{"id":196,"date":"2011-11-22T15:38:45","date_gmt":"2011-11-22T18:38:45","guid":{"rendered":"https:\/\/sites.ifi.unicamp.br\/alegre\/?p=196"},"modified":"2011-11-22T15:38:45","modified_gmt":"2011-11-22T18:38:45","slug":"a-chip-scale-integrated-cavity-electro-optomechanics-platform","status":"publish","type":"post","link":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/2011\/11\/22\/a-chip-scale-integrated-cavity-electro-optomechanics-platform\/","title":{"rendered":"A chip-scale integrated cavity-electro-optomechanics platform"},"content":{"rendered":"<p><\/p>\n<h2>A chip-scale integrated cavity-electro-optomechanics platform<\/h2>\n<p>\nM. Winger, T. D. Blasius, T. P. Mayer Alegre, A. H. Safavi-Naeini, S. Meenehan, J. Cohen, S. Stobbe, and O. Painter <\/p>\n<p>Optics Express, <b>19<\/b>, 24905-24921 (2011)<br \/><a href=\"http:\/\/www.opticsinfobase.org\/oe\/abstract.cfm?uri=oe-19-25-24905\" target=\"_blank\">doi:10.1364\/OE.19.024905<\/a><\/p>\n<p>We present an integrated optomechanical and electromechanical nanocavity, in which a common mechanical degree of freedom is coupled to an ultrahigh-Q photonic crystal defect cavity and an electrical circuit. <!--more--> The system allows for wide-range, fast electrical tuning of the optical nanocavity resonances, and for electrical control of optical radiation pressure back-action effects such as mechanical amplification (phonon lasing), cooling, and stiffening. These sort of integrated devices offer a new means to efficiently interconvert weak microwave and optical signals, and are expected to pave the way for a new class of micro-sensors utilizing optomechanical back-action for thermal noise reduction and low-noise optical read-out.<\/p>\n<h3>Related Images:<\/h3>","protected":false},"excerpt":{"rendered":"<p>A chip-scale integrated cavity-electro-optomechanics platform M. Winger, T. D. Blasius, T. P. Mayer Alegre, A. H. Safavi-Naeini, S. Meenehan, J. Cohen, S. Stobbe, and O. Painter Optics Express, 19, 24905-24921 (2011)doi:10.1364\/OE.19.024905 We present an integrated optomechanical and electromechanical nanocavity, in which a common mechanical degree of freedom is coupled to an ultrahigh-Q photonic crystal defect &hellip; <\/p>\n<p><a class=\"more-link btn\" href=\"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/2011\/11\/22\/a-chip-scale-integrated-cavity-electro-optomechanics-platform\/\">Continue reading<\/a><\/p>\n","protected":false},"author":19,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"ngg_post_thumbnail":0,"footnotes":""},"categories":[33],"tags":[],"class_list":["post-196","post","type-post","status-publish","format-standard","hentry","category-papers","item-wrap"],"_links":{"self":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/196","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/users\/19"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/comments?post=196"}],"version-history":[{"count":1,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/196\/revisions"}],"predecessor-version":[{"id":197,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/196\/revisions\/197"}],"wp:attachment":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/media?parent=196"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/categories?post=196"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/tags?post=196"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}