Photoelectrochemical Properties of Cu-Ga-Se Photocathodes with Compositions Ranging from CuGaSe2 to CuGa3Se5
Behzad Mahmoudi a, Denis Eberhart a, Torsten Hölscher b, Roland Scheer b, A. Wouter Maijenburg a
a Martin-Luther-University Halle-Wittenberg, Center for Innovation Competence Sili-Nano, Halle 06099, Germany
b Martin-Luther-University Halle-Wittenberg, Institute of Physics, Germany, Halle 06099, Germany
Materials for Sustainable Development Conference (MATSUS)
Proceedings of MATSUS23 & Sustainable Technology Forum València (STECH23) (MATSUS23)
#Adinos - Advances in inorganic thin film semiconductors for solar energy conversion: From photovoltaics to solar fuels
VALÈNCIA, Spain, 2023 March 6th - 10th
Organizer: Sudhanshu Shukla
Invited Speaker, A. Wouter Maijenburg, presentation 278
DOI: https://doi.org/10.29363/nanoge.matsus.2023.278
Publication date: 22nd December 2022

Cu-Ga-Se chalcopyrite structures with a band gap of 1.68 eV (CuGaSe2) to 1.85 eV (CuGa3Se5) are considered to be promising materials to be used as the photocathode in a tandem photoelectrochemical (PEC) water splitting configuration. Therefore, we prepared polycrystalline Cu-Ga-Se films with different compositions ranging from Cu-poor CuGaSe2 (Cu/Ga = 0.85) to extremely Cu-poor CuGa3Se5 (Cu/Ga = 0.33) and investigated the effect of the Cu/Ga ratio on the crystal structure, morphology and PEC performance of the films. Without any surface treatment or formation of a p-n junction, we report remarkable saturated photocurrent densities of -19.0 and -12.1 mA/cm2 (measured at -0.40 V vs. RHE) for our films with Cu/Ga = 0.85 and Cu/Ga = 0.33, respectively, using an LED-based solar simulator. These outstanding results cover 86% and 68% of the maximum theoretical photocurrents for materials with a band gap of 1.68 eV and 1.85 eV, respectively. Furthermore, we were able to obtain and validate a realistic equivalent circuit via potentiodynamic electrochemical impedance spectroscopy (P-EIS), which among others confirmed that the obtained difference in onset potential (270 mV) between these two films was in agreement with the obtained difference in flat-band potential (290 mV).

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