8 research outputs found
Air-Stable Surface Charge Transfer Doping of MoS<sub>2</sub> by Benzyl Viologen
Air-stable
doping of transition metal dichalcogenides is of fundamental
importance to enable a wide range of optoelectronic and electronic
devices while exploring their basic material properties. Here we demonstrate
the use of benzyl viologen (BV), which has one of the highest reduction
potentials of all electron-donor organic compounds, as a surface charge
transfer donor for MoS<sub>2</sub> flakes. The n-doped samples exhibit
excellent stability in both ambient air and vacuum. Notably, we obtained
a high electron sheet density of ∼1.2 × 10<sup>13</sup> cm<sup>–2</sup>, which corresponds to the degenerate doping
limit for MoS<sub>2</sub>. The BV dopant molecules can be reversibly
removed by immersion in toluene, providing the ability to control
the carrier sheet density as well as selective removal of surface
dopants on demand. By BV doping of MoS<sub>2</sub> at the metal junctions,
the contact resistances are shown to be reduced by a factor of >3.
As a proof of concept, top-gated field-effect transistors were fabricated
with BV-doped n<sup>+</sup> source/drain contacts self-aligned with
respect to the top gate. The device architecture, resembling that
of the conventional Si transistors, exhibited excellent switching
characteristics with a subthreshold swing of ∼77 mV/decade
Field-Effect Transistors Built from All Two-Dimensional Material Components
We demonstrate field-effect transistors using heterogeneously stacked two-dimensional materials for all of the components, including the semiconductor, insulator, and metal layers. Specifically, MoS<sub>2</sub> is used as the active channel material, hexagonal-BN as the top-gate dielectric, and graphene as the source/drain and the top-gate contacts. This transistor exhibits n-type behavior with an ON/OFF current ratio of >10<sup>6</sup>, and an electron mobility of ∼33 cm<sup>2</sup>/V·s. Uniquely, the mobility does not degrade at high gate voltages, presenting an important advantage over conventional Si transistors where enhanced surface roughness scattering severely reduces carrier mobilities at high gate-fields. A WSe<sub>2</sub>–MoS<sub>2</sub> diode with graphene contacts is also demonstrated. The diode exhibits excellent rectification behavior and a low reverse bias current, suggesting high quality interfaces between the stacked layers. In this work, all interfaces are based on van der Waals bonding, presenting a unique device architecture where crystalline, layered materials with atomically uniform thicknesses are stacked on demand, without the lattice parameter constraints. The results demonstrate the promise of using an all-layered material system for future electronic applications
Strain-Induced Indirect to Direct Bandgap Transition in Multilayer WSe<sub>2</sub>
Transition
metal dichalcogenides, such as MoS<sub>2</sub> and WSe<sub>2</sub>, have recently gained tremendous interest for electronic
and optoelectronic applications. MoS<sub>2</sub> and WSe<sub>2</sub> monolayers are direct bandgap and show bright photoluminescence
(PL), whereas multilayers exhibit much weaker PL due to their indirect
optical bandgap. This presents an obstacle for a number of device
applications involving light harvesting or detection where thicker
films with direct optical bandgap are desired. Here, we experimentally
demonstrate a drastic enhancement in PL intensity for multilayer WSe<sub>2</sub> (2–4 layers) under uniaxial tensile strain of up to
2%. Specifically, the PL intensity of bilayer WSe<sub>2</sub> is amplified
by ∼35× , making it comparable to that of an unstrained
WSe<sub>2</sub> monolayer. This drastic PL enhancement is attributed
to an indirect to direct bandgap transition for strained bilayer WSe<sub>2</sub>, as confirmed by density functional theory (DFT) calculations.
Notably, in contrast to MoS<sub>2</sub> multilayers, the energy difference
between the direct and indirect bandgaps of WSe<sub>2</sub> multilayers
is small, thus allowing for bandgap crossover at experimentally feasible
strain values. Our results present an important advance toward controlling
the band structure and optoelectronic properties of few-layer WSe<sub>2</sub> via strain engineering, with important implications for practical
device applications
Dynamic Changes in Heparan Sulfate Nanostructure in Human Pluripotent Stem Cell Differentiation
Heparan sulfate (HS) is a heterogeneous,
cell-surface polysaccharide
critical for transducing signals essential for mammalian development.
Imaging of signaling proteins has revealed how their localization
influences their information transfer. In contrast, the contribution
of the spatial distribution and nanostructure of information-rich,
signaling polysaccharides like HS is not known. Using expansion microscopy
(ExM), we found striking changes in HS nanostructure occur as human
pluripotent stem (hPS) cells differentiate, and these changes correlate
with growth factor signaling. Our imaging studies show that undifferentiated
hPS cells are densely coated with HS displayed as hair-like protrusions.
This ultrastructure can recruit fibroblast growth factor for signaling.
When the hPS cells differentiate into the ectoderm lineage, HS is
localized into dispersed puncta. This striking change in HS distribution
coincides with a decrease in fibroblast growth factor binding to neural
cells. While developmental variations in HS sequence were thought
to be the primary driver of alterations in HS-mediated growth factor
signaling, our high-resolution images indicate a role for the HS nanostructure.
