5 research outputs found

    Using TiO<sub>2</sub> as a Conductive Protective Layer for Photocathodic H<sub>2</sub> Evolution

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    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

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    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)

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    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
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