Yanzhao Zhang's research while affiliated with The University of Queensland and other places

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Publications (14)


(A) Five fields affected by the green hydrogen. (B) The global clean hydrogen market size was valued at USD, estimated from 2021 to 2030. The data is collected from ref[15]. (C) Overall hydrogen evolution reaction mechanism including Volmer, Tafel and Heyrovsky steps. (D) Oxygen evolution reaction mechanism in an alkaline environment.
(A) Conventional alkaline water splitting electrolyzer. (B) Anion exchange membrane electrolyzer. (C) Capillary-fed electrolysis cell[36]. Copyright 2022, The Authors, published by Springer Nature.
(A) TEM, enlarged TEM, and HRTEM images for α-Ni(OH)2 hollow spheres, respectively. Inset in (C) shows the corresponding SAED pattern. TEM, enlarged TEM, and HRTEM images for β-Ni(OH)2 nanoplates, respectively. Inset in (F) shows the corresponding SAED pattern. Copyright 2014, American Chemical Society[49]. (B) Impact of facets on the OER activity descriptor. Inset, eg occupancy of six- and seven-coordinated configurations. Reproduced with permission. Copyright 2018, Wiley-VCH[53]. (C) Synthesis schematic of AuSA-MnFeCoNiCu LDH. (D) EDS elemental mapping of Mn, Fe, Co, Ni, Cu, O, Au. The scale bar is 1 μm (E) Projected density of states (EF: Fermi level, εO-2p: O 2p band center) (F) Schematic band diagrams. (G) Computed free energies (ΔG) of OER steps on AuSA-MnFeCoNiCuOOH and MnFeCoNiCuOOH. Copyright 2023, The Authors, published by Springer Nature[63]. UHB: Upper Hubbard band; LHB: lower Hubbard band; N(e): state density.
(A) Calculated free energies of H2O adsorption, activated H2O adsorption, OH adsorption and H adsorption. Copyright 2017, The Authors, published by Springer Nature[71]. (B) Non-volatile solid carbon precursors (for example, CNT) may have different impacts on the chemical composition and microstructure of the carburization product. Copyright 2016, The Authors, published by Springer Nature[79]. (C) Comparison of the overpotentials required at 10 mA cm⁻² among our catalyst and available reported HER catalysts. (D) Comparison of the current densities delivered at -200 mV among our catalyst and available reported HER catalysts. Copyright 2018, The Authors, published by Springer Nature[94].
(A) Equilibrium and thermoneutral voltages for water electrolysis as a function of temperature. (B) Schematic structures of an electrolytic cell, gap electrode assembly, and zero-gap electrode assembly. Copyright 2018, American Chemical Society[39]. (C) Engineering electrocatalysts for direct seawater electrolysis. Protocols for cathode modification of electronic structure modulation, tailoring local environment, and interface engineering. (D) Protocols for anode modification of building protective layer, tailoring local environment, and building Cl⁻ repulsion layer.

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Advancing strategies on green H2 production via water electrocatalysis: bridging the benchtop research with industrial scale-up
  • Article
  • Full-text available

April 2024

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68 Reads

Microstructures

Microstructures

Yanzhao Zhang

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Dazhi Yao

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Jinzhe Liu

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[...]

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Lianzhou Wang

Water splitting provides clean hydrogen via different technologies such as alkaline water electrolysis, proton exchange membrane electrolyzers, solid oxide electrolysis cells, and photoelectrolysis, each with advantages and challenges. The focus on alkaline water electrolysis highlights its maturity compared to emerging methods. Non-noble metal catalysts offer increased stability, low cost and operational lifespan. Challenges such as low current density, gas crossover, corrosive electrolytes, and limited efficiency are still to be addressed. These advanced electrocatalysts are summarized for alkaline oxygen and hydrogen evolution reactions. Meanwhile, different factors including product gas bubble management, operation conditions, separator and electrolyte affecting the performance were concluded and discussed. For the promising approach, seawater splitting is still far from large-scale application. Salinity, pH fluctuations, and complex composition are significant obstacles. The review underscores the need for improvements in electrocatalysts to enhance the efficiency, stability, and practicality of water splitting for hydrogen production, ultimately contributing to the growth of the clean hydrogen market and supporting the transition to sustainable energy systems.

