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Third Harmonic Mechanism in Complex Plasmonic Fano Structures

[Image: see text] We perform third harmonic spectroscopy of dolmen-type nanostructures, which exhibit plasmonic Fano resonances in the near-infrared. Strong third harmonic emission is predominantly radiated close to the low energy peak of the Fano resonance. Furthermore, we find that the third harmo...

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Autores principales: Metzger, Bernd, Schumacher, Thorsten, Hentschel, Mario, Lippitz, Markus, Giessen, Harald
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2014
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4270418/
https://www.ncbi.nlm.nih.gov/pubmed/25540812
http://dx.doi.org/10.1021/ph5000677
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author Metzger, Bernd
Schumacher, Thorsten
Hentschel, Mario
Lippitz, Markus
Giessen, Harald
author_facet Metzger, Bernd
Schumacher, Thorsten
Hentschel, Mario
Lippitz, Markus
Giessen, Harald
author_sort Metzger, Bernd
collection PubMed
description [Image: see text] We perform third harmonic spectroscopy of dolmen-type nanostructures, which exhibit plasmonic Fano resonances in the near-infrared. Strong third harmonic emission is predominantly radiated close to the low energy peak of the Fano resonance. Furthermore, we find that the third harmonic polarization of the subradiant mode interferes destructively and diminishes the nonlinear signal in the far-field. By comparing the experimental third harmonic spectra with finite element simulations and an anharmonic oscillator model, we find strong indications that the source of the third harmonic is the optical nonlinearity of the bare gold enhanced by the resonant plasmonic polarization.
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spelling pubmed-42704182014-12-22 Third Harmonic Mechanism in Complex Plasmonic Fano Structures Metzger, Bernd Schumacher, Thorsten Hentschel, Mario Lippitz, Markus Giessen, Harald ACS Photonics [Image: see text] We perform third harmonic spectroscopy of dolmen-type nanostructures, which exhibit plasmonic Fano resonances in the near-infrared. Strong third harmonic emission is predominantly radiated close to the low energy peak of the Fano resonance. Furthermore, we find that the third harmonic polarization of the subradiant mode interferes destructively and diminishes the nonlinear signal in the far-field. By comparing the experimental third harmonic spectra with finite element simulations and an anharmonic oscillator model, we find strong indications that the source of the third harmonic is the optical nonlinearity of the bare gold enhanced by the resonant plasmonic polarization. American Chemical Society 2014-05-02 2014-06-18 /pmc/articles/PMC4270418/ /pubmed/25540812 http://dx.doi.org/10.1021/ph5000677 Text en Copyright © 2014 American Chemical Society Terms of Use (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html)
spellingShingle Metzger, Bernd
Schumacher, Thorsten
Hentschel, Mario
Lippitz, Markus
Giessen, Harald
Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title_full Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title_fullStr Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title_full_unstemmed Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title_short Third Harmonic Mechanism in Complex Plasmonic Fano Structures
title_sort third harmonic mechanism in complex plasmonic fano structures
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4270418/
https://www.ncbi.nlm.nih.gov/pubmed/25540812
http://dx.doi.org/10.1021/ph5000677
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