11 research outputs found
Investigation of Etching Behavior of Single-Walled Carbon Nanotubes Using Different Etchants
As
gas-phase etching has become an important method to obtain single-walled
carbon nanotubes (SWCNTs) with specific electronic structures, numerous
etchants were studied in the past decades. However, the understanding
of the dynamic process as well as the etching state is still limited.
Herein, we investigated the etching process of SWCNTs at the level
of the individual tube in real time using an improved polarized optical
microscope equipped with a miniature chemical vapor deposition (CVD)
system. Experiments showed a universal etching behavior in a SWCNT
oxidation process under different etchants (O<sub>2</sub>, H<sub>2</sub>O, and CO<sub>2</sub>), that is, the random appearance of etching
sites and the self-terminating phenomenon. We built a new etching
model at the level of the individual tubes to describe the etching
rate. Based on this model, a new constant <i>R</i>, the
ratio of etching rates between metallic and semiconducting SWCNTs,
was defined to describe the etching selectivity. Optical spectroscopy
was used to identify the chirality of SWCNTs, and it was found that
the etching selectivities followed the order: H<sub>2</sub>O (<i>R</i> = 17.1, 850 °C) > CO<sub>2</sub> (<i>R</i> = 3.6, 850 °C) > O<sub>2</sub> (<i>R</i> = 1.2,
610
°C). Field effect transistor (FET) performance of the SWCNT arrays
also verified the statistical results
Diameter-Specific Growth of Semiconducting SWNT Arrays Using Uniform Mo<sub>2</sub>C Solid Catalyst
Semiconducting single-walled nanotube
(s-SWNT) arrays with specific
diameters are urgently demanded in the applications in nanoelectronic
devices. Herein, we reported that by using uniform Mo<sub>2</sub>C
solid catalyst, aligned s-SWNT (∼90%) arrays with narrow-diameter
distribution (∼85% between 1.0 and 1.3 nm) on quartz substrate
can be obtained. Mo<sub>2</sub>C nanoparticles with monodisperse sizes
were prepared by using molybdenum oxide-based giant clusters, (NH<sub>4</sub>)<sub>42</sub>[Mo<sub>132</sub>O<sub>372</sub>(H<sub>3</sub>CCOO)<sub>30</sub>(H<sub>2</sub>O)<sub>72</sub>]·10H<sub>3</sub>CCOONH<sub>4</sub>·300H<sub>2</sub>OÂ(Mo<sub>132</sub>), as the
precursor that was carburized by a gas mixture of C<sub>2</sub>H<sub>5</sub>OH/H<sub>2</sub> during a temperature-programmed reduction.
In this approach, the formation of volatile MoO<sub>3</sub> was inhibited
due to the annealing and reduction at a low temperature. As a result,
uniform Mo<sub>2</sub>C nanoparticles are formed, and their narrow
size-dispersion strictly determines the diameter distribution of SWNTs.
During the growth process, Mo<sub>2</sub>C selectively catalyzes the
scission of C–O bonds of ethanol molecules, and the resultant
absorbed oxygen (O<sub>ads</sub>) preferentially etches metallic SWNTs
(m-SWNTs), leading to the high-yield of s-SWNTs. Raman spectroscopic
analysis showed that most of the s-SWNTs can be identified as (14,
4), (13, 6), or (10, 9) tubes. Our findings open up the possibility
of the chirality-controlled growth of aligned-SWNTs using uniform
carbide nanoparticles as solid catalysts for practical nanoelectronics
applications
Anomalous Polarized Raman Scattering and Large Circular Intensity Differential in Layered Triclinic ReS<sub>2</sub>
The Raman tensor
of a crystal is the derivative of its polarizability
tensor and is dependent on the symmetries of the crystal and the Raman-active
vibrational mode. The intensity of a particular mode is determined
by the Raman selection rule, which involves the Raman tensor and the
polarization configurations. For anisotropic two-dimensional (2D)
layered crystals, polarized Raman scattering has been used to reveal
the crystalline orientations. However, due to its complicated Raman
tensors and optical birefringence, the polarized Raman scattering
of triclinic 2D crystals has not been well studied yet. Herein, we
report the anomalous polarized Raman scattering of 2D layered triclinic
rhenium disulfide (ReS<sub>2</sub>) and show a large circular intensity
differential (CID) of Raman scattering in ReS<sub>2</sub> of different
thicknesses. The origin of CID and the anomalous behavior in polarized
Raman scattering were attributed to the appearance of nonzero off-diagonal
Raman tensor elements and the phase factor owing to optical birefringence.
