9 research outputs found
Spectroscopic Signatures for Interlayer Coupling in MoS<sub>2</sub>–WSe<sub>2</sub> van der Waals Stacking
Stacking of MoS<sub>2</sub> and WSe<sub>2</sub> monolayers is conducted by transferring triangular MoS<sub>2</sub> monolayers on top of WSe<sub>2</sub> monolayers, all grown by chemical vapor deposition (CVD). Raman spectroscopy and photoluminescence (PL) studies reveal that these mechanically stacked monolayers are not closely coupled, but after a thermal treatment at 300 °C, it is possible to produce van der Waals solids consisting of two interacting transition metal dichalcogenide (TMD) monolayers. The layer-number sensitive Raman out-of-plane mode A<sup>2</sup><sub>1g</sub> for WSe<sub>2</sub> (309 cm<sup>–1</sup>) is found sensitive to the coupling between two TMD monolayers. The presence of interlayer excitonic emissions and the changes in other intrinsic Raman modes such as E″ for MoS<sub>2</sub> at 286 cm<sup>–1</sup> and A<sup>2</sup><sub>1g</sub> for MoS<sub>2</sub> at around 463 cm<sup>–1</sup> confirm the enhancement of the interlayer coupling
Second Harmonic Generation from Artificially Stacked Transition Metal Dichalcogenide Twisted Bilayers
Optical second harmonic generation (SHG) is known as a sensitive probe to the crystalline symmetry of few-layer transition metal dichalcogenides (TMDs). Layer-number dependent and polarization resolved SHG have been observed for the special case of Bernal stacked few-layer TMDs, but it remains largely unexplored for structures deviated from this ideal stacking order. Here we report on the SHG from homo- and heterostructural TMD bilayers formed by artificial stacking with an arbitrary stacking angle. The SHG from the twisted bilayers is a coherent superposition of the SH fields from the individual layers, with a phase difference depending on the stacking angle. Such an interference effect is insensitive to the constituent layered materials and thus applicable to hetero-stacked bilayers. A proof-of-concept demonstration of using the SHG to probe the domain boundary and crystal polarity of mirror twins formed in chemically grown TMDs is also presented. We show here that the SHG is an efficient, sensitive, and nondestructive characterization for the stacking orientation, crystal polarity, and domain boundary of van der Waals heterostructures made of noncentrosymmetric layered materials
Ultrafast Transient Terahertz Conductivity of Monolayer MoS<sub>2</sub> and WSe<sub>2</sub> Grown by Chemical Vapor Deposition
We have measured ultrafast charge carrier dynamics in monolayers and trilayers of the transition metal dichalcogenides MoS<sub>2</sub> and WSe<sub>2</sub> using a combination of time-resolved photoluminescence and terahertz spectroscopy. We recorded a photoconductivity and photoluminescence response time of just 350 fs from CVD-grown monolayer MoS<sub>2</sub>, and 1 ps from trilayer MoS<sub>2</sub> and monolayer WSe<sub>2</sub>. Our results indicate the potential of these materials as high-speed optoelectronic materials
Large-Area Synthesis of Highly Crystalline WSe<sub>2</sub> Monolayers and Device Applications
The monolayer transition metal dichalcogenides have recently attracted much attention owing to their potential in valleytronics, flexible and low-power electronics, and optoelectronic devices. Recent reports have demonstrated the growth of large-size two-dimensional MoS<sub>2</sub> layers by the sulfurization of molybdenum oxides. However, the growth of a transition metal selenide monolayer has still been a challenge. Here we report that the introduction of hydrogen in the reaction chamber helps to activate the selenization of WO<sub>3</sub>, where large-size WSe<sub>2</sub> monolayer flakes or thin films can be successfully grown. The top-gated field-effect transistors based on WSe<sub>2</sub> monolayers using ionic gels as the dielectrics exhibit ambipolar characteristics, where the hole and electron mobility values are up to 90 and 7 cm<sup>2</sup>/Vs, respectively. These films can be transferred onto arbitrary substrates, which may inspire research efforts to explore their properties and applications. The resistor-loaded inverter based on a WSe<sub>2</sub> film, with a gain of ∼13, further demonstrates its applicability for logic-circuit integrations
Observing Grain Boundaries in CVD-Grown Monolayer Transition Metal Dichalcogenides
Two-dimensional monolayer transition metal dichalcogenides (TMdCs), driven by graphene science, revisit optical and electronic properties, which are markedly different from bulk characteristics. These properties are easily modified due to accessibility of all the atoms viable to ambient gases, and therefore, there is no guarantee that impurities and defects such as vacancies, grain boundaries, and wrinkles behave as those of ideal bulk. On the other hand, this could be advantageous in engineering such defects. Here, we report a method of observing grain boundary distribution of monolayer TMdCs by a selective oxidation. This was implemented by exposing directly the TMdC layer grown on sapphire without transfer to ultraviolet light irradiation under moisture-rich conditions. The generated oxygen and hydroxyl radicals selectively functionalized defective grain boundaries in TMdCs to provoke morphological changes at the boundary, where the grain boundary distribution was observed by atomic force microscopy and scanning electron microscopy. This paves the way toward the investigation of transport properties engineered by defects and grain boundaries
Multilayer Graphene–WSe<sub>2</sub> Heterostructures for WSe<sub>2</sub> Transistors
Two-dimensional (2D) materials are
drawing growing attention for next-generation electronics and optoelectronics
owing to its atomic thickness and unique physical properties. One
of the challenges posed by 2D materials is the large source/drain
(S/D) series resistance due to their thinness, which may be resolved
