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. 2023 Jul 4;120(27):e2300493120.
doi: 10.1073/pnas.2300493120. Epub 2023 Jun 26.

Ru-P pair sites boost charge transport in hematite photoanodes for exceeding 1% efficient solar water splitting

Affiliations

Ru-P pair sites boost charge transport in hematite photoanodes for exceeding 1% efficient solar water splitting

Rui-Ting Gao et al. Proc Natl Acad Sci U S A. .

Abstract

Fast transport of charge carriers in semiconductor photoelectrodes are a major determinant of the solar-to-hydrogen efficiency for photoelectrochemical (PEC) water slitting. While doping metal ions as single atoms/clusters in photoelectrodes has been popularly used to regulate their charge transport, PEC performances are often low due to the limited charge mobility and severe charge recombination. Here, we disperse Ru and P diatomic sites onto hematite (DASs Ru-P:Fe2O3) to construct an efficient photoelectrode inspired by the concept of correlated single-atom engineering. The resultant photoanode shows superior photocurrent densities of 4.55 and 6.5 mA cm-2 at 1.23 and 1.50 VRHE, a low-onset potential of 0.58 VRHE, and a high applied bias photon-to-current conversion efficiency of 1.00% under one sun illumination, which are much better than the pristine Fe2O3. A detailed dynamic analysis reveals that a remarkable synergetic ineraction of the reduced recombination by a low Ru doping concentration with substitution of Fe site as well as the construction of Ru-P bonds in the material increases the carrier separation and fast charge transportation dynamics. A systematic simulation study further proves the superiority of the Ru-P bonds compared to the Ru-O bonds, which allows more long-lived carriers to participate in the water oxidation reaction. This work offers an effective strategy for enhancing charge carrier transportation dynamics by constructing pair sites into semiconductors, which may be extended to other photoelectrodes for solar water splitting.

Keywords: charge carrier transfer; electron-hole recombination; hematite photoelectrodes; metal and nonmetal pair sites; photoelectrochemical water oxidation.

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Conflict of interest statement

The authors declare no competing interest.

Figures

Fig. 1.
Fig. 1.
Characterization of DASs Ru-P:Fe2O3. (A) Schematic illustration for the preparation of DASs Ru-P:Fe2O3. (B) HAADF-STEM image. A large numbers of Ru atoms were atomically dispersed on the Fe2O3. Inset of the B shows the another angle of Ru single atoms. (C and D) high-resolution HAADF-STEM images. The Inset of the D shows the corresponding fast Fourier transform pattern, indicating the single crystallinity structure of hematite nanoflakes. (E and F) The lines represent the line profiles from the HAADF intensity analysis labeled in D. (G) STEM-EDS elemental mapping of Fe, O, Ru, and P. Scale bars in B, C, D, and G are 2 nm, 1 nm, 1 nm, and 50 nm, respectively.
Fig. 2.
Fig. 2.
Coordination environment analysis of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3. (A) Ru 3p XPS spectra, (B) P 2p XPS spectra, and (C) Raman spectra of Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. (D) The normalized Ru K-edge XANES spectra of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3 as well as Ru foil, RuO2, and RuP references. (E) The Ru K-edge Fourier transformed EXAFS spectra (R-space) of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3 as well as Ru foil, RuO2, and RuP references. (F) The schematic models of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3. (G–I) WT-EXAFS plots of SAs Ru:Fe2O3, DASs Ru-P:Fe2O3, and RuP.
Fig. 3.
Fig. 3.
Photoelectrochemical activities of Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. (A) J-V curves. (B) Chopped J-V curve of DASs Ru-P:Fe2O3. (C) ABPE values. (D) Surface charge separation efficiencies (ƞsurface). (E) IPCE values in a Xe lamp. (F) OCP-derived carrier lifetimes. (G) PEIS at 1.23 VRHE. Inset shows the corresponding circuit. (H) Stability measurement, (I) gas productions, and (I) Faraday efficiencies of DASs Ru-P:Fe2O3. All electrochemical measurements were performed in 1 M KOH under AM 1.5G illumination (100 mW cm−2).
Fig. 4.
Fig. 4.
Band edge energetics characterizations. (A) Mott–Schottky plots under dark, (B) UV-vis absorption spectra, and (C) UPS curves of Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. Tauc plots of UV-vis absorption spectra are shown in the Inset of B. The blue dashed lines in C denote the area shown in the zoomed-in image in the Inset of C. (D) Band diagrams of corresponding photoanodes.
Fig. 5.
Fig. 5.
Photogenerated charge carrier dynamics. (A and B) Transient absorption decay curves at (A) 570 nm and (B) 620 nm for Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. The fits for the decays were shown as solid lines, and the circles represent the experimental data. (C) Transient absorption spectra of DASs Ru-P:Fe2O3 when excited with 380 nm. (D) Charge transfer rate constants (ktrans), (E) charge recombination rate constants (krec), and (F) charge transfer efficiencies extracted from IMPS analysis for the corresponding photoanodes.
Fig. 6.
Fig. 6.
DFT analysis. (A) Side view of ELF and (B) PDOS of Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. (C) Differential charge densities of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3. (D) Charge trapping and recombination, and (E) free energies of OER reaction steps of Fe2O3, SAs Ru:Fe2O3, and DASs Ru-P:Fe2O3. (F) The OER proceeding on the surfaces of SAs Ru:Fe2O3 and DASs Ru-P:Fe2O3.

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