Photoelectrochemical properties of Cu2O/PANI/Si-based photocathodes for CO2 conversion

光电阴极 材料科学 二氧化碳电化学还原 光催化 光电流 法拉第效率 二氧化钛 氧化物 甲醇 化学工程 无机化学 二氧化碳 电化学 电极 一氧化碳 化学 光电子学 催化作用 复合材料 有机化学 冶金 物理化学 电子 工程类 物理 量子力学
作者
L. Talbi,I. Bozetine,Sabiha Anas Boussaa,K. Benfadel,Djaouida Allam,Nesrine Rahim,Yasmine Ould Mohamed,Markus Leitgeb,C. Torki,Smaïn Hocine,Fatima Boudeffar,Amar Manseri,S. Kaci
出处
期刊:Emerging Materials Research [Thomas Telford Ltd.]
卷期号:12 (1): 78-91 被引量:4
标识
DOI:10.1680/jemmr.22.00167
摘要

The present study was aimed at converting carbon dioxide (CO 2 ) into value-added products such as methanol, which can provide not only a potential solution for controlling the carbon dioxide concentration level in the atmosphere but also can offer an alternative approach for the production of renewable energy sources. From this perspective, various hybrid photoelectrocatalysts were synthesized, characterized and used as photocathodes for photoelectrochemical (PEC) reduction of carbon dioxide to methanol in an aqueous medium under visible light irradiation. Flat silicon (Si) and pyramidal textured silicon (SiPY) substrates, covered with polyaniline (PANI) with or without sensitization with copper (I) oxide (Cu 2 O) particles, were investigated. It was observed that the combination of PANI and copper (I) oxide greatly increased PEC carbon dioxide reduction to methanol owing to the enhancement in the carbon dioxide chemisorption capacity by the photocathode surface and at the same time facilitated the separation of photogenerated electron–hole (e − /h + ) pairs. The PEC results demonstrated that the applied potential impacts the photocurrent stability. Sensitization with copper (I) oxide effectively separated the photogenerated e − /h + pairs and, therefore, enhanced the PEC carbon dioxide reduction activity of the hybrid photocatalyst. The best faradaic efficiency for methanol formation reached 57.66%, which was recorded when the copper (I) oxide/PANI/SiPY heterostructure was used as a photocathode at an applied potential of −1.2 V against the saturated calomel electrode.
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