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a) TEM image and b) Corresponding selected area electron diffraction (SAED) pattern for CAC2. c) Atomic‐resolution HAADF‐STEM image of CAC2. d) HAADF‐STEM image and corresponding EDS elemental mapping of CAC2.
a) XANES and b) Corresponding EXAFS spectra for Au L3‐edge for CAC2, CA2, and Au‐foil. c) XANES and d) Corresponding EXAFS spectra for Co K‐edge for CAC2, CC2, and Co‐foil. WT analysis for the k³‐weighted EXAFS spectra at Au L3‐edge for e) CA2 and f) CAC2. WT analysis for the k³‐weighted EXAFS spectra at Co K‐edge for g) CAC2 and h) CC2.
a) Photocatalytic CO2 reduction for, CdS, CA1, CC1, CC2, CA2, CAC1, CAC2, CAC3, and CAC4 under visible‐light illumination (λ > 400 nm). b) Photocatalytic CO2 reduction for CAN2, CAI2, CAC2, and CPC2 under visible‐light illumination (λ > 400 nm). c) Stability test for CAC2 under visible‐light illumination (λ > 400 nm). Each test was for 7 h. d) UV–vis spectra for CdS, CA2, CC2, and CAC2. e) Schematic for band structures for CdS, CA2, CC2, and CAC2.
a) High‐resolution XPS spectra for Au 4f for CA2 with light‐on and ‐off, respectively. b) High‐resolution XPS spectra for Co 2p for CC2 with light‐on and ‐off, respectively. c) High‐resolution XPS spectra for Au 4f for CAC2 with light‐on and ‐off, respectively. d) High‐resolution XPS spectra for Co 2p for CAC2 with light‐on and ‐off, respectively. e) Charge density distribution of CAC before (top side) and following (bottom side) introduction of extra electrons in the model. The iso‐surface value is 0.0045e Å⁻³. Charge depletion and accumulation are labeled in cyan‐color and yellow, respectively. f) Scheme for charge redistribution between DSA and CdS nanoparticles under illumination. g) Electrostatic potential energy along the x‐axis for CAC model.
a) CO2 TPD findings for CdS, CC2, CA2, and CAC2. b) in situ DRIFTS spectra for CO2 adsorption on CAC2 in darkness from 0 to 40 min. The charge difference distributions for c) CC and d) CAC following CO2 adsorption. The iso‐surfaces are 0.003 e Å⁻³. Charge depletion and accumulation are labeled in, respectively, cyan‐color and yellow. Cd, S, O, C, Co, and Au are shown as green‐color, pink, red, brown, blue, and yellow, balls, respectively. e) In situ DRIFTS spectra for CO2 photoreduction for CAC2 from 0 to 40 min under illumination. Computed Gibbs free energy and corresponding configuration for steps in photocatalytic CO2‐to‐CH4 conversion on f) CAC and g) CC.
Reversed Electron Transfer in Dual Single Atom Catalyst for Boosted Photoreduction of CO2

September 2023

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93 Reads

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35 Citations

Photogenerated charge localization on material surfaces significantly affects photocatalytic performance, especially for multi‐electron CO 2 reduction. Dual single atom (DSA) catalysts with flexibly designed reactive sites have received significant research attention for CO 2 photoreduction. However, the charge transfer mechanism in DSA catalysts remains poorly understood. Here we report for the first time a reversed electron transfer mechanism on Au and Co DSA catalysts. In situ characterizations confirm that for CdS nanoparticles (NPs) loaded with Co or Au single atoms, photogenerated eletrons are localized around the single atom of Co or Au. In DSA catalysts however electrons are delocalized from Au and accumulate around Co atoms. Importantly, combined advanced spectroscopic findings and theoretical computation evidence that this reversed electron transfer in Au/Co DSA boosts charge redistribution and activation of CO 2 molecules, leading to highly significantly increased photocatalytic CO 2 reduction, for example, Au/Co DSA loaded CdS exhibits, respectively, ca . 2800% and 700% greater yields for CO and CH 4 compared with that for CdS alone. Reversed electron transfer in DSA can be used for practical design for charge redistribution and to boost photoreduction of CO 2 . Findings will be of benefit to researchers and manufacturers in DSA loaded catalysts for generation of solar fuels. This article is protected by copyright. All rights reserved


Hybrid water electrolysis with integrated and cascading reactions by two-dimensional electrocatalysts

