5 research outputs found
Real-Time Detection of Acetaldehyde in Electrochemical CO Reduction on Cu Single Crystals
Copper
is known to be versatile in producing various products from
electrochemical CO2 reduction reaction (eCO2RR), and the
product preference depends on reaction environments. The literature
has reported that alkaline electrolytes favor acetate production and
proposed hypotheses on reaction pathways accordingly. However, our
work shows acetate can also come from the fast non-Faradaic chemical
oxidation of acetaldehyde in alkaline environments. This adds uncertainties
into measurements of both acetaldehyde and acetate production and
leads to untrustful investigations on the reaction mechanism as a
consequence. With an electrochemistry-mass spectrometry combined (EC-MS)
system, we not only demonstrate why and how the imprecise acetaldehyde
and acetate production occurs in previous research but also present
immediate detection of acetaldehyde as a function of applied potential
on single crystal Cu electrodes during electrochemical CO reduction
reaction (eCORR). Moreover, the quantified acetaldehyde-to-ethylene
production rate ratio provides insightful information on the acetaldehyde-to-ethylene
bifurcation point in eCO2RR and thus helps understand the reaction
pathways
Tuning Surface Reactivity and Electric Field Strength via Intermetallic Alloying
Many electrosynthesis reactions, such as CO2 reduction
to multicarbon products, involve the formation of dipolar and polarizable
transition states during the rate-determining step. Systematic and
independent control over surface reactivity and electric field strength
would accelerate the discovery of highly active electrocatalysts for
these reactions by providing a means of reducing the transition state
energy through field stabilization. Herein, we demonstrate that intermetallic
alloying enables independent and systematic control over d-band energetics
and work function through the variation of alloy composition and oxophilic
constituent identity, respectively. We identify several intermetallic
phases exhibiting properties that should collectively yield higher
intrinsic activity for CO reduction compared to conventional Cu-based
electrocatalysts. However, we also highlight the propensity of these
alloys to segregate in air as a significant roadblock to investigating
their electrocatalytic activity
Using TiO<sub>2</sub> as a Conductive Protective Layer for Photocathodic H<sub>2</sub> Evolution
Surface passivation is a general issue for Si-based photoelectrodes
because it progressively hinders electron conduction at the semiconductor/electrolyte
interface. In this work, we show that a sputtered 100 nm TiO<sub>2</sub> layer on top of a thin Ti metal layer may be used to protect an
n<sup>+</sup>p Si photocathode during photocatalytic H<sub>2</sub> evolution. Although TiO<sub>2</sub> is a semiconductor, we show
that it behaves like a metallic conductor would under photocathodic
H<sub>2</sub> evolution conditions. This behavior is due to the fortunate
alignment of the TiO<sub>2</sub> conduction band with respect to the
hydrogen evolution potential, which allows it to conduct electrons
from the Si while simultaneously protecting the Si from surface passivation.
By using a Pt catalyst the electrode achieves an H<sub>2</sub> evolution
onset of 520 mV vs NHE and a Tafel slope of 30 mV when illuminated
by the red part (λ > 635 nm) of the AM 1.5 spectrum. The
saturation
photocurrent (H<sub>2</sub> evolution) was also significantly enhanced
by the antireflective properties of the TiO<sub>2</sub> layer. It
was shown that with proper annealing conditions these electrodes could
run 72 h without significant degradation. An Fe<sup>2+</sup>/Fe<sup>3+</sup> redox couple was used to help elucidate details of the band
diagram
Protection of p<sup>+</sup>‑n-Si Photoanodes by Sputter-Deposited Ir/IrO<sub><i>x</i></sub> Thin Films
Sputter deposition of Ir/IrO<sub><i>x</i></sub> on p<sup>+</sup>-n-Si without interfacial
corrosion protection layers yielded
photoanodes capable of efficient water oxidation (OER) in acidic media
(1 M H<sub>2</sub>SO<sub>4</sub>). Stability of at least 18 h was
shown by chronoamperomety at 1.23 V versus RHE (reversible hydrogen
electrode) under 38.6 mW/cm<sup>2</sup> simulated sunlight irradiation
(λ > 635 nm, AM 1.5G) and measurements with quartz crystal
microbalances.
Films exceeding a thickness of 4 nm were shown to be highly active
though metastable due to an amorphous character. By contrast, 2 nm
IrO<sub><i>x</i></sub> films were stable, enabling OER at
a current density of 1 mA/cm<sup>2</sup> at 1.05 V vs. RHE. Further
improvement by heat treatment resulted in a cathodic shift of 40 mV
and enabled a current density of 10 mA/cm<sup>2</sup> (requirements
for a 10% efficient tandem device) at 1.12 V vs. RHS under irradiation.
Thus, the simple IrO<sub><i>x</i></sub>/Ir/p<sup>+</sup>-n-Si structures not only provide the necessary overpotential for
OER at realistic device current, but also harvest ∼100 mV of
free energy (voltage) which makes them among the best-performing Si-based
photoanodes in low-pH media
Comparison of the Performance of CoP-Coated and Pt-Coated Radial Junction n<sup>+</sup>p‑Silicon Microwire-Array Photocathodes for the Sunlight-Driven Reduction of Water to H<sub>2</sub>(g)
The electrocatalytic performance
for hydrogen evolution has been
evaluated for radial-junction n<sup>+</sup>p-Si microwire (MW) arrays
with Pt or cobalt phosphide, CoP, nanoparticulate catalysts in contact
with 0.50 M H<sub>2</sub>SO<sub>4</sub>(aq). The CoP-coated (2.0 mg
cm<sup>–2</sup>) n<sup>+</sup>p-Si MW photocathodes were stable
for over 12 h of continuous operation and produced an open-circuit
photovoltage (<i>V</i><sub>oc</sub>) of 0.48 V, a light-limited
photocurrent density (<i>J</i><sub>ph</sub>) of 17 mA cm<sup>–2</sup>, a fill factor (ff) of 0.24, and an ideal regenerative
cell efficiency (η<sub>IRC</sub>) of 1.9% under simulated 1
Sun illumination. Pt-coated (0.5 mg cm<sup>–2</sup>) n<sup>+</sup>p-Si MW-array photocathodes produced <i>V</i><sub>oc</sub> = 0.44 V, <i>J</i><sub>ph</sub> = 14 mA cm<sup>–2</sup>, ff = 0.46, and η = 2.9% under identical conditions.
Thus, the MW geometry allows the fabrication of photocathodes entirely
comprised of earth-abundant materials that exhibit performance comparable
to that of devices that contain Pt