Abstract:Despite major progress, these materials still face several significant challenges. In particular: 1) metal oxides usually possess a large bandgap that limits the sunlight absorption, 2) not all metal oxides have a favorable band alignment to realize both redox processes (water reduction and oxidation), 3) low electrical conductivity and limited hole diffusion length, 4) charge recombination can occur easily in the bulk and on the surface, limiting the efficiency of the system.Recently, extensive efforts have b… Show more
“…It has been demonstrated that the performance of photodetectors is significantly improved by integrating QDs as light-absorbing layers or active layers. [21][22][23][24][25][26]72 In addition, high-performance photodetectors decorated by QDs are also attracting increasing attention thanks to their great lightharvesting abilities and charge transfer characteristics. [27][28][29]46 As an example, Bi et al demonstrated that the photocurrent of a ZnO NWs device was enhanced from 0.167 to 1.84 mA by decorating binary CdS QDs.…”
Benefitting from the excellent thermal and moisture stability, inorganic halide perovskite materials have established themselves quickly as promising candidates for fabricating photoelectric devices. However, due to high trap state density...
“…It has been demonstrated that the performance of photodetectors is significantly improved by integrating QDs as light-absorbing layers or active layers. [21][22][23][24][25][26]72 In addition, high-performance photodetectors decorated by QDs are also attracting increasing attention thanks to their great lightharvesting abilities and charge transfer characteristics. [27][28][29]46 As an example, Bi et al demonstrated that the photocurrent of a ZnO NWs device was enhanced from 0.167 to 1.84 mA by decorating binary CdS QDs.…”
Benefitting from the excellent thermal and moisture stability, inorganic halide perovskite materials have established themselves quickly as promising candidates for fabricating photoelectric devices. However, due to high trap state density...
“…The consumption of holes can ensure that the subsequent holes continue to migrate and improve the PEC efficiency. Commonly used sacrificial agents in PEC systems include Na 2 S-Na 2 SO 3 [20,21] , triethanolamine (TEOA) [22,23] and H 2 O 2 [24][25][26] and these have been widely used to evaluate interfacial charge transfer properties. Thorne et al measured the photocurrent-voltage curves of a hematite photoanode and found that the photoanode with H 2 O 2 as hole scavengers has lower onset potential values [24] .…”
Utilizing clean energy derived from photoelectrocatalytic reactions is expected to be an excellent choice to fundamentally solve the problem of the human energy crisis. Photoelectrochemical (PEC) cell can effectively promote charge separation and improve solar energy conversion efficiency since it combines the advantages of photocatalysis and electrocatalysis. However, the hole transfer and subsequent oxidation reaction in the PEC process are slow, resulting in the rapid recombination of photogenerated electron-hole pairs and low PEC performance. The half-oxidation reaction involving photogenerated holes is the bottleneck of PEC water splitting. Therefore, hole modulation has been an important research area in the field of catalysis. However, compared with electron modulation, research on hole modulation is limited and still faces great challenges. It is therefore of great significance to develop effective modulation strategies for photogenerated holes. This review summarizes the hole modulation strategies developed in the last five years, including hole sacrificial agents, nanostructural modification, heterostructure construction and cocatalyst modification. Hole modulation dynamics studies, such as transient absorption spectroscopy, time-resolved photoluminescence spectroscopy, transient photovoltage and scanning electrochemical microscopy, are also summarized. Moreover, relevant conclusions and an outlook are proposed.
“…Recently, 0D/2D heterojunctions have attracted much attention because of their excellent interfacial charge transfer characteristics [33–35] . Specifically, 0D nanoparticles have shorter charge transfer distances, and 2D nanosheets as carriers can avoid the self‐aggregation of 0D nanoparticles, which can provide more migration paths for the effective separation of photogenerated charge carriers [36,37] . Inspired by this, exploring an appropriate 0D semiconductor to compound with 2D LaTiO 2 N is expected to further improve the photocatalytic CO 2 reduction activity of LaTiO 2 N.…”
The efficiency of photocatalytic reduction of CO 2 with water to hydrocarbons is largely limited by high recombination rate of photogenerated electrons and holes in the photocatalysts. Herein, 0D/2D CeO 2 /LaTiO 2 N S-scheme heterojunction photocatalyst prepared by simple in-situ hydrothermal approach realizes the overall conversion of gaseous CO 2 and H 2 O without any sacrificial reagent and cocatalyst. The yields of CH 4 and CO over CeO 2 /LaTiO 2 N sample under visible light for 3 h are 1.5 and 7.2 μmol g À 1 , and the corresponding utilized photoelectron number (UPN) is 26.4 μmol g À 1 , about 7.3 and 7.8 times that of individual LaTiO 2 N and CeO 2 , respectively. The enhanced photocatalytic activity of 0D/2D CeO 2 /LaTiO 2 N is attributed to the constitution of the S-scheme heterojunction, which effectively inhibits the recombination of photogenerated carriers. This study is expected to provide a new insight into the construction of efficient 0D/2D photocatalysts for visible-light-driven photocatalytic CO 2 reduction.
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