January 2023

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47 Reads

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8 Citations

Journal of Materials Chemistry A

Electrocatalytic water splitting is promising for green hydrogen production. However, the high energy barrier and sluggish kinetics of the anodic oxygen evolution reaction (OER) lead to high energy consumption, burdening the large-scale industrial application. Hybrid water electrolysis using two-dimensional (2D) electrocatalysts is considered as a promising way to reduce the cost of electrocatalytic green hydrogen production. It reduces the electricity cost by earth-abundant electrode materials, alternative energy-saving reactions, and novel electrolyzers. In this review, we systematically analyze the promising hybrid water electrocatalysis by 2D electrocatalysts. The advantages and status quo, as well as important future directions and feasibilities of this emerging field, are carefully discussed. We reveal that developing well-matched alternative reactions and stable reactors/devices are two critical factors for efficient hybrid water electrolysis. To improve the practical and economic feasibility of hybrid water electrocatalysis, it is promising to integrate tandem reactions with hybrid water electrocatalysis and advanced electrolyzers to achieve higher efficiency and selectivity. We conclude that developing stable 2D electrocatalysts, finding matched reactions, and efficient devices are the core for advancing hybrid water electrocatalysis.


a) Scheme for BMO nanosheet crystal structure. Bismuth, molybdenum, oxygen and oxygen vacancy are denoted as balls, respectively, yellow, grey, red and white; b) TEM image and SAED, c) XRD patterns for BMO and BMO‐R; d) STEM image and e) series of O K‐edge EELS spectra from bulk to surface of BMO‐R; Bi L3 edge XAS experiment and fitted data for f) BMO‐R and g) BMO; h) Raman spectra for BMO and BMO‐R.
In situ DRIFTS test for CO2 and H2O interaction with a) BMO‐R and b) BMO in dark; Projected crystal orbital Hamilton population (pCOHP) between carbon atom in CO2 and Mo active site on c) BMO‐R and d) BMO; Charge difference distributions for e) BMO‐R and f) BMO following CO2 adsorption (charge depletion is in yellow and accumulation in blue, positive values for Δq indicate electron accumulation on CO2 Eads is CO2 adsorption energy on surface). Isosurfaces are 0.003 e Å⁻³. Oxygen, carbon, bismuth and molybdenum atoms are denoted as balls, respectively red, brown, purple and grey.
a) Photocatalytic CO2 reduction for BMO, BMO‐R, BVO, BVO‐R, BWO and BWO‐R under Xenon lamp illumination; b) Repeated photocatalytic CO2 reduction test for BMO‐R; c) UV/Vis diffuse reflectance spectroscopy and band gap for BMO and BMO‐R; d) CO2 photoreduction for BMO and BMO‐R under 540 nm LED illumination for 7 h; e) TSPL spectra for BMO and BMO‐R; f) Transient photocurrent density for BMO and BMO‐R in 0.5 M Na2SO4 aqueous solution.
a) In situ DRIFTS test for CO2 and H2O interaction with BMO‐R under constant Xenon lamp illumination; b) Computed Gibbs free energy for main reactions in photocatalytic CO2 reduction to CH4 for BMO and BMO‐R; Key steps of CO2 photoreduction to CO/CH4 for c) BMO and d) BMO‐R, in which BMO‐R convert *CO to *OCH. Oxygen of absorbed intermediates, oxygen of BMO/BMO‐R, carbon, bismuth and molybdenum atoms are denoted as balls, respectively red, pink, brown, purple and grey.
Facet‐specific Active Surface Regulation of BixMOy (M=Mo, V, W) Nanosheets for Boosted Photocatalytic CO2 reduction

November 2022

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41 Reads

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61 Citations

Photocatalytic performance can be optimized via introduction of reactive sites. However, it is practically difficult to engineer these on specific photocatalyst surfaces, because of limited understanding of atomic‐level structure‐activity. Here we report a facile sonication‐assisted chemical reduction for specific facets regulation via oxygen deprivation on Bi‐based photocatalysts. The modified Bi2MoO6 nanosheets exhibit 61.5 and 12.4 μmol g⁻¹ for CO and CH4 production respectively, ≈3 times greater than for pristine catalyst, together with excellent stability/reproducibility of ≈20 h. By combining advanced characterizations and simulation, we confirm the reaction mechanism on surface‐regulated photocatalysts, namely, induced defects on highly‐active surface accelerate charge separation/transfer and lower the energy barrier for surface CO2 adsorption/activation/reduction. Promisingly, this method appears generalizable to a wider range of materials.


