Issue 12, 2023

Unraveling the flexible aromaticity of C13H9+/0/−: a 2D superatomic-molecule theory

Abstract

Phenalenyl (C13H9) is the smallest triangular unit of a graphene nanosheet, and has been experimentally verified to be stable in radical (C13H9˙), cationic (C13H9+), and anionic (C13H9) states. All these three species feature high symmetry and stability as well as delocalized π electrons, a visible sign of aromaticity, but their aromatic origin remains a challenge. This work reports new chemical insights into the π electrons of C13H9+/0/− and deciphers their aromaticity using a recently emerged two-dimensional (2D) superatomic-molecule theory. 12π-C13H9+, 13π-C13H9˙, and 14π-C13H9 are seen as triangular 2D superatomic molecules O3, O3, and O32−, respectively, where O denotes a 2D benzenoid superatom bearing 4 π electrons. Visualized superatomic Lewis structures show that each O can dynamically adjust its π electrons to satisfy the superatomic sextet rule of benzene via superatomic lone pairs and covalent bonds. C13H9+/0/− are representatives of adaptive aromaticity in the 2D superatomic-molecule system, exhibiting flexible π electronic structures to achieve shell-closure. Moreover, we specially adopt a progressive methodology to study the evolution of 2D periodic materials, by applying this theory to the similar family of C6H3N7, C18H6N22 and graphitic carbon nitride (g-C3N4) crystals, and meanwhile accounting for the special stability of g-C3N4. This work enriches 2D superatomic bonding chemistry and provides a useful strategy to design new 2D functional nanostructured materials.

Graphical abstract: Unraveling the flexible aromaticity of C13H9+/0/−: a 2D superatomic-molecule theory

Supplementary files

Article information

Article type
Paper
Submitted
10 Jan 2023
Accepted
21 Feb 2023
First published
23 Feb 2023

Phys. Chem. Chem. Phys., 2023,25, 8439-8445

Unraveling the flexible aromaticity of C13H9+/0/−: a 2D superatomic-molecule theory

D. Li, C. Yan, Q. Yuan, L. Shi and L. Cheng, Phys. Chem. Chem. Phys., 2023, 25, 8439 DOI: 10.1039/D3CP00125C

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