Groenhof Gerrit, Climent Clàudia, Feist Johannes, Morozov Dmitry, Toppari J Jussi
Departamento de Física Teórica de la Materia Condensada and Condensed Matter Physics Center (IFIMAC) , Universidad Autónoma de Madrid , 28049 Madrid , Spain.
J Phys Chem Lett. 2019 Sep 19;10(18):5476-5483. doi: 10.1021/acs.jpclett.9b02192. Epub 2019 Sep 4.
When photoactive molecules interact strongly with confined light modes in optical cavities, new hybrid light-matter states form. They are known as polaritons and correspond to coherent superpositions of excitations of the molecules and of the cavity photon. The polariton energies and thus potential energy surfaces are changed with respect to the bare molecules, such that polariton formation is considered a promising paradigm for controlling photochemical reactions. To effectively manipulate photochemistry with confined light, the molecules need to remain in the polaritonic state long enough for the reaction on the modified potential energy surface to take place. To understand what determines this lifetime, we have performed atomistic molecular dynamics simulations of room-temperature ensembles of rhodamine chromophores strongly coupled to a single confined light mode with a 15 fs lifetime. We investigated three popular experimental scenarios and followed the relaxation after optically pumping (i) the lower polariton, (ii) the upper polariton, or (iii) uncoupled molecular states. The results of the simulations suggest that the lifetimes of the optically accessible lower and upper polaritons are limited by (i) ultrafast photoemission due to the low cavity lifetime and (ii) reversible population transfer into the "dark" state manifold. Dark states are superpositions of molecular excitations but with much smaller contributions from the cavity photon, decreasing their emission rates and hence increasing their lifetimes. We find that population transfer between polaritonic modes and dark states is determined by the overlap between the polaritonic and molecular absorption spectra. Importantly, excitation can also be transferred "upward" from the lower polariton into the dark-state reservoir due to the broad absorption spectra of the chromophores, contrary to the common conception of these processes as a "one-way" relaxation from the dark states down to the lower polariton. Our results thus suggest that polaritonic chemistry relying on modified dynamics taking place within the lower polariton manifold requires cavities with sufficiently long lifetimes and, at the same time, strong light-matter coupling strengths to prevent the back-transfer of excitation into the dark states.
当光活性分子与光学腔中的受限光模式强烈相互作用时,会形成新的混合光-物质态。它们被称为极化激元,对应于分子激发态与腔光子的相干叠加。相对于裸分子,极化激元能量以及势能面会发生变化,因此极化激元的形成被认为是控制光化学反应的一种很有前景的范例。为了用受限光有效地操纵光化学,分子需要在极化激元态保持足够长的时间,以便在修改后的势能面上发生反应。为了理解决定这种寿命的因素,我们对与具有15飞秒寿命的单一受限光模式强耦合的若丹明发色团的室温系综进行了原子分子动力学模拟。我们研究了三种常见的实验情形,并跟踪了光泵浦(i)下极化激元、(ii)上极化激元或(iii)未耦合分子态后的弛豫过程。模拟结果表明,光学可及的下极化激元和上极化激元的寿命受限于:(i)由于腔寿命短导致的超快光发射,以及(ii)向“暗”态流形的可逆布居转移。暗态是分子激发态的叠加,但腔光子的贡献要小得多,这降低了它们的发射速率,从而增加了它们的寿命。我们发现,极化激元模式与暗态之间的布居转移由极化激元与分子吸收光谱之间的重叠决定。重要的是,由于发色团的宽吸收光谱,激发也可以从下极化激元“向上”转移到暗态库中,这与这些过程通常被认为是从暗态到下极化激元的“单向”弛豫的观念相反。因此,我们的结果表明,依赖于在下极化激元流形内发生的修改动力学的极化激元化学需要具有足够长寿命的腔,同时需要强光-物质耦合强度,以防止激发反向转移到暗态。