Facet‐specific Active Surface Regulation of BixMOy (M=Mo, V, W) Nanosheets for Boosted Photocatalytic CO2 reduction

October 2022

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25 Reads

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9 Citations

Angewandte Chemie

Photocatalytic performance can be optimized via introduction of reactive sites. However, it is practically difficult to engineer these on specific photocatalyst surfaces, because of limited understanding of atomic‐level structure‐activity. Here we report a facile sonication‐assisted chemical reduction for specific facets regulation via oxygen deprivation on Bi‐based photocatalysts. The modified Bi2MoO6 nanosheets exhibit 61.5 and 12.4 μmol g–1 for CO and CH4 production respectively, ~3 times greater than for pristine catalyst, together with excellent stability/reproducibility of ~20 h. By combining advanced characterizations and simulation, we confirm the reaction mechanism on surface‐regulated photocatalysts, namely, induced defects on highly‐active surface accelerate charge separation/transfer and lower the energy barrier for surface CO2 adsorption/activation/reduction. Promisingly, this method appears generalizable to a wider range of materials.


TiO2/FePS3 S‐Scheme Heterojunction for Greatly Raised Photocatalytic Hydrogen Evolution

October 2022

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152 Reads

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132 Citations

The aggravating extreme climate changes and natural disasters stimulate the exploration of low‐carbon/zero‐carbon alternatives to traditional carbon‐based fossil fuels. Solar‐to‐hydrogen (STH) transformation is considered as appealing route to convert renewable solar energy into carbon‐free hydrogen. Restricted by the low efficiency and high cost of noble metal cocatalysts, high‐performance and cost‐effective photocatalysts are required to realize the realistic STH transformation. Herein, the 2D FePS3 (FPS) nanosheets anchored with TiO2 nanoparticles (TiO2/FePS3) are synthesized and tested for the photocatalytic hydrogen evolution reaction. With the integration of FPS, the photocatalytic H2‐evolution rate on TiO2/FePS3 is radically increased by ≈1686%, much faster than that of TiO2 alone. The origin of the greatly raised activity is revealed by theoretical calculations and various advanced characterizations, such as transient‐state photoluminescence spectroscopy/surface photovoltage spectroscopy, in situ atomic force microscopy combined with Kelvin probe force microscopy (AFM‐KPFM), in situ X‐ray photoelectron spectroscopy (XPS), and synchrotron‐based X‐ray absorption near edge structure. Especially, the in situ AFM‐KPFM and in situ XPS together confirm the electron transport pathway in TiO2/FePS3 with light illumination, unveiling the efficient separation/transfer of charge carrier in TiO2/FePS3 step‐scheme heterojunction. This work sheds light on designing and fabricating novel 2D material‐based S‐scheme heterojunctions in photocatalysis.



Metal-organic framework with atomically dispersed Ni-N4 sites for greatly-raised visible-light photocatalytic H2 production

December 2021

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64 Reads

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25 Citations

Chemical Engineering Journal

The depletion of traditional fossil fuels and related environmental issues have increased the demand for clean and sustainable energy resources to achieve carbon neutrality. Active, robust and cheap photocatalysts are required for large-scale photocatalytic H2 evolution reaction (p-HER), which transforms solar energy into chemical energy. Here we report the decoration of Ni-imidazole framework (NiIm) with CdS nanorods for p-HER. The p-HER rate of CdS/NiIm hybrid sharply increased by about 14.23 times to 21,712 µmol h⁻¹ g⁻¹ when compared with that of CdS alone. Physicochemical characterizations and theoretical calculations reveal strong interactions at the CdS/NiIm interface and the presence of numerous Ni-N4 active sites on NiIm leading to the significant performance enhancement. This work demonstrates that NiIm acts as an affordable and abundant co-catalyst that remarkably enhances the p-HER, and enlightens the further development in the design and preparation of metal-organic framework-based materials for various applications in photocatalysis and related subjects.