This can provide a method to identify the vertical orientation of
triclinic layered materials. These findings may help to further understand
the Raman scattering process in 2D materials of low symmetry and may
indicate important applications in chiral recognition by using 2D
materials
Ultrasensitive Size-Selection of Plasmonic Nanoparticles by Fano Interference Optical Force
In this paper, we propose a solution for the ultrasensitive optical selection of plasmonic nanoparticles using Fano interference-induced scattering forces. Under a Gaussian beam excitation, the scattering of a plasmonic nanoparticle at its Fano resonance becomes strongly asymmetric in the lateral direction and consequently results in a net transverse scattering force, that is, Fano interference-induced force. The magnitude of this transverse scattering force is comparable with the gradient force in conventional optical manipulation experiments. More interestingly, the Fano scattering force is ultrasensitive to the particle size and excitation frequency due to the phase sensitivity of the interference between adjacent plasmon modes in the particle. Utilizing this distinct feature, we show the possibility of size-selective sorting of silver and gold nanoparticles with an accuracy of about ±10 nm and silica-gold core–shell nanoparticles with shell thickness down to several nanometers. These results would add to the toolbox of optical manipulation and fabrication
Light-Concentrating Plasmonic Au Superstructures with Significantly Visible-Light-Enhanced Catalytic Performance
Noble metals are well-known for their
surface plasmon resonance
effect that enables strong light absorption typically in the visible
regions for gold and silver. However, unlike semiconductors, noble
metals are commonly considered incapable of catalyzing reactions via
photogenerated electron–hole pairs due to their continuous
energy band structures. So far, photonically activated catalytic system
based on pure noble metal nanostructures has seldom been reported.
Here, we report the development of three different novel plasmonic
Au superstructures comprised of Au nanoparticles, multiple-twinned
nanoparticles and nanoworms assembling on the surfaces of SiO<sub>2</sub> nanospheres respectively via a well-designed synthetic strategy.
It is found that these novel Au superstructures show enhanced broadband
visible-light absorption due to the plasmon resonance coupling within
the superstructures, and thus can effectively focus the energy of
photon fluxes to generate much more excited hot electrons and holes
for promoting catalytic reactions. Accordingly, these Au superstructures
exhibit significantly visible-light-enhanced catalytic efficiency
(up to ∼264% enhancement) for the commercial reaction of p-nitrophenol
reduction
Synthesis of Ultrathin Graphdiyne Film Using a Surface Template
Graphdiyne
is predicted to have a natural band gap and simultaneously possesses
superior carrier mobility, which makes it potential for electronic
devices. Synthesis of ultrathin graphdiyne film is highly demanded.