Our study highlights the utility of high-resolution glycan imaging
using ExM. In the case of HS, we found that changes in how the polysaccharide
is displayed link to profound differences in growth factor binding
Dynamic Changes in Heparan Sulfate Nanostructure in Human Pluripotent Stem Cell Differentiation
Heparan sulfate (HS) is a heterogeneous,
cell-surface polysaccharide
critical for transducing signals essential for mammalian development.
Imaging of signaling proteins has revealed how their localization
influences their information transfer. In contrast, the contribution
of the spatial distribution and nanostructure of information-rich,
signaling polysaccharides like HS is not known. Using expansion microscopy
(ExM), we found striking changes in HS nanostructure occur as human
pluripotent stem (hPS) cells differentiate, and these changes correlate
with growth factor signaling. Our imaging studies show that undifferentiated
hPS cells are densely coated with HS displayed as hair-like protrusions.
This ultrastructure can recruit fibroblast growth factor for signaling.
When the hPS cells differentiate into the ectoderm lineage, HS is
localized into dispersed puncta. This striking change in HS distribution
coincides with a decrease in fibroblast growth factor binding to neural
cells. While developmental variations in HS sequence were thought
to be the primary driver of alterations in HS-mediated growth factor
signaling, our high-resolution images indicate a role for the HS nanostructure.
Our study highlights the utility of high-resolution glycan imaging
using ExM. In the case of HS, we found that changes in how the polysaccharide
is displayed link to profound differences in growth factor binding
Dynamic Changes in Heparan Sulfate Nanostructure in Human Pluripotent Stem Cell Differentiation
Heparan sulfate (HS) is a heterogeneous,
cell-surface polysaccharide
critical for transducing signals essential for mammalian development.
Imaging of signaling proteins has revealed how their localization
influences their information transfer. In contrast, the contribution
of the spatial distribution and nanostructure of information-rich,
signaling polysaccharides like HS is not known. Using expansion microscopy
(ExM), we found striking changes in HS nanostructure occur as human
pluripotent stem (hPS) cells differentiate, and these changes correlate
with growth factor signaling. Our imaging studies show that undifferentiated
hPS cells are densely coated with HS displayed as hair-like protrusions.
This ultrastructure can recruit fibroblast growth factor for signaling.
When the hPS cells differentiate into the ectoderm lineage, HS is
localized into dispersed puncta. This striking change in HS distribution
coincides with a decrease in fibroblast growth factor binding to neural
cells. While developmental variations in HS sequence were thought
to be the primary driver of alterations in HS-mediated growth factor
signaling, our high-resolution images indicate a role for the HS nanostructure.
Our study highlights the utility of high-resolution glycan imaging
using ExM. In the case of HS, we found that changes in how the polysaccharide
is displayed link to profound differences in growth factor binding
Air Stable p‑Doping of WSe<sub>2</sub> by Covalent Functionalization
Covalent functionalization of transition metal dichalcogenides (TMDCs) is investigated for air-stable chemical doping. Specifically, p-doping of WSe<sub>2</sub> <i>via</i> NO<sub><i>x</i></sub> chemisorption at 150 °C is explored, with the hole concentration tuned by reaction time. Synchrotron based soft X-ray absorption spectroscopy (XAS) and X-ray photoelectron spectroscopy (XPS) depict the formation of various WSe<sub>2–<i>x</i>–<i>y</i></sub>O<sub><i>x</i></sub>N<sub><i>y</i></sub> species both on the surface and interface between layers upon chemisorption reaction. <i>Ab initio</i> simulations corroborate our spectroscopy results in identifying the energetically favorable complexes, and predicting WSe<sub>2</sub>:NO at the Se vacancy sites as the predominant dopant species. A maximum hole concentration of ∼10<sup>19</sup> cm<sup>–3</sup> is obtained from XPS and electrical measurements, which is found to be independent of WSe<sub>2</sub> thickness. This degenerate doping level facilitates 5 orders of magnitude reduction in contact resistance between Pd, a common p-type contact metal, and WSe<sub>2</sub>. More generally, the work presents a platform for manipulating the electrical properties and band structure of TMDCs using covalent functionalization
Engineering Light Outcoupling in 2D Materials
When light is incident on 2D transition
metal dichalcogenides (TMDCs), it engages in multiple reflections
within underlying substrates, producing interferences that lead to
enhancement or attenuation of the incoming and outgoing strength of
light. Here, we report a simple method to engineer the light outcoupling
in semiconducting TMDCs by modulating their dielectric surroundings.
We show that by modulating the thicknesses of underlying substrates
and capping layers, the interference caused by substrate can significantly
enhance the light absorption and emission of WSe<sub>2</sub>, resulting
in a ∼11 times increase in Raman signal and a ∼30 times
increase in the photoluminescence (PL) intensity of WSe<sub>2</sub>. On the basis of the interference model, we also propose a strategy
to control the photonic and optoelectronic properties of thin-layer
WSe<sub>2</sub>. This work demonstrates the utilization of outcoupling
engineering in 2D materials and offers a new route toward the realization
of novel optoelectronic devices, such as 2D LEDs and solar cells