催化学报 ›› 2026, Vol. 83: 1-23.DOI: 10.1016/S1872-2067(26)64986-8
• 综述 • 下一篇
李思娴a,1, 段有雨c,1, 梁新元a, 李宇涵a,*(
), 张蝶青b,*(
)
收稿日期:2025-10-18
接受日期:2025-12-16
出版日期:2026-04-18
发布日期:2026-03-04
通讯作者:
* 电子信箱: lyhctbu@126.com (李宇涵),
dqzhang@shnu.edu.cn (张蝶青).作者简介:1共同第一作者.
基金资助:
Sixian Lia,1, Youyu Duanc,1, Xinyuan Lianga, Yuhan Lia,*(
), Dieqing Zhangb,*(
)
Received:2025-10-18
Accepted:2025-12-16
Online:2026-04-18
Published:2026-03-04
Contact:
* E-mail:lyhctbu@126.com(Y. Li),dqzhang@shnu.edu.cn(D. Zhang)
About author:Yuhan Li (Institute for Frontier Interdisciplinary Research in Intelligence and Environment, School of Big Data, Chongqing Technology and Business University) received her Ph.D. degree from the Department of Environmental Sciences at The Education University of Hong Kong between September 2015 and November 2017. In November 2017, she was recruited as an Outstanding Doctoral Talent to the Engineering Research Center of Waste Oil Resource Utilization Technology and Equipment, Ministry of Education, Chongqing Technology and Business University, where she has since been engaged in research on air pollution control. To date, she has served as the principal investigator of two projects funded by the National Natural Science Foundation of China, as well as the China Postdoctoral Innovative Talent Support Program, leading a total of 18 research projects. She has published 68 SCI-indexed papers as first or corresponding author, including 13 ESI Highly Cited Papers and 2 ESI Hot Papers. She holds 11 authorized Chinese invention patents and has published three academic monographs as first author with Science Press. She currently serves as a Young Editorial Board Member for Journal of Magnesium and Alloys, Advanced Powder Materials, Rare Metals, Exploration, Eco-Environment & Health, EcoEnergy, and CleanMat, as a Guest Editor for Discover Environment, and as an Associate Editor of Frontiers in Chemistry.Supported by:摘要:
光催化技术为利用太阳能驱动能源转化与环境污染治理提供了一条极具前景的绿色途径. 其整体效率与反应选择性从根本上取决于催化剂表面的活性位点, 即反应物吸附、活化与转化所发生的关键微观区域. 活性位点的原子构型、电子结构及局域微环境直接调控光生载流子的分离与迁移行为, 并决定表面氧化还原反应的动力学路径与产物分布. 尽管活性位点的重要性已形成广泛共识, 但如何在高时空分辨率下精准识别这些微观位点, 并阐明其在真实反应条件下的动态演化及构效关系, 仍是制约光催化研究由经验探索迈向理性设计的核心科学挑战. 因此, 系统梳理光催化活性位点的研究进展, 对于深化反应机制理解并指导高性能催化剂的定向开发具有重要意义.
本综述旨在系统构建光催化活性位点由“精准识别”走向“理性设计”的整体研究框架. 首先, 提出了一套较为完整的活性位点分类体系, 将其归纳为四大类: 金属位点(如单原子、原子团簇及纳米颗粒)、非金属位点(如异质原子掺杂与表面官能团)、界面位点(如异质结界面与核-壳结构界面)以及缺陷位点(如阴离子或阳离子空位). 系统阐述了不同类型活性位点在增强光吸收、调控电荷动力学以及优化反应路径方面所发挥的独特作用及其潜在协同机制. 针对活性位点的复杂性与多样性, 本文重点评述了多尺度、先进表征技术的联用策略: 光谱技术(如红外光谱与X-射线光电子能谱)用于解析表面化学态及反应中间体; 波谱技术(如电子顺磁共振)对顺磁缺陷与自由基物种具有高度灵敏性; 显微技术(如扫描与透射电子显微镜)实现了原子尺度的结构与形貌可视化; 而原位操作条件下的表征技术(如原位X-射线吸收光谱)与理论计算方法(如密度泛函理论)的深度结合, 则能够动态揭示反应过程中活性位点的结构演变、电子转移机制及反应能垒, 从而实现微观结构信息与宏观催化性能之间的可靠关联. 本文的核心观点在于强调活性位点的动态本质, 并指出突破静态表征局限、依托多技术协同获取完整物理化学图景的必要性.
