Chou Pi-Tai, Pu Shih-Chieh, Cheng Yi-Ming, Yu Wei-Shan, Yu Yueh-Chi, Hung Fa-Tsai, Hu Wei-Ping
Department of Chemistry, National Taiwan University, Taipei, Taiwan, ROC.
J Phys Chem A. 2005 May 5;109(17):3777-87. doi: 10.1021/jp044205w.
The excitation behaviors for 4'-N,N-diethylamino-3-hydroxyflavone (Ia) have been investigated via femtosecond fluorescence upconversion approaches to gain detailed insights into the mechanism of the proton/charge-transfer coupling reaction. In polar solvents such as CH2Cl2 and CH3CN, in addition to a slow, solvent-polarity-dependent rate (a few tens of picoseconds(-1)) of excited-state intramolecular proton transfer (ESIPT) reported previously, early femtosecond relaxation dynamics clearly reveal that the proton-transfer tautomer emission consists of a rise component of a few hundred femtoseconds. The temporal spectral evolution at the time domain of zero to a few hundred femtoseconds further resolves two distinct emission bands consisting of a proton-transfer tautomer emission and a time-dependent Stokes shifted emission. The results, in combination with ab initio calculations on the dipolar vectors for normal and tautomer species, lead us to unveil the importance of the relationship of the dipolar vectors among various states, and hence the corresponding solvation energetics in the overall ESIPT reaction. We conclude a similar dipolar character between ground-state normal (N) and excited proton-transfer tautomer (T*) species, whereas due to the excited-state intramolecular charge transfer (ESICT), the normal excited state (N*) possesses a large dipolar change with respect to N and T*. ESIPT is thus energetically favorable at the Franck-Condon excited N*, and its rate is competitive with respect to the solvation relaxation process. After reaching the solvent equilibration, there exists an equilibrium between N* and T* states in, for example, CH3CN. Due to the greatly different equilibrium polarization between N* and T*, both forward and reversed ESIPT dynamics are associated with a solvent-induced barrier. The latter viewpoint of the equilibrium type of ESIPT in Ia is in agreement with the previous reports based on steady-state, picosecond, and femtosecond dynamic approaches.
通过飞秒荧光上转换方法研究了4'-N,N-二乙氨基-3-羟基黄酮(Ia)的激发行为,以深入了解质子/电荷转移偶联反应的机制。在二氯甲烷和乙腈等极性溶剂中,除了先前报道的激发态分子内质子转移(ESIPT)的缓慢、溶剂极性依赖性速率(几十皮秒(-1))外,早期飞秒弛豫动力学清楚地表明,质子转移互变异构体发射由几百飞秒的上升分量组成。从零到几百飞秒时域的时间光谱演化进一步解析了由质子转移互变异构体发射和时间相关的斯托克斯位移发射组成的两个不同发射带。这些结果与对正常和互变异构体物种偶极矢量的从头算相结合,使我们揭示了不同状态间偶极矢量关系的重要性,以及因此在整个ESIPT反应中相应的溶剂化能量学。我们得出结论,基态正常(N)和激发态质子转移互变异构体(T*)物种之间具有相似的偶极特征,而由于激发态分子内电荷转移(ESICT),正常激发态(N*)相对于N和T具有较大的偶极变化。因此,ESIPT在弗兰克-康登激发的N处能量上是有利的,其速率相对于溶剂化弛豫过程具有竞争力。达到溶剂平衡后,例如在乙腈中,N和T态之间存在平衡。由于N和T之间的平衡极化差异很大,正向和反向ESIPT动力学都与溶剂诱导的势垒相关。Ia中ESIPT平衡类型的后一种观点与基于稳态、皮秒和飞秒动力学方法的先前报道一致。