5 research outputs found
Layer Control of WSe<sub>2</sub> <i>via</i> Selective Surface Layer Oxidation
We
report Raman and photoluminescence spectra of mono- and few-layer
WSe<sub>2</sub> and MoSe<sub>2</sub> taken before and after exposure
to a remote oxygen plasma. For bilayer and trilayer WSe<sub>2</sub>, we observe an increase in the photoluminescence intensity and a
blue shift of the photoluminescence peak positions after oxygen plasma
treatment. The photoluminescence spectra of trilayer WSe<sub>2</sub> exhibit features of a bilayer after oxygen plasma treatment. Bilayer
WSe<sub>2</sub> exhibits features of a monolayer, and the photoluminescence
of monolayer WSe<sub>2</sub> is completely absent after the oxygen
plasma treatment. These changes are observed consistently in more
than 20 flakes. The mechanism of the changes observed in the photoluminescence
spectra of WSe<sub>2</sub> is due to the selective oxidation of the
topmost layer. As a result, <i>N</i>-layer WSe<sub>2</sub> is reduced to <i>N</i>–1 layers. Raman spectra
and AFM images taken from the WSe<sub>2</sub> flakes before and after
the oxygen treatment corroborate these findings. Because of the low
kinetic energy of the oxygen radicals in the remote oxygen plasma,
the oxidation is self-limiting. By varying the process duration from
1 to 10 min, we confirmed that the oxidation will only affect the
topmost layer of the WSe<sub>2</sub> flakes. X-ray photoelectron spectroscopy
shows that the surface layer WO<sub><i>x</i></sub> of the
sample can be removed by a quick dip in KOH solution. Therefore, this
technique provides a promising way of controlling the thickness of
WSe<sub>2</sub> layer by layer
Microscopic Study of Atomic Layer Deposition of TiO<sub>2</sub> on GaAs and Its Photocatalytic Application
We
report a microscopic study of <i>p</i>-GaAs/TiO<sub>2</sub> heterojunctions using cross-sectional high resolution transmission
electron microscopy (HRTEM). The photocatalytic performance for both
H<sub>2</sub> evolution and CO<sub>2</sub> reduction of these heterostructures
shows a very strong dependence on the thickness of the TiO<sub>2</sub> over the range of 0–15 nm. Thinner films (1–10 nm)
are amorphous and show enhanced catalytic performance with respect
to bare GaAs. HRTEM images and electron energy loss spectroscopy (EELS)
maps show that the native oxide of GaAs is removed by the TiCl<sub>4</sub> atomic layer deposition (ALD) precursor, which is corrosive.
Ti<sup>3+</sup> defect states (i.e., O vacancies) in the TiO<sub>2</sub> film provide catalytically active sites, which improve the photocatalytic
efficiency. Density functional theory (DFT) calculations show that
water molecules and CO<sub>2</sub> molecules bind stably to these
Ti<sup>3+</sup> states. Thicker
TiO<sub>2</sub> films (15 nm) are crystalline and have poor charge
transfer due to their insulating nature, while thinner amorphous TiO<sub>2</sub> films are conducting
Field-Dependent Orientation and Free Energy of D<sub>2</sub>O at an Electrode Surface Observed via SFG Spectroscopy
Polarization-selected vibrational sum frequency generation
(SFG)
spectroscopy of D2O is used to obtain the orientation of
the free OD bond at a monolayer graphene electrode. We modulate the
interfacial field by varying the applied electrochemical potential,
and we measure the resulting change in the orientation. A hyperpolarizability
model is used for the orientational analysis, which assumes a quadratic
free energy orienting potential in the absence of the field, whose
minimum and curvature determine the average tilt angle and the Gaussian
width of the orientational distribution. The average free OD tilt
angle changes in an approximately linear fashion with the applied
field, from 46° from normal at −0.9 V vs Ag/AgCl (E = −0.02 V/Å) to 32° at −3.9 V
vs Ag/AgCl (E = −0.17 V/Å). Using this
approach, we map the free energy profile for the molecular orientation
of interfacial water by measuring the reversible response to an external
perturbation, i.e., a torque applied by an electric field acting on
the molecule’s permanent dipole moment. This allows us to extract
the curvature of the free energy orienting potential of interfacial
water, which is (4.0 ± 0.8) × 10–20 J/rad2 (or 0.25 ± 0.05 eV/rad2 )
Direct <i>In Situ</i> Measurement of Quantum Efficiencies of Charge Separation and Proton Reduction at TiO<sub>2</sub>‑Protected GaP Photocathodes
Photoelectrochemical solar fuel generation at the semiconductor/liquid
interface consists of multiple elementary steps, including charge
separation, recombination, and catalytic reactions. While the overall
incident light-to-current conversion efficiency (IPCE) can be readily
measured, identifying the microscopic efficiency loss processes remains
difficult. Here, we report simultaneous in situ transient
photocurrent and transient reflectance spectroscopy (TRS) measurements
of titanium dioxide-protected gallium phosphide photocathodes for
water reduction in photoelectrochemical cells. Transient reflectance
spectroscopy enables the direct probe of the separated charge carriers
responsible for water reduction to follow their kinetics. Comparison
with transient photocurrent measurement allows the direct probe of
the initial charge separation quantum efficiency (Ï•CS) and provides support for a transient photocurrent model that divides
IPCE into the product of quantum efficiencies of light absorption
(Ï•abs), charge separation (Ï•CS),
and photoreduction (Ï•red), i.e.,
IPCE = ϕabsϕCSϕred. Our study shows that there are two general key loss pathways: recombination
within the bulk GaP that reduces Ï•CS and interfacial
recombination at the junction that decreases Ï•red. Although both loss pathways can be reduced at a more negative applied
bias, for GaP/TiO2, the initial charge separation loss
is the key efficiency limiting factor. Our combined transient reflectance
and photocurrent study provides a time-resolved view of microscopic
steps involved in the overall light-to-current conversion process
and provides detailed insights into the main loss pathways of the
photoelectrochemical system
Confined Liquid-Phase Growth of Crystalline Compound Semiconductors on Any Substrate
The growth of crystalline
compound semiconductors on amorphous
and non-epitaxial substrates is a fundamental challenge for state-of-the-art
thin-film epitaxial growth techniques. Direct growth of materials
on technologically relevant amorphous surfaces, such as nitrides or
oxides results in nanocrystalline thin films or nanowire-type structures,
preventing growth and integration of high-performance devices and
circuits on these surfaces. Here, we show crystalline compound semiconductors
grown directly on technologically relevant amorphous and non-epitaxial
substrates in geometries compatible with standard microfabrication
technology. Furthermore, by removing the traditional epitaxial constraint,
we demonstrate an <i>atomically sharp lateral heterojunction</i> between indium phosphide and tin phosphide, two materials with vastly
different crystal structures, a structure that cannot be grown with
standard vapor-phase growth approaches. Critically, this approach
enables the growth and manufacturing of crystalline materials without
requiring a nearly lattice-matched substrate, potentially impacting
a wide range of fields, including electronics, photonics, and energy
devices