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Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts

SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium...

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Published in:Sustainable energy & fuels 2019-01, Vol.3 (1), p.208-218
Main Authors: Murthy, Dharmapura H K, Matsuzaki, Hiroyuki, Wang, Qian, Suzuki, Yohichi, Seki, Kazuhiko, Hisatomi, Takashi, Yamada, Taro, Kudo, Akihiko, Domen, Kazunari, Furube, Akihiro
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container_title Sustainable energy & fuels
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creator Murthy, Dharmapura H K
Matsuzaki, Hiroyuki
Wang, Qian
Suzuki, Yohichi
Seki, Kazuhiko
Hisatomi, Takashi
Yamada, Taro
Kudo, Akihiko
Domen, Kazunari
Furube, Akihiro
description SrTiO3 (STO) has favorable opto-electronic properties for overall water splitting. Nevertheless, realizing a higher efficiency is impeded by its band gap which can only harvest UV light. In order to extend the spectral response towards visible light, STO is (co)doped with lanthanum (La) and rhodium (Rh). However, notwithstanding the amount of visible light absorbed, the H2 evolution rates are remarkably governed by the valence state of Rh, La doping level and ruthenium (Ru) cocatalyst loading. Hence, it is essential to unravel the underlying effect of doping on the photophysical processes to gain insight into material design. To this end, charge carrier dynamics was probed over a wide time (sub-picosecond to microsecond) and spectral (visible to IR) region using transient absorption spectroscopy. Depending on the dopant composition, an interplay between the electron trapping and the kinetics of the electron transfer to the Ru cocatalyst was rationalized. For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. Engineering the energetic position of the dopant within the band gap to avoid undesirable carrier trapping is crucial to enhance the efficiency of photocatalytic reactions.
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For Rh4+:STO, free electrons probed at 3435 nm decayed virtually completely by 20 ps resulting in a kinetic competition between the electron trapping and the electron transfer to Ru cocatalyst. In the case of Rh3+:STO, free electrons decayed by a factor of three by 100 ps, thus demonstrating the effect of Rh valence state on the electron lifetime. The time constant and quantum yield of electron transfer from Rh3+:STO to the Ru cocatalyst were found to be 1.6 ps and 14.7%, respectively. In addition to a longer electron lifetime, enhanced electron transfer to the Ru cocatalyst makes Rh3+:STO one of the promising photocatalysts for H2 generation. 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source Royal Society of Chemistry:Jisc Collections:Royal Society of Chemistry Read and Publish 2022-2024 (reading list)
subjects Absorption spectroscopy
Current carriers
Dopants
Doping
Efficiency
Electron transfer
Electronic properties
Electrons
Energy gap
Free electrons
Hydrogen evolution
Hydrogen production
Infrared spectroscopy
Kinetics
Lanthanum
Optoelectronics
Photocatalysis
Photocatalysts
Reaction kinetics
Rhodium
Ruthenium
Spectral sensitivity
Strontium titanates
Time constant
Trapping
Ultraviolet radiation
Water splitting
title Revealing the role of the Rh valence state, La doping level and Ru cocatalyst in determining the H2 evolution efficiency in doped SrTiO3 photocatalysts
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