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Determining the Conduction Band-Edge Potential of Solar-Cell-Relevant Nb<sub>2</sub>O<sub>5</sub> Fabricated by Atomic Layer Deposition
16
Citations
82
References
2017
Year
Often key to boosting photovoltages in photoelectrochemical and related solar-energy-conversion devices is the preferential slowing of rates of charge recombination-especially recombination at semiconductor/solution, semiconductor/polymer, or semiconductor/perovskite interfaces. In devices featuring TiO<sub>2</sub> as the semiconducting component, a common approach to slowing recombination is to install an ultrathin metal oxide barrier layer or trap-passivating layer atop the semiconductor, with the needed layer often being formed via atomic layer deposition (ALD). A particularly promising barrier layer material is Nb<sub>2</sub>O<sub>5</sub>. Its conduction-band-edge potential E<sub>CB</sub> is low enough that charge injection from an adsorbed molecular, polymeric, or solid-state light absorber and into the semiconductor can still occur, but high enough that charge recombination is inhibited. While a few measurements of E<sub>CB</sub> have been reported for conventionally synthesized, bulk Nb<sub>2</sub>O<sub>5</sub>, none have been described for ALD-fabricated versions. Here, we specifically determine the conduction-band-edge energy of ALD-fabricated Nb<sub>2</sub>O<sub>5</sub> relative to that of TiO<sub>2</sub>. We find that, while the value for ALD-Nb<sub>2</sub>O<sub>5</sub> is indeed higher than that for TiO<sub>2</sub>, the difference is less than anticipated based on measurements of conventionally synthesized Nb<sub>2</sub>O<sub>5</sub> and is dependent on the thermal history of the material. The implications of the findings for optimization of competing interfacial rate processes, and therefore photovoltages, are briefly discussed.
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