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Ultrastrong Coupling of a Single Molecule to a Plasmonic Nanocavity: A First-Principles Study.
Kuisma, Mikael; Rousseaux, Benjamin; Czajkowski, Krzysztof M; Rossi, Tuomas P; Shegai, Timur; Erhart, Paul; Antosiewicz, Tomasz J.
Afiliación
  • Kuisma M; Department of Chemistry, University of Jyväskylä, FI-40014 Jyväskylä, Finland.
  • Rousseaux B; Laboratoire de Physique de l'École Normale Supérieure, ENS, Université PSL, CNRS, Sorbonne Université, Université de Paris, F-75005 Paris, France.
  • Czajkowski KM; Faculty of Physics, University of Warsaw, Pasteura 5, PL-02-093 Warsaw, Poland.
  • Rossi TP; Department of Applied Physics, Aalto University, FI-00076 Aalto, Finland.
  • Shegai T; Department of Physics, Chalmers University of Technology, SE-412 96 Gothenburg, Sweden.
  • Erhart P; Department of Physics, Chalmers University of Technology, SE-412 96 Gothenburg, Sweden.
  • Antosiewicz TJ; Faculty of Physics, University of Warsaw, Pasteura 5, PL-02-093 Warsaw, Poland.
ACS Photonics ; 9(3): 1065-1077, 2022 Mar 16.
Article en En | MEDLINE | ID: mdl-35308405
ABSTRACT
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 k B T at room temperature.