Larsen Ross E, Schwartz Benjamin J
Department of Chemistry and Biochemistry, University of California-Los Angeles, Los Angeles, CA 90095-1569, USA.
J Phys Chem B. 2006 May 18;110(19):9681-91. doi: 10.1021/jp055322+.
The hydrated dielectron is composed of two excess electrons dissolved in liquid water that occupy a single cavity; in both its singlet and triplet spin states there is a significant exchange interaction so the two electrons cannot be considered to be independent. In this paper and the following paper,we present the results of mixed quantum/classical molecular dynamics simulations of the nonadiabatic relaxation dynamics of photoexcited hydrated dielectrons, where we use full configuration interaction (CI) to solve for the two-electron wave function at every simulation time step. To the best of our knowledge, this represents the first systematic treatment of excited-state solvation dynamics where the multiple-electron problem is solved exactly. The simulations show that the effects of exchange and correlation contribute significantly to the relaxation dynamics. For example, spin-singlet dielectrons relax to the ground state on a time scale similar to that of single electrons excited at the same energy, but spin-triplet dielectrons relax much faster. The difference in relaxation dynamics is caused by exchange and correlation: The Pauli exclusion principle imposes very different electronic structure when the electrons' spins are singlet paired than when they are triplet paired, altering the available nonadiabatic relaxation pathways. In addition, we monitor how electronic correlation changes dynamically during nonadiabatic relaxation and show that solvent dynamics cause electron correlation to evolve quite differently for singlet and triplet dielectrons. Despite such differences, our calculations show that both spin states are stable to excited-state dissociation, but that the excited-state stability has different origins for the two spin states. For singlet dielectrons, the stability depends on whether the solvent structure can rearrange to create a second cavity before the ground state is reached. For triplet dielectrons, in contrast, electronic correlation ensures that the two electrons do not dissociate, even if the dielectron is artificially kept from reaching the ground state. In addition, both singlet and triplet dielectrons change shape dramatically during relaxation, so that linear response fails to describe the solvation dynamics for either spin state. In the following paper (Larsen, R. E.; Schwartz, B. J. J. Phys. Chem. B 2006, 110, 9692), we use these simulations to calculate the pump-probe spectroscopic signal expected for photoexcited hydrated dielectrons and to predict an experiment to observe hydrated dielectrons directly.
水合双电子由溶解在液态水中的两个额外电子组成,它们占据一个单腔;在其单重态和三重态自旋状态下,都存在显著的交换相互作用,因此这两个电子不能被视为独立的。在本文及后续论文中,我们展示了光激发水合双电子非绝热弛豫动力学的混合量子/经典分子动力学模拟结果,其中我们在每个模拟时间步使用全组态相互作用(CI)来求解双电子波函数。据我们所知,这代表了对激发态溶剂化动力学的首次系统处理,其中多电子问题得到了精确求解。模拟结果表明,交换和关联效应在弛豫动力学中起着重要作用。例如,自旋单重态双电子弛豫到基态的时间尺度与相同能量激发的单电子相似,但自旋三重态双电子弛豫得快得多。弛豫动力学的差异是由交换和关联引起的:泡利不相容原理在电子自旋为单重态配对时与三重态配对时施加了非常不同的电子结构,改变了可用的非绝热弛豫途径。此外,我们监测了非绝热弛豫过程中电子关联如何动态变化,并表明溶剂动力学导致单重态和三重态双电子的电子关联以截然不同的方式演化。尽管存在这些差异,但我们的计算表明,两种自旋态对激发态解离都是稳定的,但激发态稳定性对于两种自旋态有不同的来源。对于单重态双电子,稳定性取决于溶剂结构是否能在达到基态之前重新排列以形成第二个腔。相比之下,对于三重态双电子,电子关联确保两个电子不会解离,即使人为阻止双电子达到基态。此外,单重态和三重态双电子在弛豫过程中形状都会发生显著变化,因此线性响应无法描述任何一种自旋态的溶剂化动力学。在后续论文(Larsen, R. E.; Schwartz, B. J. J. Phys. Chem. B 2006, 110, 9692)中,我们使用这些模拟来计算光激发水合双电子预期的泵浦 - 探测光谱信号,并预测一个直接观测水合双电子的实验。