18 research outputs found
High-Performance Broadband Floating-Base Bipolar Phototransistor Based on WSe<sub>2</sub>/BP/MoS<sub>2</sub> Heterostructure
Recently,
there are increasing interests in two-dimensional materials,
as a result of their outstanding electrical and optical properties
and numerous potential applications in optoelectronic devices. Here,
we first report on a bipolar phototransistor based on WSe<sub>2</sub>-BP-MoS<sub>2</sub> van der Waals heterostructure, showing its broadband
photoresponse from visible to the infrared spectral regions. Broadband
photoresponsivities for visible (532 nm) and the infrared (1550 nm)
light waves reach up to 6.32 and 1.12 A W<sup>1–</sup>, respectively,
which are both improved by tens of times in comparison with similar
photodiode devices composed of WSe<sub>2</sub>-BP. The phototransistor
also exhibits ultrasensitive shot noise limit specific detectivities
which are 1.25 × 10<sup>11</sup> Jones for visible light at wavelength
λ = 532 nm and 2.21 × 10<sup>10</sup> Jones for the near-infrared
light at wavelength λ = 1550 nm at room temperature. It is a
promising candidate for progressive development of photodetector,
with implementation of smaller sensor elements, large sensing area,
super-high integration, and broadband photoresponse
Near-Infrared Photodetector Based on MoS<sub>2</sub>/Black Phosphorus Heterojunction
Two-dimensional (2D) materials present
their excellent properties
in electronic and optoelectronic applications, including in ultrafast
carrier dynamics, layer-dependent energy bandgap, tunable optical
properties, low power dissipation, high mobility, transparency, flexibility,
and the ability to confine electromagnetic energy to extremely small
volumes. Herein, we demonstrate a photodetector with visible to near-infrared
detection range, based on the heterojunction fabricated by van der
Waals assembly between few-layer black phosphorus (BP) and few-layer
molybdenum disulfide (MoS<sub>2</sub>). The heterojunction with electrical
characteristics which can be electrically tuned by a gate voltage
achieves a wide range of current-rectifying behavior with a forward-to-reverse
bias current ratio exceeding 10<sup>3</sup>. The photoresponsivity
(<i>R</i>) of the photodetector is about 22.3 A W<sup>–1</sup> measured at λ = 532 nm and 153.4 mA W<sup>–1</sup> at
λ = 1.55 μm with a microsecond response speed (15 μs).
In addition, its specific detectivity <i>D</i>* is calculated
to have the maximum values of 3.1 × 10<sup>11</sup> Jones at
λ = 532 nm, while 2.13 × 10<sup>9</sup> Jones at λ
= 1550 nm at room temperature
Iridium-Catalyzed Anti-Stereoselective Asymmetric Ring-Opening Reactions of Azabenzonorbornadienes with Carboxylic Acids
The first anti-stereoselective
asymmetric ring-opening reactions
of azabenzonorbornadienes with carboxylic acids have been realized
with an iridium catalyst assisted by <sup><i>n</i></sup>Bu<sub>4</sub>NBr. The reaction features broad substrate scope and
good functional group tolerance and allows the synthesis of chiral
dihydronaphthalene derivatives with high optical purities
Facile Preparation of Superelastic and Ultralow Dielectric Boron Nitride Nanosheet Aerogels via Freeze-Casting Process
As a structural analogue of graphene,
boron nitride nanosheets
(BNNSs) have attracted ever-growing research interest in the past
few years, due to their remarkably mechanical, electrical, and thermal
properties. The preparation of BNNS aerogels is considered to be one
of the most effective approaches for their practical applications.
However, it has remained a great challenge to fabricate BNNS aerogels
with superelasticity by a facile method. Here, we report the preparation
of BNNS aerogels via a facile method involving polymer-assisted cross-linking
and freeze-casting strategies. The resulting aerogels exhibit a well-ordered
and anisotropic microstructure, leading to anisotropic superelasticity,
high compressive strength, and excellent energy absorption ability.
