{"id":1414,"date":"2025-03-21T16:59:23","date_gmt":"2025-03-21T06:59:23","guid":{"rendered":"https:\/\/qo.lab.uq.edu.au\/?p=1414"},"modified":"2025-05-13T12:01:32","modified_gmt":"2025-05-13T02:01:32","slug":"conference-presentation-superfluid-nanocavities","status":"publish","type":"post","link":"https:\/\/qo.lab.uq.edu.au\/?p=1414","title":{"rendered":"Conference Presentation: Superfluid nanocavities"},"content":{"rendered":"<figure class=\"wp-block-post-featured-image\"><img decoding=\"async\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/cavity-filled-unfilled-2.png\" class=\"attachment-post-thumbnail size-post-thumbnail wp-post-image\" alt=\"\" style=\"object-fit:cover;\" \/><\/figure>\n\n\n<p>21 Mar 2025<\/p>\n\n\n\n<p><a href=\"https:\/\/qo.lab.uq.edu.au\/index.php\/team-members\/nicole-luu\/\">Nicole<\/a> presented on a work-in-progress about superfluid optomechanics at APS March Meeting in Anaheim, California.<\/p>\n\n\n\n<h4 class=\"wp-block-heading\">Abstract<\/h4>\n\n\n\n<p>Superfluid helium has been proven to be an effective optomechanical system due to its low electromagnetic and acoustic dissipation [1]. However, its low refractive index (n<sub>He<\/sub>~1.029) introduces difficulties in confining light and optimizing the co-localization between light and sound in small interaction volumes; current techniques being used to confine superfluid helium are not able to achieve subwavelength-scale interaction volumes [2]. Using integrated photonic circuitry [3], we demonstrate the ability to initialize extremely confined volumes of bulk superfluid helium co-located with high Q optical modes. For the first time, we are able to persistently trap and observe nanoscale volumes of superfluid helium. These sustain GHz first sound modes which, at millikelvin temperatures are in their motional quantum ground state. Building on recent advancements in quantum optomechanics with liquids [4], this work paves the road for the study of superfluid helium in confined volumes and roton physics [5].<\/p>\n\n\n\n<p>References<\/p>\n\n\n\n<p>[1] A. Kashkanova, A. Shkarin, C. Brown, N. Flowers-Jacobs, L. Childress, S. Hoch, L. Hohmann, K. Ott, J. Reichel, and J. Harris, \u201cSuperfluid brillouin optomechanics,\u201d Nat. Phys. 13(1), 74\u201379 (2017).<\/p>\n\n\n\n<p>[2] Glen I. Harris, Andreas Sawadsky, Yasmine L. Sfendla, Walter W. Wasserman, Warwick P. Bowen, and Christopher G. Baker, &#8220;Proposal for a quantum traveling Brillouin resonator,&#8221; Opt. Express 28, 22450-22461 (2020).<\/p>\n\n\n\n<p>[3] W. W. Wasserman, R. A. Harrison, G. I. Harris, A. Sawadsky, Y. L. Sfendla, W. P. Bowen, and C. G. Baker, &#8220;Cryogenic and hermetically sealed packaging of photonic chips for optomechanics,&#8221; Opt. Express 30, 30822-30831 (2022)<\/p>\n\n\n\n<p>[4] He, X., Harris, G.I., Baker, C.G.&nbsp;<em>et al.<\/em>&nbsp;Strong optical coupling through superfluid Brillouin lasing.&nbsp;<em>Nat. Phys.<\/em>&nbsp;16, 417\u2013421 (2020).<\/p>\n\n\n\n<p>[5] V. Milner, A.A. Milner. Controlled excitation of rotons in superfluid helium with an optical centrifuge. Phys. Rev. Lett., 131:166001, Oct 2023.<\/p>\n\n\n\n<p><br><a href=\"https:\/\/summit.aps.org\/events\/MAR-W26\/2\">See details here<\/a><\/p>\n\n\n\n<div style=\"height:250px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-group alignwide is-nowrap is-layout-flex wp-container-core-group-is-layout-6c531013 wp-block-group-is-layout-flex\">\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-6c531013 wp-block-group-is-layout-flex\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"352\" height=\"93\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/qqol.png\" alt=\"\" class=\"wp-image-1058\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/qqol.png 352w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/qqol-300x79.png 300w\" sizes=\"auto, (max-width: 352px) 100vw, 352px\" \/><\/figure>\n\n\n<div class=\"wp-block-ub-divider ub_divider ub-divider-orientation-vertical\" id=\"ub_divider_b70199bf-bc4f-43fb-abbd-bcdc60a99354\"><div class=\"ub_divider_wrapper\" style=\"position: relative; width: 2px; height: 100px; \" data-divider-alignment=\"center\"><div class=\"ub_divider_line\" style=\"border-left: 2px solid #ccc; width: fit-content; height: 100px; \"><\/div><\/div><\/div>\n\n\n<div class=\"wp-block-group is-vertical is-layout-flex wp-container-core-group-is-layout-fe9cc265 wp-block-group-is-layout-flex\">\n<p>Copyright \u00a9 2025 University of Queensland <\/p>\n\n\n\n<p><a href=\"https:\/\/www.uq.edu.au\/legal\/copyright-privacy-disclaimer\/\"><mark style=\"background-color:rgba(0, 0, 0, 0);color:#000000\" class=\"has-inline-color\">UQ Privacy Policy<\/mark><\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>21 Mar 2025 Nicole presented on a work-in-progress about superfluid optomechanics at APS March Meeting in Anaheim, California. Abstract Superfluid helium has been proven to be an effective optomechanical system due to its low electromagnetic and acoustic dissipation [1]. However, its low refractive index (nHe~1.029) introduces difficulties in confining light and optimizing the co-localization between [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":1416,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"cybocfi_hide_featured_image":"","footnotes":""},"categories":[1],"tags":[],"class_list":["post-1414","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-uncategorised"],"featured_image_src":"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/cavity-filled-unfilled-2.png","author_info":{"display_name":false,"author_link":"https:\/\/qo.lab.uq.edu.au\/?author=1"},"jetpack_featured_media_url":"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/cavity-filled-unfilled-2.png","_links":{"self":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1414","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1414"}],"version-history":[{"count":4,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1414\/revisions"}],"predecessor-version":[{"id":1657,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1414\/revisions\/1657"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/media\/1416"}],"wp:attachment":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1414"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1414"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1414"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}