Abstract:Artificial photosynthesis of clean fuels shows fascinating prospects for solving the energy crisis and environmental pollution. However, the solar conversion efficiency is too low to fulfill industrialization requirements, which is confined by the poor photon utilization, severe recombination of electrons and holes, and insufficient reactive sites. Fortunately, junction engineering displays outstanding performance in conquering the aforementioned problems. Herein, an updated fundamental understanding of variou… Show more
“…[ 4,5 ] Many photocathode materials have been reported to obtain various C1C3 products including CO, [ 6,7 ] HCOOH, [ 8,9 ] methanol, [ 10,11 ] ethanol, [ 12,13 ] and propanol. [ 14 ] However, over the past decades, the stumbling block for PEC CO 2 reduction lies in its low efficiency and uncontrolled product selectivity due to the poor light absorption ability, sluggish charge transfer properties, and high overpotential of commonly used photocathode materials, [ 15,16 ] such as Cu 2 O [ 17 ] and ZnTe. [ 18 ]…”
Copper‐based chalcogenides have been considered as potential photocathode materials for photoelectrochemical (PEC) CO2 reduction due to their excellent photovoltaic performance and favorable conduction band alignment with the CO2 reduction potential. However, they suffer from low PEC efficiency due to the sluggish charge transfer kinetics and poor selectivity, resulting from random CO2 reduction reaction pathways. Herein, a facile heat treatment (HT) of a Cu2ZnSnS4(CZTS)/CdS photocathode is demonstrated to enable significant improvement in the photocurrent density (−0.75 mA cm−2 at −0.6 V vs RHE), tripling that of pristine CZTS, as a result of the enhanced charge transfer and promoted band alignment originating from the elemental inter‐diffusion at the CZTS/CdS interface. In addition, rationally regulated CO2 reduction selectivity toward CO or alcohols can be obtained by tailoring the surficial sulfur vacancies by HT in different atmospheres (air and nitrogen). Sulfur vacancies replenished by O‐doping is shown to favor CO adsorption and the CC coupling pathway, and thereby produce methanol and ethanol, whilst the CdS surface with more S vacancies promotes CO desorption capability with higher selectivity toward CO. The strategy in this work rationalizes the interface charge transfer optimization and surface vacancy engineering simultaneously, providing a new insight into PEC CO2 reduction photocathode design.
“…[ 4,5 ] Many photocathode materials have been reported to obtain various C1C3 products including CO, [ 6,7 ] HCOOH, [ 8,9 ] methanol, [ 10,11 ] ethanol, [ 12,13 ] and propanol. [ 14 ] However, over the past decades, the stumbling block for PEC CO 2 reduction lies in its low efficiency and uncontrolled product selectivity due to the poor light absorption ability, sluggish charge transfer properties, and high overpotential of commonly used photocathode materials, [ 15,16 ] such as Cu 2 O [ 17 ] and ZnTe. [ 18 ]…”
Copper‐based chalcogenides have been considered as potential photocathode materials for photoelectrochemical (PEC) CO2 reduction due to their excellent photovoltaic performance and favorable conduction band alignment with the CO2 reduction potential. However, they suffer from low PEC efficiency due to the sluggish charge transfer kinetics and poor selectivity, resulting from random CO2 reduction reaction pathways. Herein, a facile heat treatment (HT) of a Cu2ZnSnS4(CZTS)/CdS photocathode is demonstrated to enable significant improvement in the photocurrent density (−0.75 mA cm−2 at −0.6 V vs RHE), tripling that of pristine CZTS, as a result of the enhanced charge transfer and promoted band alignment originating from the elemental inter‐diffusion at the CZTS/CdS interface. In addition, rationally regulated CO2 reduction selectivity toward CO or alcohols can be obtained by tailoring the surficial sulfur vacancies by HT in different atmospheres (air and nitrogen). Sulfur vacancies replenished by O‐doping is shown to favor CO adsorption and the CC coupling pathway, and thereby produce methanol and ethanol, whilst the CdS surface with more S vacancies promotes CO desorption capability with higher selectivity toward CO. The strategy in this work rationalizes the interface charge transfer optimization and surface vacancy engineering simultaneously, providing a new insight into PEC CO2 reduction photocathode design.
“…[4,5] Although numerous semiconductor materials have been proven to work for CO 2 photoreduction, the development of semiconductors alone as potential photo catalysts still suffers from their inherent limitations on the light harvesting and utilization. [6][7][8][9][10][11] Thus, it is necessary to exploit new replaceable materials or smart strategies to avoid the drawbacks of semiconductor photocatalysts. Plasmonic nanomaterials are widely considered as fre quencytunable "optical nanoantennas" due to their unique localized surface plasmon resonance (LSPR).…”
Plasmonic nanostructures have tremendous potential to be applied in photocatalytic CO 2 reduction, since their localized surface plasmon resonance can collect low-energy-photons to derive energetic "hot electrons" for reducing the CO 2 activation-barrier. However, the hot electron-driven CO 2 reduction is usually limited by poor efficiency and low selectivity for producing kinetically unfavorable hydrocarbons. Here, a new idea of plasmonic active "hot spot"confined photocatalysis is proposed to overcome this drawback. W 18 O 49 nanowires on the outer surface of Au nanoparticles-embedded TiO 2 electrospun nanofibers are assembled to obtain lots of Au/TiO 2 /W 18 O 49 sandwichlike substructures in the formed plasmonic heterostructure. The short distance (< 10 nm) between Au and adjacent W 18 O 49 can induce an intense plasmon-coupling to form the active "hot spots" in the substructures. These active "hot spots" are capable of not only gathering the incident light to enhance "hot electrons" generation and migration, but also capturing protons and CO through the dual-hetero-active-sites (Au-O-Ti and W-O-Ti) at the Au/TiO 2 /W 18 O 49 interface, as evidenced by systematic experiments and simulation analyses. Thus, during photocatalytic CO 2 reduction at 43± 2 °C, these active "hot spots" enriched in the well-designed Au/TiO 2 /W 18 O 49 plasmonic heterostructure can synergistically confine the hot-electron, proton, and CO intermediates for resulting in the CH 4 and CO productionrates at ≈35.55 and ≈2.57 µmol g −1 h −1 , respectively, and the CH 4 -product selectivity at ≈93.3%.
“…Heterojunctions contain different semiconductor components with matched crystal lattice and dissimilar band energy such as Z‐scheme junction [40] . Morphology and structure of heterojunction influence the photocatalytic performance.…”
Section: Fundamental Concepts Of Photocatalysismentioning
Photocatalysis has been known as one of the promising technologies due to its eco‐friendly nature. However, the potential application of many photocatalysts is limited owing to their large bandgaps and inefficient use of the solar spectrum. One strategy to overcome this problem is to combine the advantages of heteroatom‐containing supports with active metal centers to accurately adjust the structural parameters. Metal nanoparticles (MNPs) and single atom catalysts (SACs) are excellent candidates due to their distinctive coordination environment which enhances photocatalytic activity. Metal‐organic frameworks (MOFs), covalent organic frameworks (COFs) and carbon nitride (g‐C3N4) have shown great potential as catalyst support for SACs and MNPs. The numerous combinations of organic linkers with various heteroatoms and metal ions provide unique structural characteristics to achieve advanced materials. This review describes the recent advancement of the modified MOFs, COFs and g‐C3N4 with SACs and NPs for enhanced photocatalytic applications with emphasis on environmental remediation.
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