Key Laboratory of Theoretical Chemistry of Environment, Ministry of Education, School of Chemistry & Environment of South China Normal University, Guangzhou 51006, P. R. China.
Phys Chem Chem Phys. 2018 Sep 26;20(37):23885-23897. doi: 10.1039/c8cp02767f.
Global nonadiabatic switching on-the-fly trajectory surface hopping simulations at the 5SA-CASSCF(6,6)/6-31G quantum level have been employed to probe the photoisomerization mechanism of trans-azobenzene upon ππ* excitation within four coupled singlet low-lying electronic states (S0, S1, S2, and S3). We have performed 586 sampling trajectories (331 starting from S2 and 255 from S3), and we found about half of the sampling trajectories staying on S1 or S2 states as resonances and the other half of them ending on the ground S0 state as active trajectories. The present simulation has demonstrated that there are six distinct photoisomerization pathways which can be summarized as three categories; one is the newly opened inversion-inversion nonreactive isomerization pathway accounting for 40% (34%) of active trajectories at a time constant of 80 fs (320 fs), the other is the inversion-torsion reactive and nonreactive isomerization pathways accounting for 40% (20%) of active trajectories at a time constant of 880 fs (1700 fs), and the third is the torsion-torsion reactive and nonreactive isomerization pathways accounting for 20% (46%) of active trajectories at a time constant of 780 fs (1000 fs) upon S2 (S3) ππ* excitation. The simulated total reactive quantum yield for trans-azobenzene photoisomerization upon S2 (S3) ππ* excitation is about 0.11 (0.13) which is in good agreement with recent experimental results of 0.09-0.20. Furthermore, the newly opened inversion-inversion nonreactive isomerization pathway from the present simulation agrees well with cascade experimental measurements of the Sn → S1 → S0 relaxation mechanism in both branching ratio and time constant.
采用 5SA-CASSCF(6,6)/6-31G 量子水平的全局非绝热快速跃迁轨迹表面跳跃模拟,研究了在四个耦合单重低能电子态(S0、S1、S2 和 S3)内ππ激发下反式偶氮苯的光致异构化机制。我们进行了 586 次采样轨迹(331 次从 S2 开始,255 次从 S3 开始),发现一半左右的采样轨迹作为共振留在 S1 或 S2 态,另一半作为活性轨迹结束在基态 S0 上。本模拟表明,存在六种不同的光致异构化途径,可分为三类;一种是新开辟的反转-反转非反应异构化途径,占活性轨迹的 40%(34%),时间常数为 80 fs(320 fs),另一种是反转-扭转反应和非反应异构化途径,占活性轨迹的 40%(20%),时间常数为 880 fs(1700 fs),第三种是扭转-扭转反应和非反应异构化途径,占活性轨迹的 20%(46%),时间常数为 780 fs(1000 fs),分别对应于 S2(S3)ππ激发。S2(S3)ππ*激发时反式偶氮苯光致异构化的模拟总反应量子产率约为 0.11(0.13),与最近的实验结果 0.09-0.20 吻合较好。此外,本模拟中新开辟的反转-反转非反应异构化途径与 Sn→S1→S0 弛豫机制的级联实验测量在分支比和时间常数上吻合较好。