6 research outputs found
Growth of High-Crystalline, Single-Layer Hexagonal Boron Nitride on Recyclable Platinum Foil
Hexagonal boron nitride (h-BN) is
gaining significant attention
as a two-dimensional dielectric material, along with graphene and
other such materials. Herein, we demonstrate the growth of highly
crystalline, single-layer h-BN on Pt foil through a low-pressure chemical
vapor deposition method that allowed h-BN to be grown over a wide
area (8 × 25 mm<sup>2</sup>). An electrochemical bubbling-based
method was used to transfer the grown h-BN layer from the Pt foil
onto an arbitrary substrate. This allowed the Pt foil, which was not
consumed during the process, to be recycled repeatedly. The UV–visible
absorption spectrum of the single-layer h-BN suggested an optical
band gap of 6.06 eV, while a high-resolution transmission electron
microscopy image of the same showed the presence of distinct hexagonal
arrays of B and N atoms, which were indicative of the highly crystalline
nature and single-atom thickness of the h-BN layer. This method of
growing single-layer h-BN over large areas was also compatible with
use of a sapphire substrate
Catalyst-Free Synthesis of Si-SiO<sub><i>x</i></sub> Core-Shell Nanowire Anodes for High-Rate and High-Capacity Lithium-Ion Batteries
Si-SiO<sub><i>x</i></sub> core-shell nanowires (NWs) ranging from
10 to 30 nm in diameter are prepared by a simple evaporation of silicon
monoxide and control of substrate temperatures without any catalyst.
The Si-SiO<sub><i>x</i></sub> NWs grown at 735 and 955 °C
are strongly anchored to the Cu current collector by forming copper
silicide at the interface between Si and Cu, and subsequently used
as anodes in lithium-ion batteries, in which no binder or conducting
materials are used. The Si-SiO<sub><i>x</i></sub> NWs anodes
show excellent electrochemical performances in terms of capacity retention
and rate capability. In particular, the Si-SiO<sub><i>x</i></sub> NW anode grown at 955 °C shows a reversible capacity
of ∼1000 mAh g<sup>–1</sup> even at a high-rate of 50
C. This catalyst-free synthetic route of Si-SiO<sub><i>x</i></sub> NWs that are strongly anchored to the Cu current collector
opens up an effective process for fabricating other high-capacity
anodes in lithium-ion batteries (LIBs)
Synthesis and Characterization of Patronite Form of Vanadium Sulfide on Graphitic Layer
With the exploding interest in transition
metal chalcogenides,
sulfide minerals containing the dianion S<sub>2</sub><sup>2–</sup>, such as pyrite (FeS<sub>2</sub>), cattierite (CoS<sub>2</sub>),
and vaesite (NiS<sub>2</sub>), have recently attracted much attention
for potential applications in energy conversion and storage devices.
However, the synthesis of the patronite structure (VS<sub>4</sub>,
V<sup>4+</sup>(S<sub>2</sub><sup>2–</sup>)<sub>2</sub>) and
its applications have not yet been clearly demonstrated because of
experimental difficulties and the existence of nonstoichiometric phases.
Herein, we report the synthesis of VS<sub>4</sub> using a simple,
facile hydrothermal method with a graphene oxide (GO) template and
the characterization of the resulting material. Tests of various templates
such as CNT, pyrene, perylene-3,4,9,10-tetracarboxylic dianhydride
(PTCDA), and graphite led us to the conclusion that the graphitic
layer plays a role in the nucleation during growth of VS<sub>4</sub>. Furthermore, the VS<sub>4</sub>/rGO hybrid was proved to be a promising
functional material in energy storage devices
Oxidation Resistance of Iron and Copper Foils Coated with Reduced Graphene Oxide Multilayers
Protecting the surface of metals such as Fe and Cu from oxidizing is of great importance due to their widespread use. Here, oxidation resistance of Fe and Cu foils was achieved by coating them with reduced graphene oxide (rG-O) sheets. The rG-O-coated Fe and Cu foils were prepared by transferring rG-O multilayers from a SiO<sub>2</sub> substrate onto them. The oxidation resistance of these rG-O-coated metal foils was investigated by Raman spectroscopy, optical microscopy, and scanning electron microscopy after heat treatment at 200 °C in air for 2 h. The bare metal surfaces were severely oxidized, but the rG-O-coated metal surfaces were protected from oxidation. This simple solution process using rG-O is one advantage of the present study
Flexible Thermochromic Window Based on Hybridized VO<sub>2</sub>/Graphene
Large-scale integration of vanadium dioxide (VO<sub>2</sub>) on mechanically flexible substrates is critical to the realization of flexible smart window films that can respond to environmental temperatures to modulate light transmittance. Until now, the formation of highly crystalline and stoichiometric VO<sub>2</sub> on flexible substrate has not been demonstrated due to the high-temperature condition for VO<sub>2</sub> growth. Here, we demonstrate a VO<sub>2</sub>-based thermochromic film with unprecedented mechanical flexibility by employing graphene as a versatile platform for VO<sub>2</sub>. The graphene effectively functions as an atomically thin, flexible, yet robust support which enables the formation of stoichiometric VO<sub>2</sub> crystals with temperature-driven phase transition characteristics. The graphene-supported VO<sub>2</sub> was capable of being transferred to a plastic substrate, forming a new type of flexible thermochromic film. The flexible VO<sub>2</sub> films were then integrated into the mock-up house, exhibiting its efficient operation to reduce the in-house temperature under infrared irradiation. These results provide important progress for the fabrication of flexible thermochromic films for energy-saving windows
Probing Evolution of Twist-Angle-Dependent Interlayer Excitons in MoSe<sub>2</sub>/WSe<sub>2</sub> van der Waals Heterostructures
Interlayer
excitons were observed at the heterojunctions in van
der Waals heterostructures (vdW HSs). However, it is not known how
the excitonic phenomena are affected by the stacking order. Here,
we report twist-angle-dependent interlayer excitons in MoSe<sub>2</sub>/WSe<sub>2</sub> vdW HSs based on photoluminescence (PL) and vdW-corrected
density functional theory calculations. The PL intensity of the interlayer
excitons depends primarily on the twist angle: It is enhanced at coherently
stacked angles of 0° and 60° (owing to strong interlayer
coupling) but disappears at incoherent intermediate angles. The calculations
confirm twist-angle-dependent interlayer coupling: The states at the
edges of the valence band exhibit a long tail that stretches over
the other layer for coherently stacked angles; however, the states
are largely confined in the respective layers for intermediate angles.
This interlayer hybridization of the band edge states also correlates
with the interlayer separation between MoSe<sub>2</sub> and WSe<sub>2</sub> layers. Furthermore, the interlayer coupling becomes insignificant,
irrespective of twist angles, by the incorporation of a hexagonal
boron nitride monolayer between MoSe<sub>2</sub> and WSe<sub>2</sub>