Rider Marie S, Arul Rakesh, Baumberg Jeremy J, Barnes William L
Department of Physics and Astronomy, University of Exeter, Stocker Road, Devon, EX4 4QL, UK.
NanoPhotonics Centre, Department of Physics, University of Cambridge, Cambridge, CB3 0HE, UK.
Nanophotonics. 2022 Aug 3;11(16):3695-3708. doi: 10.1515/nanoph-2022-0301. eCollection 2022 Sep 1.
The strong coupling of molecules with surface plasmons results in hybrid states which are part molecule, part surface-bound light. Since molecular resonances may acquire the spatial coherence of plasmons, which have mm-scale propagation lengths, strong-coupling with molecular resonances potentially enables long-range molecular energy transfer. Gratings are often used to couple incident light to surface plasmons, by scattering the otherwise non-radiative surface plasmon inside the light-line. We calculate the dispersion relation for surface plasmons strongly coupled to molecular resonances when grating scattering is involved. By treating the molecules as independent oscillators rather than the more typically considered single collective dipole, we find the full multi-band dispersion relation. This approach offers a natural way to include the dark states in the dispersion. We demonstrate that for a molecular resonance tuned near the crossing point of forward and backward grating-scattered plasmon modes, the interaction between plasmons and molecules gives a five-band dispersion relation, including a bright state not captured in calculations using a single collective dipole. We also show that the role of the grating in breaking the translational invariance of the system appears in the position-dependent coupling between the molecules and the surface plasmon. The presence of the grating is thus not only important for the experimental observation of molecule-surface-plasmon coupling, but also provides an additional design parameter that tunes the system.
分子与表面等离子体激元的强耦合产生了混合态,这种混合态部分是分子,部分是表面束缚光。由于分子共振可能获得具有毫米级传播长度的等离子体激元的空间相干性,因此与分子共振的强耦合有可能实现长程分子能量转移。光栅常被用于将入射光耦合到表面等离子体激元,方法是在光线范围内散射原本非辐射的表面等离子体激元。当涉及光栅散射时,我们计算了与分子共振强耦合的表面等离子体激元的色散关系。通过将分子视为独立的振荡器,而不是更典型的单个集体偶极子,我们得到了完整的多波段色散关系。这种方法提供了一种在色散中纳入暗态的自然方式。我们证明,对于调谐到向前和向后光栅散射等离子体激元模式交点附近的分子共振,等离子体激元和分子之间的相互作用给出了一个五波段色散关系,包括在使用单个集体偶极子的计算中未捕获的亮态。我们还表明,光栅在打破系统平移不变性方面的作用出现在分子与表面等离子体激元之间位置依赖的耦合中。因此,光栅的存在不仅对分子 - 表面 - 等离子体激元耦合的实验观察很重要,而且还提供了一个调节系统的额外设计参数。