Kuisma Mikael, Rousseaux Benjamin, Czajkowski Krzysztof M, Rossi Tuomas P, Shegai Timur, Erhart Paul, Antosiewicz Tomasz J
Department of Chemistry, University of Jyväskylä, FI-40014 Jyväskylä, Finland.
Laboratoire de Physique de l'École Normale Supérieure, ENS, Université PSL, CNRS, Sorbonne Université, Université de Paris, F-75005 Paris, France.
ACS Photonics. 2022 Mar 16;9(3):1065-1077. doi: 10.1021/acsphotonics.2c00066. Epub 2022 Mar 2.
Ultrastrong coupling (USC) is a distinct regime of light-matter interaction in which the coupling strength is comparable to the resonance energy of the cavity or emitter. In the USC regime, common approximations to quantum optical Hamiltonians, such as the rotating wave approximation, break down as the ground state of the coupled system gains photonic character due to admixing of vacuum states with higher excited states, leading to ground-state energy changes. USC is usually achieved by collective coherent coupling of many quantum emitters to a single mode cavity, whereas USC with a single molecule remains challenging. Here, we show by time-dependent density functional theory (TDDFT) calculations that a single organic molecule can reach USC with a plasmonic dimer, consisting of a few hundred atoms. In this context, we discuss the capacity of TDDFT to represent strong coupling and its connection to the quantum optical Hamiltonian. We find that USC leads to appreciable ground-state energy modifications accounting for a non-negligible part of the total interaction energy, comparable to at room temperature.
超强耦合(USC)是光与物质相互作用的一种独特状态,其中耦合强度与腔或发射体的共振能量相当。在超强耦合状态下,量子光学哈密顿量的常见近似,如旋转波近似,会失效,因为耦合系统的基态由于真空态与更高激发态的混合而获得光子特性,导致基态能量发生变化。超强耦合通常通过许多量子发射体与单模腔的集体相干耦合来实现,而单个分子实现超强耦合仍然具有挑战性。在这里,我们通过含时密度泛函理论(TDDFT)计算表明,单个有机分子可以与由几百个原子组成的等离子体二聚体达到超强耦合。在此背景下,我们讨论了TDDFT表示强耦合的能力及其与量子光学哈密顿量的联系。我们发现,超强耦合会导致基态能量发生可观的变化,这在总相互作用能量中占不可忽略的一部分,与室温下的情况相当。