Center of Molecular Spectroscopy and Dynamics, Institute of Basic Science (IBS) , 145 Anam-ro, Seongbuk-gu, Seoul 02841, Republic of Korea.
Department of Chemistry, Korea University , 145 Anam-ro, Seongbuk-gu, Seoul 02841, Republic of Korea.
Acc Chem Res. 2017 Apr 18;50(4):968-976. doi: 10.1021/acs.accounts.7b00002. Epub 2017 Mar 27.
The vibrational frequency of a chosen normal mode is one of the most accurately measurable spectroscopic properties of molecules in condensed phases. Accordingly, infrared absorption and Raman scattering spectroscopy have provided valuable information on both distributions and ensemble-average values of molecular vibrational frequencies, and these frequencies are now routinely used to investigate structure, conformation, and even absolute configuration of chemical and biological molecules of interest. Recent advancements in coherent time-domain nonlinear vibrational spectroscopy have allowed the study of heterogeneous distributions of local structures and thermally driven ultrafast fluctuations of vibrational frequencies. To fully utilize IR probe functional groups for quantitative bioassays, a variety of biological and chemical techniques have been developed to site-specifically introduce vibrational probe groups into proteins and nucleic acids. These IR-probe-labeled biomolecules and chemically reactive systems are subject to linear and nonlinear vibrational spectroscopic investigations and provide information on the local electric field, conformational changes, site-site protein contacts, and/or function-defining features of biomolecules. A rapidly expanding library of data from such experiments requires an interpretive method with atom-level chemical accuracy. However, despite prolonged efforts to develop an all-encompassing theory for describing vibrational solvatochromism and electrochromism as well as dynamic fluctuations of instantaneous vibrational frequencies, purely empirical and highly approximate theoretical models have often been used to interpret experimental results. They are, in many cases, based on the simple assumption that the vibrational frequency of an IR reporter is solely dictated by electric potential or field distribution around the vibrational chromophore. Such simplified description of vibrational solvatochromism generally referred to as vibrational Stark effect theory has been considered to be quite appealing and, even in some cases, e.g., carbonyl stretch modes in amide, ester, ketone, and carbonate compounds or proteins, it works quantitatively well, which makes it highly useful in determining the strength of local electric field around the IR chromophore. However, noting that the vibrational frequency shift results from changes of solute-solvent intermolecular interaction potential along its normal coordinate, Pauli exclusion repulsion, polarization, charge transfer, and dispersion interactions, in addition to the electrostatic interaction between distributed charges of both vibrational chromophore and solvent molecules, are to be properly included in the theoretical description of vibrational solvatochromism. Since the electrostatic and nonelectrostatic intermolecular interaction components have distinctively different distance and orientation dependences, they affect the solvatochromic vibrational properties in a completely different manner. Over the past few years, we have developed a systematic approach to simulating vibrational solvatochromic data based on the effective fragment potential approach, one of the most accurate and rigorous theories on intermolecular interactions. We have further elucidated the interplay of local electric field with the general vibrational solvatochromism of small IR probes in either solvents or complicated biological systems, with emphasis on contributions from non-Coulombic intermolecular interactions to vibrational frequency shifts and fluctuations. With its rigorous foundation and close relation to quantitative interpretation of experimental data, this and related theoretical approaches and experiments will be of use in studying and quantifying the structure and dynamics of biomolecules with unprecedented time and spatial resolution when combined with time-resolved vibrational spectroscopy and chemically sensitive vibrational imaging techniques.
所选的正则模式的振动频率是凝聚相分子最准确的可测量光谱特性之一。因此,红外吸收和拉曼散射光谱学为分子振动频率的分布和总体平均值提供了有价值的信息,并且这些频率现在通常用于研究化学和生物感兴趣分子的结构、构象甚至绝对构型。相干时域非线性振动光谱学的最新进展允许研究局部结构的不均匀分布和振动频率的热驱动超快波动。为了充分利用 IR 探针官能团进行定量生物测定,已经开发了各种生物和化学技术,将振动探针基团特异性地引入蛋白质和核酸中。这些 IR 探针标记的生物分子和化学反应性系统受到线性和非线性振动光谱学研究的影响,并提供有关局部电场、构象变化、蛋白质间的相互作用以及生物分子的功能定义特征的信息。来自此类实验的快速扩展的数据库需要具有原子级化学精度的解释方法。然而,尽管为描述振动溶剂化和电致变色以及瞬时振动频率的动态波动而长期努力开发全面的理论,但纯粹经验和高度近似的理论模型经常用于解释实验结果。在许多情况下,这些模型基于 IR 报告器的振动频率仅由振动发色团周围的电势或电场分布决定的简单假设。这种对振动溶剂化作用的简化描述通常被称为振动斯塔克效应理论,它被认为非常有吸引力,即使在某些情况下,例如酰胺、酯、酮和碳酸盐化合物或蛋白质中的羰基伸缩模式,它也能很好地进行定量,这使得它在确定 IR 发色团周围局部电场强度方面非常有用。然而,需要注意的是,振动频率的位移是由于溶质-溶剂分子间相互作用势能沿着其正则坐标的变化引起的,除了振动发色团和溶剂分子的分布式电荷之间的静电相互作用外,还包括 Pauli 排斥、极化、电荷转移和色散相互作用。因此,在振动溶剂化作用的理论描述中应适当包含这些相互作用。由于静电和非静电分子间相互作用成分具有明显不同的距离和取向依赖性,因此它们以完全不同的方式影响溶剂化振动性质。在过去的几年中,我们基于最准确和严格的分子间相互作用理论之一——有效片段势能方法,开发了一种模拟振动溶剂化数据的系统方法。我们进一步阐明了局部电场与小分子 IR 探针在溶剂或复杂生物系统中的一般振动溶剂化作用之间的相互作用,重点是非库仑分子间相互作用对振动频率位移和波动的贡献。这种理论方法及其相关实验具有严格的基础,并与实验数据的定量解释密切相关,当与时间分辨振动光谱学和化学敏感振动成像技术结合使用时,将用于以前所未有的时间和空间分辨率研究和量化生物分子的结构和动力学。