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Structural insight from intermolecular interactions and energy framework analyses of 2-substituted 6,7,8,9-tetrahydro-11 <i>H</i> -pyrido[2,1-b]quinazolin-11-ones

Akmaljon TojiboevLaboratory of Multiphase Systems Thermophysics, Arifov Institute of Ion-Plasma and Laser Technologies of Uzbekistan Academy of Sciences, Durmon yuli str. 33, Tashkent, 100125, UzbekistanBurkhon ElmuradovDepartment of Organic Synthesis and Plant protection, S.Yunusov Institute of Chemistry of Plant Substances, Academy of Sciences of Uzbekistan, Mirzo Ulugbek Str. 77, Tashkent, 100170, UzbekistanHalima MouhibDépartement COSYS, Laboratoire Instrumentation, Simulation et Informatique Scientifique, Université Gustave Eiffel, Cité Descartes, Champs sur Marne, Marne la Vallée Cedex 2, F-77447, FranceK. K. TurgunovLaboratory of Physical Methods of Investigations, S.Yunusov Institute of Chemistry of Plant Substances, Academy of Sciences of Uzbekistan, Mirzo Ulugbek Str. 77, Tashkent, 100170, UzbekistanА. Ш. АбдуразаковLaboratory of Technology of Synthetic Preparations, S.Yunusov Institute of Chemistry of Plant Substances, Academy of Sciences of Uzbekistan, Mirzo Ulugbek Str. 77, Tashkent, 100170, UzbekistanCharos E. MakhmadiyarovaDepartment of Chemistry, Karshi State University, Kuchabog street, 17, Qarshi, UzbekistanB. TashkhodjaevLaboratory of Physical Methods of Investigations, S.Yunusov Institute of Chemistry of Plant Substances, Academy of Sciences of Uzbekistan, Mirzo Ulugbek Str. 77, Tashkent, 100170, UzbekistanS. Z. MirzaevLaboratory of Multiphase Systems Thermophysics, Arifov Institute of Ion-Plasma and Laser Technologies of Uzbekistan Academy of Sciences, Durmon yuli str. 33, Tashkent, 100125, Uzbekistan
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The crystal structures of three mackinazolinone derivatives (2-amino-6,7,8,9-tetrahydro-11H-pyrido[2,1-b]quinazolin-11-one at room temperature, and 2-nitro-6,7,8,9-tetrahydro-11H-pyrido[2,1-b]quinazolin-11-one and N-(11-oxo-6,8,9,11-tetrahydro-7H-pyrido[2,1-b]quinazolin-2-yl)benzamide at 100 K) are explored using X-ray crystallography. To delineate the different intermolecular interactions and the respective interaction energies in the crystal architectures, energy framework analyses were carried out using the CE-B3LYP/6-31G(d,p) method implemented in the CrystalExplorer software. In the structures the different molecules are linked by C-H...O, C-H...N and N-H...O hydrogen bonds. Together with these hydrogen bonds, C-H...π and C-O...π interactions are involved in the formation of a three-dimensional crystal network. A Hirshfeld surface analysis allows the visualization of the two-dimensional fingerprint plots and the quantification of the contributions of H...H, H...C/C...H and H...O/O...H contacts throughout the different crystal structures. To obtain additional information on the intrinsic properties of our targets and to compare the experimental crystal structures with their respective conformations in the gas phase, quantum chemical calculations at the B3LYP-D3BJ/6-311++G(d,p) level of theory, including Grimme's D3 correction term and BJ damping functions, were carried out to account for intramolecular dispersion interactions. The identified energy gaps between the highest occupied and the lowest unoccupied molecular orbitals (HOMO-LUMO gap) of our targets in the gas phase and in two implicit solvents (methanol and dimethyl sulfoxide) allow us to quantify the impact of different substituents on the reactivity of mackinazolinone derivatives.

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