Synergizing the internal electric field and ferroelectric polarization of the BiFeO3/ZnIn2S4 Z-scheme heterojunction for photocatalytic overall water splitting
Abstract:Coupling internal electric field and ferroelectric polarization through the modulation of surface electronic structures to achieve high carrier separation and migration efficiency is attractive, but challenging in solar-to-chemical energy conversion....
“…27,28 For example, a few heterojunctions based on BiFeO 3 , such as BiFeO 3 @TiO 2 , 29 BiFeO 3 /BiVO 4 , 22 and BiFeO 3 /ZnIn 2 S 4 (ref. 30), have been demonstrated for various photocatalytic systems. However, research on boosting spatial charge separation induced by single-domain ferroelectric heterojunction photocatalysts, which incorporate polarization electric fields and a built-in-electric field at the heterojunction interface, both of which act as dual driving forces (DDFs) following a Z-scheme charge transfer mode, is lacking.…”
Utilizing the inherent spontaneous polarization of single-domain ferroelectric materials is crucial for achieving spacial charge separation via the induction of a built-in electric field. Herein, a single-domain Z-scheme heterojunction of...
“…27,28 For example, a few heterojunctions based on BiFeO 3 , such as BiFeO 3 @TiO 2 , 29 BiFeO 3 /BiVO 4 , 22 and BiFeO 3 /ZnIn 2 S 4 (ref. 30), have been demonstrated for various photocatalytic systems. However, research on boosting spatial charge separation induced by single-domain ferroelectric heterojunction photocatalysts, which incorporate polarization electric fields and a built-in-electric field at the heterojunction interface, both of which act as dual driving forces (DDFs) following a Z-scheme charge transfer mode, is lacking.…”
Utilizing the inherent spontaneous polarization of single-domain ferroelectric materials is crucial for achieving spacial charge separation via the induction of a built-in electric field. Herein, a single-domain Z-scheme heterojunction of...
“…Metallic sulfide semiconductors (e.g., CdS, CdIn 2 S 4, and In 2 S 3 ) have garnered significant attention as ultrathin materials due to their adjustable electronic and photoelectric properties. − ZnIn 2 S 4 , as a typical visible response ternary sulfide semiconductor with a suitable band gap and a compact interface, has been widely considered and explored. , The ultrathin ZnIn 2 S 4 nanosheet structure can improve the performance to a certain extent, but the photocatalytic activity is not yet sufficient to meet the requirements of a wider range of applications . The main reason for the low photocatalytic efficiency is that the photoelectron–hole pairs in the excited state are unstable and easy to recombine .…”
The effective combination of two metallic sulfides to form a heterojunction and regulate semiconductor structure can significantly improve the response of photocatalysts under visible light. In this study, we have successfully grown Ag-doped ZnIn 2 S 4 nanosheets randomly on carefully designed hollow Co 9 S 8 polyhedral nanocages to construct the Co 9 S 8 /Ag:ZnIn 2 S 4 heterojunction. The optimized 1.0 wt % Co 9 S 8 /Ag:ZnIn 2 S 4 heterostructure shows excellent activity with the H 2 generation rate of 1947.7 μmol g −1 h −1 , which is 1.58 times greater than the Ag:ZnIn 2 S 4 (1232.0 μmol g −1 h −1 ). However, pure Co 9 S 8 has a narrow band gap but almost no response in visible light due to the fast photogenerated carrier recombination rate. The degradation trend of methyl orange (MO) in all as-prepared samples is the same as that of hydrogen production. The compound with the Co 9 S 8 mass fraction of 1.0 wt % has the fastest degradation rate and can completely degrade MO within 16 min. In addition, the Co 9 S 8 / Ag:ZnIn 2 S 4 heterostructure has also shown long-term stability after 20 photocatalytic hydrogen evolution and MO degradation cycle experiments, respectively. This work highlights the significance of improving the photocatalytic performance by modulating the morphology of metallic semiconductors and constructing heterostructures.
“…Nevertheless, the performance of pure BFO in oxygen evolution is limited by the small number of surface-active sites and poor photoelectric conversion efficiency . To address these issues, several approaches such as surface modifications, heteroatom doping, morphological design, and engineering defects have been employed to improve photocatalytic performance by increasing the photoelectric conversion efficiency and surface-active sites. , The construction of heterojunction with other semiconductors such as AuAg/BiFeO 3 , Ag@BiPO 4 /BiOBr/BiFeO 3 , graphene oxide/BiFeO 3 , BiFeO 3 /ZnFe 2 O 4 , BiVO 4 –BiFeO 3 , g-C 3 N 4 /BiFeO 3 , WO 3 /BiFeO 3 , BiFeO 3 /Znln 2 S 4 and BiFeO 3 @COF have been reported, however, the photocatalytic response still needs to be improved.…”
BiFeO3 (BFO) has gained significant attention
recently
in photocatalytic water splitting due to its visible light active
profile and facile synthesis design. However, a single component photocatalyst
usually suffers from significant photoexcited charge-carrier recombination.
To overcome this problem, BFO nanocuboids are coupled with two-dimensional
Ca2Nb3O10 (CNO) nanosheets via a
facile electrostatic self-assembly method. The surface charge of BFO
nanocuboids is modulated via deposition of Co-nanoparticles to obtained
positively charged BFO-Co nanocuboids. Resultantly, the combination
of positively charged BFO-Co nanocuboids and negative charged CNO
nanosheets demonstrated a direct Z-scheme heterojunction. The optimized
BFO-Co/CNO heterostructure achieved outstanding photocatalytic O2 evolution (48.19 mmol g–1), which is 6.72
times higher than pristine BFO (7.17 mmol h–1 g–1). Different characterization confirmed that BFO-Co/CNO
heterostructures exhibited improved charge-carrier separation and
utilization compared to individual components. This improved response
can be associated with a better contact interface between the oppositely
charged surfaces with the added advantage of the perovskite nature
of both components. As a result, BFO-Co/CNO heterostructures achieved
the highest O2 evolution response for BFO-based heterostructures
to date. This study offers a novel strategy for modulating the BFO
nanocuboids surface charge via Co-nanoparticles deposition, which
concomitantly worked as a cocatalyst, a potential strategy that can
be applied for the design of various heterostructures.
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