{"id":195,"date":"2021-02-03T11:11:53","date_gmt":"2021-02-03T11:11:53","guid":{"rendered":"https:\/\/qo.lab.uq.edu.au\/?page_id=195"},"modified":"2025-05-16T19:18:58","modified_gmt":"2025-05-16T09:18:58","slug":"sensing","status":"publish","type":"page","link":"https:\/\/qo.lab.uq.edu.au\/?page_id=195","title":{"rendered":"Precision sensing &#038; magnetometry"},"content":{"rendered":"\n<p class=\"has-drop-cap\">Optical techniques offer exquisite precision in measurements of motion. This is most prominently illustrated by the recent successful detection of gravitational waves in kilometre scale interferometer which required measurements with attometre resolution &#8211; a thousandth of the width of a proton. However, optical measurements have far broader applications, from observation of nanoscale motion in biology to clocks and inertial sensors in mobile electronics. In our laboratory we seek to apply the precision technologies developed for gravitational wave detection and other major scientific endeavors, into these applications. We focus on silicon chip-integrated sensors and apply them in areas ranging from precision room temperature magnetometry, to accelerometry and acoustic sensing. <\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"384\" height=\"268\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/02\/magnetometry2.jpg\" alt=\"\" class=\"wp-image-173\" style=\"width:640px;height:auto\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/02\/magnetometry2.jpg 384w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/02\/magnetometry2-300x209.jpg 300w\" sizes=\"auto, (max-width: 384px) 100vw, 384px\" \/><\/figure>\n<\/div>\n\n\n<div style=\"height:100px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h2 class=\"wp-block-heading\">Recent Work<\/h2>\n\n\n<div class=\"wp-block-ub-divider ub_divider ub-divider-orientation-horizontal\" id=\"ub_divider_a07f3cea-4962-4578-b46b-6898c6757739\"><div class=\"ub_divider_wrapper\" style=\"position: relative; margin-bottom: 2px; width: 100%; height: 2px; \" data-divider-alignment=\"center\"><div class=\"ub_divider_line\" style=\"border-top: 2px solid #ccc; margin-top: 2px; \"><\/div><\/div><\/div>\n\n\n<h2 class=\"wp-block-heading has-text-align-left has-large-font-size\">Fibre-coupled photonic crystal hydrophone<\/h2>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"695\" height=\"288\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrophone-deployment.png\" alt=\"\" class=\"wp-image-1453\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrophone-deployment.png 695w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrophone-deployment-300x124.png 300w\" sizes=\"auto, (max-width: 695px) 100vw, 695px\" \/><\/figure>\n<\/div>\n\n\n<p>This work presents a micron-scale, free-standing silicon photonic hydrophone that achieves acoustic sensitivities comparable to commercial piezoelectric hydrophones, while being over four orders of magnitude smaller in volume. The device demonstrates pressure sensitivity on the order of mPa\/\u221aHz from 10\u2013200 kHz, with a minimum detectable pressure of 145 \u00b5Pa\/\u221aHz at 22 kHz. Performance was validated both in controlled lab settings and in a wave flume, confirming its suitability for underwater sensing and communication. Its miniature size opens the door to high-resolution acoustic imaging, including the potential to detect micron-scale features such as cellular vibrations.<\/p>\n\n\n\n<p><span style=\"text-decoration:underline;\">Read more:<\/span><\/p>\n\n\n\n<p>L. McQueen, <em>et. al.,<\/em> <a href=\"https:\/\/doi.org\/10.48550\/arXiv.2501.11289\">Fibre-coupled photonic crystal hydrophone<\/a>, <em>arXiv:<\/em>2501.11289, (2025). <\/p>\n\n\n<div class=\"wp-block-ub-divider ub_divider ub-divider-orientation-horizontal\" id=\"ub_divider_58bf3fd1-546c-480d-8173-e4e242d17d31\"><div class=\"ub_divider_wrapper\" style=\"position: relative; margin-bottom: 2px; width: 100%; height: 2px; \" data-divider-alignment=\"center\"><div class=\"ub_divider_line\" style=\"border-top: 2px solid #ccc; margin-top: 2px; \"><\/div><\/div><\/div>\n\n\n<h2 class=\"wp-block-heading has-text-align-left has-large-font-size\">Quantitative profilometric measurement of thin-films<\/h2>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"1333\" height=\"515\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/mangetostrictive_thinfilms.jpg\" alt=\"\" class=\"wp-image-1636\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/mangetostrictive_thinfilms.jpg 1333w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/mangetostrictive_thinfilms-300x116.jpg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/mangetostrictive_thinfilms-1024x396.jpg 