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. 2025 Jul 1;16(1):5989.
doi: 10.1038/s41467-025-60919-7.

Planar asymmetric surface FeIV = O synthesis with pyrite and chlorite for efficient oxygen atom transfer reactions

Affiliations

Planar asymmetric surface FeIV = O synthesis with pyrite and chlorite for efficient oxygen atom transfer reactions

Wengao Lian et al. Nat Commun. .

Abstract

Surface high-valent iron-oxo species (≡FeIV=O) are reliable and green oxygen atom transfer reagents, but the ability is seriously inhibited by the maximal orbital overlap of axial Fe = O double bond in a symmetric planar coordination environment. Herein, we report the synthesis of planar asymmetric surface FeIV = O (PA-≡FeIV = O) on pyrite using chlorite as the oxidant, where the in-situ generated ClO2 can transform a planar Fe-S bond to Fe-Cl by oxidizing and subsequently substituting planar sulfur atoms. Different from planar symmetric surface FeIV = O (PS-≡FeIV = O) with electron localization around axial Fe = O, PA-≡FeIV = O delocalizes electrons among Fe, axial oxo moiety and its planar ligands owing to the stronger electron-withdrawing capacity of Cl, which effectively weakens the orbital overlap of axial Fe = O bonding and thus facilitates the rapid electron transfer from the substrates to the unoccupied antibonding orbital of PA-≡FeIV = O, realizing more efficient oxygen atom transfer oxidation of methane, methyl phenyl sulfide, triphenylphosphonate and styrene than PS-≡FeIV = O. This study offers a facile approach for the synthesis of planar asymmetric surface FeIV = O, and also underscores the importance of planar coordination environment of high-valent metal-oxo species in the oxygen atom transfer reactions.

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Conflict of interest statement

Competing interests: The authors declare no competing interests.

Figures

Fig. 1
Fig. 1. Synthesis and characterization of PA-≡FeIV = O.
a In-situ Raman spectra to investigate the formation of δ(H···Cl–O) and the generation process of ≡FeIV = O with FeS2 and ClO2. b EPR spectra to determine ClO2 generated by FeS2 and ClO2 without any trapping agent. c UV–vis spectra to detect the transformation from ClO2 (262 nm) to ClO2 (350 nm). d XPS spectra of Cl 2p scan on R-FeS2-ClO2 and R-FeS2. e Raman spectra of the Fe-Cl bond and Fe-S bond signals in R-FeS2-ClO2, R-FeS2, original FeS2 and FeCl3. EXAFS spectra and corresponding fitting lines of (f) R-FeS2-ClO2 and g R-FeS2. h Illustration of the transformation process from Fe-S to Fe-Cl bond for PA-≡FeIV = O synthesis with ClO2 as the inducer. The blue ball refers to the Fe atom, the yellow ball refers to the S atom, the green ball refers to the Cl atom and the red ball refers to the O atom. Experiment conditions: [FeS2]0 = 1.0 g/L (if not specified), [ClO2]0 = 1.0 mmol/L (if not specified), [Na2S2O3]0 = 1.0 mmol/L (if not specified).
Fig. 2
Fig. 2. Comparison of coordination and electronic structures between PA-≡FeIV = O and PS-≡FeIV = O.
a Electrostatic potential in Fe, O, S, and Cl atoms in PA-≡FeIV = O and PS-≡FeIV = O. The blue ball refers to the Fe atom, the yellow ball refers to the S atom, the green ball refers to the Cl atom and the red ball refers to the O atom. b Fe K-edge XANES spectra of R-FeS2-ClO2, R-FeS2, original FeS2 and FeCl3. c XPS spectra on Fe 2p scan of R-FeS2-ClO2 and R-FeS2. d Mössbauer spectra to differentiate the electronic structure of PA-≡FeIV = O and PS-≡FeIV = O. e Schematic illustration of the work functions of PA-≡FeIV = O and PS-≡FeIV = O. Ef represents the Fermi level. Experiment conditions: [FeS2]0 = 1.0 g/L (if not specified), [ClO2]0 = 1.0 mmol/L (if not specified), [Na2S2O3]0 = 1.0 mmol/L (if not specified).
Fig. 3
Fig. 3. Theoretical analysis on the enhanced oxygen atom transfer capacity of PA-≡FeIV = O.
a Comparison of electron spin density between PA-≡FeIV = O and PS-≡FeIV = O. b Electron localization function (ELF) analysis of PA-≡FeIV = O and PS-≡FeIV = O. The blue ball refers to Fe atom, the yellow ball refers to S atom, the green ball refers to Cl atom and the red ball refers to the O atom. c Differences of oxygen atom transfer energy barrier in the two steps between PA-≡FeIV = O and PS-≡FeIV = O. d Density of states analysis on PS-≡FeIV = O. e Density of states analysis on PA-≡FeIV = O.
Fig. 4
Fig. 4. Oxygen atom transfer reactions.
a Comparison of CH3OH yield by PA-≡FeIV = O and PS-≡FeIV = O. b Comparison of CH3OH yield rates in this PA-≡FeIV = O driven system with those in light- or thermal-driven CH4 activation systems. c Illustration of CH4 oxidation process by ≡FeIV = O. d EPR spectra to identify the ·CH3 intermediate after H abstraction by PA-≡FeIV = O and PS-≡FeIV = O. e CH4 consumption and CH3OH generation by PA-≡FeIV = O through in-situ Fourier Transform infrared spectroscopy. f Energy barriers of CH4 conversion process by PA-≡FeIV = O and PS-≡FeIV = O. g MPS and h Ph3P oxidation efficiencies by PA-≡FeIV = O and PS-≡FeIV = O in comparison. i Comparison of efficiencies over PA-≡FeIV = O and PS-≡FeIV = O for styrene epoxidation to styrene oxide. Experiment conditions: [FeS2]0 = 0.02 g (for CH4 oxidation), [FeS2]0 = 0.1 g (for other reactions), [ClO2]0 = 1.0 mmol L−1 (if not specified), aqueous CH4-containing solution volume = 20 mL, other solution volume = 100 mL. The error bars represent the standard deviation derived from two repeated experiments.

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