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QM/MM nonadiabatic dynamics simulation on ultrafast excited-state relaxation in osmium(II) compounds in solution

机译:QM / MM非抗动力学动力学模拟超快兴奋状态松弛在溶液中锇(II)化合物

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Photoinduced excited-state relaxation dynamics of organometallic compounds, due to their potential applications in solar cells, organic light-emitting diodes, photocatalysis, etc., have been recently explored by a wealth of ultrafast experimental techniques. However, the corresponding nonadiabatic dynamics simulations are rarely reported. In this work, the early-time excited-state relaxation dynamics of two Os(11) compounds i.e. Os(bpy)(3) and Os(bpy)(2)(dpp) (Os1 and Os2) have been investigated by our recently implemented TD-DFT based generalized surface-hopping dynamics simulation method in combination with the quantum mechanics/molecular mechanics (QM/MM) approach. The metal-to-ligand charge transfer (MLCT) excited singlet states from the Os atom to the bpy and dpp ligands are first populated in the Franck-Condon region. These initially populated excited singlet states will be converted through a series of ultrafast internal conversion and intersystem crossing processes to the lowest triplet state as a result of significant nonadiabatic and spin-orbit couplings among singlet and triplet electronic excited states. The intersystem crossing rates are estimated to be 72 and 53 fs for Os1 and Os2, respectively, which are consistent with experimental measured 100 fs and less than 50 fs. The time-dependent transition density analysis reveals that the MLCT excited states are dominant in the entire relaxation dynamics for either Os1 or Os2; however, the MLCT character changes in these processes. In Os1, the initially populated MLCT state is mainly from the Os atom to one bpy ligand, which is changed to the other two MLCT states. In Os2, the MLCT state that is mainly from the Os atom to the two bpy ligands is converted to the MLCT state from the Os to the dpp ligand. Finally, we have found that inter-ligand electron transfer plays a major role in the excited-state relaxation dynamics of Os1 and Os2; while, the hole transfer is minor. Our results also show that the ligand p
机译:有机金属化合物的光导兴奋状态松弛动力学,由于它们在太阳能电池,有机发光二极管,光催化等中的潜在应用,最近已经通过大量超快实验技术探索。然而,很少报道相应的非抗动动力学模拟。在这项工作中,我们最近研究了两种OS(11)化合物IE OS(BPY)(3)和OS(BPY)(2)(DPP)(DPP)(DPP)(DPP)(DPP)(OS1和OS2)的早期激发状态松弛动态基于TD-DFT基的广义表面跳跃动力学模拟方法,与量子力学/分子机械(QM / MM)接近结合。将来自OS原子的金属到配体电荷转移(MLCT)激发单态态到BPY和DPP配体的首先填充在Franck-Condon区域中。由于单线态和三联电子兴奋状态之间的显着非等压和旋转轨道耦合,这些初始填充的兴奋单态将通过一系列超快内部转换和线性交叉过程转换为最低的三重态态。间接系统交叉率分别估计为OS1和OS2的72和53 FS,其与实验测量的100 fs和小于50 fs一致。时间依赖的过渡密度分析显示,MLCT激发态在OS1或OS2的整个松弛动态中都是显着的;但是,MLCT字符在这些过程中发生变化。在OS1中,最初填充的MLCT状态主要来自OS原子到一个BPY配体,其被改变为另一个两个MLCT状态。在OS2中,主要来自OS原子到两个BPY配体的MLCT状态被转换为从OS到DPP配体的MLCT状态。最后,我们发现,配体间电子转移在OS1和OS2的兴奋状态松弛动态中起着重要作用;虽然,孔转移很小。我们的结果还表明配体P.

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