2020
DOI: 10.1209/0295-5075/129/24005
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Mode locking in an optomechanical cavity

Abstract: R m r m e i(ms+θm) 2 , where N R is the number of ORC modes within the FBG filtering band, and the positive r m and the real θ m are the amplitude and phase, respectively, of the m'th ORC mode.

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“…The optical finesse in this situation is relatively low (of the order of 10), due to a lower FBG reflectivity, in comparison to the ultralow loss Bragg coated fiber tips. They designed various configurations, with the metallic beam directly fixed on the polished fiber end, inducing a passive alignment 19 21 , or with the light focused on the micromechanical resonator by means of a graded index lens spliced to the end facet of the fiber 22 , 23 . Bolometric self-sustained oscillations above a certain input threshold have been observed, using the heating of the metallic mirror due to optical absorption.…”
Section: Introductionmentioning
confidence: 99%
“…The optical finesse in this situation is relatively low (of the order of 10), due to a lower FBG reflectivity, in comparison to the ultralow loss Bragg coated fiber tips. They designed various configurations, with the metallic beam directly fixed on the polished fiber end, inducing a passive alignment 19 21 , or with the light focused on the micromechanical resonator by means of a graded index lens spliced to the end facet of the fiber 22 , 23 . Bolometric self-sustained oscillations above a certain input threshold have been observed, using the heating of the metallic mirror due to optical absorption.…”
Section: Introductionmentioning
confidence: 99%