Improving the Back Surface Field on an Amorphous Silicon Carbide Thin Film Photocathode for Solar Water Splitting

Journal Article (2018)
Author(s)

Paula Perez-Rodriguez (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Drialys Cardenas-Morcoso (Universitat Jaume I)

Ibadillah A. Digdaya (TU Delft - Applied Sciences)

Andrea Mangel Raventos (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Paul Procel (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Olindo Isabella (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Sixto Gimenez (Universitat Jaume I)

Miro Zeman (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Wilson A. Smith (TU Delft - Applied Sciences)

Arno H.M. Smets (TU Delft - Electrical Engineering, Mathematics and Computer Science)

Research Group
Photovoltaic Materials and Devices
DOI related publication
https://doi.org/10.1002/cssc.201800782 Final published version
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Publication Year
2018
Language
English
Research Group
Photovoltaic Materials and Devices
Bibliographical Note
Accepted Author Manuscript
Journal title
ChemSusChem
Issue number
11
Volume number
11
Pages (from-to)
1797-1804
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366
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Abstract

Amorphous silicon carbide (a-SiC:H) is a promising material for photoelectrochemical water splitting owing to its relatively small band-gap energy and high chemical and optoelectrical stability. This work studies the interplay between charge-carrier separation and collection, and their injection into the electrolyte, when modifying the semiconductor/electrolyte interface. By introducing an n-doped nanocrystaline silicon oxide layer into a p-doped/intrinsic a-SiC:H photocathode, the photovoltage and photocurrent of the device can be significantly improved, reaching values higher than 0.8V. This results from enhancing the internal electric field of the photocathode, reducing the Shockley-Read-Hall recombination at the crucial interfaces because of better charge-carrier separation. In addition, the charge-carrier injection into the electrolyte is enhanced by introducing a TiO2 protective layer owing to better band alignment at the interface. Finally, the photocurrent was further enhanced by tuning the absorber layer thickness, arriving at a thickness of 150nm, after which the current saturates to 10mAcm-2 at 0V vs. the reversible hydrogen electrode in a 0.2m aqueous potassium hydrogen phthalate (KPH) electrolyte at pH4.

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