Department of Chemistry and Oregon Center for Optics, University of Oregon, Eugene, Oregon 97403, USA.
J Chem Phys. 2009 Dec 14;131(22):224302. doi: 10.1063/1.3257597.
The preceding paper [J. D. Biggs and J. A. Cina, J. Chem. Phys. 131, 224101 (2009)] (referred to here as Paper 1), describes a strategy for externally influencing the course of short-time electronic excitation transfer (EET) in molecular dimers and observing the process by nonlinear wave-packet interferometry (nl-WPI). External influence can, for example, be exerted by inducing coherent intramolecular vibration in one of the chromophores prior to short-pulse electronic excitation of the other. Within a sample of isotropically oriented dimers having a specified internal geometry, a vibrational mode internal to the acceptor chromophore can be preferentially driven by electronically nonresonant impulsive stimulated Raman (or resonant infrared) excitation with a short polarized "control" pulse. A subsequent electronically resonant polarized pump then preferentially excites the donor, and EET ensues. Paper 1 investigates control-pulse-influenced nl-WPI as a tool for the spectroscopic evaluation of the effect of coherent molecular vibration on excitation transfer, presenting general expressions for the nl-WPI difference signal from a dimer following the action of a control pulse of arbitrary polarization and shape. Electronic excitation is to be effected and its interchromophore transfer monitored by resonant pump and probe "pulses," respectively, each consisting of an optical-phase-controlled ultrashort pulse-pair having arbitrary polarization, duration, center frequency, and other characteristics. Here we test both the control strategy and its spectroscopic investigation-with some sacrifice of amplitude-level detail-by calculating the pump-probe difference signal. That signal is the limiting case of the control-influenced nl-WPI signal in which the two pulses in the pump pulse-pair coincide, as do the two pulses in the probe pulse-pair. We present calculated pump-probe difference signals for (1) a model excitation-transfer complex in which two equal-energy monomers each support one moderately Franck-Condon active intramolecular vibration; (2) a simplified model of the covalent dimer dithia-anthracenophane, representing its EET dynamics following selective impulsive excitation of the weakly Franck-Condon active nu(12) anthracene vibration at 385 cm(-1); and (3) a model complex featuring moderate electronic-vibrational coupling in which the site energy of the acceptor chromophore is lower than that of the donor.
前文[J. D. Biggs 和 J. A. Cina, J. Chem. Phys. 131, 224101 (2009)](这里称为 Paper 1)描述了一种通过非线性波包干涉法(nl-WPI)外部影响短时间电子激发转移(EET)过程并观察其进程的策略。外部影响可以通过在另一个发色团的短脉冲电子激发之前,诱导一个发色团内的相干分子振动来施加。在具有特定内部几何形状的各向同性取向二聚体样品中,可以通过用短偏振“控制”脉冲进行非共振脉冲激发来优先驱动受激拉曼(或共振红外)激发的处于接受体发色团内的振动模式。随后,随后的电子共振极化泵浦优先激发供体,随后发生 EET。Paper 1 研究了控制脉冲影响的 nl-WPI 作为评估相干分子振动对激发转移影响的光谱工具,提出了用于描述控制脉冲作用后二聚体 nl-WPI 差分信号的一般表达式,控制脉冲具有任意偏振和形状。电子激发是通过分别由具有任意偏振、持续时间、中心频率和其他特性的光学相控超短脉冲对组成的共振泵浦和探测“脉冲”来实现的,并监测其两个发色团之间的转移。在这里,我们通过计算泵浦-探测差分信号来测试控制策略及其光谱研究-牺牲了一些幅度细节。该信号是控制影响 nl-WPI 信号的极限情况,其中泵浦脉冲对中的两个脉冲重合,探针脉冲对中的两个脉冲也重合。我们为(1)一个模型激发转移复合物,其中两个等能量单体各支持一个中等 Franck-Condon 活性的分子内振动;(2)简化的二硫代蒽并菲共价二聚体模型,代表其在 385 cm(-1) 处对弱 Franck-Condon 活性 nu(12)蒽振动进行选择性脉冲激发后的 EET 动力学;和(3)一个具有中等电子-振动耦合的模型复合物,其中接受体发色团的位能低于供体。