11 research outputs found
Effect of Pretreatment Conditions on the Precise Nanoporosity of Graphene Oxide
Nanoscale pores in graphene oxide (GO) control various
important
functions. The nanoporosity of GO is sensitive to low-temperature
heating. Therefore, it is important to carefully process GO and GO-based
materials to achieve superior functions. Optimum pretreatment conditions,
such as the pre-evacuation temperature and time, are important during
gas adsorption in GO to obtain accurate pore structure information.
This study demonstrated that the pre-evacuation temperature and time
for gas adsorption in GO must be approximately 333â353 K and
4 h, respectively, to avoid the irreversible alteration of nanoporosity.
In situ temperature-dependent Fourier-transform infrared spectra and
thermogravimetric analysisâmass spectrometry suggested significant
structural changes in GO above the pre-evacuation temperature (353
K) through the desorption of âphysically adsorbed waterâ
and decomposition of unstable surface functional groups. The nanoporosity
of GO significantly changed above the aforementioned pre-evacuation
temperature and time. Thus, standard pretreatment is indispensable
for understanding the intrinsic interface properties of GO
Low-Temperature Solution Synthesis of Transition Metal Dichalcogenide Alloys with Tunable Optical Properties
Nanostructures
of layered transition metal dichalcogenide (TMD)
alloys with tunable compositions are promising candidates for a broad
scope of applications in electronics, optoelectronics, topological
devices, and catalysis. Most TMD alloy nanostructures are synthesized
as films on substrates using gas-phase methods at high temperatures.
However, lower temperature solution routes present an attractive alternative
with the potential for larger-scale, higher-yield syntheses of freestanding,
higher surface area materials. Here, we report the direct solution
synthesis of colloidal few-layer TMD alloys, Mo<sub><i>x</i></sub>W<sub>1â<i>x</i></sub>Se<sub>2</sub> and WS<sub>2<i>y</i></sub>Se<sub>2(1â<i>y</i>)</sub>, exhibiting fully tunable metal and chalcogen compositions that
span the MoSe<sub>2</sub>âWSe<sub>2</sub> and WS<sub>2</sub>âWSe<sub>2</sub> solid solutions, respectively. Chemical guidelines
for achieving the targeted compounds are presented, along with comprehensive
structural characterizations (X-ray diffraction, electron microscopy,
Raman, and UVâvisible spectroscopies). High-resolution microscopic
imaging confirms the formation of TMD alloys and identifies a random
distribution of the alloyed elements. Analysis of the tilt-angle dependency
of the intensities associated with atomic-resolution annular dark
field imaging line scans reveals the types of point vacancies present
in the samples, thus providing atomic-level insights into the structures
of colloidal TMD alloy nanostructures that were previously only accessible
for substrate-confined films. The A excitonic transition of the TMD
alloy nanostructures can be readily adjusted between 1.51 and 1.93
eV through metal and chalcogen alloying, correlating the compositional
modulation to the realization of tunable optical properties
Intricate Resonant Raman Response in Anisotropic ReS<sub>2</sub>
The
strong in-plane anisotropy of rhenium disulfide (ReS<sub>2</sub>)
offers an additional physical parameter that can be tuned for advanced
applications such as logic circuits, thin-film polarizers, and polarization-sensitive
photodetectors. ReS<sub>2</sub> also presents advantages for optoelectronics,
as it is both a direct-gap semiconductor for few-layer thicknesses
(unlike MoS<sub>2</sub> or WS<sub>2</sub>) and stable in air (unlike
black phosphorus). Raman spectroscopy is one of the most powerful
characterization techniques to nondestructively and sensitively probe
the fundamental photophysics of a 2D material. Here, we perform a
thorough study of the resonant Raman response of the 18 first-order
phonons in ReS<sub>2</sub> at various layer thicknesses and crystal
orientations. Remarkably, we discover that, as opposed to a general
increase in intensity of all of the Raman modes at excitonic transitions,