Aberration‐corrected HAADF‐STEM images of a) CdS NPs and b) ReS2 NSs. c) Simulated model for ReS2. The red and yellow colored spheres denote Re and S, respectively, and the blue‐dotted line denotes the Re4 diamond chain. d) AFM image of ReS2 NSs and measured thickness of ReS2. e) TEM of ReS2 NSs and CdS NPs. f) EDX mapping of CR12 from red‐dotted rectangle of (e).
a) High‐resolution XPS spectrum of Re 4f for CR12. b) High‐resolution XPS spectrum of Re 4f for ReS2. c) High‐resolution XPS spectrum of Cd 3d for CdS and CR12. d) XANES S K edge of CdS and CR12.
a) Photocatalytic CO2 reduction activities of CdS, CR4, CR8, and CR12 under visible‐light illumination (λ ≥ 420 nm). b) Photocatalytic CO2 reduction activity of CR12 recycle test with 7 h per cycle test. c) UV–vis diffuse reflectance spectroscopy and band edge for CdS, CR4, CR8, and CR12. d) TSPL spectra for CdS and CR12.
a,d) High‐resolution XPS spectrum for C 1s and S 2p for RS1. b,e) High‐resolution XPS spectrum for C 1s and S 2p for RS2. c,f) High‐resolution XPS spectrum for C 1s and S 2p for RS3. g) Side‐view (elevation) and h) top‐view (plan) of the electron density distribution of absorbed CO2 on Vs‐ReS2. The red, yellow, gray, and brown colored spheres denote O, S, Re, and C atoms, respectively. The isosurface value is set to 0.002e Å⁻³. i) Schematic of photocatalytic CO2 reduction in CR12 system under visible‐light illumination (λ ≥ 420 nm). The purple, red, yellow, orange, white, and black colored spheres denote Cd, O, S, Re, H, and C atoms, respectively.
ReS 2 Nanosheets with In Situ Formed Sulfur Vacancies for Efficient and Highly Selective Photocatalytic CO 2 Reduction

January 2021

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95 Reads

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71 Citations

Artificial photosynthesis can provide valuable fuels and positively impact greenhouse effects, via transforming carbon dioxide (CO2) and water (H2O) into hydrocarbons using semiconductor‐based photocatalysts. However, the inefficient charge‐carrier dissociation and transportation as well as the lack of surface active sites are two major drawbacks to boosting their activity and selectivity in photocatalytic CO2 reduction. Recently, ReS2 has received tremendous attention in photocatalysis area owing to its intriguing physicochemical properties. Nevertheless, the application of ReS2 in photocatalytic CO2 reduction is scarcely covered. In this study, we report a heterojunction formed between ReS2 nanosheets and CdS nanoparticles, achieving an apparently‐raised CO production of 7.1 μmol g‐1 and high selectivity of 93.4%. The as‐prepared ReS2/CdS heterojunction exhibits the strengthened visible‐light absorption, high‐efficiency electron‐hole pairs separation/transfer and increased adsorption/activation/reduction of CO2 on in situ created sulphur vacancies of ReS2, thus all favouring CO2 photoreduction. These are corroborated by advanced characterization techniques, e.g., synchrotron‐based X‐ray absorption near‐edge structure, and density functional theory based computations. Our findings will be of a broad interest in practical design and fabrication of surface active sites and semiconductor heterojunctions for applications in catalysis, electronics and optoelectronics. This article is protected by copyright. All rights reserved.


