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. 2022 Jul 26;28(42):e202200974.
doi: 10.1002/chem.202200974. Epub 2022 Jun 10.

Electrochemistry and Reactivity of Chelation-stabilized Hypervalent Bromine(III) Compounds

Affiliations

Electrochemistry and Reactivity of Chelation-stabilized Hypervalent Bromine(III) Compounds

Nayereh Mohebbati et al. Chemistry. .

Abstract

Hypervalent bromine(III) reagents possess a higher electrophilicity and a stronger oxidizing power compared to their iodine(III) counterparts. Despite the superior reactivity, bromine(III) reagents have a reputation of hard-to-control and difficult-to-synthesize compounds. This is partly due to their low stability, and partly because their synthesis typically relies on the use of the toxic and highly reactive BrF3 as a precursor. Recently, we proposed chelation-stabilized hypervalent bromine(III) compounds as a possible solution to both problems. First, they can be conveniently prepared by electro-oxidation of the corresponding bromoarenes. Second, the chelation endows bromine(III) species with increased stability while retaining sufficient reactivity, comparable to that of iodine(III) counterparts. Finally, their intrinsic reactivity can be unlocked in the presence of acids. Herein, an in-depth mechanistic study of both the electrochemical generation and the reactivity of the bromine(III) compounds is disclosed, with implications for known applications and future developments in the field.

Keywords: bromane; cyclic voltammetry; hypervalent halogen; oxidative coupling; unified pH.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Scheme 1
Scheme 1
Electrochemical generation of aryl‐λ 3‐bromanes 2 (Eq. (1)) and applications as reagent (Eq. (2)).
Figure 1
Figure 1
A and B: Background and iR drop‐corrected CVs of 5 mM 1a and 5 mM 1e at different scan rates (solvent: HFIP, working electrode: glassy carbon, supporting electrolyte: 0.1 M Bu4NBF4). C: Plot of the peak current densities (j P) vs. v 0.5.
Figure 2
Figure 2
Proposed mechanism for anodic bromane formation.
Figure 3
Figure 3
Comparison between the spin density distributions of 1a .+ and 1e .+.
Figure 4
Figure 4
Top: Absorption spectra of pure 1e (green line) and 2e (blue line) recorded in HFIP along with the predicted spectrum of 1e .+ (dotted red line). Bottom: Spectroelectrochemical analysis of the anodic oxidation of 1e at E=2.0 V vs. Ag/AgNO3 (anode: Pt grid).
Figure 5
Figure 5
Top: Background and iR drop corrected linear sweep voltammograms (LSV) of bromanes 2a‐g (c = 5 mM) recorded at 10 mV s−1 in CH3CN. Bottom left: Half‐peak potentials E P/2(obs.) measured in CH3CN and the values predicted using σ R and σ F substituent constants (E P/2(pred.), for details see the Supporting Information). Bottom right: Correlation between E P/2(obs.) and E P/2(pred.) for 2 in CH2Cl2 and CH3CN.
Scheme 2
Scheme 2
Results of preparative‐scale cathodic reduction of 2a in CH3CN.
Scheme 3
Scheme 3
Mechanistic studies of oxidative aminations induced by 2a (calculated free energies in kcal mol−1).
Scheme 4
Scheme 4
Activation of 2a for oxidative biaryl homo‐coupling.
Figure 6
Figure 6
A) Adduct formation between TfOH and 2a with calculated Gibbs free energy in kcal mol−1. B) Comparison between the observed shifts of 1H and 19F signals for 2a upon the addition of TfOH (2.0 equiv) in CD2Cl2 (trifluorotoluene as the internal standard) and the computed shifts. The positive signs refer to downfield displacements. a Averaged chemical shifts. C) Computed optimized geometry of 2aTfOH. D) Displacement of 19F chemical shifts for 2a in the presence of various amounts of TfOH. E) Reference compounds for titration experiments.

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