each of the 18 modes behave <i>differently</i> relative
to each other as a function of laser excitation, layer thickness,
and orientation in a manner that highlights the importance of electronâphonon
coupling in ReS<sub>2</sub>. In addition, we correct an unrecognized
error in the calculation of the optical interference enhancement of
the Raman signal of transition metal dichalcogenides on SiO<sub>2</sub>/Si substrates that has propagated through various reports. For ReS<sub>2</sub>, this correction is critical to properly assessing the resonant
Raman behavior. We also implemented a perturbation approach to calculate
frequency-dependent Raman intensities based on first-principles and
demonstrate that, despite the neglect of excitonic effects, useful
trends in the Raman intensities of monolayer and bulk ReS<sub>2</sub> at different laser energies can be accurately captured. Finally,
the phonon dispersion calculated from first-principles is used to
address the possible origins of unexplained peaks observed in the
Raman spectra, such as infrared-active modes, defects, and second-order
processes
Photoluminescence Segmentation within Individual Hexagonal Monolayer Tungsten Disulfide Domains Grown by Chemical Vapor Deposition
We
show that hexagonal domains of monolayer tungsten disulfide
(WS<sub>2</sub>) grown by chemical vapor deposition (CVD) with powder
precursors can have discrete segmentation in their photoluminescence
(PL) emission intensity, forming symmetric patterns with alternating
bright and dark regions. Two-dimensional maps of the PL reveal significant
reduction within the segments associated with the longest sides of
the hexagonal domains. Analysis of the PL spectra shows differences
in the exciton to trion ratio, indicating variations in the exciton
recombination dynamics. Monolayers of WS<sub>2</sub> hexagonal islands
transferred to new substrates still exhibit this PL segmentation,
ruling out local strain in the regions as the dominant cause. High-power
laser irradiation causes preferential degradation of the bright segments
by sulfur removal, indicating the presence of a more defective region
that is higher in oxidative reactivity. Atomic force microscopy (AFM)
images of topography and amplitude modes show uniform thickness of
the WS<sub>2</sub> domains and no signs of segmentation. However,
AFM phase maps do show the same segmentation of the domain as the
PL maps and indicate that it is caused by some kind of structural
difference that we could not clearly identify. These results provide
important insights into the spatially varying properties of these
CVD-grown transition metal dichalcogenide materials, which may be
important for their effective implementation in fast photo sensors
and optical switches
Defect-Assisted Heavily and Substitutionally Boron-Doped Thin Multiwalled Carbon Nanotubes Using High-Temperature Thermal Diffusion
Carbon nanotubes have shown great
potential as conductive fillers in various composites, macro-assembled
fibers, and transparent conductive films due to their superior electrical
conductivity. Here, we present an effective defect engineering strategy
for improving the intrinsic electrical conductivity of nanotube assemblies
by thermally incorporating a large number of boron atoms into substitutional
positions within the hexagonal framework of the tubes. It was confirmed
that the defects introduced after vacuum ultraviolet and nitrogen
plasma treatments facilitate the incorporation of a large number of
boron atoms (ca. 0.496 atomic %) occupying the trigonal sites on the
tube sidewalls during the boron doping process, thus eventually increasing
the electrical conductivity of the carbon nanotube film. Our approach
provides a potential solution for the industrial use of macro-structured
nanotube assemblies, where properties, such as high electrical conductance,
high transparency, and lightweight, are extremely important
Formation of Nitrogen-Doped Graphene Nanoribbons <i>via</i> Chemical Unzipping