展望未来, 光催化活性位点研究将向动态原位观测、数据驱动设计及原子级精准调控方向深入发展.本文系统梳理了活性位点结构演化与反应机制的最新进展, 整合先进表征、理论模拟与可控合成策略, 构建了较为清晰的研究框架, 为高效、高选择性光催化剂的理性设计与实际应用提供了重要参考与理论指引.
李思娴, 段有雨, 梁新元, 李宇涵, 张蝶青. 光催化活性位点的原子结构解析与调控: 从精准识别到理性设计[J]. 催化学报, 2026, 83: 1-23.
Sixian Li, Youyu Duan, Xinyuan Liang, Yuhan Li, Dieqing Zhang. Decoding the atomic architecture of photocatalytic active sites: From precise identification to rational design principles[J]. Chinese Journal of Catalysis, 2026, 83: 1-23.
Fig. 1. (a) Schematic representation of the relationship between active sites and catalytic activity. Ea1 and Eg1 denote the activation energy and bandgap of inactive sites, whereas Ea2 and Eg2 correspond to the active sites responsible for catalytic turnover. (b) Overview of active site classification, identification techniques, and future research directions. (c) Timeline of key advancements in photocatalytic active site research (2014-2024), illustrating the evolution from fundamental structure-activity studies to atomic-level design strategies [3,41,44-49].
Fig. 2. Schematic illustration of the classification and synergistic mechanisms of photocatalytic active sites. The diagram delineates four primary categories of active sites including metal sites, defect sites, interface sites, and non-metal sites within a representative heterojunction photocatalyst.
| Time | Catalyst | Active sites types | Active site | Active site identification technique | Application | Photocatalytic performance | Ref. |
|---|---|---|---|---|---|---|---|
| 2023 | La-Ni diatomic active center catalyst supported in a COF | metal sites | La-Ni dual-atom | In-situ IR (1800-1900 cm−1) | photocatalytic CO2 reduction | under the condition of no additional photosensitizer, the CO production rate of LaNi-Phen/COF-5 catalyst is 605.8 μmol g‒1 h−1, which is 15.2 times higher than that of COF-5; The CO selectivity is 98.2% | [ |
| 2022 | Pt0.3-ZIS | metal sites | Pt single-atom | FT-IR | photocatalytic hydrogen evolution | the hydrogen production rate of Pt0.3-ZIS is 17500 μmol g‒1 h‒1, which is 22 times higher than that of original ZnIn2S4; Its AQE can reach 50.4% | [ |
| 2020 | Fe(III) chelates g-C3N4 | metal sites | Fe3+-chelate sites | FT-IR | photocatalytic nitrogen fixation | Fe(III) doping can improve the mobility of photogenerated electrons and produce more hydroxyl radicals through Fenton reaction, thus improving the photocatalytic redox performance | [ |
| 2021 | MCN-0.5 | non- metal sites | cyano group | FT-IR | photocatalytic CO2 reduction | the CO and CH4 yields reached 13.7 and 0.6 μmol g‒1 h‒1, respectively, which were 2.5 and 2 times that of g-C3N4 (TCN) prepared by traditional calcination method | [ |
| 2023 | MOF-808-PBA-MV | metal sites | Zr-oxo clusters | EPR (g = 1.98, 2.01) | photocatalytic CO2 reduction | MOF-808-PBA-MV showed high catalytic efficiency, which can produce 1460 μmol g‒1 h‒1 (pH = 5) of CH4 in aqueous solution under visible light irradiation, and showed greater than 99% selectivity | [ |
| 2024 | D-O-ZIS | defect sites | Zn vacancies | EPR | photocatalytic water decomposition | D-O-ZIS achieves an efficiency of 0.57% of solar energy conversion to hydrogen energy, which is currently the most efficient single group of spectroscopic catalysts | [ |
| 2020 | RuO2 loaded TiO2-MXene | metal sites | Ru0/RuOx nanoparticles | XPS | photocatalytic nitrogen fixation | the catalyst showed high activity and stability, achieving 425 μmol ammonia generation per gram of catalyst, which was significantly higher than TiO2-MXene and pure RuO2 | [ |
| 2019 | r-GO@PMo10V2 composite material | metal sites | Mo/V polyoxometalate clusters | XPS | photocatalytic nitrogen fixation | the efficiency of solar energy conversion to ammonia can reach 0.028%, and the ammonia generation rate is 2070 μmol g‒1 h‒1 | [ |