Figure 2. (a) Possible reaction routes for the nitrobenzene hydrogenation producing aniline (the preferential one is in blue). (b) Energy diagrams of the reaction routes for nitrobenzene hydrogenation producing aniline over Pt/g-C 3 N 4 single-atom photocatalyst and (c) light absorption spectra of the g-C 3 N 4 with and without Pt single-atom loading. Reproduced with permission from ref 80. Copyright 2020 Springer Nature.
Figure 3. (a) Scheme of the process of preparation of CoPc/P-CN nanostructures; (b) TEM and (c) HAADF-STEM images of 0.5CoPc/9P-CN and (d) the corresponding elemental mapping images; (e) EPR spectra of 0.5CoPc/9P-CN under light irradiation (λ = 405 nm); (f) photocatalytic performance test for 2,4-DCP degradation by CoPc/P-CN; (g) diagram of O 2 activation on the CoPc/P-CN heterojunction under visible-light irradiation; (h) selective photocatalytic oxidation of different aryl-alcohols over 1.8CoPc/12P-CN. (Photocatalytic reaction conditions: in the presence of O 2 , under visible-light irradiation). Reproduced with permission from ref 85 (with CC BY 4.0 License). Copyright 2020 John Wiley & Sons, Inc.
Figure 4. (a) The synthesis process of SA-Cu-TCN. (b) TEM image of SA-Cu-TCN and (c) the enlarged TEM image of the marked area in Figure 4b and the elemental mapping images of (d) N, (e) C, and (f) Cu elements. (g) A typical HAADF-STEM image of SA-Cu-TCN. (h) XANES spectra of the Cu K edge for SA-Cu-TCN, CSC, Cu foil, Cu 2 O, and CuO samples. (i) Fourier transform (FT) of the K 2 -weighted EXAFS Cu K edge of SA-Cu-TCN, Cu foil, and CSC. (j, k) Experimental and computed XANES spectra of the Cu K edge for the samples with the corresponding structure models (inset). (l, m) Differential charge surfaces of the Cu−N 3 and Cu−N 4 coordination structures. (n) Catalytic activity of SA-Cu-TCN for oxidation of benzene performed at 50 °C using visible light illumination for 12 h. Reproduced with permission from ref 41. Copyright 2020 John Wiley & Sons, Inc.
Figure 6. (a) Illustration of a single-atom Ru embedded Cu alloy photocatalyst. The reactants and products of MDR are displayed on the left panels. (b) Photocatalytic MDR activities and stabilities of pure Cu NPs (Cu 20 ) and Ru/Cu alloys with different Ru contents (Cu 19.95 Ru 0.05 , Cu 19.9 Ru 0.1 , Cu 19.8 Ru 0.2 and Cu 19.5 Ru 0.5 ) using white light irradiation. The reactor for conducting the photocatalytic MDR reaction was maintained at room temperature. (c) Photocatalytic MDR selectivity of pure Cu NPs (Cu 20 ) and Ru/Cu alloys with different Ru contents (Cu 19.95 Ru 0.05 , Cu 19.9 Ru 0.1 , Cu 19.8 Ru 0.2 , and Cu 19.5 Ru 0.5 ) using white light irradiation. The reactor for conducting the photocatalytic MDR reaction was maintained at room temperature. The formation rate ratio of H 2 to CO is defined as the selectivity. Schematic illustration for the influence of Cu x Ru y composition on the coke resistance for (d) Cu alone, (e) Cu x Ru y with low Ru loading content, and (f) Cu x Ru y with high Ru loading content. (g) Infrared spectra of CO adsorbed on single-atom Ru embedded Cu alloy surface at room temperature and saturation coverage following pretreatment at 200 °C in 10% CO in Ar (100 mL min −1 ) for 60 min. Rate-determining (h) CH 4 and (i) CH activation on Cu (111) and CuRu (111), respectively. Left, middle, and right panels indicate reactant, transient state, and product structure, respectively. Ground-and excited-state energy curves for CH 4 activation on (j) Cu (111) and (k) CH activation on CuRu (111) from e-NEVPT2. From the ground to the highest energy excited state, the color saturation of the curves turns from dark to light. Reproduced with permission from ref 78. Copyright 2020 Springer Nature.
Figure 7. (a) HAADF-STEM image and the relevant elemental mapping images of CoPSA-CdS. (b) X-ray absorption spectra of Co and (c) the corresponding k 3 -weighted FT space at R space. (d) Atomic-level structure configuration of CoPSA-CdS based on first-principles simulation. (e) Comparison of the photocatalytic activities for FA dehydrogenation on all the as-prepared samples. The test of photocatalytic FA dehydrogenation reaction was conducted in the 100 mL 20 vol % FA aqueous solution using visible light illumination (λ > 420 nm) at room temperature. (f) Transient-state photoluminescence spectra of the as-prepared samples. (g) In situ IR spectrum analysis for photocatalytic dehydrogenation of FA on (g) CoPSA-CdS. (h) Free energy profiles calculated for the photocatalytic FA dehydrogenation process on P-CdS, CoSSA-CdS, and CoPSA-CdS. The differential charge density maps between CdS and adsorbed FA on (i) P-CdS, (j) CoSSA-CdS, and (k) CoPSA-CdS. (l) Photocatalytic FA dehydrogenation and H 2 evolution mechanism on CoPSA-CdS. Reproduced with permission from ref 94. Copyright 2020 John Wiley and Sons, Inc.
Single-Atom Photocatalysts for Emerging Reactions

