2017
DOI: 10.1021/jacs.6b12273
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Giant Electron–Hole Interactions in Confined Layered Structures for Molecular Oxygen Activation

Abstract: Numerous efforts have been devoted to understanding the excitation processes of photocatalysts, whereas the potential Coulomb interactions between photogenerated electrons and holes have been long ignored. Once these interactions are considered, excitonic effects will arise that undoubtedly influence the sunlight-driven catalytic processes. Herein, by taking bismuth oxyhalide as examples, we proposed that giant electron-hole interactions would be expected in confined layered structures, and excitons would be t… Show more

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Cited by 269 publications
(168 citation statements)
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References 38 publications
(53 reference statements)
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“…Second, to investigate another function of oxygen vacancies working as active sites, we carried out temperature programmed desorption (TPD‐CO 2 ) analysis on In 2 O 3− x nanosheets (Figure b) . The peak at 410 °C is attributed to CO 2 adsorption on the photoinduced oxygen vacancy sites .…”
Section: Methodsmentioning
confidence: 96%
“…Second, to investigate another function of oxygen vacancies working as active sites, we carried out temperature programmed desorption (TPD‐CO 2 ) analysis on In 2 O 3− x nanosheets (Figure b) . The peak at 410 °C is attributed to CO 2 adsorption on the photoinduced oxygen vacancy sites .…”
Section: Methodsmentioning
confidence: 96%
“…have discovered that a high concentration of excess electrons can greatly improve the charge transportation and suppress the recommendation rate of photogenerated electron‐hole pairs . In addition, Bi‐ter BiOBr {001} facets could be suitable for the photocatalytic molecular oxygen activation due to the enormous excitonic effects . There are OV‐induced defect states localized in the middle of the forbidden band of the O‐ter+H facet with OVs (Figure d), and the defect states are mainly composed of the Bi 6 p orbital (Figure d).…”
Section: Resultsmentioning
confidence: 99%
“…As displayed in Figure , the (2×2) supercell was employed to simulate the BiOBr {001} facets with different atomic terminations . To test the thickness of the atomic layers of the slabs, the (1×1) surface was applied to all the models, and the thicknesses of slabs adopted in this paper are sufficient to reach the convergence for the cleavage energy (Table S1).…”
Section: Computational Models and Methodsmentioning
confidence: 99%
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