Chinese Journal of Catalysis ›› 2022, Vol. 43 ›› Issue (10): 2592-2605.DOI: 10.1016/S1872-2067(22)64094-4
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Pengyu Donga,†, Aicaijun Zhangb,†, Ting Chengc, Jinkang Panb, Jun Songa, Lei Zhanga, Rongfeng Guana, Xinguo Xic,*(), Jinlong Zhangd,#(
)
Received:
2022-01-17
Accepted:
2022-03-08
Online:
2022-10-18
Published:
2022-09-30
Contact:
Xinguo Xi, Jinlong Zhang
About author:
†Contributed equally to this work.
Supported by:
Pengyu Dong, Aicaijun Zhang, Ting Cheng, Jinkang Pan, Jun Song, Lei Zhang, Rongfeng Guan, Xinguo Xi, Jinlong Zhang. 2D/2D S-scheme heterojunction with a covalent organic framework and g-C3N4 nanosheets for highly efficient photocatalytic H2 evolution[J]. Chinese Journal of Catalysis, 2022, 43(10): 2592-2605.
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URL: https://www.cjcatal.com/EN/10.1016/S1872-2067(22)64094-4
Fig. 1. (a) PXRD patterns; (b) FT-IR spectra. (c) Raman spectra (excited at 532 nm). (d) N2 adsorption isotherms tested at 77 K (inset: pore size distributions). C 1s (e) and N 1s (f) high-resolution XPS spectra.
Fig. 2. SEM images of g-C3N4 NS (a), TpPa-1-COF NS (b), and TPCNNS-2 (c). TEM images of g-C3N4 NS (d), TpPa-1-COF NS (e), and TPCNNS-2 (f). (g?j) TEM-EDS mapping images (scale bar: 500 nm) of TPCNNS-2.
Fig. 4. (a) Photocatalytic H2 evolution of as-prepared samples deposited with Pt co-catalyst (3 wt%) under visible light irradiation in 8 h. (b) Comparison of photocatalytic H2 evolution rate bar chart of all samples with error bar. (c) Cycle tests of photocatalytic H2 evolution over TPCNNS-2 and TpPa-1-COF NS. (d) AQE values at various wavelengths and the corresponding diffuse reflectance absorption spectrum of TPCNNS-2. XRD patterns (e) and FTIR spectra (f) of TPCNNS-2, before and after photocatalysis.
Fig. 5. (a) Steady-state PL spectra (excited at 280 nm). (b) Transient PL decay profiles of the light emission at 430 nm (excitation wavelength: 280 nm). (c) Photocurrent responses (I-t). (d) EIS Nyquist plots of various samples (inset shows the equivalent circuit model and the fitted results).
Fig. 6. (a) UV-vis diffuse reflectance absorption spectra; (b) Corresponding Tauc plots; (c) UPS spectra; (d) Schematic energy levels diagram of TpPa-1-COF NS and g-C3N4 NS.
Fig. 7. Electrostatic potential of TpPa-1-COF (001) surface (a) and g-C3N4 (001) surface (b) along the Z-axis direction (the insets show the corresponding optimized slab structures). The construction for simulating the interfaces of TpPa-1-COF (001)/g-C3N4 (001) heterojunction before geometry optimization (c,d) and after geometry optimization (e,f) from the top side and cross views with brown, grey, red, and light-pink representing N, C, O, and H, respectively. The calculated charge density differences in the TpPa-1-COF (001)/g-C3N4 (001) heterojunction from the top (g) and side views (h). The cyan region represents charge depletion, and the yellow region denotes charge accumulation. The isosurface value is 0.025 e Å-3 (i) Planar-averaged electron density difference of the TpPa-1-COF (001)/g-C3N4 (001) heterostructure.
Fig. 8. (a) DMPO spin-trapping EPR spectra of TpPa-1-COF NS, g-C3N4 NS, and TPCNNS. (b) Schematic illustration of two potential mechanisms (i.e., the systems of type II and S-scheme heterojunction) for charge-transfer of TPCNNS. (c) Schematic explanation of the charge migration mechanism in S-scheme TPCNNS heterostructure before contact, after contact in darkness, and irradiated with visible light.
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