Photoelectrochemical
(PEC) solar water splitting has received extensive
attention because it promises to provide an alternative and sustainable
source of energy. A key challenge is to achieve a stable PEC system
in either acidic or basic electrolyte without degradation of the (photo)electrodes.
We have used a cubic Cu2O film and porous granular bilayer
Cu2O/CuO composite with a carbon protection layer as photocathode
materials. The films were deposited under different conditions, such
as variation of the electrodeposition time, thermal oxidation of the
Cu2O films in air versus nitrogen atmosphere, and deposition
of the carbon materials, and were investigated structurally and with
regard to their PEC performance. The optimized electrodes showed photocurrents
up to 6.5 and 7.5 mA/cm–2 at potentials of 0 and
−0.1 V vs RHE at pH 5.5, respectively. The stabilities of the
Cu2O/C and Cu2O/CuO/C photocathodes, at a low
bias of 0.3 V vs RHE, were retained after 50 h. The strongly improved
photostability of the photocathodes in comparison to electrodes in
the absence of a carbon overlayer is attributed to a more effective
charge transfer and a protective role of carbon against photocorrosion.
Large research efforts
have been devoted to optimizing the output
of earth-abundant photoabsorbers in solar-to-fuel (S2F) devices. Here,
we report a Cu2O/Ga2O3 heterojunction/Si
microwire photocathode with an underlying buried radial Si p–n
junction, which achieves efficient light harvesting across the visible
spectrum to over 600 nm, reaching an external quantum yield for hydrogen
generation close to 80%, with a photocurrent onset above +1.35 V vs
RHE, a photocurrent density of ∼10 mA/cm2 at 0 V
vs RHE, and an ideal regenerative efficiency of 5.51%. We show step-by-step
the effects of every photocathode design element (i.e., Si p–n
junction, Cu2O layer thickness, microwire length, microwire
pitch, etc.) on the overall efficiency of our final microwire Si/Cu2O photocathode by comparing every addition to a baseline Cu2O photocathode. Lastly, we show a stable operation exceeding
200 h at a bias potential of +1.0 V vs RHE, with an average current
density of 4.5 mA/cm2.
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