In this work, we carried out chemical oxidation studies of nitrogen-doped multiwalled carbon nanotubes (CNx-MWCNTs) using potassium permanganate in order to obtain nitrogen-doped graphene nanoribbons. Reaction parameters such as oxidation reaction, reaction time, the oxidizer to nanotube mass ratio, and the temperature were varied, and their effect was carefully analyzed. The presence of nitrogen atoms makes CNx-MWCNTs more reactive toward oxidation when compared to undoped multiwalled carbon nanotubes (MWCNTs). High-resolution transmission electron microscopy studies indicate that the oxidation of the graphitic layers within CNx-MWCNTs results in the unzipping of large diameter nanotubes and the formation of a disordered oxidized carbon coating on small diameter nanotubes. The nitrogen content within unzipped CNx-MWCNTs decreased as a function of the oxidation time, temperature, and oxidizer concentration. By controlling the degree of oxidation, the N atomic % could be reduced from 1.56% in pristine CNx-MWCNTs down to 0.31 atom % in nitrogen-doped oxidized graphene nanoribbons. A comparative thermogravimetric analysis reveals a lower thermal stability of the (unzipped) oxidized CNx-MWCNTs when compared to MWCNT samples. The oxidized graphene nanoribbons were chemically and thermally reduced and yielded nitrogen-doped graphene nanoribbons (N-GNRs). The thermal reduction at relatively low temperature (300 °C) results in graphene nanoribbons with 0.37 atom % of nitrogen. This method represents a novel route to preparation of bulk quantities of nitrogen-doped unzipped carbon nanotubes, which is able to control the doping level in the resulting reduced GNR samples. Finally, the electrochemical properties of these materials were evaluated
Monolayer WS<sub>2</sub> Nanopores for DNA Translocation with Light-Adjustable Sizes
Two-dimensional
materials are promising for a range of applications,
as well as testbeds for probing the physics of low-dimensional systems.
Tungsten disulfide (WS<sub>2</sub>) monolayers exhibit a direct band
gap and strong photoluminescence (PL) in the visible range, opening
possibilities for advanced optoelectronic applications. Here, we report
the realization of two-dimensional nanometer-size pores in suspended
monolayer WS<sub>2</sub> membranes, allowing for electrical and optical
response in ionic current measurements. A focused electron beam was
used to fabricate nanopores in WS<sub>2</sub> membranes suspended
on silicon-based chips and characterized using PL spectroscopy and
aberration-corrected high-resolution scanning transmission electron
microscopy. It was observed that the PL intensity of suspended WS<sub>2</sub> monolayers is âŒ10â15 times stronger when compared
to that of substrate-supported monolayers, and low-dose scanning transmission
electron microscope viewing and drilling preserves the PL signal of
WS<sub>2</sub> around the pore. We establish that such nanopores allow
ionic conductance and DNA translocations. We also demonstrate that
under low-power laser illumination in solution, WS<sub>2</sub> nanopores
grow slowly in size at an effective rate of âŒ0.2â0.4
nm/s, thus allowing for atomically controlled nanopore size using
short light pulses
Ordered and Atomically Perfect Fragmentation of Layered Transition Metal Dichalcogenides <i>via</i> Mechanical Instabilities
Thermoplastic
polymers subjected to a continuous tensile stress
experience a state of mechanical instabilities, resulting in neck
formation and propagation. The necking process with strong localized
strain enables the transformation of initially brittle polymeric materials
into robust, flexible, and oriented forms. Here we harness the polymer-based
mechanical instabilities to control the fragmentation of atomically
thin transition metal dichalcogenides (TMDs). We develop a simple
and versatile nanofabrication tool to precisely fragment atom-thin
TMDs sandwiched between thermoplastic polymers into ordered and atomically
perfect TMD nanoribbons in arbitrary directions regardless of the
crystal structures, defect content, and original geometries. This
method works for a very broad spectrum of semiconducting TMDs with
thicknesses ranging from monolayers to bulk crystals. We also explore
the electrical properties of the fabricated monolayer nanoribbon arrays,
