{"id":192,"date":"2011-10-05T16:16:32","date_gmt":"2011-10-05T19:16:32","guid":{"rendered":"https:\/\/sites.ifi.unicamp.br\/alegre\/?p=192"},"modified":"2011-10-05T16:16:32","modified_gmt":"2011-10-05T19:16:32","slug":"laser-cooling-of-a-nanomechanical-oscillator-into-its-quantum-ground-state-2","status":"publish","type":"post","link":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/2011\/10\/05\/laser-cooling-of-a-nanomechanical-oscillator-into-its-quantum-ground-state-2\/","title":{"rendered":"Laser cooling of a nanomechanical oscillator into its quantum ground state"},"content":{"rendered":"<p><\/p>\n<h2><a href=\"http:\/\/feeds.nature.com\/%7Er\/nature\/rss\/current\/%7E3\/ALHlai5aNTk\/nature10461\" target=\"_blank\">Laser cooling of a nanomechanical oscillator into its quantum ground state<\/a><\/h2>\n<div>\n<p>from <a href=\"https:\/\/www.google.com\/reader\/view\/feed\/http%3A%2F%2Fwww.nature.com%2Fnature%2Fcurrent_issue%2Frss%2F\" target=\"_blank\">Nature<\/a> by Oskar Painter<\/p>\n<div>\n<div><a name=\"15215249648164305440\" href=\"https:\/\/www.google.com\/reader\/view\/user\/15215249648164305440\/state\/com.google\/broadcast\" target=\"_blank\"><\/a><\/div>\n<\/div>\n<\/div>\n<p><strong>Laser cooling of a nanomechanical oscillator into its quantum ground state<\/strong><\/p>\n<p>Nature 478, 7367 (2011). <a href=\"http:\/\/dx.doi.org\/10.1038\/nature10461\" target=\"_blank\">doi:10.1038\/nature10461<\/a><\/p>\n<p>Authors: Jasper Chan, T. P. Mayer <strong>Alegre<\/strong>, Amir H. Safavi-Naeini, Jeff T. Hill, Alex Krause, Simon Gr\u00f6blacher, Markus Aspelmeyer &amp; Oskar Painter<\/p>\n<p>The simple mechanical oscillator, canonically consisting of a  coupled mass\u2013spring system, is used in a wide variety of sensitive  measurements, including the detection of weak forces and small masses. <!--more--> On the one hand, a classical oscillator has a well-defined amplitude of  motion; a quantum oscillator, on the other hand, has a lowest-energy  state, or ground state, with a finite-amplitude uncertainty  corresponding to zero-point motion. On the macroscopic scale of our  everyday experience, owing to interactions with its highly fluctuating  thermal environment a mechanical oscillator is filled with many energy  quanta and its quantum nature is all but hidden. Recently, in  experiments performed at temperatures of a few hundredths of a kelvin,  engineered nanomechanical resonators coupled to electrical circuits have  been measured to be oscillating in their quantum ground state. These  experiments, in addition to providing a glimpse into the underlying  quantum behaviour of mesoscopic systems consisting of billions of atoms,  represent the initial steps towards the use of mechanical devices as  tools for quantum metrology or as a means of coupling hybrid quantum  systems. Here we report the development of a coupled, nanoscale optical  and mechanical resonator formed in a silicon microchip, in which  radiation pressure from a laser is used to cool the mechanical motion  down to its quantum ground state (reaching an average phonon occupancy  number of ). This cooling is realized at an environmental temperature of  20\u2009K, roughly one thousand times larger than in previous experiments  and paves the way for optical control of mesoscale mechanical  oscillators in the quantum regime.<\/p>\n<h3>Related Images:<\/h3>","protected":false},"excerpt":{"rendered":"<p>Laser cooling of a nanomechanical oscillator into its quantum ground state from Nature by Oskar Painter Laser cooling of a nanomechanical oscillator into its quantum ground state Nature 478, 7367 (2011). doi:10.1038\/nature10461 Authors: Jasper Chan, T. P. Mayer Alegre, Amir H. Safavi-Naeini, Jeff T. Hill, Alex Krause, Simon Gr\u00f6blacher, Markus Aspelmeyer &amp; Oskar Painter The &hellip; <\/p>\n<p><a class=\"more-link btn\" href=\"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/2011\/10\/05\/laser-cooling-of-a-nanomechanical-oscillator-into-its-quantum-ground-state-2\/\">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":[4,33,15],"tags":[],"class_list":["post-192","post","type-post","status-publish","format-standard","hentry","category-on-web","category-papers","category-via-google-reader","item-wrap"],"_links":{"self":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/192","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=192"}],"version-history":[{"count":1,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/192\/revisions"}],"predecessor-version":[{"id":193,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/posts\/192\/revisions\/193"}],"wp:attachment":[{"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/media?parent=192"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/categories?post=192"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/sites.ifi.unicamp.br\/alegre\/en\/wp-json\/wp\/v2\/tags?post=192"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}