Built-in electric field for photocatalytic overall water splitting through a TiO2/BiOBr P–N heterojunction

Photocatalytic overall water splitting to simultaneously obtain abundant hydrogen and oxygen is still the mountain that stands in the way for the practical applications of hydrogen energy, in which composite semiconductor photocatalysts are critical for providing both electrons and holes to promote...

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Veröffentlicht in:Nanoscale 2021-02, Vol.13 (8), p.4496-4504
Hauptverfasser: Chi, Qianqian, Zhu, Genping, Jia, Dongmei, Ye, Wei, Wang, Yikang, Wang, Jun, Ting Tao, Xu, Fuchun, Gan Jia, Li, Wenhao, Gao, Peng
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container_end_page 4504
container_issue 8
container_start_page 4496
container_title Nanoscale
container_volume 13
creator Chi, Qianqian
Zhu, Genping
Jia, Dongmei
Ye, Wei
Wang, Yikang
Wang, Jun
Ting Tao
Xu, Fuchun
Gan Jia
Li, Wenhao
Gao, Peng
description Photocatalytic overall water splitting to simultaneously obtain abundant hydrogen and oxygen is still the mountain that stands in the way for the practical applications of hydrogen energy, in which composite semiconductor photocatalysts are critical for providing both electrons and holes to promote the following redox reaction. However, the interface between different components forms a deplete layer to hinder the charge transfer to a large extent. In order to enhance the charger transfer from an interface to the surface and promote the spatial separation of electron–hole pairs, a built-in electric field induced by a p–n heterojunction emerges as the best choice. As a touchstone, a p–n heterojunction of TiO2/BiOBr with a strong built-in electric field has been constructed, which presents a wide spectrum response owing to its interleaved band gaps after composition. The built-in electric field greatly enhances the separation and transportation of photogenerated carriers, resulting in fluorescence quenching due to the carrier recombination. The sample also displayed exceptional photoelectron responses: its photocurrent density (43.3 μA cm−2) was over 10 times that of TiO2 (3.5 μA cm−2) or BiOBr (4.2 μA cm−2). In addition, the sample with a molar ratio of 3 : 1 between TiO2 and BiOBr showed the best photocatalytic overall water splitting performance under visible light (λ > 420 nm): the hydrogen and oxygen production rate were 472.7 μmol gcat.−1 h−1 and 95.7 μmol gcat.−1 h−1, respectively, which are the highest values under visible light without other cocatalysts to have been reported in literature for the photocatalyst.
doi_str_mv 10.1039/d0nr08928a
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In addition, the sample with a molar ratio of 3 : 1 between TiO2 and BiOBr showed the best photocatalytic overall water splitting performance under visible light (λ &gt; 420 nm): the hydrogen and oxygen production rate were 472.7 μmol gcat.−1 h−1 and 95.7 μmol gcat.−1 h−1, respectively, which are the highest values under visible light without other cocatalysts to have been reported in literature for the photocatalyst.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d0nr08928a</doi><tpages>9</tpages></addata></record>
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source Royal Society Of Chemistry Journals 2008-
subjects Carrier recombination
Charge transfer
Construction
Electric fields
Fluorescence
Heterojunctions
Hydrogen-based energy
Mountains
Oxygen production
P-n junctions
Photocatalysis
Photocatalysts
Photoelectric effect
Photoelectric emission
Photoelectrons
Redox reactions
Separation
Titanium dioxide
Water splitting
title Built-in electric field for photocatalytic overall water splitting through a TiO2/BiOBr P–N heterojunction
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