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紧密间隔的多发色团体系间的激发能转移:能带混合和带内弛豫的影响

Excitation energy transfer between closely spaced multichromophoric systems: effects of band mixing and intraband relaxation.

作者信息

Didraga C, Malyshev V A, Knoester J

机构信息

Institute for Theoretical Physics and Materials Science Centre, University of Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands.

出版信息

J Phys Chem B. 2006 Sep 28;110(38):18818-27. doi: 10.1021/jp0569281.

Abstract

We theoretically analyze the excitation energy transfer between two closely spaced linear molecular J-aggregates, whose excited states are Frenkel excitons. The aggregate with the higher (lower) exciton band edge energy is considered as the donor (acceptor). The celebrated theory of Förster resonance energy transfer (FRET), which relates the transfer rate to the overlap integral of optical spectra, fails in this situation. We point out that, in addition to the well-known fact that the point-dipole approximation breaks down (enabling energy transfer between optically forbidden states), also the perturbative treatment of the electronic interactions between donor and acceptor system, which underlies the Förster approach, in general loses its validity due to overlap of the exciton bands. We therefore propose a nonperturbative method, in which donor and acceptor bands are mixed and the energy transfer is described in terms of a phonon-assisted energy relaxation process between the two new (renormalized) bands. The validity of the conventional perturbative approach is investigated by comparing to the nonperturbative one; in general, this validity improves for lower temperature and larger distances (weaker interactions) between the aggregates. We also demonstrate that the interference between intraband relaxation and energy transfer renders the proper definition of the transfer rate and its evaluation from experiment a complicated issue that involves the initial excitation condition. Our results suggest that the best way of determining this transfer rate between two J-aggregates is to measure the fluorescence kinetics of the acceptor J-band after resonant excitation of the donor J-band.

摘要

我们从理论上分析了两个紧密间隔的线性分子J聚集体之间的激发能量转移,其激发态为弗伦克尔激子。具有较高(较低)激子带边能量的聚集体被视为供体(受体)。著名的福斯特共振能量转移(FRET)理论,即将转移速率与光谱重叠积分相关联的理论,在这种情况下失效。我们指出,除了众所周知的点偶极近似失效(使得在光学禁戒态之间能够进行能量转移)这一事实外,福斯特方法所基于的供体和受体系统之间电子相互作用的微扰处理,通常也由于激子带的重叠而失去其有效性。因此,我们提出一种非微扰方法,其中供体和受体带混合,并且能量转移用两个新的(重整化的)带之间的声子辅助能量弛豫过程来描述。通过与非微扰方法比较来研究传统微扰方法的有效性;一般来说,对于较低温度以及聚集体之间较大距离(较弱相互作用),这种有效性会提高。我们还证明,带内弛豫和能量转移之间的干涉使得转移速率的恰当定义及其从实验中的评估成为一个涉及初始激发条件的复杂问题。我们的结果表明,确定两个J聚集体之间这种转移速率的最佳方法是在供体J带共振激发后测量受体J带的荧光动力学。

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