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. 2022 May 6;28(26):e202200313.
doi: 10.1002/chem.202200313. Epub 2022 Mar 30.

Diradicals Photogeneration from Chloroaryl-Substituted Carboxylic Acids

Affiliations

Diradicals Photogeneration from Chloroaryl-Substituted Carboxylic Acids

Lorenzo Di Terlizzi et al. Chemistry. .

Abstract

With the aim of generating new, thermally inaccessible diradicals, potentially able to induce a double-strand DNA cleavage, the photochemistry of a set of chloroaryl-substituted carboxylic acids in polar media was investigated. The photoheterolytic cleavage of the Ar-Cl bond occurred in each case to form the corresponding triplet phenyl cations. Under basic conditions, the photorelease of the chloride anion was accompanied by an intramolecular electron-transfer from the carboxylate group to the aromatic radical cationic site to give a diradical species. This latter intermediate could then undergo CO2 loss in a structure-dependent fashion, according to the stability of the resulting diradical, or abstract a hydrogen atom from the medium. In aqueous environment at physiological pH (pH=7.3), both a phenyl cation and a diradical chemistry was observed. The mechanistic scenario and the role of the various intermediates (aryl cations and diradicals) involved in the process was supported by computational analysis.

Keywords: diradicals; heterolytic cleavage; intramolecular electron transfer; phenyl cations; photochemistry.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Scheme 1
Scheme 1
Literature precedents relevant to the present investigation.
Scheme 2
Scheme 2
Proposed approach for the formation of diradicals based on Intramolecular Electron Transfer (IET).
Figure 1
Figure 1
Structures of compounds 1 ae.
Figure 2
Figure 2
Potential energy surfaces (PESs) of the S0 (blue line with square symbols) and T1 (red line with circle symbols) states for: 1 a (part a), 1 e (part b), 1′ a (part c), 1′ e (part d) at the ωB97xD/def2TZV level of theory in bulk methanol. The reported structures are the optimized geometries for the S0 (lower part) and T1 (upper part) states. The values reported in magenta do refer to the charge localized at the chlorine atom (green) at the equilibrium geometry and upon elongation of the C−Cl bond (evaluated on the last point of each curve). The values reported in blue (for S0 states) and red (for T1 states) refer to the energy change associated with the last point with respect to the minimum for each curve.
Figure 3
Figure 3
Spin density plots for intermediates 3 21+ arising from 1 a (part a) and 1 e (part b), and intermediates 3 22 arising from 1′ a (part c) and 1′ e (part d), as determined from ωB97xD/def2TZV calculations in bulk methanol.
Figure 4
Figure 4
Singlet‐triplet (S−T) gaps for intermediates 21+ (green bars), 22 (red bars) and 23 (blue bars) as determined from ωB97xD/def2TZV calculations in bulk methanol. A positive bar indicates a singlet ground‐state intermediate.
Scheme 3
Scheme 3
Proposed mechanistic scenario for the photoreactivity of compounds 1 ae.

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