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Dynamical effects in line shapes for coupled chromophores: Time-averaging approximation

机译:耦合生色团的线形动力学效应:时间平均近似

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For an isolated resonance of an isolated chromophore in a condensed phase, the absorption line shape is often more sharply peaked than the distribution of transition frequencies as a result of motional narrowing. The latter arises from the time-dependent fluctuations of the transition frequencies. It is well known that one can incorporate these dynamical effects into line shape calculations within a semiclassical approach. For a system of coupled chromophores, both the transition frequencies and the interchromophore couplings fluctuate in time. In principle one can again solve this more complicated problem with a related semiclassical approach, but in practice, for large numbers of chromophores, the computational demands are prohibitive. This has led to the development of a number of approximate theoretical approaches to this problem. In this paper we develop another such approach, using a time-averaging approximation. The idea is that, for a single chromophore, a motionally narrowed line shape can be thought of as a distribution of time-averaged frequencies. This idea is developed and tested on both stochastic and more realistic models of isolated chromophores, and also on realistic models of coupled chromophores, and it is found that in all cases this approximation is quite satisfactory, without undue computational demands. This approach should find application for the vibrational spectroscopy of neat liquids, and also for proteins and other complicated multichromophore systems.
机译:对于孤立生色团在凝聚相中的孤立共振,由于运动变窄,吸收线的形状往往比跃迁频率的分布更尖锐。后者源于过渡频率随时间变化的波动。众所周知,可以在半经典方法中将这些动力学效果纳入线形计算中。对于耦合生色团的系统,跃迁频率和生色团间耦合都随时间波动。原则上,可以用一种相关的半经典方法再次解决这一更复杂的问题,但是在实践中,对于大量的生色团,其计算需求是令人望而却步的。这导致针对该问题的许多近似理论方法的发展。在本文中,我们使用时间平均逼近法开发了另一种方法。这个想法是,对于单个生色团,可以将运动上变窄的线形视为时间平均频率的分布。这个想法是在孤立的发色团的随机模型和更现实的模型上以及耦合发色团的现实模型上开发和测试的,并且发现在所有情况下,这种近似都是令人满意的,没有过多的计算需求。这种方法应该在纯液体的振动光谱学中以及蛋白质和其他复杂的多发色团系统中找到应用。

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