Department of Chemistry, Graduate School of Science, Hiroshima University, Higashi-Hiroshima 739-8526, Japan.
Phys Chem Chem Phys. 2018 Jul 4;20(26):17583-17598. doi: 10.1039/c8cp00414e.
An experimental and theoretical study has been carried out to elucidate the nonradiative decay (NRD) and trans(E) → cis(Z) isomerization from the S1 (1ππ*) state of structural isomers of hydroxy methylcinnamate (HMC); ortho-, meta- and para-HMC (o-, m- and p-HMC). A low temperature matrix-isolation Fourier Transform Infrared (FTIR) spectroscopic study revealed that all the HMCs are cis-isomerized upon UV irradiation. A variety of laser spectroscopic methods have been utilized for jet-cooled gas phase molecules to investigate the vibronic structure and lifetimes of the S1 state, and to detect the transient state appearing in the NRD process. In p-HMC, the zero-point level of the S1 state decays as quickly as 9 ps. A transient electronic state reported by Tan et al. (Faraday Discuss. 2013, 163, 321-340) was reinvestigated by nanosecond UV-tunable deep UV pump-probe spectroscopy and was assigned to the T1 state. For m- and o-HMC, the lifetime at the zero-point energy level of S1 is 10 ns and 6 ns, respectively, but it becomes substantially shorter at an excess energy higher than 1000 cm-1 and 600 cm-1, respectively, indicating the onset of NRD. Different from p-HMC, no transient state (T1) was observed in m- nor o-HMC. These experimental results are interpreted with the aid of TDDFT calculations by considering the excited-state reaction pathways and the radiative/nonradiative rate constants. It is concluded that in p-HMC, the trans → cis isomerization proceeds via a [trans-S1 → 1nπ* → T1 → cis-S0] scheme. On the other hand, in o- and m-HMC, the isomerization proceeds via a [trans-S1 → twisting along the C[double bond, length as m-dash]C double bond by 90° on S1 → cis-S0] scheme. The calculated barrier height along the twisting coordinate agrees well with the observed onset of the NRD channel for both o- and m-HMC.
已经进行了一项实验和理论研究,以阐明羟基肉桂酸(HMC)结构异构体的 S1(1ππ*)态的非辐射衰减(NRD)和 trans(E)→cis(Z)异构化; 邻-、间-和对-羟基肉桂酸(o-、m-和 p-HMC)。低温基质隔离傅里叶变换红外(FTIR)光谱研究表明,所有 HMC 在紫外线照射下均发生顺式异构化。各种激光光谱方法已被用于喷射冷却气相分子,以研究 S1 态的振电子结构和寿命,并检测 NRD 过程中出现的瞬态。在 p-HMC 中,S1 态的零点级迅速衰减至 9 ps。Tan 等人报道的瞬态电子态(Faraday Discuss. 2013, 163, 321-340)通过纳秒可调紫外深紫外泵浦探测光谱进行了重新研究,并被分配到 T1 态。对于 m-和 o-HMC,S1 的零点能级的寿命分别为 10 ns 和 6 ns,但在超过 1000 cm-1 和 600 cm-1 的过剩能量时,寿命会大大缩短,表明 NRD 的开始。与 p-HMC 不同,在 m-或 o-HMC 中均未观察到瞬态(T1)。这些实验结果通过考虑激发态反应途径和辐射/非辐射速率常数,借助 TDDFT 计算进行了解释。得出的结论是,在 p-HMC 中,trans→cis 异构化通过[trans-S1→1nπ*→T1→cis-S0]方案进行。另一方面,在 o-和 m-HMC 中,异构化通过[trans-S1→沿 C[双键,长度为 m-dash]C 双键扭曲 90°在 S1→cis-S0]方案进行。沿扭曲坐标计算的势垒高度与 o-和 m-HMC 中 NRD 通道的观测起始很好地吻合。