4 research outputs found
Surface-Tailored InP Nanowires via Self-Assembled Au Nanodots for Efficient and Stable Photoelectrochemical Hydrogen Evolution
With
a band gap close to the Shockley–Quiesser limit and
excellent conduction band alignment with the water reduction potential,
InP is an ideal photocathode material for photoelectrochemical (PEC)
water reduction. Here, we develop facile self-assembled Au nanodots
based on dewetting phenomena as a masking technique to fabricate wafer-scale
InP nanowires (NWs) via a top-down approach. In addition, we report
dual-function wet treatment using sulfur-dissolved oleylamine (S-OA)
to remove a plasma-damaged surface in a controlled manner and stabilize
InP NWs against surface corrosion in harsh electrolyte solutions.
The resulting InP NW photocathodes exhibit an excellent photocurrent
density of 33 mA/cm2 under 1 sun illumination in 1 M HCl
with a highly stabilized performance without needing additional protection
layers. Our approach combining large-area NW fabrication and surface
engineering synergistically enhances light harvesting and PEC performance
and stability, thereby providing a pathway for the development of
efficient and durable InP photoelectrodes in a scalable manner
InGaAsP as a Promising Narrow Band Gap Semiconductor for Photoelectrochemical Water Splitting
While photoelectrochemical
(PEC) water splitting is a very promising
route toward zero-carbon energy, conversion efficiency remains limited.
Semiconductors with narrower band gaps can absorb a much greater portion
of the solar spectrum, thereby increasing efficiency. However, narrow
band gap (∼1 eV) III–V semiconductor photoelectrodes
have not yet been thoroughly investigated. In this study, the narrow
band gap quaternary III–V alloy InGaAsP is demonstrated for
the first time to have great potential for PEC water splitting, with
the long-term goal of developing high-efficiency tandem PEC devices.
TiO2-coated InGaAsP photocathodes generate a photocurrent
density of over 30 mA/cm2 with an onset potential of 0.45
V versus reversible hydrogen electrode, yielding an applied bias efficiency
of over 7%. This is an excellent performance, given that nearly all
power losses can be attributed to reflection losses. X-ray photoelectron
spectroscopy and photoluminescence spectroscopy show that InGaAsP
and TiO2 form a type-II band alignment, greatly enhancing
carrier separation and reducing recombination losses. Beyond water
splitting, the tunable band gap of InGaAsP could be of further interest
in other areas of photocatalysis, including CO2 reduction
Manipulating Intermediates at the Au–TiO<sub>2</sub> Interface over InP Nanopillar Array for Photoelectrochemical CO<sub>2</sub> Reduction
Photoelectrochemical
(PEC) reduction of CO2 with H2O is a promising
approach to convert solar energy and greenhouse
gas into value-added chemicals or fuels. However, the exact role of
structures and interfaces of photoelectrodes in governing the photoelectrocatalytic
processes in terms of both activity and selectivity remains elusive.
Herein, by systematically investigating the InP photocathodes with
Au–TiO2 interfaces, we discover that nanostructuring
of InP can not only enhance the photoresponse owing to increased light
absorption and prolonged minority carrier lifetime, but also improve
selectivity toward CO production by providing more abundant interfacial
contact points between Au and TiO2 than planar photocathodes.
In addition, theoretical studies on the Au–TiO2 interface
demonstrate that the charge transfer between Au and TiO2, which is locally confined to the interface, strengthens the binding
of the CO* intermediate on positively charged Au interfacial sites,
thus improving CO2 photoelectroreduction to form CO. An
optimal Au–TiO2/InP nanopillar-array photocathode
exhibits an onset potential of +0.3 V vs reversible hydrogen electrode
(RHE) and a Faradaic efficiency of 84.2% for CO production at −0.11
V vs RHE under simulated AM 1.5G illumination at 1 sun. The present
findings of the synergistic effects of the structure and interface
on the photoresponse and selectivity of a photoelectrode provide insights
into the development of III–V semiconductor-based PEC systems
for solar fuel generation
