Yamaji Minoru, Ogasawara Michiyo, Inomata Susumu, Nakajima Satoru, Tero-Kubota Shozo, Tobita Seiji, Marciniak Bronislaw
Department of Chemistry, Gunma University, Kiryu 376-8515, Japan.
J Phys Chem A. 2006 Sep 21;110(37):10708-14. doi: 10.1021/jp062671a.
Photochemical properties of photoinduced omega-bond dissociation in naphthyl phenyl ketones having a phenylthiyl moiety as a leaving group, p-(alpha-naphthoyl)benzyl phenyl sulfide (NBPS) and 4-benzoyl-1-naphthylmethyl phenyl sulfide (BNMPS), in solution were investigated by laser flash photolysis techniques. Both ketones were shown to undergo photoinduced omega-bond cleavage of the C-S bond to release the phenyl thiyl radical (PTR) at room temperature. Irrespective of excitation wavelengths of NBPS, a quantum yield (Phi(rad)) of the PTR formation was obtained to be 0.1, whereas that for BNMPS was found to depend on the excitation wavelength, i.e., absorption bands from the ground state (S0) to the excited singlet states, S3, S2, and S1 of BNMPS; Phi(rad)(S3) = 0.77 and Phi(rad)(S2) = Phi(rad)(S1) = 1.0. By using triplet sensitization of p-phenylbenzophenone (PBP), efficiencies (alpha(rad)) of the radical formation in the lowest triplet state (T1(pi,pi*)) of NBPS and BNMPS were determined to be 0 and 1.0, respectively. The agreement between Phi(rad)(S1) and alpha(rad) values for BNMPS indicates that the C-S bond dissociation occurs in the T1 state via the S1 state via a fast intersystem crossing from the S1 to the T1 state. The wavelength dependence of the radical yields upon direct excitation of BNMPS was interpreted in terms of the C-S bond cleavage in the S3 state competing with internal conversion from the S3 to the S2 state. The smaller value of Phi(rad)(S3) than those of Phi(rad)(S1) and Phi(rad)(S2) was proposed to originate from the geminate recombination of singlet radical pairs produced by the bond dissociation via the S3 state. Photoinduced omega-cleavage of NBPS was concluded to take place only in the S1(n,pi*) state. Difference in reactivity of omega-cleavage between the triplet states of NBPS and BNMPS was interpreted in terms of localized triplet exciton in the naphthoyl moieties.
采用激光闪光光解技术研究了以苯硫基为离去基团的萘基苯基酮(对-α-萘甲酰基苄基苯基硫醚(NBPS)和4-苯甲酰基-1-萘基甲基苯基硫醚(BNMPS))在溶液中的光诱导ω键解离的光化学性质。结果表明,两种酮在室温下均能发生光诱导的C-S键ω键断裂,释放出苯硫基自由基(PTR)。无论NBPS的激发波长如何,PTR形成的量子产率(Φ(rad))均为0.1,而BNMPS的量子产率则取决于激发波长,即BNMPS从基态(S0)到激发单重态S3、S2和S1的吸收带;Φ(rad)(S3)=0.77,Φ(rad)(S2)=Φ(rad)(S1)=1.0。通过对二苯甲酮(PBP)进行三重态敏化,测定了NBPS和BNMPS在最低三重态(T1(π,π*))下自由基形成的效率(α(rad)),分别为0和1.0。BNMPS的Φ(rad)(S1)和α(rad)值之间的一致性表明,C-S键解离通过从S1到T1态的快速系间窜越在T1态中经由S1态发生。BNMPS直接激发时自由基产率的波长依赖性是根据S3态中的C-S键断裂与从S3到S2态的内转换竞争来解释的。Φ(rad)(S3)的值小于Φ(rad)(S1)和Φ(rad)(S2)的值,这被认为是由于通过S3态的键解离产生的单线态自由基对的偕二重组所致。得出结论,NBPS的光诱导ω-裂解仅在S1(n,π*)态发生。NBPS和BNMPS三重态之间ω-裂解反应性的差异是根据萘甲酰基部分的局域三重态激子来解释的。