Department of Chemistry, University of Michigan, Ann Arbor, Michigan 48109-1055, USA.
Acc Chem Res. 2009 Sep 15;42(9):1299-309. doi: 10.1021/ar800280s.
Multidimensional electronic and vibrational spectroscopies have established themselves over the last decade as uniquely detailed probes of intramolecular structure and dynamics. However, these spectroscopies can also provide powerful tools for probing solute-solvent interactions and the solvation dynamics that they give rise to. To this end, it should be noted that multidimensional spectra can be expressed in terms of optical response functions that differ with respect to the chromophore's quantum state during the various time intervals separating light-matter interactions. The dynamics of the photoinactive degrees of freedom during those time intervals (that is, between pulses) is dictated by potential energy surfaces that depend on the corresponding state of the chromophore. One therefore expects the system to hop between potential surfaces in a manner dictated by the optical response functions. Thus, the corresponding spectra should reflect the system's dynamics during the resulting sequence of nonequilibrium solvation processes. However, the interpretation of multidimensional spectra is often based on the assumption that they reflect the equilibrium dynamics of the photoinactive degrees of freedom on the potential surface that corresponds to the chromophore's ground state. In this Account, we present a systematic analysis of the signature of nonequilibrium solvation dynamics on multidimensional spectra and the ability of various computational methods to capture it. The analysis is performed in the context of the following three model systems: (A) a two-state chromophore with shifted harmonic potential surfaces that differ in frequency, (B) a two-state atomic chromophore in an atomic liquid, and (C) the hydrogen stretch of a moderately strong hydrogen-bonded complex in a dipolar liquid. The following computational methods are employed and compared: (1) exact quantum dynamics (model A only), (2) the semiclassical forward-backward initial value representation (FB-IVR) method (models A and B only), (3) the linearized semiclassical (LSC) method (all three models), and (4) the standard ground-state equilibrium dynamics approach (all three models). The results demonstrate how multidimensional spectra can be used to probe nonequilibrium solvation dynamics in real time and with an unprecedented level of detail. We also show that, unlike the standard method, the LSC and FB-IVR methods can accurately capture the signature of solvation dynamics on the spectra. Our results also suggest that LSC and FB-IVR yield similar results in the presence of rapid dephasing, which is typical in complex condensed-phase systems. This observation gives credence to the use of the LSC method for modeling spectra in complex systems for which an exact or even FB-IVR-based calculation is prohibitively expensive.
多维电子和振动光谱在过去十年中已成为研究分子内结构和动力学的独特而详细的探针。然而,这些光谱也可以为探测溶质-溶剂相互作用及其引发的溶剂化动力学提供有力的工具。为此,应该注意到,多维光谱可以用光学响应函数来表示,这些函数在光与物质相互作用的各个时间间隔内与发色团的量子态有关。在这些时间间隔内(即在脉冲之间),光致非活性自由度的动力学由依赖于发色团相应状态的势能面决定。因此,人们期望系统以由光学响应函数决定的方式在势能面上跳跃。因此,相应的光谱应该反映系统在相应的非平衡溶剂化过程序列中的动力学。然而,多维光谱的解释通常基于这样的假设,即它们反映了与发色团基态对应的势能面上光致非活性自由度的平衡动力学。在本综述中,我们对多维光谱中非平衡溶剂化动力学的特征以及各种计算方法捕捉它的能力进行了系统的分析。该分析是在以下三个模型系统的背景下进行的:(A)具有不同频率的移位谐和势能面的两态发色团,(B)原子液体中的两态原子发色团,以及(C)偶极液体中中等强度氢键复合物的氢伸缩振动。采用并比较了以下计算方法:(1)精确量子动力学(仅模型 A),(2)半经典前向-后向初始值表示(FB-IVR)方法(仅模型 A 和 B),(3)线性化半经典(LSC)方法(所有三个模型),以及(4)标准基态平衡动力学方法(所有三个模型)。结果表明,多维光谱如何可用于实时探测非平衡溶剂化动力学,并具有前所未有的细节水平。我们还表明,与标准方法不同,LSC 和 FB-IVR 方法可以准确地捕捉光谱上溶剂化动力学的特征。我们的结果还表明,在存在快速退相的情况下,LSC 和 FB-IVR 方法会产生相似的结果,这在复杂的凝聚相系统中很常见。这一观察结果为在精确或甚至基于 FB-IVR 的计算过于昂贵的复杂系统中使用 LSC 方法来模拟光谱提供了依据。