of the best-performing catalyst 1 wt % Au-NYF/g-C<sub>3</sub>N<sub>4</sub> (0.032 h<sup>â1</sup> mg<sup>â1</sup>) far surpasses that of NYF/g-C<sub>3</sub>N<sub>4</sub> and g-C<sub>3</sub>N<sub>4</sub> (0.009 h<sup>â1</sup> mg<sup>â1</sup>) by 3.6 times under Îť > 420 nm light irradiation. The high
performance of the Au-NYF/g-C<sub>3</sub>N<sub>4</sub> nanocomposite
under different light irradiations was ascribed to the distinctively
promoted charge separation and suppressed recombination, and the efficient
transfer of charge carriers and energy among these components. The
promoted charge separation and transfer were further confirmed by
photoelectrochemical measurements. The 1 wt % Au-NYF/g-C<sub>3</sub>N<sub>4</sub> exhibits enhanced photocurrent density (âź6.36
ÎźA cm<sup>â2</sup>) by a factor of âź5.5 with respect
to that of NYF/g-C<sub>3</sub>N<sub>4</sub> sample (âź1.15 ÎźA
cm<sup>â2</sup>). Different mechanisms of the photodegradation
under separate UV, visible, and NIR illuminations are unveiled and
discussed in detail. Under simulated solar light illumination, the
involved reactive species were identified by performing trapping experiments.
This work highlights the great potential of developing highly efficient
g-C<sub>3</sub>N<sub>4</sub>-based broadband photocatalysts for full
solar spectrum utilization by integrating plasmonic nanostructures
and upconverting materials
Tuning the Charge-Transfer Property of PbS-Quantum Dot/TiO<sub>2</sub>-Nanobelt Nanohybrids via Quantum Confinement
A newly designed photoactive nanohybrid structure based on the combination of near-infrared PbS quantum dots (QDs) as light harvester and one-dimensional TiO<sub>2</sub> nanobelts (NBs) to guide the flow of photogenerated charge carriers is reported. Efficient electron transfer from photoexcited PbS QDs to TiO<sub>2</sub> NBs has been demonstrated to occur in the developed PbS-QD/TiO<sub>2</sub>-NB nanohybrids, and the charge-transfer property can be tuned through the size quantization effect of PbS QDs. Moreover, the use of TiO<sub>2</sub> NBs instead of TiO<sub>2</sub> NPs permits a larger critical size of PbS QDs capable of injecting electrons into TiO<sub>2</sub> NBs, which, in turn, markedly extends the âeffectiveâ absorption of the PbS-QD/TiO<sub>2</sub>-NB nanohybrids to a longer wavelength region up to 1400 nm. Such an extension of the âeffectiveâ absorption is a major asset for improving the overall photoconversion efficiency of PbS-QD/TiO<sub>2</sub>-NB nanohybrids-based photovoltaic devices
Size Dependence of Temperature-Related Optical Properties of PbS and PbS/CdS Core/Shell Quantum Dots
The
effect of PbS core size on the temperature-dependent photoluminescence
(PL) of PbS/CdS quantum dots (QDs) in the temperature range of 100â300
K was thoroughly investigated and compared with shell-free PbS QDs.
The core/shell QDs show significantly smaller PL intensity variation
with temperature at a smaller PbS size, while a larger activation
energy when the PbS domain size is relatively large, suggesting both
different density and different distribution of defects/traps in the
PbS and PbS/CdS QDs. The most remarkable difference consists in the
PbS size dependence of the energy gap temperature coefficient (d<i>E</i>/d<i>T</i>). The PbS/CdS QDs show unusual non-monotonic
d<i>E</i>/d<i>T</i> variation, resulting in the
reversal of the d<i>E</i>/d<i>T</i> difference
between the PbS and PbS/CdS QDs at a larger PbS size. In combination
with theoretical calculations, we find that, although lattice dilation
and carrier-phonon coupling are generally considered as dominant terms,
the unique negative contribution to d<i>E</i>/d<i>T</i> from the core/shell interfacial strain becomes most important in
the relatively larger-core PbS@CdS QDs
Detection of Adenosine Triphosphate with an Aptamer Biosensor Based on Surface-Enhanced Raman Scattering
A simple, ultrasensitive, highly selective, and reagent-free
aptamer-based
biosensor has been developed for quantitative detection of adenosine
triphosphate (ATP) using surface-enhanced Raman scattering (SERS).