| 2021 | TiO2 (110) surface | defect sites | Oxygen vacancies | STM | photocatalytic CO2 reduction | CO2 dissociation is a single-electron process with a threshold energy of 1.4 eV or more at the bottom of the TiO2 conduction band | [ |
| 2019 | Ru/CNs | metal sites | Ru nanoparticle | TEM | photocatalytic nitrogen reduction | the ammonia yield of 7.5 wt% Ru/CNs catalyst was the highest, reaching 2213 μmol g‒1 h‒1, which was 6 times that of pure CNs | [ |
| 2019 | Ru and K bulk graphite carbon nitride | interface sites | Ru nanoparticle | TEM+ DFT | photocatalytic nitrogen fixation | the ammonia yield of Ru-K/B-g-C3N4 was as high as 283.3 μmol g‒1 h‒1, and the synergistic effect between Ru nanoparticles and B-g-C3N4 carrier further reduced the N2 activation energy barrier | [ |
| 2022 | Au@Cu7S4 | interface sites | Au-Cu7S4 heterojunction | DFT + in-situ XAS | photocatalytic hydrogen production | under the irradiation of visible light to near-infrared light, Au@Cu7S4 shows remarkable photocatalytic hydrogen production. The quantum yield is 9.4% at 500 nm and 7.3% at 2200 nm. ΔGH = −0.15 eV (DFT); TOF = 9.4 s‒1 | [ |
| 2022 | PBOC | metal sites | Pb, Bi dual-site | DFT+ XPS | photocatalytic CO2 reduction | compared with PBCOC, the photocatalytic activity of PBOC increased 7-10 times, showing higher CO2 conversion efficiency; ΔG(COOH) = −0.35 eV | [ |
Table 1 Identification methods and examples of different active sites.
| Time | Catalyst | Active sites types | Active site | Active site identification technique | Application | Photocatalytic performance | Ref. |
|---|---|---|---|---|---|---|---|
| 2023 | La-Ni diatomic active center catalyst supported in a COF | metal sites | La-Ni dual-atom | In-situ IR (1800-1900 cm−1) | photocatalytic CO2 reduction | under the condition of no additional photosensitizer, the CO production rate of LaNi-Phen/COF-5 catalyst is 605.8 μmol g‒1 h−1, which is 15.2 times higher than that of COF-5; The CO selectivity is 98.2% | [ |
| 2022 | Pt0.3-ZIS | metal sites | Pt single-atom | FT-IR | photocatalytic hydrogen evolution | the hydrogen production rate of Pt0.3-ZIS is 17500 μmol g‒1 h‒1, which is 22 times higher than that of original ZnIn2S4; Its AQE can reach 50.4% | [ |
| 2020 | Fe(III) chelates g-C3N4 | metal sites | Fe3+-chelate sites | FT-IR | photocatalytic nitrogen fixation | Fe(III) doping can improve the mobility of photogenerated electrons and produce more hydroxyl radicals through Fenton reaction, thus improving the photocatalytic redox performance | [ |
| 2021 | MCN-0.5 | non- metal sites | cyano group | FT-IR | photocatalytic CO2 reduction | the CO and CH4 yields reached 13.7 and 0.6 μmol g‒1 h‒1, respectively, which were 2.5 and 2 times that of g-C3N4 (TCN) prepared by traditional calcination method | [ |
| 2023 | MOF-808-PBA-MV | metal sites | Zr-oxo clusters | EPR (g = 1.98, 2.01) | photocatalytic CO2 reduction | MOF-808-PBA-MV showed high catalytic efficiency, which can produce 1460 μmol g‒1 h‒1 (pH = 5) of CH4 in aqueous solution under visible light irradiation, and showed greater than 99% selectivity | [ |
| 2024 | D-O-ZIS | defect sites | Zn vacancies | EPR | photocatalytic water decomposition | D-O-ZIS achieves an efficiency of 0.57% of solar energy conversion to hydrogen energy, which is currently the most efficient single group of spectroscopic catalysts | [ |
| 2020 | RuO2 loaded TiO2-MXene | metal sites | Ru0/RuOx nanoparticles | XPS | photocatalytic nitrogen fixation | the catalyst showed high activity and stability, achieving 425 μmol ammonia generation per gram of catalyst, which was significantly higher than TiO2-MXene and pure RuO2 | [ |
