Cheng Yi-Ming, Pu Shih-Chieh, Hsu Chia-Jung, Lai Chin-Hung, Chou Pi-Tai
Department of Chemistry National Taiwan University, Taipei, Taiwan 10617, Taiwan.
Chemphyschem. 2006 Jun 12;7(6):1372-81. doi: 10.1002/cphc.200600017.
Detailed insights into the excited-state enol(N*)-keto(T*) intramolecular proton transfer (ESIPT) reaction in 2-(2'-hydroxy-4'-diethylaminophenyl)benzothiazole (HABT) have been investigated via steady-state and femtosecond fluorescence upconversion approaches. In cyclohexane, in contrast to the ultrafast rate of ESIPT for the parent 2-(2'-hydroxyphenyl)benzothiazole (>2.9+/-0.3 x 10(13) s(-1)), HABT undergoes a relatively slow rate (approximately 5.4+/-0.5 x 10(11) s(-1)) of ESIPT. In polar aprotic solvents competitive rate of proton transfer and rate of solvent relaxation were resolved in the early dynamics. After reaching the solvation equilibrium in the normal excited state (N(eq)), ESIPT takes place with an appreciable barrier. The results also show N(eq)(enol)<-->T(eq)(keto) equilibrium, which shifts toward N(eq) as the solvent polarity increases. Temperature-dependent relaxation dynamics further resolved a solvent-induced barrier of 2.12 kcal mol(-1) for the forward reaction in CH(2)Cl(2). The observed spectroscopy and dynamics are rationalized by a significant difference in dipole moment between N(eq)* and T(eq), while the dipolar vector for the enol form in the ground state (N) is in between that of N(eq) and T(eq). Upon N-->N Franck-Condon excitation, ESIPT is energetically favorable, and its rate is competitive with the solvation relaxation process. Upon reaching equilibrium configurations N(eq)* and T(eq), forward and/or backward ESIPT takes place with an appreciable solvent polarity induced barrier due to differences in polarization equilibrium between N(eq) and T(eq)*.
通过稳态和飞秒荧光上转换方法,对2-(2'-羟基-4'-二乙氨基苯基)苯并噻唑(HABT)中激发态烯醇(N*) - 酮(T*)分子内质子转移(ESIPT)反应进行了详细研究。在环己烷中,与母体2-(2'-羟基苯基)苯并噻唑超快的ESIPT速率(>2.9±0.3×10(13) s(-1))相比,HABT的ESIPT速率相对较慢(约5.4±0.5×10(11) s(-1))。在极性非质子溶剂中,质子转移的竞争速率和溶剂弛豫速率在早期动力学中得到解析。在正常激发态(N(eq))达到溶剂化平衡后,ESIPT以可观的势垒发生。结果还显示了N(eq)(烯醇)⇌T(eq)*(酮)平衡,随着溶剂极性增加,该平衡向N(eq)*移动。温度依赖的弛豫动力学进一步解析了在CH(2)Cl(2)中正向反应的溶剂诱导势垒为2.12 kcal mol(-1)。观察到的光谱和动力学通过N(eq)*和T(eq)*之间偶极矩的显著差异得到合理解释,而基态(N)中烯醇形式的偶极矢量介于N(eq)*和T(eq)之间。在N→N弗兰克 - 康登激发后,ESIPT在能量上是有利的,其速率与溶剂化弛豫过程竞争。在达到平衡构型N(eq)*和T(eq)*后,由于N(eq)*和T(eq)*之间极化平衡的差异,正向和/或反向ESIPT以可观的溶剂极性诱导势垒发生。