We demonstrate broadband tuning of an optomechanical microcavity optical resonance by exploring the large optomechanical coupling of a double-wheel microcavity and its uniquely low mechanical stiffness. Using a pump laser with only 13 mW at telecom wavelengths we show tuning of the silicon nitride microcavity resonances over 32 nm. This corresponds to a tuning power efficiency of only 400 mW/nm. By choosing a relatively low optical Q resonance (≈18,000) we prevent the cavity from reaching the regime of regenerative optomechanical oscillations. The static mechanical displacement induced by optical gradient forces is estimated to be as large as 60 nm.
%0 Journal Article
%1 Wiederhecker2011Broadband
%A Wiederhecker, Gustavo S.
%A Manipatruni, Sasikanth
%A Lee, Sunwoo
%A Lipson, Michal
%D 2011
%I OSA
%J Opt. Express
%K optomechanics chip dipole
%N 3
%P 2782--2790
%R 10.1364/oe.19.002782
%T Broadband tuning of optomechanical cavities
%U http://dx.doi.org/10.1364/oe.19.002782
%V 19
%X We demonstrate broadband tuning of an optomechanical microcavity optical resonance by exploring the large optomechanical coupling of a double-wheel microcavity and its uniquely low mechanical stiffness. Using a pump laser with only 13 mW at telecom wavelengths we show tuning of the silicon nitride microcavity resonances over 32 nm. This corresponds to a tuning power efficiency of only 400 mW/nm. By choosing a relatively low optical Q resonance (≈18,000) we prevent the cavity from reaching the regime of regenerative optomechanical oscillations. The static mechanical displacement induced by optical gradient forces is estimated to be as large as 60 nm.
@article{Wiederhecker2011Broadband,
abstract = {{We demonstrate broadband tuning of an optomechanical microcavity optical resonance by exploring the large optomechanical coupling of a double-wheel microcavity and its uniquely low mechanical stiffness. Using a pump laser with only 13 mW at telecom wavelengths we show tuning of the silicon nitride microcavity resonances over 32 nm. This corresponds to a tuning power efficiency of only 400 mW/nm. By choosing a relatively low optical Q resonance (≈18,000) we prevent the cavity from reaching the regime of regenerative optomechanical oscillations. The static mechanical displacement induced by optical gradient forces is estimated to be as large as 60 nm.}},
added-at = {2013-09-09T23:59:35.000+0200},
author = {Wiederhecker, Gustavo S. and Manipatruni, Sasikanth and Lee, Sunwoo and Lipson, Michal},
biburl = {https://www.bibsonomy.org/bibtex/28e171fa7fcd9fda22a8a516fd5b6fcbb/jacksankey},
citeulike-article-id = {9073776},
citeulike-linkout-0 = {http://dx.doi.org/10.1364/oe.19.002782},
citeulike-linkout-1 = {http://www.opticsinfobase.org/abstract.cfm?id=209807},
day = 31,
doi = {10.1364/oe.19.002782},
interhash = {2e0a8b54b873376d561976aae1afa3a4},
intrahash = {8e171fa7fcd9fda22a8a516fd5b6fcbb},
journal = {Opt. Express},
keywords = {optomechanics chip dipole},
month = jan,
number = 3,
pages = {2782--2790},
posted-at = {2011-03-29 01:06:49},
priority = {2},
publisher = {OSA},
timestamp = {2013-09-10T00:08:22.000+0200},
title = {{Broadband tuning of optomechanical cavities}},
url = {http://dx.doi.org/10.1364/oe.19.002782},
volume = 19,
year = 2011
}