Low-Loss, Extreme Subdiffraction Photon Confinement via Silicon Carbide Localized Surface Phonon Polariton Resonators

Plasmonics provides great promise for nanophotonic applications. However, the high optical losses inherent in metal-based plasmonic systems have limited progress. Thus, it is critical to identify alternative low-loss materials. One alternative is polar dielectrics that support surface phonon polarit...

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Veröffentlicht in:Nano letters 2013-08, Vol.13 (8), p.3690-3697
Hauptverfasser: Caldwell, Joshua D, Glembocki, Orest J, Francescato, Yan, Sharac, Nicholas, Giannini, Vincenzo, Bezares, Francisco J, Long, James P, Owrutsky, Jeffrey C, Vurgaftman, Igor, Tischler, Joseph G, Wheeler, Virginia D, Bassim, Nabil D, Shirey, Loretta M, Kasica, Richard, Maier, Stefan A
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container_end_page 3697
container_issue 8
container_start_page 3690
container_title Nano letters
container_volume 13
creator Caldwell, Joshua D
Glembocki, Orest J
Francescato, Yan
Sharac, Nicholas
Giannini, Vincenzo
Bezares, Francisco J
Long, James P
Owrutsky, Jeffrey C
Vurgaftman, Igor
Tischler, Joseph G
Wheeler, Virginia D
Bassim, Nabil D
Shirey, Loretta M
Kasica, Richard
Maier, Stefan A
description Plasmonics provides great promise for nanophotonic applications. However, the high optical losses inherent in metal-based plasmonic systems have limited progress. Thus, it is critical to identify alternative low-loss materials. One alternative is polar dielectrics that support surface phonon polariton (SPhP) modes, where the confinement of infrared light is aided by optical phonons. Using fabricated 6H-silicon carbide nanopillar antenna arrays, we report on the observation of subdiffraction, localized SPhP resonances. They exhibit a dipolar resonance transverse to the nanopillar axis and a monopolar resonance associated with the longitudinal axis dependent upon the SiC substrate. Both exhibit exceptionally narrow linewidths (7–24 cm–1), with quality factors of 40–135, which exceed the theoretical limit of plasmonic systems, with extreme subwavelength confinement of (λres 3/V eff)1/3 = 50–200. Under certain conditions, the modes are Raman-active, enabling their study in the visible spectral range. These observations promise to reinvigorate research in SPhP phenomena and their use for nanophotonic applications.
doi_str_mv 10.1021/nl401590g
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However, the high optical losses inherent in metal-based plasmonic systems have limited progress. Thus, it is critical to identify alternative low-loss materials. One alternative is polar dielectrics that support surface phonon polariton (SPhP) modes, where the confinement of infrared light is aided by optical phonons. Using fabricated 6H-silicon carbide nanopillar antenna arrays, we report on the observation of subdiffraction, localized SPhP resonances. They exhibit a dipolar resonance transverse to the nanopillar axis and a monopolar resonance associated with the longitudinal axis dependent upon the SiC substrate. Both exhibit exceptionally narrow linewidths (7–24 cm–1), with quality factors of 40–135, which exceed the theoretical limit of plasmonic systems, with extreme subwavelength confinement of (λres 3/V eff)1/3 = 50–200. Under certain conditions, the modes are Raman-active, enabling their study in the visible spectral range. 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subjects Collective excitations (including excitons, polarons, plasmons and other charge-density excitations)
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Confinement
Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures
Exact sciences and technology
Fullerenes and related materials
Infrared
Nanostructure
Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation
Optical properties of low-dimensional, mesoscopic, and nanoscale materials and structures
Phonons
Physics
Plasmonics
Polaritons
Silicon carbide
Spectra
Surface and interface electron states
Visible and ultraviolet spectra
title Low-Loss, Extreme Subdiffraction Photon Confinement via Silicon Carbide Localized Surface Phonon Polariton Resonators
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