Proceedings of Materials for Sustainable Development Conference (MAT-SUS) (NFM22)
DOI: https://doi.org/10.29363/nanoge.nfm.2022.106
Publication date: 11th July 2022
Photoelectrochemical (PEC) solar water splitting could be a potential route to large-scale production of green hydrogen. However, systems based on earth-abundant metal oxides do not yet achieve the high efficiencies required for economically feasible applications. One obstacle to the realization of higher efficiency devices is the appropriate design of the semiconductor-electrolyte interface. In this context, we point out a common misconception that the built-in electric field at the solid-liquid interface is essential for charge separation [1]. A similar discussion, controversial at the time, regarding the role of the built-in field took place in photovoltaic (PV) research community. The purpose of this talk is to present the state-of-the-art knowledge in this field and to seek common ground for an interpretation valid for both photovoltaics and PEC. We hope to provide a more detailed understanding of the energy loss mechanisms and the driving forces that determine charge separation, transport, and recombination of electron and hole pairs in PEC devices. We believe this will be critical for selecting the most appropriate design routes. We emphasize the well-established viewpoint in the photovoltaic research community that the gradient of electrochemical potential is the main driving force for charge separation and efficient solar energy conversion [2]. Based on this insight, we argue that improved (selective) contact design in PEC devices should be one of the most important research directions in PEC device development. To address this challenge, we take a closer look at how optimized contacts have been designed to date and provide examples of potential approaches that may be implement to further improve the performance of PEC devices [3].
Keywords: Water splitting, PEC, charge selective contacts, charge separation, charge transport, interfaces, drift and diffusion, quasi fermi level gradients