The sensor contains a SERS probe made of gold nanostar@Raman label@SiO<sub>2</sub> coreâshell nanoparticles in which the Raman label
(malachite green isothiocyanate, MGITC) molecules are sandwiched between
a gold nanostar core and a thin silica shell. Such a SERS probe brings
enhanced signal and low background fluorescence, shows good water-solubility
and stability, and exhibits no sign of photobleaching. The aptamer
labeled with the SERS probe is designed to hybridize with the cDNA
on a gold film to form a rigid duplex DNA. In the presence of ATP,
the interaction between ATP and the aptamer results in the dissociation
of the duplex DNA structure and thereby removal of the SERS probe
from the gold film, reducing the Raman signal. The response of the
SERS biosensor varies linearly with the logarithmic ATP concentration
up to 2.0 nM with a limit of detection of 12.4 pM. Our work has provided
an effective method for detection of small molecules with SERS
Plasmonic Nanorice Antenna on Triangle Nanoarray for Surface-Enhanced Raman Scattering Detection of Hepatitis B Virus DNA
The sensitivity and the limit of detection of Raman sensors
are
limited by the extremely small scattering cross section of Raman labels.
Silver nanorice antennae are coupled with a patterned gold triangle
nanoarray chip to create spatially broadened plasmonic âhot
spotsâ, which enables a large density of Raman labels to experience
strong local electromagnetic field. Finite difference time domain
simulations have confirmed that the quasi-periodic structure increases
the intensity and the area of the surface plasmon resonance (SPR),
which enhances the surface-enhanced Raman scattering (SERS) signal
significantly. The SERS signal of the nanorice/DNA/nanoarray chip
is compared with that of the nanorice/DNA/film chip. The SERS signal
is greatly enhanced when the Ag nanorices are coupled to the periodic
Au nanoarray instead of the planar film chip. The resulting spatially
broadened SPR field enables the SERS biosensor with a limit of detection
of 50 aM toward hepatitis B virus DNA with the capability of discriminating
a single-base mutant of DNA. This sensing platform can be extended
to detect other chemical species and biomolecules such as proteins
and small molecules
Silver Nanorice Structures: Oriented Attachment-Dominated Growth, High Environmental Sensitivity, and Real-Space Visualization of Multipolar Resonances
We have synthesized and investigated the anisotropic
growth of
interesting silver nanorice. Its growth is kinetically controlled
at 100 °C, and both oriented attachment and Ostwald ripening
are involved, with the former growth mode dominating the anisotropic
growth of the nanorice along the â¨111⊠direction. This
one-directional growth is initiated by an indispensable seed-selection
process, in which oxygen plays a critical role in oxidatively etching
twinned silver crystals. The inhibition of this process by removing
oxygen essentially blocks the nanorice growth. Although increasing
reaction temperature to 120 °C accelerates the one-dimensional
growth along the â¨111⊠direction, further temperature
increase to 160 °C makes the oriented attachment dominated one-directional
growth disappear; instead, the diffusion-controlled two-dimensional
growth leads to the emergence of highly faceted truncated triangular
and hexagonal plates mainly bound by low energy faces of {111}. Interestingly,
we also found that the longitudinal surface plasmon resonance of the
nanorice structures is highly sensitive to the refractive index of
surrounding dielectric media, which predicts their promising applications
as chemical or biological sensors. Moreover, the multipolar plasmonic
resonances in these individual nanorice structures are visualized
in real space, using high-resolution electron energy-loss spectroscopy
Facile and Mild Strategy to Construct Mesoporous CeO<sub>2</sub>âCuO Nanorods with Enhanced Catalytic Activity toward CO Oxidation
CeO<sub>2</sub>âCuO nanorods with mesoporous structure were synthesized
by a facile and mild strategy, which involves an interfacial reaction
between Ce<sub>2</sub>(SO<sub>4</sub>)<sub>3</sub> precursor and NaOH
ethanol solution at room temperature to obtain mesoporous CeO<sub>2</sub> nanorods, followed by a solvothermal treatment of as-prepared
CeO<sub>2</sub> and CuÂ(CH<sub>3</sub>COO)<sub>2</sub>. Upon solvothermal
treatment, CuO species is highly dispersed onto the CeO<sub>2</sub> nanorod surface to form CeO<sub>2</sub>âCuO composites, which
still maintain the mesoporous feature. A preliminary CO catalytic
oxidation study demonstrated that the CeO<sub>2</sub>âCuO samples
exhibited strikingly high catalytic activity, and a high CO conversion
rate was observed without obvious loss in activity even after thermal
treatment at a high temperature of 500 °C. Raman spectroscopy,
X-ray photoelectron spectroscopy (XPS), and hydrogen temperature-programmed
reduction (H<sub>2</sub>-TPR) analysis revealed that there is a strong
interaction between CeO<sub>2</sub> and CuO. Moreover, it was found
that the introduction of CuO species into CeO<sub>2</sub> generates
oxygen vacancies, which is highly likely to be responsible for high
catalytic activity toward CO oxidation of the mesoporous CeO<sub>2</sub>âCuO nanorods