1024w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/mangetostrictive_thinfilms-768x297.jpg 768w\" sizes=\"auto, (max-width: 1333px) 100vw, 1333px\" \/><\/figure>\n<\/div>\n\n\n<p>This work presents a DC, non-contact method for quantifying magnetostrictive strain in thin films with an experimentally observed sensitivity of 0.1 ppm. Using optical profilometry the curvature change in coated glass substrate under applied magnetic fields is measured. by applying Stoney\u2019s formula to the curvature, the magnetostrictive stress and strain are extracted without the need for cantilever-based AC techniques, which are more complex and vibration-sensitive. The method also enables insights into film which is difficult with previous techniques. Measurements on galfenol films reveal performance degradation and altered coercivity above 206 nm thickness, motivating further material optimization.<\/p>\n\n\n\n<p><span style=\"text-decoration:underline;\">Read more:<\/span><\/p>\n\n\n\n<p>H. Greenall, <em>et. al.,<\/em> <a href=\"https:\/\/doi.org\/10.1016\/j.apsusc.2024.160105\">Quantitative profilometric measurement of magnetostriction in thin-films<\/a>, <em>Applied Surface Science<\/em>, (2024). <\/p>\n\n\n<div class=\"wp-block-ub-divider ub_divider ub-divider-orientation-horizontal\" id=\"ub_divider_78db5d58-0df6-487a-974f-9cabc9780f2a\"><div class=\"ub_divider_wrapper\" style=\"position: relative; margin-bottom: 2px; width: 100%; height: 2px; \" data-divider-alignment=\"center\"><div class=\"ub_divider_line\" style=\"border-top: 2px solid #ccc; margin-top: 2px; \"><\/div><\/div><\/div>\n\n\n<h2 class=\"wp-block-heading has-text-align-left has-large-font-size\">Waveguide-integrated chip-scale optomechanical magnetometer<\/h2>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"966\" height=\"498\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2023\/10\/galphenol_featured.png\" alt=\"\" class=\"wp-image-1588\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2023\/10\/galphenol_featured.png 966w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2023\/10\/galphenol_featured-300x155.png 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2023\/10\/galphenol_featured-768x396.png 768w\" sizes=\"auto, (max-width: 966px) 100vw, 966px\" \/><\/figure>\n<\/div>\n\n\n<p>This work introduces an optomechanical magnetometer that uses on-chip suspended optical waveguides for excitation and readout, eliminating the need for bulky free-space or tapered fiber coupling. The device consists of a silica microdisk coated with a magnetostrictive galfenol (FeGa) film, which enables magnetic field sensing via mechanically induced shifts in the optical resonance. The sensor operates under ambient conditions, achieves a sensitivity of 2&nbsp;\u03bcT\/\u221aHz reaching the thermomechanical noise limit of the device. It achieves this performance using compact, off-the-shelf portable electronics, paving the way for practical, field-deployable magnetometry systems.<\/p>\n\n\n\n<p><span style=\"text-decoration:underline;\">Read more:<\/span><\/p>\n\n\n\n<p>F. Gotardo, <em>et. al.,<\/em> <a href=\"https:\/\/doi.org\/10.1364\/OE.501960\">Waveguide-integrated chip-scale optomechanical magnetometer<\/a>, <em>Opt. Express<\/em>, (2023). <\/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_8fbdc9c5-d498-4419-8dc6-bb2a809bbcc0\"><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\/\">UQ Privacy Policy<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>Optical techniques offer exquisite precision in measurements of motion. This is most prominently illustrated by the recent successful detection of gravitational waves in kilometre scale interferometer which required measurements with attometre resolution &#8211; a thousandth of the width of a proton. However, optical measurements have far broader applications, from observation of nanoscale motion in biology [&hellip;]<\/p>\n","protected":false},"author":4,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"cybocfi_hide_featured_image":"","footnotes":""},"class_list":["post-195","page","type-page","status-publish","hentry"],"featured_image_src":null,"_links":{"self":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/pages\/195","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=195"}],"version-history":[{"count":5,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/pages\/195\/revisions"}],"predecessor-version":[{"id":1679,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/pages\/195\/revisions\/1679"}],"wp:attachment":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=195"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}