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Coupling of the First and Second Excited States of R6G Dye with the Fabry–Perot Cavity
Author(s) -
Tanyi Ekembu K.,
Harrison Erin,
On Cansu,
Noginov Mikhail A.
Publication year - 2019
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.201800045
Subject(s) - excited state , resonance (particle physics) , coupling (piping) , standing wave , atomic physics , excitation , molecular physics , fabry–pérot interferometer , absorption (acoustics) , dispersion (optics) , chemistry , physics , materials science , optics , wavelength , quantum mechanics , metallurgy
Coupling of macroscopic ensembles of highly concentrated R6G molecules with aluminum and silver Fabry–Perot cavities of different sizes, in which one or two standing wave modes are in resonance with the absorption transition(s) of the dye molecules, have been studied. (i) It has been found that strong coupling of the cavity with one molecular eigenstate (S 0 →S 1 transition) does not perturb the energies of the other molecular states. (ii) The S 0 →S 2 absorption transition is too weak to strongly couple to the resonant cavity (“λ” standing wave mode). However, the resonant cavity causes a blue shift of the S 0 →S 2 excitation band. (iii) The splitting of the dispersion curve is theoretically predicted and experimentally observed at strong coupling of the cavity resonance (“λ” standing wave mode) with the material resonances of Ag, including bound electron and “epsilon equal zero” transitions.