Brillouin lasing in whispering gallery micro-resonators

Thresholds of stimulated Brillouin scattering (SBS) in solid-state whispering gallery mode (WGM) microresonators are analyzed. It is shown that the SBS interaction is substantially different here from that known in the bulk case and in the case of water droplet resonators. The reason is the absence...

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Main Authors: B Sturman, I Breunig
Format: Article
Language:English
Published: IOP Publishing 2015-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/17/12/125006
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author B Sturman
I Breunig
author_facet B Sturman
I Breunig
author_sort B Sturman
collection DOAJ
description Thresholds of stimulated Brillouin scattering (SBS) in solid-state whispering gallery mode (WGM) microresonators are analyzed. It is shown that the SBS interaction is substantially different here from that known in the bulk case and in the case of water droplet resonators. The reason is the absence of pure longitudinal acoustic WGMs owing to strong coupling of the longitudinal ( l ) and transverse ( t ) acoustic displacements at the surface of the resonator. As a result, a considerable increase of the SBS thresholds takes place, and the lowest thresholds correspond to the hybrid tl -modes with very large radial indices. Nevertheless, the thresholds lie in the μ W range of the pump power. Dependence of the SBS power thresholds on the modal numbers and the possibility of self-tuning to the SBS resonance are analyzed.
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spelling doaj.art-2af9e88d6d314f78b2781088177037e62023-08-08T14:24:05ZengIOP PublishingNew Journal of Physics1367-26302015-01-01171212500610.1088/1367-2630/17/12/125006Brillouin lasing in whispering gallery micro-resonatorsB Sturman0I Breunig1Institute of Automation and Electrometry , Russian Academy of Sciences, 630090 Novosibirsk, RussiaUniversity of Freiburg , IMTEK, Georges-Köhler-Allee 102, 79110 Freiburg, GermanyThresholds of stimulated Brillouin scattering (SBS) in solid-state whispering gallery mode (WGM) microresonators are analyzed. It is shown that the SBS interaction is substantially different here from that known in the bulk case and in the case of water droplet resonators. The reason is the absence of pure longitudinal acoustic WGMs owing to strong coupling of the longitudinal ( l ) and transverse ( t ) acoustic displacements at the surface of the resonator. As a result, a considerable increase of the SBS thresholds takes place, and the lowest thresholds correspond to the hybrid tl -modes with very large radial indices. Nevertheless, the thresholds lie in the μ W range of the pump power. Dependence of the SBS power thresholds on the modal numbers and the possibility of self-tuning to the SBS resonance are analyzed.https://doi.org/10.1088/1367-2630/17/12/125006whispering gallery modesresonant frequenciesSBS power thresholdsoverlap factorsphase matching
spellingShingle B Sturman
I Breunig
Brillouin lasing in whispering gallery micro-resonators
New Journal of Physics
whispering gallery modes
resonant frequencies
SBS power thresholds
overlap factors
phase matching
title Brillouin lasing in whispering gallery micro-resonators
title_full Brillouin lasing in whispering gallery micro-resonators
title_fullStr Brillouin lasing in whispering gallery micro-resonators
title_full_unstemmed Brillouin lasing in whispering gallery micro-resonators
title_short Brillouin lasing in whispering gallery micro-resonators
title_sort brillouin lasing in whispering gallery micro resonators
topic whispering gallery modes
resonant frequencies
SBS power thresholds
overlap factors
phase matching
url https://doi.org/10.1088/1367-2630/17/12/125006
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