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How To Excite Nuclear Wavepackets into Electronically Degenerate States in Spin-Vibronic Quantum Dynamics Simulations

机译:如何在旋转式峰值量子动态模拟中激发核波丝进入电子堕落状态

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摘要

The excited-state dynamics of two functional Fe-carbene complexes, [Fe(bmip)(2)](2+) (bmip = 2,6-bis(3-methyl-imidazole-1-ylidene)-pyridine) and [Fe(btbip)(2)](2+) (btbip = 2,6-bis(3-tert-butyl-imidazole-1-ylidene)pyridine), are studied using the spin-vibronic model. In contrast to the usual projection of the ground state nuclear wave function onto an excited state surface, the dynamics are initiated by an explicit interaction term between the external time-dependent electric field (laser pulse) and the transition dipole moment of the molecule. The results show that the spin-vibronic model, as constructed directly from electronic structure calculations, exhibits erroneous, polarization-dependent relaxation dynamics stemming from artificial interference of coupled relaxation pathways. This is due to the lack of rotational invariance in the description of excitation into degenerate states. We introduce and discuss a correction using the spherical basis and complex transition dipole moments. This modification in the interaction Hamiltonian leads to rotationally invariant excitation and produces polarization-independent population dynamics.
机译:利用自旋振动模型研究了两种功能性铁卡宾配合物[Fe(bmip)(2)](2+)(bmip=2,6-二(3-甲基咪唑-1-亚基)-吡啶)和[Fe(btbip)(2)](2+)(btbip=2,6-二(3-叔丁基咪唑-1-亚基)吡啶)的激发态动力学。与基态核波函数通常投射到激发态表面不同,动力学是由外部时变电场(激光脉冲)和分子跃迁偶极矩之间的显式相互作用项引发的。结果表明,由电子结构计算直接建立的自旋-振动模型,由于耦合弛豫路径的人为干扰,表现出错误的、依赖于极化的弛豫动力学。这是因为对简并态激发的描述缺乏旋转不变性。我们介绍并讨论了一种利用球面基和复跃迁偶极矩的校正方法。这种相互作用哈密顿量的改变导致了旋转不变的激发,并产生了与偏振无关的种群动力学。

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