by thickening the source and drain regions. Recently explored lateral
graphene–MoS<sub>2</sub>− and graphene–WS<sub>2</sub>, heterostructures shed light on resolving the mentioned
issues owing to their superior ohmic contact behaviors. However, recently
reported field-effect transistors (FETs) based on graphene–TMD
heterostructures have only shown n-type characteristics. The lack
of p-type transistor limits their applications in complementary metal-oxide
semiconductor electronics. In this work, we demonstrate p-type FETs
based on graphene–WSe<sub>2</sub> lateral heterojunctions grown
with the scalable CVD technique. Few-layer WSe<sub>2</sub> is overlapped
with the multilayer graphene (MLG) at MLG–WSe<sub>2</sub> junctions
such that the contact resistance is reduced. Importantly, the few-layer
WSe<sub>2</sub> only forms at the junction region while the channel
is still maintained as a WSe<sub>2</sub> monolayer for transistor
operation. Furthermore, by imposing doping to graphene S/D, 2 orders
of magnitude enhancement in <i>I</i><sub>on</sub>/<i>I</i><sub>off</sub> ratio to ∼10<sup>8</sup> and the
unipolar p<i>-</i>type characteristics are obtained regardless
of the work function of the metal in ambient air condition. The MLG
is proposed to serve as a 2D version of emerging raised source/drain
approach in electronics
Selectively Plasmon-Enhanced Second-Harmonic Generation from Monolayer Tungsten Diselenide on Flexible Substrates
Monolayer
two-dimensional transition-metal dichalcogenides (2D
TMDCs) exhibit promising characteristics in miniaturized nonlinear
optical frequency converters, due to their inversion asymmetry and
large second-order nonlinear susceptibility. However, these materials
usually have very short light interaction lengths with the pump laser
because they are atomically thin, such that second-harmonic generation
(SHG) is generally inefficient. In this paper, we fabricate a judiciously
structured 150 nm-thick planar surface consisting of monolayer tungsten
diselenide and sub-20 nm-wide gold trenches on flexible substrates,
reporting ∼7000-fold SHG enhancement without peak broadening
or background in the spectra as compared to WSe<sub>2</sub> on as-grown
sapphire substrates. Our proof-of-concept experiment yields effective
second-order nonlinear susceptibility of 2.1 × 10<sup>4</sup> pm/V. Three orders of magnitude enhancement is maintained with pump
wavelength ranging from 800 to 900 nm, breaking the limitation of
narrow pump wavelength range for cavity-enhanced SHG. In addition,
SHG amplitude can be dynamically controlled <i>via</i> selective
excitation of the lateral gap plasmon by rotating the laser polarization.
Such a fully open, flat, and ultrathin profile enables a great variety
of functional samples with high SHG from one patterned silicon substrate,
favoring scalable production of nonlinear converters. The surface
accessibility also enables integration with other optical components
for information processing in an ultrathin and flexible form
Photoluminescence Enhancement and Structure Repairing of Monolayer MoSe<sub>2</sub> by Hydrohalic Acid Treatment
Atomically thin two-dimensional transition-metal
dichalcogenides
(TMDCs) have attracted much attention recently due to their unique
electronic and optical properties for future optoelectronic devices.
The chemical vapor deposition (CVD) method is able to generate TMDCs
layers with a scalable size and a controllable thickness. However,
the TMDC monolayers grown by CVD may incorporate structural defects,
and it is fundamentally important to understand the relation between
photoluminescence and structural defects. In this report, point defects
(Se vacancies) and oxidized Se defects in CVD-grown MoSe<sub>2</sub> monolayers are identified by transmission electron microscopy and
X-ray photoelectron spectroscopy. These defects can significantly
trap free charge carriers and localize excitons, leading to the smearing
of free band-to-band exciton emission. Here, we report that the simple
hydrohalic acid treatment (such as HBr) is able to efficiently suppress
the trap-state emission and promote the neutral exciton and trion
emission in defective MoSe<sub>2</sub> monolayers through the <i>p</i>-doping process, where the overall photoluminescence intensity
at room temperature can be enhanced by a factor of 30. We show that
HBr treatment is able to activate distinctive trion and free exciton
emissions even from highly defective MoSe<sub>2</sub> layers. Our
results suggest that the HBr treatment not only reduces the <i>n</i>-doping in MoSe<sub>2</sub> but also reduces the structural
defects. The results provide further insights of the control and tailoring
the exciton emission from CVD-grown monolayer TMDCs
Monolayer MoSe<sub>2</sub> Grown by Chemical Vapor Deposition for Fast Photodetection
Monolayer molybdenum disulfide (MoS<sub>2</sub>) has become a promising building block in optoelectronics for its high photosensitivity. However, sulfur vacancies and other defects significantly affect the electrical and optoelectronic properties of monolayer MoS<sub>2</sub> devices. Here, highly crystalline molybdenum diselenide (MoSe<sub>2</sub>) monolayers have been successfully synthesized by the chemical vapor deposition (CVD) method. Low-temperature photoluminescence comparison for MoS<sub>2</sub> and MoSe<sub>2</sub> monolayers reveals that the MoSe<sub>2</sub> monolayer shows a much weaker bound exciton peak; hence, the phototransistor based on MoSe<sub>2</sub> presents a much faster response time (<25 ms) than the corresponding 30 s for the CVD MoS<sub>2</sub> monolayer at room temperature in ambient conditions. The images obtained from transmission electron microscopy indicate that the MoSe exhibits fewer defects than MoS<sub>2</sub>. This work provides the fundamental understanding for the differences in optoelectronic behaviors between MoSe<sub>2</sub> and MoS<sub>2</sub> and is useful for guiding future designs in 2D material-based optoelectronic devices