| 2019 | r-GO@PMo10V2 composite material | metal sites | Mo/V polyoxometalate clusters | XPS | photocatalytic nitrogen fixation | the efficiency of solar energy conversion to ammonia can reach 0.028%, and the ammonia generation rate is 2070 μmol g‒1 h‒1 | [ |
| 2021 | TiO2 (110) surface | defect sites | Oxygen vacancies | STM | photocatalytic CO2 reduction | CO2 dissociation is a single-electron process with a threshold energy of 1.4 eV or more at the bottom of the TiO2 conduction band | [ |
| 2019 | Ru/CNs | metal sites | Ru nanoparticle | TEM | photocatalytic nitrogen reduction | the ammonia yield of 7.5 wt% Ru/CNs catalyst was the highest, reaching 2213 μmol g‒1 h‒1, which was 6 times that of pure CNs | [ |
| 2019 | Ru and K bulk graphite carbon nitride | interface sites | Ru nanoparticle | TEM+ DFT | photocatalytic nitrogen fixation | the ammonia yield of Ru-K/B-g-C3N4 was as high as 283.3 μmol g‒1 h‒1, and the synergistic effect between Ru nanoparticles and B-g-C3N4 carrier further reduced the N2 activation energy barrier | [ |
| 2022 | Au@Cu7S4 | interface sites | Au-Cu7S4 heterojunction | DFT + in-situ XAS | photocatalytic hydrogen production | under the irradiation of visible light to near-infrared light, Au@Cu7S4 shows remarkable photocatalytic hydrogen production. The quantum yield is 9.4% at 500 nm and 7.3% at 2200 nm. ΔGH = −0.15 eV (DFT); TOF = 9.4 s‒1 | [ |
| 2022 | PBOC | metal sites | Pb, Bi dual-site | DFT+ XPS | photocatalytic CO2 reduction | compared with PBCOC, the photocatalytic activity of PBOC increased 7-10 times, showing higher CO2 conversion efficiency; ΔG(COOH) = −0.35 eV | [ |
| Technique | Key Information Provided | Advantage | Disadvantage |
|---|---|---|---|
| IR/FT-IR | molecular vibrations, surface adsorbates, functional groups | (1) high sensitivity to surface species (2) in-situ capability for real-time monitoring (3) non-destructive | (1) limited spatial resolution (2) overlapping peaks may complicate interpretation (3) requires reference spectra for accurate assignment |
| XPS | elemental composition, oxidation states, surface chemistry | (1) quantitative chemical state analysis (2) surface-sensitive (∼10 nm) (3) wide applicability to various materials | (1) ultra-high vacuum required (2) limited to surface region (3) possible beam damage or reduction of species |
| EPR | unpaired electrons, radical intermediates, defect states | (1) high sensitivity to paramagnetic centers (2) identifies defect types (e.g., vacancies) (3) in situ and operando potential | (1) limited to paramagnetic species (2) does not provide spatial information (3) complex spectra interpretation |
| Electron microscopy (TEM/STM) | morphology, atomic structure, defect visualization | (1) atomic-resolution imaging (2) direct visualization of active sites (3) combining with EDS for elemental mapping | (1) high vacuum required (2) sample preparation may alter structure (3) limited to static or ex-situ conditions |
| XAS | local coordination, oxidation state, electronic structure | (1) element-specific and site-sensitive (2) suitable for operando studies (3) probes both crystalline and amorphous phases | (1) requires synchrotron radiation source (2) data interpretation requires theoretical support (3) limited spatial resolution |
| DFT | electronic structure, adsorption energy, reaction pathways | (1) atomic-level insights (2) predicts active sites and mechanisms (3) complements experimental data | (1) relies on model accuracy (2) computationally expensive (3) may oversimplify real reaction conditions |
Table 2 Summary of key insights and future perspectives in photocatalytic active site research.
