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The nature of π-hole interactions between iodide anions and quinoid rings in the crystalline state

The investigated co-crystal of 3-chloro-N-methyl­pyridinium iodide with tetra­bromo­quinone (3-Cl-N-MePy·I·Br(4)Q) reveals a π-hole interaction between an iodide anion and a quinoid ring involving an n → π* charge transfer. The quinoid ring has a partial negative charge (estimated to be in the range...

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Detalles Bibliográficos
Autores principales: Milašinović, Valentina, Vuković, Vedran, Krawczuk, Anna, Molčanov, Krešimir, Hennig, Christoph, Bodensteiner, Michael
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9980391/
https://www.ncbi.nlm.nih.gov/pubmed/36692857
http://dx.doi.org/10.1107/S2052252523000052
Descripción
Sumario:The investigated co-crystal of 3-chloro-N-methyl­pyridinium iodide with tetra­bromo­quinone (3-Cl-N-MePy·I·Br(4)Q) reveals a π-hole interaction between an iodide anion and a quinoid ring involving an n → π* charge transfer. The quinoid ring has a partial negative charge (estimated to be in the range 0.08–0.11e) and a partial radical character, which is related to the black colour of the crystals (crystals of neutral tetra­bromo­quinone are yellow). A detailed X-ray charge density study revealed two symmetry-independent bond critical points between the iodide anions and carbon atoms of the ring. Their maximum electron density of 0.065 e Å(−3) was reproduced by quantum chemical modelling. The energy of the interaction is estimated to be −11.16 kcal mol(−1), which is comparable to the strength of moderate hydrogen bonding (about −10 kcal mol(−1)); it is dominantly electrostatic in nature, with a considerable dispersion component.