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. 2021 Oct 11;12(1):5923.
doi: 10.1038/s41467-021-26219-6.

Van Der Waals gap-rich BiOCl atomic layers realizing efficient, pure-water CO2-to-CO photocatalysis

Affiliations

Van Der Waals gap-rich BiOCl atomic layers realizing efficient, pure-water CO2-to-CO photocatalysis

Yanbiao Shi et al. Nat Commun. .

Abstract

Photocatalytic CO2 reduction (PCR) is able to convert solar energy into chemicals, fuels, and feedstocks, but limited by the deficiencies of photocatalysts in steering photon-to-electron conversion and activating CO2, especially in pure water. Here we report an efficient, pure water CO2-to-CO conversion photocatalyzed by sub-3-nm-thick BiOCl nanosheets with van der Waals gaps (VDWGs) on the two-dimensional facets, a graphene-analog motif distinct from the majority of previously reported nanosheets usually bearing VDWGs on the lateral facets. Compared with bulk BiOCl, the VDWGs-rich atomic layers possess a weaker excitonic confinement power to decrease exciton binding energy from 137 to 36 meV, consequently yielding a 50-fold enhancement in the bulk charge separation efficiency. Moreover, the VDWGs facilitate the formation of VDWG-Bi-VO••-Bi defect, a highly active site to accelerate the CO2-to-CO transformation via the synchronous optimization of CO2 activation, *COOH splitting, and *CO desorption. The improvements in both exciton-to-electron and CO2-to-CO conversions result in a visible light PCR rate of 188.2 μmol g-1 h-1 in pure water without any co-catalysts, hole scavengers, or organic solvents. These results suggest that increasing VDWG exposure is a way for designing high-performance solar-fuel generation systems.

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Conflict of interest statement

The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. Characterizations of VDWGs-rich structure of BiOCl atomic layers.
a TEM image, b dark-filed STEM image, ce elemental mappings, f AFM image, g theoretical crystalline structures, h aberration-corrected HAADF-STEM image, i three-dimensional topographic color-coded intensity image (taken from h), and j intensity profiles (taken along the lines of h) of BOC-VDWGs-AL. k PAS, l EPR, m Bi L3-edge EXAFS, and n O K-edge XANES of BOC-VDWGs-AL, CBOC-VDWGs, and BOC-VDWGs-76. The inset in k is the simulation result of the positron density distribution of VDWG-Bi-VO••-Bi.
Fig. 2
Fig. 2. Pure-water PCR performances of VDWGs-rich BiOCl atomic layers.
a CO yields of four parallel experiments of pure-water PCRs. The first used BOC-VDWGs-AL under visible light in the presence of CO2, the second did not involve BOC-VDWGs-AL but still using visible light and CO2, the third involved BOC-VDWGs-AL and CO2 but under dark, and the fourth employed BOC-VDWGs-AL and visible light but fed with argon. b Cycling tests of pure-water PCR performances over BOC-VDWGs-AL for 50 hours. c Mass spectra of the product generated from pure-water PCR over visible-light-irradiated BOC-VDWGs-AL fed with 13CO2. The inset in panel c shows the corresponding GC pattern. d Yield of O2 detected during pure-water PCR photocatalyzed by BOC-VDWGs-AL, as well as the calculated yield ratio of CO to O2. This set of data were obtained from an online PCR system. e Statistical result for the CO/O2 yield ratio. f Comparison of CO-evolving rate of BOC-VDWGs-AL, CBOC-VDWGs, and BOC-VDWGs-76, all under visible light in the presence of pure-water and CO2. g Comparison of pure-water, CO-evolving rate of BOC-VDWGs-AL and some representative layered photocatalysts. The nanosheet photocatalysts with VDWGs on lateral facets were obtained by conventional exfoliation method, while VDWGs-dominated nanosheets were synthesized by our developed exfoliation strategy. The error bars derived from triplicate experiments.
Fig. 3
Fig. 3. Promoting effect of VDWGs on exciton binding energy and, consequently, on electron–hole separation.
a, b PL of BOC-VDWGs-AL (a) and BOC-VDWGs-76 (b) as a function of operation temperature. c Comparisons of Eb and VDWG coverage percentage of BOC-VDWGs-AL, CBOC-VDWGs, and BOC-VDWGs-76. d Comparisons of Eb of BOC-VDWGs-AL and some representative layered photocatalysts. e Time-resolved PL of BOC-VDWGs-AL and BOC-VDWGs-76. f, g Transient photocurrent responses (f) and bulk charge separation efficiencies (g) of BOC-VDWGs-AL, CBOC-VDWGs, and BOC-VDWGs-76.
Fig. 4
Fig. 4. Promoting effect of VDWGs-associated defect on CO2-to-CO catalysis.
a C–O bond length and O–C–O bond angle of free CO2 (a1), CO2 adsorbed on VDWG-Bi-O-Bi (a2), and CO2 adsorbed on VDWG-Bi-VO••-Bi (a3). b1 Optimized geometric structures (parts containing charge density differences) and b2 schematic illustration of intermediates generated during CO2-to-CO catalysis over VDWG-Bi-VO••-Bi. c Gibbs free energy diagrams of intermediates generated during CO2-to-CO catalysis over VDWG-Bi-O-Bi and VDWG-Bi-VO••-Bi. d CO2-TPD of BOC-VDWGs-AL and BOC-VDWGs-AL-O2. e In situ FTIR of intermediates generated during pure-water PCR over BOC-VDWGs-AL. f Comparison of FTIR signal intensity of *CO intermediates from BOC-VDWGs-AL and BOC-VDWGs-AL-O2-driven pure-water PCR. g CO-TPD of BOC-VDWGs-AL and BOC-VDWGs-AL-O2. The VDWG-Bi-O-Bi was constructed by the calcination of VDWG-Bi-VO••-Bi (BOC-VDWGs-AL) under O2 atmonsphere.

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