January 2021

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114 Reads

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104 Citations

ACS Central Science

Single-atom photocatalysts have demonstrated an enormous potential in producing value-added chemicals and/or fuels using sustainable and clean solar light to replace fossil fuels causing global energy and environmental issues. These photocatalysts not only exhibit outstanding activities, selectivity, and stabilities due to their distinct electronic structures and unsaturated coordination centers but also tremendously reduce the consumption of catalytic metals owing to the atomic dispersion of catalytic species. Besides, the single-atom active sites facilitate the elucidation of reaction mechanisms and understanding of the structure-performance relationships. Presently, apart from the well-known reactions (H2 production, N2 fixation, and CO2 conversion), various novel reactions are successfully catalyzed by single-atom photocatalysts possessing high efficiency, selectivity, and stability. In this contribution, we summarize and discuss the design and fabrication of single-atom photocatalysts for three different kinds of emerging reactions (i.e., reduction reactions, oxidation reactions, as well as redox reactions) to generate desirable chemicals and/or fuels. The relationships between the composition/structure of single-atom photocatalysts and their activity/selectivity/stability are explained in detail. Additionally, the insightful reaction mechanisms of single-atom photocatalysts are also introduced. Finally, we propose the possible opportunities in this area for the design and fabrication of brand-new high-performance single-atom photocatalysts.


Citations (13)


... The bicarbonate (HCO 3 À , 1143, 1242, and 1395 cm À 1 ), monodentate carbonate (m-CO 3 À , 1438 and 1507 cm À 1 ), and bidentate carbonate species (b-CO 3 2À , 1296, and 1617 cm À 1 ) resulting from the dissolution of CO 2 in H 2 O could be observed in the beginning ventilation environment without light irradiation. [57,58] Upon the light irradiation, the intensities of these characteristic absorption bands were gradually increased with prolonged adsorption time; meanwhile, an intermediate of formate (*COOH, 1187, 1491, 1536, and 1662 cm À 1 ) appeared and increased gradually, formed through the interaction between adsorbed *CO 2 and protons. [59] Under the influence of protons, the *COOH intermediate was then converted into the chemisorbed CO species (*CO, 2101 cm À 1 ), [60] and ultimately escaped the active site to release free CO molecules. ...

Reference:

Covalent Organic Framework with Donor‐Acceptor‐Donor Motifs Regulating Local Charge of Intercalated Single Cobalt Sites for Photocatalytic CO2 Reduction to Syngas
Reversed Electron Transfer in Dual Single Atom Catalyst for Boosted Photoreduction of CO2
Advanced Materials

Advanced Materials

... Water splitting for hydrogen generation represents a promising avenue for large-scale hydrogen production [16,17] . Various technologies, such as photocatalysis [18][19][20][21][22] , alkaline electrocatalysis [10,23] , proton exchange membrane (PEM) electrolyzers [24] , solid oxide electrolysis cells (SOEC) [25] , and photoelectrolysis [26,27] , offer distinct approaches to this process, each with its advantages and limitations [ Table 1]. ...

Hybrid water electrolysis with integrated and cascading reactions by two-dimensional electrocatalysts
  • Citing Article
  • January 2023

Journal of Materials Chemistry A

... Lithium-sulfur (Li-S) batteries, with high theoretical gravimetric energy density (2600 Wh kg −1 ) [1], low cost, and environmentally friendly nature, stand out among many rechargeable energy storage devices [2][3][4][5][6]. Nevertheless, several critical challenges hinder the application of Li-S batteries, including slow conversion kinetics, the shuttle effect, and huge volume expansion (80%) [7]. ...

Facet‐specific Active Surface Regulation of BixMOy (M=Mo, V, W) Nanosheets for Boosted Photocatalytic CO2 reduction
Angewandte Chemie International Edition

Angewandte Chemie International Edition

... Recently, lithium-sulfur (Li-S) batteries with a high theoretical gravimetric energy density (2600 Wh kg −1 ), which is 3-5 times that of the state-of-the-art Li-ion batteries, are promising to be the next-generation energy storage systems. [1][2][3][4][5] Nevertheless, Li-S batteries are still confronted with several issues hindering their practical applications, for instance, the insulating nature of sulfur and its discharge products, 6 the soluble polysulfides (Li 2 S x , 4 ≤ x ≤ 8) shuttle between anode and cathode, namely, shuttle effect, 7 and the sluggish conversion kinetics from liquid-state Li 2 S x to solidstate Li 2 S. 8 These aforementioned drawbacks result in low sulfur utilization, low Coulombic efficiency, and fast capacity decay. 9,10 Therefore, to overcome the aforementioned issues, the introduction of active centers with absorption and catalytic capabilities is crucial for the cathode to improve sulfur utilization and accelerate the reversible conversion between liquid-state Li 2 S x and solid-state Li 2 S. 11 Up to now, carbon nanotubes with high surface area and porous structure have been frequently used as cathode materials for Li-S batteries. ...