In this work, we proposed an approach for synthesis of ultrathin graphdiyne
film using graphene as a surface template, which can induce confined
reaction on substrate. With all-carbon, conjugated, atomically flat
structure, graphene has a strong interaction with the graphdiyne system,
resulting the formation of continuous flat ultrathin graphdiyne film
with thickness less than 3 nm. Raman spectra, grazing incidence X-ray
diffraction, and transmission electron microscopy characterization
all confirmed the features of graphdiyne. Furthermore, this strategy
was also extended to the hexagonal boron nitride (hBN) surface with
resembling structure, serving as a perfect dielectric layer. Field-effect
transistor devices based on graphdiyne film grown on hBN were fabricated
directly, and electrical transport measurements demonstrate the good
conductivity with <i>p</i>-type characteristics of the as-obtained
graphdiyne film
Synthesis of Hierarchical Graphdiyne-Based Architecture for Efficient Solar Steam Generation
Synthesis of Hierarchical Graphdiyne-Based Architecture
for Efficient Solar Steam Generatio
Enhanced Raman Scattering on In-Plane Anisotropic Layered Materials
Surface-enhanced Raman scattering
(SERS) on two-dimensional (2D)
layered materials has provided a unique platform to study the chemical
mechanism (CM) of the enhancement due to its natural separation from
electromagnetic enhancement. The CM stems from the charge interactions
between the substrate and molecules. Despite the extensive studies
of the energy alignment between 2D materials and molecules, an understanding
of how the electronic properties of the substrate are explicitly involved
in the charge interaction is still unclear. Lately, a new group of
2D layered materials with anisotropic structures, including orthorhombic
black phosphorus (BP) and triclinic rhenium disulfide (ReS<sub>2</sub>), has attracted great interest due to their unique anisotropic electrical
and optical properties. Herein, we report a unique anisotropic Raman
enhancement on few-layered BP and ReS<sub>2</sub> using copper phthalocyanine
(CuPc) molecules as a Raman probe, which is absent on isotropic graphene
and h-BN. According to detailed Raman tensor analysis and density
functional theory calculations, anisotropic charge interactions between
the 2D materials and molecules are responsible for the angular dependence
of the Raman enhancement. Our findings not only provide new insights
into the CM process in SERS, but also open up new avenues for the
exploration and application of the electronic properties of anisotropic
2D layered materials
Template Synthesis of an Ultrathin β‑Graphdiyne-Like Film Using the Eglinton Coupling Reaction
β-Graphdiyne (β-GDY)
is a two-dimensional carbon material with zero band gap and highly
intrinsic carrier mobility and a promising material with potential
applications in electronic devices. However, the synthesis of continuous
single or ultrathin β-GDY has not been realized yet. Here, we
proposed an approach for ultrathin β-GDY-like film synthesis
using graphene as a template because of the strong π–π
interaction between β-GDY and graphene. The as-synthesized film
presents smooth and continuous morphology and has good crystallinity.
Electrical measurement reveals that the film presented a conductivity
of 1.30 × 10<sup>–2</sup> S·m<sup>–1</sup> by fabricating electronic devices on β-GDY grown on a dielectric
hexagonal boron nitride template
Hydrogen Radical-Induced Electrocatalytic N<sub>2</sub> Reduction at a Low Potential
Realizing efficient hydrogenation of N2 molecules
in
the electrocatalytic nitrogen reduction reaction (NRR) is crucial
in achieving high activity at a low potential because it theoretically
requires a higher equilibrium potential than other steps. Analogous
to metal hydride complexes for N2 reduction, achieving
this step by chemical hydrogenation can weaken the potential dependence
of the initial hydrogenation process. However, this strategy is rarely
reported in the electrocatalytic NRR, and the catalytic mechanism
remains ambiguous and lacks experimental evidence. Here, we show a
highly efficient electrocatalyst (ruthenium single atoms anchored
on graphdiyne/graphene sandwich structures) with a hydrogen radical-transferring
mechanism, in which graphdiyne (GDY) generates hydrogen radicals (H•), which can effectively activate N2 to
generate NNH radicals (•NNH). A dual-active site
is constructed to suppress competing hydrogen evolution, where hydrogen
preferentially adsorbs on GDY and Ru single atoms serve as the adsorption
site of •NNH to promote further hydrogenation of
NH3 synthesis. As a result, high activity and selectivity
are obtained simultaneously at −0.1 V versus a reversible hydrogen
electrode. Our findings illustrate a novel hydrogen transfer mechanism
that can greatly reduce the potential and maintain the high activity
and selectivity in NRR and provide powerful guidelines for the design
concept of electrocatalysts