Koch Denise M, Timerghazin Qadir K, Peslherbe Gilles H, Ladanyi Branka M, Hynes James T
Centre for Research in Molecular Modeling, Department of Chemistry & Biochemistry, Concordia University, Montréal, Québec, Canada H4B 1R6.
J Phys Chem A. 2006 Feb 2;110(4):1438-54. doi: 10.1021/jp054692v.
We have investigated the photodissociation dynamics of NaI(H(2)O)(n) [n = 1-4] clusters using the molecular dynamics with quantum transitions method and a quantum mechanics/molecular mechanics description of NaI(H(2)O)(n), which involves a semiempirical valence-bond approach to describe the NaI electronic structure and classical solvent-solvent and solute-solvent interaction potentials. Our simulation results show that the NaI(H(2)O)(n) excited-state population decay upon reaching the NaI curve-crossing region increases with cluster size due to the stabilization of the ionic branch of the NaI excited state by the surrounding water molecules, and the resulting increase in nonadiabatic transition probability. After reaching the curve-crossing region for the first time, however, the excited-state population decay resembles that of bare NaI because of rapid evaporation of 99% and 95% of the water molecules for NaI(H(2)O) and NaI(H(2)O)(n) [n = 2-4], respectively. This extensive evaporation is due to the reversed NaI polarity in the Franck-Condon region of the NaI first excited state, which causes strong repulsive NaI-H(2)O forces and induces rapid nonstatistical water evaporation, where product water molecules are formed more rotationally than translationally hot. A few water molecules (5% or less) remain transiently or permanently bound to NaI, forming long-lived clusters, when NaI remains predominantly ionic, i.e., remains in the excited state, after reaching the curve-crossing region. To connect simulation results with experiment, we have simulated femtosecond probe signals resulting from two-photon and one-photon excitation to the X and I NaI(+) probe states. In agreement with experimental findings, the probe signals resulting from the two-photon probe scheme, where excitation occurs from the covalent branch of the excited state, decay exponentially over the NaI first excited-state vibrational period, with very little evidence of long-time dynamics. The one-photon probe scheme (not used for experimental cluster studies) is shown to be less sensitive to solvation, in that excitation energies will remain similar over a range of cluster sizes, as the ionic branch of the excited state and the NaI(+) probe states are stabilized to the same extent by the presence of water molecules. The resulting probe signals are also more revealing of the NaI(H(2)O)(n) photodissociation dynamics than the two-photon probe signals, as they may allow monitoring of solvation effects on the NaI nonadiabatic dynamics and of successive evaporation of water molecules. Time-resolved photoelectron spectra provide limited additional information regarding the NaI(H(2)O)(n) photodissociation dynamics. A key consequence of the rapid water evaporation demonstrated here is that experimentally observed signals may arise from the photodissociation of much larger NaI(H(2)O)(n) parent clusters.
我们使用量子跃迁分子动力学方法以及对NaI(H₂O)ₙ的量子力学/分子力学描述,研究了NaI(H₂O)ₙ[n = 1 - 4]团簇的光解离动力学,其中对NaI(H₂O)ₙ采用了半经验价键方法来描述NaI的电子结构,并使用经典的溶剂 - 溶剂和溶质 - 溶剂相互作用势。我们的模拟结果表明,由于周围水分子对NaI激发态离子分支的稳定作用以及非绝热跃迁概率的增加,NaI(H₂O)ₙ在到达NaI曲线交叉区域时激发态布居衰减随团簇尺寸增大。然而,在首次到达曲线交叉区域后,由于NaI(H₂O)和NaI(H₂O)ₙ[n = 2 - 4]中分别有99%和95%的水分子快速蒸发,激发态布居衰减类似于裸NaI的情况。这种大量的蒸发是由于NaI第一激发态的弗兰克 - 康登区域中NaI极性反转,这导致强烈的NaI - H₂O排斥力并引发快速的非统计性水蒸发,产物水分子形成时转动比平动更热。当NaI在到达曲线交叉区域后仍主要保持离子态,即仍处于激发态时,少数水分子(5%或更少)会短暂或永久地与NaI结合,形成长寿命团簇。为了将模拟结果与实验联系起来,我们模拟了双光子和单光子激发到X和I NaI⁺探针态产生的飞秒探测信号。与实验结果一致,双光子探测方案产生的探测信号在NaI第一激发态振动周期内呈指数衰减,其中激发从激发态的共价分支发生,几乎没有长期动力学的证据。单光子探测方案(未用于实验团簇研究)对溶剂化不太敏感,因为在一系列团簇尺寸范围内激发能将保持相似,这是由于激发态的离子分支和NaI⁺探针态在水分子存在下被稳定到相同程度。由此产生的探测信号也比双光子探测信号更能揭示NaI(H₂O)ₙ的光解离动力学,因为它们可能允许监测溶剂化对NaI非绝热动力学的影响以及水分子的连续蒸发。时间分辨光电子能谱提供了关于NaI(H₂O)ₙ光解离动力学的有限额外信息。这里展示的快速水蒸发的一个关键结果是,实验观察到的信号可能来自大得多的NaI(H₂O)ₙ母团簇的光解离。