The unique microstructure also endows the aerogels with ultralow dielectric
constant (1.24) and loss (∼0.003). The successful fabrication
of such fascinating materials paves the way for application of BNNSs
in energy-absorbing services, catalyst carrier, and environmental
remediation, etc
High-Quality Large-Area Graphene from Dehydrogenated Polycyclic Aromatic Hydrocarbons
Recent studies show that, at the initial stage of chemical
vapor
deposition (CVD) of graphene, the isolated carbon monomers will form
defective carbon clusters with pentagons that degrade the quality
of synthesized graphene. To circumvent this problem, we demonstrate
that high-quality centimeter-sized graphene sheets can be synthesized
on Cu foils by a self-assembled approach from defect-free polycyclic
aromatic hydrocarbons (PAHs) in a high vacuum (HV) chamber without
hydrogen. Different molecular motifs, namely coronene, pentacene,
and rubrene, can lead to significant difference in the quality of
resulting graphene. For coronene, monolayer graphene flakes with an
adequate quality can be achieved at a growth temperature as low as
550 °C. For the graphene obtained at 1000 °C, transport
measurements performed on back-gated field-effect transistors (FETs)
with large channel lengths (∼30 μm) exhibit a carrier
mobility up to ∼5300 cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>at room temperature. The underlying growth mechanism,
which mainly involves surface-mediated nucleation process of dehydrogenated
PAHs rather than segregation or precipitation process of small carbon
species decomposed from the precursors, has been systematically investigated
through the first-principles calculations. Our findings pave the way
for optimizing selection of solid carbon precursors and open up a
new route for graphene synthesis
Variable thermal transport in black, blue, and violet phosphorene from extensive atomistic simulations with a neuroevolution potential
Phosphorus has diverse chemical bonds, and even in its two-dimensional form, there are three stable allotropes: black phosphorene (Black-P), blue phosphorene (Blue-P), and violet phosphorene (Violet-P). Due to the complexity of these structures, no efficient and accurate classical interatomic potential has been developed for them. In this paper, we develop an efficient machine-learned neuroevolution potential model for these allotropes and apply it to study thermal transport in them via extensive molecular dynamics (MD) simulations. Based on the homogeneous nonequilibrium MD method, the thermal conductivities are predicted to be 12.5±0.2 (Black-P in armchair direction), 78.4±0.4 (Black-P in zigzag direction), 128±3 (Blue-P), and 2.36±0.05 (Violet-P) Wm−1K−1. The underlying reasons for the significantly different thermal conductivity values in these allotropes are unraveled through spectral decomposition, phonon eigenmodes, and phonon participation ratio. Under external tensile strain, the thermal conductivity in black-P and violet-P are finite, while that in blue-P appears unbounded due to the linearization of the flexural phonon dispersion that increases the phonon mean free paths in the zero-frequency limit.</p
Facile Preparation of Superelastic and Ultralow Dielectric Boron Nitride Nanosheet Aerogels via Freeze-Casting Process
As a structural analogue of graphene,
boron nitride nanosheets
(BNNSs) have attracted ever-growing research interest in the past
few years, due to their remarkably mechanical, electrical, and thermal
properties. The preparation of BNNS aerogels is considered to be one
of the most effective approaches for their practical applications.
However, it has remained a great challenge to fabricate BNNS aerogels
with superelasticity by a facile method. Here, we report the preparation
of BNNS aerogels via a facile method involving polymer-assisted cross-linking
and freeze-casting strategies. The resulting aerogels exhibit a well-ordered
and anisotropic microstructure, leading to anisotropic superelasticity,
high compressive strength, and excellent energy absorption ability.
