Department of Chemistry, University of Coimbra, Coimbra, Portugal.
J Phys Chem A. 2012 Mar 8;116(9):2131-40. doi: 10.1021/jp211249k. Epub 2012 Feb 27.
Diketene (C(4)H(4)O(2)) monomers were isolated in cryogenic Ar (15 K) and Xe (30 K) matrices. The infrared (IR) spectra of the freshly deposited matrices show that diketene monomers exclusively adopt the 4-methylene-oxetan-2-one form. In situ photochemical transformations of diketene were induced by tunable UV laser light. Diketene was found to be photostable when exposed to near-UV irradiations (λ> 300 nm). Irradiations in the middle-UV domain showed different types of photochemical reactivity occurring upon irradiations with 280 > λ > 240 nm and λ = 225 nm. The photoproducts were characterized by IR spectroscopy supported by B3LYP/6-311++G(d,p) calculations. Upon irradiation in the 280 > λ > 225 nm range, diketene was found to decompose in two ways: (i) with production of two parent ketene molecules (O═C═CH(2)), and (ii) with production of cyclopropanone (CP) plus carbon monoxide. For irradiations in the 280 > λ > 240 nm range, diketene exhibited two additional reactions: (iii) decomposition to allene (H(2)C═C═CH(2)) and carbon dioxide, and (iv) isomerization into cyclobutane-1,3-dione (CB). Of the above photoproducts, CP and CB were consumed by the same UV irradiations that resulted in their generation. Positive spectroscopic identification of CP and CB turned out to be possible with near-UV irradiations: CP decomposes to ethylene and carbon monoxide upon irradiation with λ = 345 nm; CB decomposes exclusively to two parent ketene molecules, without isomerization back to diketene or decarbonylation, upon irradiation with λ = 330 nm. Natural bond orbital (NBO) analysis showed that the two lowest excited singlet states of diketene are almost degenerate in energy and correspond to π* orbitals of C═C and C═O moieties. The NBO calculations helped to establish that the third excited singlet state, in terms of energy, has σ*(3s) Rydberg character, in accord with the literature.
二乙烯酮(C(4)H(4)O(2))单体在低温氩气(15 K)和氙气(30 K)基质中被分离出来。新沉积的基质的红外(IR)光谱表明,二乙烯酮单体仅采用 4-亚甲基-恶唑烷-2-酮形式。通过可调谐紫外激光光诱导二乙烯酮的原位光化学转化。发现二乙烯酮在暴露于近紫外辐射(λ> 300 nm)时是光稳定的。在中紫外区域的辐照显示出在 280 > λ > 240 nm 和 λ = 225 nm 的辐照下发生的不同类型的光化学反应性。光产物通过 IR 光谱进行了表征,并得到了 B3LYP/6-311++G(d,p)计算的支持。在 280 > λ > 225 nm 范围内辐照时,发现二乙烯酮有两种分解方式:(i)生成两个母体乙烯酮分子(O═C═CH(2)),和(ii)生成环丙酮(CP)和一氧化碳。对于 280 > λ > 240 nm 范围内的辐照,二乙烯酮表现出另外两种反应:(iii)分解为丙烯(H(2)C═C═CH(2))和二氧化碳,和(iv)异构化为环丁烷-1,3-二酮(CB)。在上述光产物中,CP 和 CB 被相同的紫外辐射消耗,而这些辐射导致了它们的生成。通过近紫外辐射可以对 CP 和 CB 进行正光谱鉴定:CP 在 λ = 345 nm 辐照下分解为乙烯和一氧化碳;CB 仅在 λ = 330 nm 辐照下分解为两个母体乙烯酮分子,没有异构化回二乙烯酮或脱羰反应。自然键轨道(NBO)分析表明,二乙烯酮的两个最低激发单重态在能量上几乎简并,对应于 C═C 和 C═O 部分的π轨道。NBO 计算有助于确定第三激发单重态,就能量而言,具有 σ(3s) Rydberg 特征,与文献一致。