Facet‐specific Active Surface Regulation of BixMOy (M=Mo, V, W) Nanosheets for Boosted Photocatalytic CO2 reduction
  • Citing Article
  • October 2022

Angewandte Chemie

... With the integration of FPS, the photocatalytic H 2 evolution rate on TiO 2 /FePS 3 is radically increased by ≈1686%, much faster than that of TiO 2 alone. [71] 3.4 | D-scheme heterostructures As mentioned above, monolayer dipole materials, such as Janus structures, possess an internal electric field within the material due to the asymmetric structure, which can drive the photogenerated holes and electrons to separate effectively. Meanwhile, the interfacial electric field in type II, Z-scheme, or S-scheme heterostructures determines the motion and recombination of photogenerated carriers. ...

TiO2/FePS3 S‐Scheme Heterojunction for Greatly Raised Photocatalytic Hydrogen Evolution
Advanced Energy Materials

Advanced Energy Materials

... To achieve net-zero emissions and accommodate the escalating need for renewable energy sources, hydrogen produced from renewable energy emerges as a pivotal force in diminishing reliance on fossil fuels, thereby fostering economic and environmental sustainability [1][2][3][4][5][6][7][8][9] . The significance of hydrogen spans a spectrum of fields, profoundly influencing the electricity system, energy storage, transportation, industrial processes, and gas grids [ Figure 1A] [10][11][12][13][14] . ...

Photocatalytic CO 2 Reduction: Identification and Elimination of False-Positive Results
  • Citing Article
  • April 2022

ACS Energy Letters

... To achieve net-zero emissions and accommodate the escalating need for renewable energy sources, hydrogen produced from renewable energy emerges as a pivotal force in diminishing reliance on fossil fuels, thereby fostering economic and environmental sustainability [1][2][3][4][5][6][7][8][9] . The significance of hydrogen spans a spectrum of fields, profoundly influencing the electricity system, energy storage, transportation, industrial processes, and gas grids [ Figure 1A] [10][11][12][13][14] . ...

Metal-organic framework with atomically dispersed Ni-N4 sites for greatly-raised visible-light photocatalytic H2 production
  • Citing Article
  • December 2021

Chemical Engineering Journal

... The phenomenon of strong metal-support interaction (SMSI) is well acknowledged in the realm of heterogeneous catalysis, where it has a substantial influence on impeding the diffusion and aggregation of metal nanoparticles. The scope of surface science and materials interface (SMSI) has been broadened as a result of developments in research techniques, including robust interactions between metallic components and their corresponding substrates [132]. SMSIs are likely created due to electrical flaws and surface structural imperfections [133]. ...

Single-Atom Photocatalysts for Emerging Reactions

ACS Central Science

... Until now, along with the aforementioned applications of SAPs, their usage can also be extended to other areas, including photocatalytic disinfection, 141 nitrogen reduction, 142,143 and NO oxidation. 131,144 Xia et al. synthesized atomically dispersed Ag in MnO 2 porous hollow microspheres (Ag/MnO 2 PHMs), which can effectively photocatalyze bacteria inactivation. ...

Two-dimensional building blocks for photocatalytic ammonia production
  • Citing Article
  • January 2021

Journal of Materials Chemistry A

... According to the energy band theory, the CT complex straddle mechanism in the V Re -ReS 2 @ZnO heterostructure is proposed. 47,50 According to DFT calculations, it can be seen that the V Re -ReS 2 @ZnO heterostructure has excellent electrical conductivity, and charges and holes can be quickly transferred and accumulated on the CB and VB of ReS 2 through the Zn-S bond, as shown in Fig. 4(e). 51 In the process, a region of positive and negative charges is formed, and strong internal electric fields bend the band. ...

ReS 2 Nanosheets with In Situ Formed Sulfur Vacancies for Efficient and Highly Selective Photocatalytic CO 2 Reduction
Small Science

Small Science