In the title mol-ecule, C(20)H(21)N(3)O(3), the allyl substituent is rotated out of the plane of its attached phenyl ring [torsion angle 100.66â (15)°]. In the crystal, C-H(Mthphn)â¯O(Mthphn) (Mthphn = meth-oxy-phen-yl) hydrogen bonds lead to the formation of (100) layers that are connected into a three-dimensional network by C-Hâ¯Ï(ring) inter-actions, together with Ï-Ï stacking inter-actions [centroid-to-centroid distance = 3.7318â (10)â à ] between parallel phenyl rings. Hirshfeld surface analysis indicates that the most important contributions to the crystal packing are from Hâ¯H (48.7%) and Hâ¯C/Câ¯H (23.3%) inter-actions. Computational chemistry reveals that the C-H(Mthphn)â¯O(Mthphn) hydrogen bond energy is 47.1â kJâ mol(-1). The theoretical structure, optimized by density functional theory (DFT) at the B3LYP/ 6-311â G(d,p) level, is compared with the experimentally determined mol-ecular structure. The HOMO-LUMO behaviour was elucidated to determine the energy gap.
Crystal structure, Hirshfeld surface analysis, inter-action energy and DFT studies of 4-[(4-allyl-2-meth-oxy-phen-oxy)meth-yl]-1-(4-meth-oxy-phen-yl)-1H-1,2,3-triazole.
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作者:Taia Abdelmaoujoud, Essaber Mohamed, Aatif Abdeljalil, Chkirate Karim, Hökelek Tuncer, Mague Joel T, Sebbar Nada Kheira
| 期刊: | Acta Crystallographica Section E: Crystallographic Communications | 影响因子: | 0.500 |
| 时间: | 2020 | 起止号: | 2020 May 29; 76(Pt 6):962-966 |
| doi: | 10.1107/S2056989020006994 | ||
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