The unique microstructure also endows the aerogels with ultralow dielectric
constant (1.24) and loss (∼0.003). The successful fabrication
of such fascinating materials paves the way for application of BNNSs
in energy-absorbing services, catalyst carrier, and environmental
remediation, etc
Rhodium-Catalyzed Asymmetric Cyclization/Addition Reactions of 1,6-Enynes and Oxa/Azabenzonorbornadienes
A mild, efficient, and novel rhodium
catalyzed asymmetric cyclization–addition
domino reaction of oxa/azabenzonorbornadienes and 1,6-enynes is documented.
Through the use of a [RhÂ(COD)<sub>2</sub>]ÂBF<sub>4</sub>-(<i>R</i>)-An-SDP catalytic system, highly enantioenriched cyclization–addition
products were obtained in good yields and with excellent enantioselectivities
Enhanced Performance of Polymeric Bulk Heterojunction Solar Cells via Molecular Doping with TFSA
Organic solar cells based on bisÂ(trifluoromethanesulfonyl)Âamide
(TFSA, [CF<sub>3</sub>SO<sub>2</sub>]<sub>2</sub>NH) bulk doped polyÂ[<i>N</i>-9′′-hepta-decanyl-2,7-carbazole-<i>alt</i>-5,5-(4′,7′-di-2-thienyl-2′,1′,3′-benzothiadiazole)
(PCDTBT):C<sub>71</sub>-butyric acid methyl ester (PC<sub>71</sub>BM) were fabricated to study the effect of molecular doping. By adding
TFSA (0.2–0.8 wt %, TFSA to PCDTBT) in the conventional PCDTBT:PC<sub>71</sub>BM blends, we found that the hole mobility was increased
with the reduced series resistance in photovoltaic devices. The p-doping
effect of TFSA was confirmed by photoemission spectroscopy that the
Fermi level of doped PCDTBT shifts downward to the HOMO level and
it results in a larger internal electrical field at the donor/acceptor
interface for more efficient charge transfer. Moreover, the doping
effect was also confirmed by charge modulated electroabsorption spectroscopy
(CMEAS), showing that there are additional polaron signals in the
sub-bandgap region in the doped thin films. With decreased series
resistance, the open-circuit voltage (<i>V</i><sub>oc</sub>) was increased from 0.85 to 0.91 V and the fill factor (FF) was
improved from 60.7% to 67.3%, resulting in a largely enhanced power
conversion efficiency (PCE) from 5.39% to 6.46%. Our finding suggests
the molecular doping by TFSA can be a facile approach to improve the
electrical properties of organic materials for future development
of organic photovoltaic devices (OPVs)
Solution-Processed Ambipolar Organic Thin-Film Transistors by Blending p- and n‑Type Semiconductors: Solid Solution versus Microphase Separation
Here,
we report solid solution of p- and n-type organic semiconductors as
a new type of p–n blend for solution-processed ambipolar organic
thin film transistors (OTFTs). This study compares the solid-solution
films of silylethynylated tetraazapentacene <b>1</b> (acceptor)
and silylethynylated pentacene <b>2</b> (donor) with the microphase-separated
films of <b>1</b> and <b>3</b>, a heptagon-embedded analogue
of <b>2</b>. It is found that the solid solutions of (<b>1</b>)<sub><i>x</i></sub>(<b>2</b>)<sub>1–<i>x</i></sub> function as ambipolar semiconductors, whose hole
and electron mobilities are tunable by varying the ratio of <b>1</b> and <b>2</b> in the solid solution. The OTFTs of (<b>1</b>)<sub>0.5</sub>(<b>2</b>)<sub>0.5</sub> exhibit relatively
balanced hole and electron mobilities comparable to the highest values
as reported for ambipolar OTFTs of stoichiometric donor–acceptor
cocrystals and microphase-separated p-n bulk heterojunctions. The
solid solution of (<b>1</b>)<sub>0.5</sub>(<b>2</b>)<sub>0.5</sub> and the microphase-separated blend of <b>1:3</b> (0.5:0.5)
in OTFTs exhibit different responses to light in terms of absorption
and photoeffect of OTFTs because the donor and acceptor are mixed
at molecular level with π–π stacking in the solid
solution