Hulkko E, Pikker S, Tiainen V, Tichauer R H, Groenhof G, Toppari J J
Department of Physics and Nanoscience Center, University of Jyväskylä, P.O. Box 35, FI-40014 Jyväskylä, Finland.
Department of Chemistry and Nanoscience Center, University of Jyväskylä, P.O. Box 35, FI-40014 Jyväskylä, Finland.
J Chem Phys. 2021 Apr 21;154(15):154303. doi: 10.1063/5.0037896.
When the enhanced electromagnetic field of a confined light mode interacts with photoactive molecules, the system can be driven into the regime of strong coupling, where new hybrid light-matter states, polaritons, are formed. Polaritons, manifested by the Rabi split in the dispersion, have shown potential for controlling the chemistry of the coupled molecules. Here, we show by angle-resolved steady-state experiments accompanied by multi-scale molecular dynamics simulations that the molecular Stokes shift plays a significant role in the relaxation of polaritons formed by organic molecules embedded in a polymer matrix within metallic Fabry-Pérot cavities. Our results suggest that in the case of Rhodamine 6G, a dye with a significant Stokes shift, excitation of the upper polariton leads to a rapid localization of the energy into the fluorescing state of one of the molecules, from where the energy scatters into the lower polariton (radiative pumping), which then emits. In contrast, for excitonic J-aggregates with a negligible Stokes shift, the fluorescing state does not provide an efficient relaxation gateway. Instead, the relaxation is mediated by exchanging energy quanta matching the energy gap between the dark states and lower polariton into vibrational modes (vibrationally assisted scattering). To understand better how the fluorescing state of a molecule that is not strongly coupled to the cavity can transfer its excitation energy to the lower polariton in the radiative pumping mechanism, we performed multi-scale molecular dynamics simulations. The results of these simulations suggest that non-adiabatic couplings between uncoupled molecules and the polaritons are the driving force for this energy transfer process.
当受限光模式的增强电磁场与光活性分子相互作用时,系统可被驱动至强耦合 regime,在此 regime 中会形成新的混合光物质态——极化激元。由色散中的拉比分裂所表现出的极化激元,已显示出控制耦合分子化学性质的潜力。在此,我们通过角分辨稳态实验并结合多尺度分子动力学模拟表明,分子斯托克斯位移在由嵌入金属法布里 - 珀罗腔体内聚合物基质中的有机分子形成的极化激元弛豫过程中起着重要作用。我们的结果表明,对于具有显著斯托克斯位移的罗丹明 6G 这种染料,上极化激元的激发会导致能量迅速局域到其中一个分子的荧光态,能量从该荧光态散射到下极化激元(辐射泵浦),然后下极化激元发射。相比之下,对于斯托克斯位移可忽略不计的激子 J - 聚集体,荧光态并未提供有效的弛豫通道。相反,弛豫是通过将与暗态和下极化激元之间的能隙匹配的能量量子交换到振动模式(振动辅助散射)来介导的。为了更好地理解在辐射泵浦机制中未与腔体强烈耦合的分子的荧光态如何将其激发能转移到下极化激元,我们进行了多尺度分子动力学模拟。这些模拟结果表明,未耦合分子与极化激元之间的非绝热耦合是此能量转移过程的驱动力。