obtaining an on/off ratio of âŒ10<sup>6</sup> for such MoS<sub>2</sub> arrays based field-effect transistors. Furthermore, we demonstrate
an improved hydrogen evolution reaction with the resulting monolayer
MoS<sub>2</sub> nanoribbons, thanks to the largely increased catalytic
edge sites formed by this physical fragmentation method. This capability
not only enriches the fundamental study of TMD extreme and fragmentation
mechanics, but also impacts on future developments of TMD-based devices
Low-temperature Synthesis of Heterostructures of Transition Metal Dichalcogenide Alloys (W<sub><i>x</i></sub>Mo<sub>1â<i>x</i></sub>S<sub>2</sub>) and Graphene with Superior Catalytic Performance for Hydrogen Evolution
Large-area (âŒcm<sup>2</sup>) films of vertical heterostructures
formed by alternating graphene and transition-metal dichalcogenide
(TMD) alloys are obtained by wet chemical routes followed by a thermal
treatment at low temperature. In particular, we synthesized stacked
graphene and W<sub><i>x</i></sub>Mo<sub>1â<i>x</i></sub>S<sub>2</sub> alloy phases that were used as hydrogen
evolution catalysts. We observed a Tafel slope of 38.7 mV dec<sup>â1</sup> and 96 mV onset potential (at current density of
10 mA cm<sup>â2</sup>) when the heterostructure alloy was annealed
at 300 °C. These results indicate that heterostructures formed
by graphene and W<sub>0.4</sub>Mo<sub>0.6</sub>S<sub>2</sub> alloys
are far more efficient than WS<sub>2</sub> and MoS<sub>2</sub> by
at least a factor of 2, and they are superior compared to other reported
TMD systems. This strategy offers a cheap and low temperature synthesis
alternative able to replace Pt in the hydrogen evolution reaction
(HER). Furthermore, the catalytic activity of the alloy is stable
over time, <i>i.e.</i>, the catalytic activity does not experience a significant
change even after 1000 cycles. Using density functional theory calculations,
we found that this enhanced hydrogen evolution in the W<sub><i>x</i></sub>Mo<sub>1â<i>x</i></sub>S<sub>2</sub> alloys is mainly due to the lower energy barrier created by a favorable overlap of the d-orbitals from the transition metals and the s-orbitals of H<sub>2</sub>; with the lowest energy barrier occurring for the W<sub>0.4</sub>Mo<sub>0.6</sub>S<sub>2</sub> alloy. Thus, it is now possible to further improve the performance of the âinertâ TMD basal plane <i>via</i> metal alloying, in addition to the previously reported strategies such as creation of point defects, vacancies and edges. The synthesis of graphene/W<sub>0.4</sub>Mo<sub>0.6</sub>S<sub>2</sub> produced at relatively low temperatures is scalable and could be used as an effective low cost Pt-free catalyst
Clean Nanotube Unzipping by Abrupt Thermal Expansion of Molecular Nitrogen: Graphene Nanoribbons with Atomically Smooth Edges
We report a novel physicochemical route to produce highly crystalline nitrogen-doped graphene nanoribbons. The technique consists of an abrupt N<sub>2</sub> gas expansion within the hollow core of nitrogen-doped multiwalled carbon nanotubes (CN<sub><i>x</i></sub>-MWNTs) when exposed to a fast thermal shock. The multiwalled nanotube unzipping mechanism is rationalized using molecular dynamics and density functional theory simulations, which highlight the importance of open-ended nanotubes in promoting the efficient introduction of N<sub>2</sub> molecules by capillary action within tubes and surface defects, thus triggering an efficient and atomically smooth unzipping. The so-produced nanoribbons could be few-layered (from graphene bilayer onward) and could exhibit both crystalline zigzag and armchair edges. In contrast to methods developed previously, our technique presents various advantages: (1) the tubes are not heavily oxidized; (2) the method yields sharp atomic edges within the resulting nanoribbons; (3) the technique could be scaled up for the bulk production of crystalline nanoribbons from available MWNT sources; and (4) this route could eventually be used to unzip other types of carbon nanotubes or intercalated layered materials such as BN, MoS<sub>2</sub>, WS<sub>2</sub>, <i>etc.</i