Department of Chemistry, Technical University of Denmark, Kemitorvet 207, DK-2800 Kongens Lyngby, Denmark.
Wigner Research Centre for Physics, Hungarian Academy of Sciences, P.O. Box 49, H-1525 Budapest, Hungary.
J Chem Phys. 2019 Sep 14;151(10):104307. doi: 10.1063/1.5115204.
Simulation of the ultrafast excited-state dynamics and elastic X-ray scattering of the [Fe(bmip)] [bmip = 2,6-bis(3-methyl-imidazole-1-ylidine)-4-pyridine] complex is presented and analyzed. We employ quantum wavepacket dynamics simulations on a 5-dimensional potential energy surface (PES) calculated by time-dependent density functional theory with 26 coupled diabatic states. The simulations are initiated by explicit inclusion of a time-dependent electromagnetic field. In the case of resonant excitation into singlet metal-to-ligand charge transfer (MLCT) states, kinetic (exponential) population dynamics are observed with small nuclear motion. In agreement with transient optical absorption spectroscopy experiments, we observe a subpicosecond MLCT → MLCT intersystem crossing and a subsequent decay into triplet metal-centered (MC) states on a picosecond time scale. The simulated time-resolved difference scattering signal is dominated by the MC component, for which the structural distortions are significant. On the other hand, excitation into MC states leads to ballistic (nonexponential) population dynamics with strong nuclear motion. The reason for these ballistic dynamics is that in this case, the excitation occurs into a nonequilibrium region, i.e., far from the minimum of the MC PES. This results in wavepacket dynamics along the principal breathing mode, which is clearly visible in both the population dynamics and difference scattering. Finally, the importance of decomposing the difference scattering into components by electronic states is highlighted, information which is not accessible from elastic X-ray scattering experiments.
呈现并分析了 [Fe(bmip)] [bmip = 2,6-双(3-甲基-咪唑-1-基)吡啶-4-基] 配合物的超快激发态动力学和弹性 X 射线散射的模拟。我们通过使用 26 个耦合非绝热态的含时密度泛函理论在 5 维势能表面 (PES) 上进行量子波包动力学模拟。模拟是通过显式包含时变电磁场来启动的。在共振激发到单重态金属-配体电荷转移 (MLCT) 态的情况下,我们观察到核运动较小的动力学(指数)布居动力学。与瞬态光吸收光谱实验一致,我们观察到亚皮秒 MLCT→MLCT 系间窜越,随后在皮秒时间尺度上衰减到三重态金属中心 (MC) 态。模拟的时间分辨差散射信号主要由 MC 分量主导,其结构变形显著。另一方面,激发到 MC 态会导致具有强核运动的弹道(非指数)布居动力学。这种弹道动力学的原因是,在这种情况下,激发发生在非平衡区域,即远离 MC PES 的最小值。这导致波包沿着主呼吸模式的动力学,这在布居动力学和差散射中都清晰可见。最后,强调了将差散射分解为电子态分量的重要性,这些信息是弹性 X 射线散射实验无法获得的。