| Technique | Key Information Provided | Advantage | Disadvantage |
|---|---|---|---|
| IR/FT-IR | molecular vibrations, surface adsorbates, functional groups | (1) high sensitivity to surface species (2) in-situ capability for real-time monitoring (3) non-destructive | (1) limited spatial resolution (2) overlapping peaks may complicate interpretation (3) requires reference spectra for accurate assignment |
| XPS | elemental composition, oxidation states, surface chemistry | (1) quantitative chemical state analysis (2) surface-sensitive (∼10 nm) (3) wide applicability to various materials | (1) ultra-high vacuum required (2) limited to surface region (3) possible beam damage or reduction of species |
| EPR | unpaired electrons, radical intermediates, defect states | (1) high sensitivity to paramagnetic centers (2) identifies defect types (e.g., vacancies) (3) in situ and operando potential | (1) limited to paramagnetic species (2) does not provide spatial information (3) complex spectra interpretation |
| Electron microscopy (TEM/STM) | morphology, atomic structure, defect visualization | (1) atomic-resolution imaging (2) direct visualization of active sites (3) combining with EDS for elemental mapping | (1) high vacuum required (2) sample preparation may alter structure (3) limited to static or ex-situ conditions |
| XAS | local coordination, oxidation state, electronic structure | (1) element-specific and site-sensitive (2) suitable for operando studies (3) probes both crystalline and amorphous phases | (1) requires synchrotron radiation source (2) data interpretation requires theoretical support (3) limited spatial resolution |
| DFT | electronic structure, adsorption energy, reaction pathways | (1) atomic-level insights (2) predicts active sites and mechanisms (3) complements experimental data | (1) relies on model accuracy (2) computationally expensive (3) may oversimplify real reaction conditions |
Fig. 4. (a) In-situ DRIFT spectra showing intermediates of CO2 photoreduction in the wavenumber range of 1350-2070 cm-1. Reprinted with permission from Ref. [10]. Copyright 2023, Springer Nature. (b) In-situ FT-IR spectra of CO2 adsorption on CuInSnS4. Reprinted with permission from Ref. [99]. Copyright 2023, Springer Nature. (c) In-situ DRIFT spectra comparing CO2 adsorption on pure In2O3 and CO2 adsorption/activation on La-Ni-Phen/COF-5 under H2O presence and subsequent light irradiation. (d) In-situ DRIFT spectra illustrating CO2 adsorption on 1.0% BixIn2-xO3. Reprinted with permission from Ref. [97]. Copyright 2023, Springer Nature.
Fig. 5. FT-IR spectra of CO adsorption following the Pt0.3-ZIS desorption process (a) and for Pt3.0-ZIS (b). Reprinted with permission from Ref. [87]. Copyright 2022, Springer Nature. (c) FT-IR spectra of CN and CNFe0.5 samples. Reprinted with permission from Ref. [50]. Copyright 2020, Elsevier. (d) FT-IR spectra of g-C3N4, K-C3N4, SiW12, and 30-SiW12/K-C3N4 composites. Reprinted with permission from Ref. [101]. Copyright 2018, Elsevier. FT-IR spectra of pure CN (e) and Nv&Od-CN (f). Reprinted with permission from Ref. [102]. Copyright 2020, Royal Society of Chemistry.
