The construction of S-scheme heterojunction represents a simple yet effective strategy for enhancing photogenerated charge carrier separation and optimizing the reduction and oxidation capability of the photocatalytic system. However, precise tuning of the internal electric field for optimizing charge carrier migration across the heterojunction remains challenging. Herein, we present a novel defect engineering approach to modulate the potential barrier in S-scheme heterojunctions through strategic oxygen vacancy introduction. Specifically, we first selectively introduce oxygen vacancies on Bi2WO6, followed by coupling with g-C3N4 to form oxygen-deficient Bi2WO6/g-C3N4 (OVs-BWO-CN) S-scheme heterojunction. Surprisingly, the selective oxygen vacancy engineering on OVs-BWO cannot only preserve the features of common oxygen vacancies, but also shrink the potential barrier formed between OVs-BWO and CN. This reduction in potential barrier facilitates enhanced charge carrier migration across the heterojunction interface. As a direct consequence of this optimized charge transfer, the CN/OVs-BWO heterojunction demonstrates exceptional photocatalytic CO2 conversion performance, reaching a CO production rate of 48.65 μmol h−1 g−1. Such a work on selective oxygen vacancy engineering for optimizing potential barrier can provide important guidelines for photocatalysis.
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Coupling bulk and interface electric field for enhancing photogenerated charge carrier separation represents an effective strategy toward enhancing photocatalytic performance due to the potential of superposition of electric field. However, the detailed mechanism of synergistic effect of the bulk and interface electric field in facilitating photogenerated charge carrier remains underexplored, limiting its wide applications. Herein, we integrate the bulk electric field of Bi2MoO6 (BMO) with interface electric field (IEF) of S-scheme heterojunction formed between BMO and Bi19Br3S27 (BBS) for enhancing photocatalytic performance. The two electric fields can not only superimpose for amplifying electric field strengths, but also act as the funnel for guiding photogenerated charge carrier migration towards specific regions for redox reactions. Moreover, the Mo–S bonds formed between BMO and BBS act as a channel for charge transfer, accelerating the charge transfer of the S-scheme and achieving effective charge separation. As a proof-of-concept, we employ optimized BMO/BBS S-scheme heterojunction for photocatalytic CO2 conversion, reaching about 32.4 times and 2.0 times to that of pristine BMO and unmodulated BMO/BBS for CO production. This method of promoting the IEF by coupling bulk and interface electric field provides new insights into the construction of S-scheme heterojunctions for photocatalysis.
Ag surface plasmon resonance promoted step-scheme (S-scheme) SnNb2O6/Ag3PO4 heterojunctions were constructed via simple chemical deposition and precipitation. The samples were characterized by X-ray diffractometer, field-emission scanning electron microscope, high resolution transmission electron microscope, X-ray photoelectron spectrometer, UV-Vis diffuse reflectance spectrometer and photoluminescence spectrometer. The photocatalytic activities of SnNb2O6, Ag3PO4 and SnNb2O6/Ag3PO4 composites can be determined via degradation experiments. The results show that the SnNb2O6/Ag3PO4 composite possesses an optimum degradation performance in the photocatalytic degradation of methylene blue. Besides, the pseudo–first–order rate constant (Kapp) of SnNb2O6/Ag3PO4 is 0.313 min–1, which is 13.1 times and 4.8 times greater than that of SnNb2O6 and Ag3PO4, respectively. Also, Ag surface plasmon resonance–promoted SnNb2O6/Ag3PO4 S-scheme heterojunction can accelerate the separation of electron-hole pairs, thereby enhancing the redox reaction capability of the whole system.
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