FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2892189845> ?p ?o ?g. }

• W2892189845 endingPage "4097" @default.
• W2892189845 startingPage "4089" @default.
• W2892189845 abstract "Strong coupling of plasmonic excitations and dipolar emitters, such as organic molecules, has been studied extensively in the last few years. The questions whether strong coupling can be achieved with a single molecule only and how this is unambiguously proven are still under debate. A critical issue of plasmonic in contrast to photonic systems is additional excitonic line broadening, which is often neglected when modeling such systems. This has led to too optimistic design predictions or incorrect interpretation of ambiguous experimental data, for example in models relying on Maxwell solvers without self-consistent incorporation of line broadening effects. In this paper, we present a heuristic modeling approach for strongly coupled systems based on plasmonic nanoparticles and dipolar emitters that accounts for such broadening and elucidates on recent experiments with single emitters. We explicitly focus on a clear and intuitive classical description that utilizes well-established methods, easy to use within typical Maxwell solvers. The heuristic model (i) provides experimentally relevant numbers such as emitter densities, and spectra, (ii) allows discrimination of systems which can reach the strong coupling regime from those which cannot, (iii) allows identification of optimization routes and (iv) nicely matches with experimental findings. In particular, we employ an approach related to quasi normal modes and extinction simulations where the excitonic system is represented by a frequency dependent permittivity. As examples, we investigate two configurations with many but also single emitters which have been studied in recent experiments." @default.
• W2892189845 created "2018-09-27" @default.
• W2892189845 creator A5011562033 @default.
• W2892189845 creator A5028751362 @default.
• W2892189845 creator A5031640491 @default.
• W2892189845 creator A5035889766 @default.
• W2892189845 creator A5083808334 @default.
• W2892189845 date "2018-09-14" @default.
• W2892189845 modified "2023-10-10" @default.
• W2892189845 title "Heuristic Modeling of Strong Coupling in Plasmonic Resonators" @default.
• W2892189845 cites W1964987415 @default.
• W2892189845 cites W1973305697 @default.
• W2892189845 cites W2015877251 @default.
• W2892189845 cites W2017623768 @default.
• W2892189845 cites W2018494532 @default.
• W2892189845 cites W2023147957 @default.
• W2892189845 cites W2025059325 @default.
• W2892189845 cites W2025831648 @default.
• W2892189845 cites W2030102959 @default.
• W2892189845 cites W2050741072 @default.
• W2892189845 cites W2057706146 @default.
• W2892189845 cites W2066651930 @default.
• W2892189845 cites W2067597620 @default.
• W2892189845 cites W2075381039 @default.
• W2892189845 cites W2139160852 @default.
• W2892189845 cites W2141742048 @default.
• W2892189845 cites W2148624855 @default.
• W2892189845 cites W2159688433 @default.
• W2892189845 cites W2239278858 @default.
• W2892189845 cites W2240061123 @default.
• W2892189845 cites W2248374399 @default.
• W2892189845 cites W2322202305 @default.
• W2892189845 cites W2325664304 @default.
• W2892189845 cites W2418622137 @default.
• W2892189845 cites W2432100421 @default.
• W2892189845 cites W2563765440 @default.
• W2892189845 cites W2564807226 @default.
• W2892189845 cites W2568448037 @default.
• W2892189845 cites W2591838500 @default.
• W2892189845 cites W2599610851 @default.
• W2892189845 cites W2674950166 @default.
• W2892189845 cites W2749490065 @default.
• W2892189845 cites W2761506025 @default.
• W2892189845 cites W2783079581 @default.
• W2892189845 cites W2910766595 @default.
• W2892189845 cites W3099870650 @default.
• W2892189845 cites W3100624994 @default.
• W2892189845 cites W4211100070 @default.
• W2892189845 cites W4252624634 @default.
• W2892189845 doi "https://doi.org/10.1021/acsphotonics.8b00766" @default.
• W2892189845 hasPublicationYear "2018" @default.
• W2892189845 type Work @default.
• W2892189845 sameAs 2892189845 @default.
• W2892189845 citedByCount "24" @default.
• W2892189845 countsByYear W28921898452019 @default.
• W2892189845 countsByYear W28921898452020 @default.
• W2892189845 countsByYear W28921898452021 @default.
• W2892189845 countsByYear W28921898452022 @default.
• W2892189845 countsByYear W28921898452023 @default.
• W2892189845 crossrefType "journal-article" @default.
• W2892189845 hasAuthorship W2892189845A5011562033 @default.
• W2892189845 hasAuthorship W2892189845A5028751362 @default.
• W2892189845 hasAuthorship W2892189845A5031640491 @default.
• W2892189845 hasAuthorship W2892189845A5035889766 @default.
• W2892189845 hasAuthorship W2892189845A5083808334 @default.
• W2892189845 hasBestOaLocation W28921898452 @default.
• W2892189845 hasConcept C110879396 @default.
• W2892189845 hasConcept C121332964 @default.
• W2892189845 hasConcept C121864883 @default.
• W2892189845 hasConcept C131584629 @default.
• W2892189845 hasConcept C154945302 @default.
• W2892189845 hasConcept C173523689 @default.
• W2892189845 hasConcept C173801870 @default.
• W2892189845 hasConcept C191897082 @default.
• W2892189845 hasConcept C192562407 @default.
• W2892189845 hasConcept C20788544 @default.
• W2892189845 hasConcept C30475298 @default.
• W2892189845 hasConcept C41008148 @default.
• W2892189845 hasConcept C49040817 @default.
• W2892189845 hasConcept C62520636 @default.
• W2892189845 hasConcept C97126364 @default.
• W2892189845 hasConceptScore W2892189845C110879396 @default.
• W2892189845 hasConceptScore W2892189845C121332964 @default.
• W2892189845 hasConceptScore W2892189845C121864883 @default.
• W2892189845 hasConceptScore W2892189845C131584629 @default.
• W2892189845 hasConceptScore W2892189845C154945302 @default.
• W2892189845 hasConceptScore W2892189845C173523689 @default.
• W2892189845 hasConceptScore W2892189845C173801870 @default.
• W2892189845 hasConceptScore W2892189845C191897082 @default.
• W2892189845 hasConceptScore W2892189845C192562407 @default.
• W2892189845 hasConceptScore W2892189845C20788544 @default.
• W2892189845 hasConceptScore W2892189845C30475298 @default.
• W2892189845 hasConceptScore W2892189845C41008148 @default.
• W2892189845 hasConceptScore W2892189845C49040817 @default.
• W2892189845 hasConceptScore W2892189845C62520636 @default.
• W2892189845 hasConceptScore W2892189845C97126364 @default.
• W2892189845 hasFunder F4320320879 @default.
• W2892189845 hasFunder F4320323688 @default.

• next