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Issue 44, 2016
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Understanding charge transport in non-doped pristine and surface passivated hematite (Fe2O3) nanorods under front and backside illumination in the context of light induced water splitting

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Abstract

Hematite (Fe2O3) nanorods on FTO substrates have been proven to be promising photoanodes for solar fuel production but only with high temperature thermal activation which allows diffusion of tin (Sn) ions from FTO, eventually enhancing their conductivity. Hence, there is a trade-off between the conductivity of Fe2O3, and the degradation of FTO occurring at high annealing temperatures (>750 °C). Here, we present a comprehensive study on undoped Fe2O3 nanorods under front and back illumination to find the optimum annealing temperature. Bulk/surface charge transport efficiency analysis demonstrates minimum bulk recombination indicating overall high quality crystalline Fe2O3 and the preservation of FTO conductivity. Surface recombination is further improved by growing a TiOx overlayer, which improves the photocurrent density from 0.2 mA cm−2 (backside) to 1.2 mA cm−2 under front side and 0.8 mA cm−2 under backside illumination. It is evident from this study that the performance of undoped and unpassivated hematite nanorods is limited by electron transport, whereas that of doped/passivated hematite nanorods is limited by hole transport.

Graphical abstract: Understanding charge transport in non-doped pristine and surface passivated hematite (Fe2O3) nanorods under front and backside illumination in the context of light induced water splitting

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Publication details

The article was received on 03 Aug 2016, accepted on 10 Oct 2016 and first published on 10 Oct 2016


Article type: Communication
DOI: 10.1039/C6CP05379C
Citation: Phys. Chem. Chem. Phys., 2016,18, 30370-30378
  • Open access: Creative Commons BY-NC license
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    Understanding charge transport in non-doped pristine and surface passivated hematite (Fe2O3) nanorods under front and backside illumination in the context of light induced water splitting

    P. S. Bassi, L. Xianglin, Y. Fang, J. S. C. Loo, J. Barber and L. H. Wong, Phys. Chem. Chem. Phys., 2016, 18, 30370
    DOI: 10.1039/C6CP05379C

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