Fig. 6. (a) XPS spectra of the P 4f region for the prepared Pt/TiO2-based photocatalyst. Reprinted with permission from Ref. [60]. Copyright 2014, Wiley-VCH. (b) Ti 2p XPS spectra of the TR-1.0 catalyst. Reprinted with permission from Ref. [107]. Copyright 2019, American Chemical Society. (c) XPS spectra of the Mo 3d region for r-GO@PMo10V2, accompanied by a TEM image of r-GO@PMo10V2. Reprinted with permission from Ref. [54]. Copyright 2019, American Chemical Society. (d) XPS spectra of the Li 1s region for both fresh and annealed LI-3D-GCN samples, including the N2 molecular charge density difference adsorbed by Li-3D-GCN. Reprinted with permission from Ref. [106]. Copyright 2019, Royal Society of Chemistry. (e) XPS spectra of the Ru3d peak for the RuO2@TiO2-MXene hybrid nanostructure, along with a TEM image of ultra-small RuO2 nanoparticles loaded on MXene sheets. Reprinted with permission from Ref. [49]. Copyright 2020, Elsevier. (f) High-resolution XPS spectra of Ce 4f, showing the optimal adsorption geometry of nitrogen on Ce-CUS. Reprinted with permission from Ref. [108]. Copyright 2019, American Chemical Society.
Fig. 7. (a) EPR spectra of ZIS and g-ZIS demonstrate the presence of Sv. Reprinted with permission from Ref. [85]. Copyright 2023, Springer Nature. (b) The enlarged EPR spectrum of MOF-808-PBA-MV distinctly confirms the presence of Zr (III) species. Reprinted with permission from Ref. [52]. Copyright 2023, Springer Nature. (c) EPR spectra of ZIS, D-ZIS, and D-O-ZIS are presented. Reprinted with permission from Ref. [53]. Copyright 2023, Springer Nature. (d) EPR spectra of SBNT-SSR, SBNT-HR, and SBNT-HR-x (where x = 0.3, 0.5, 1) are shown. Reprinted with permission from Ref. [110]. Copyright 2019, John Wiley and Sons.
Fig. 8. (a) STM image of the TiO2 (110) surface after CO2 adsorption at 55 K, acquired under conditions of 1.5 V and 5 pA with a scan range of 15 nm. Reprinted with permission from Ref. [46]. Copyright 2011, American Chemical Society. (b) HRTEM characterization of Ru/CN. Reprinted with permission from Ref. [55]. Copyright 2019, Elsevier. (c) TEM image of ultra-small RuO2 nanoparticles loaded on MXene flakes. Reprinted with permission from Ref. [49]. Copyright 2020, Elsevier. (d) TEM image of 1% MoS2 supported on CZ300. The white line segment in the figure represents a scale of 5 nm. Reprinted with permission from Ref. [114]. Copyright 2018, American Chemical Society.
Fig. 9. A paradigm of DFT application: Identifying the true active sites in Pt/TiO2 photocatalysts. (a) Volcano plot showing the relationship between HER rate and the hydrogen adsorption free energy (ΔGH). (b) Gibbs free energy diagrams for the HER on different active sites. (c?h) Atomic structure models of various Pt species on the anatase TiO2 (101) surface. Reprinted with permission from Ref. [118]. Copyright 2013, Royal Society of Chemistry.
Fig. 10. (a) Energy distribution associated with the formation of N2O5. Reprinted with permission from Ref. [119]. Copyright 2023, John Wiley and Sons. (b) ΔGH for hydrogen absorption at various surface sites. Reprinted with permission from Ref. [122]. Copyright 2024, Springer Nature. (c) Structural model of the outer layer of lead-bismuth oxide halides. (d) PDOS. Reprinted with permission from Ref. [57]. Copyright 2022, Springer Nature.
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