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. 2022 May 16;28(28):e202104567.
doi: 10.1002/chem.202104567. Epub 2022 Apr 19.

Disclosing Cyclic(Alkyl)(Amino)Carbenes as One-Electron Reductants: Synthesis of Acyclic(Amino)(Aryl)Carbene-Based Kekulé Diradicaloids

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Disclosing Cyclic(Alkyl)(Amino)Carbenes as One-Electron Reductants: Synthesis of Acyclic(Amino)(Aryl)Carbene-Based Kekulé Diradicaloids

Avijit Maiti et al. Chemistry. .

Abstract

Herein, we disclose cyclic(alkyl)(amino)carbenes (CAACs) to be one-electron reductants under the formation of a transient radical cation as indicated by EPR spectroscopy. The disclosed CAAC reducing reactivity was used to synthesize acyclic(amino)(aryl)carbene-based Thiele and Chichibabin hydrocarbons, a new class of Kekulé diradicaloids. The results demonstrate CAACs to be potent organic reductants. Notably, the acyclic(amino)(aryl)carbene-based Chichibabin's hydrocarbon shows an appreciable population of the triplet state at room temperature, as evidenced by both variable-temperature NMR and EPR spectroscopy.

Keywords: EPR spectroscopy; carbene; electrochemistry; radical cation; reductant.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Scheme 1
Scheme 1
One‐electron oxidation of N‐heterocyclic carbene I (top) and cyclic(alkyl)(amino)carbene V (bottom) (R=monoanionic organic substituent and the counter anions are omitted for clarity).
Figure 1
Figure 1
a) Cyclic voltammogram of 1 in THF (0.1 M Bu4NPF6) measured at a scan rate of 20 mV s−1. Inset: Differential pulse voltammograms (DPV) of 1 in THF at a scan rate of 20 mV s−1 with 0.2 M Bu4NPF6). b) Experimental X‐band EPR spectrum of a solution of 2 in toluene generated in situ at 200 K. The isotropic signal has a g value of 2.0043 and a 14N hyperfine coupling of a(N)=16.7 MHz (5.9 G).
Scheme 2
Scheme 2
Oxidation of 1 (Dip=2,6‐iPr2C6H3).
Scheme 3
Scheme 3
Reactions of 1 with 4, 5, and 6.
Figure 2
Figure 2
a) Variable‐temperature 1H NMR spectra of 9 (selected region) in [D8]THF. b) Variable‐temperature X‐band EPR spectra of 9 in THF between 255 and 300 K. C) plots of double‐integral intensity (A) vs. T. The red line shows the fit to the Bleaney–Bowers equation (experimental parameters: microwave frequency=9.38 GHz, microwave power=0.2 mW, modulation amplitude=0.5 G, modulation frequency=100 kHz). d) Molecular structure of 9 with thermal ellipsoids at the 50 % probability level. All H atoms are omitted for clarity. Selected bond lengths [Å] and angles [°]: N1C1 1.389(2), C1C8 1.479(2), C1C2 1.400(2), C2C3 1.431(2), C3C4 1.359(2), C4C5 1.425(2), C5C5’ 1.419(21), N1C1C8 114.44(14).
Figure 3
Figure 3
Energy scanning of the rotation of the C−C bond between the two phenyl rings of 9 for the broken‐symmetry singlet (orange) and the triplet (blue) states at the UBP86‐D3/Def2SVP level of theory.
Figure 4
Figure 4
Cyclic voltammograms of 4, 5, and 6 in CH3CN/0.1 M Bu4NPF6 measured at a GC working electrode.

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