Journal
INORGANIC CHEMISTRY
Volume 52, Issue 12, Pages 7172-7182Publisher
AMER CHEMICAL SOC
DOI: 10.1021/ic400788g
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Funding
- National Science Foundation [CHE-1058987]
- Government of Saudi Arabia
- Division Of Chemistry
- Direct For Mathematical & Physical Scien [1058987] Funding Source: National Science Foundation
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The molecular structures of 1-t-butyl-1,3-dihydro-2H-imidazol-2-one [H(oim(But))], 1-methyl-1,3-dihydro-2H-benzimidazol-2-one [H(obenzim(Me))], 1-t-butyl-1,3-dihydro-2H-benzimidazol-2-one [H(obenzim(But))], and 1-t-butyl-1,3-dihydro-2H-benzimidazole-2-thione [H(mbenzim(But))] have been determined by single crystal X-ray diffraction. Consideration of the C-O bond lengths in the 2-imidazolones, together with the respective values for 2-thiones and 2-selones, indicates that the C-E bonds in these compounds are intermediate between those of formal C-E single and double bonds, an observation that may be rationalized in terms of a significant contribution of zwitterionic structures that feature single C+-E- dative covalent bonds. In this regard, a natural bond orbital (NBO) analysis of the bonding in H(xim(But)) derivatives demonstrates that a doubly bonded C=E resonance structure is most significant for the oxygen derivative, whereas singly bonded C+-E- resonance structures are dominant for the tellurium derivative, despite the fact that oxygen is more electronegative. The C-E bonding in these compounds is, therefore, significantly different from that in chalcogenoformaldehyde derivatives for which the bonding is well represented by a H2C=E double bonded resonance structure. Comparison of the C-E bond lengths of the imidazolechalcogenones with those of C-E single bonds indicates that the C-O bonds are anomalously short. This observation may be rationalized in terms of the oxygen derivative having not only the most significant pi-component but also a substantial ionic component. The latter results from the C-O bond being the most polar due to a substantial polarization of the sigma-bond in the direction of oxygen, which thereby supplements the pi-polarization and increases the negative charge on oxygen. In contrast, the sigma-polarization for the heavier chalcogens opposes the zwitterionic C+E- pi-polarization and thereby reduces the negative charge on the chalcogen. As such, the C-E bond becomes less polar as the chalcogen becomes heavier, despite the fact that the zwitterionic C+-E- contribution increases.
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