{"id":1383,"date":"2025-10-23T11:33:55","date_gmt":"2025-10-23T01:33:55","guid":{"rendered":"https:\/\/qo.lab.uq.edu.au\/?p=1383"},"modified":"2026-02-20T13:46:29","modified_gmt":"2026-02-20T03:46:29","slug":"nonlinear-wave-dynamics-on-a-chip","status":"publish","type":"post","link":"https:\/\/qo.lab.uq.edu.au\/?p=1383","title":{"rendered":"Paper: Nonlinear wave dynamics on a chip"},"content":{"rendered":"<div style=\"border: 19px groove #ec6666; border-radius: 23%; background-color: inherit; \" class=\"ub-styled-box ub-bordered-box wp-block-ub-styled-box\" id=\"ub-styled-box-ef8bed62-929a-460a-9a69-3635b21d0cce\">\n<p class=\"has-x-large-font-size\" id=\"ub-styled-box-bordered-content-\">This paper has been published in <em>Science<\/em>!<\/p>\n\n\n<\/div>\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n<figure class=\"wp-block-post-featured-image\"><img loading=\"lazy\" decoding=\"async\" width=\"604\" height=\"446\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrodynamics_post-1.png\" class=\"attachment-post-thumbnail size-post-thumbnail wp-post-image\" alt=\"\" style=\"object-fit:cover;\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrodynamics_post-1.png 604w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/hydrodynamics_post-1-300x222.png 300w\" sizes=\"auto, (max-width: 604px) 100vw, 604px\" \/><\/figure>\n\n\n<p>17 Apr 2025<\/p>\n\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h4 class=\"wp-block-heading\" id=\"0-abstract\">Abstract<\/h4>\n\n\n\n<p>Shallow water waves are a striking example of nonlinear hydrodynamics, giving rise to phenomena such as tsunamis and undular waves. These dynamics are typically studied in hundreds-of-meter-long wave flumes. Here, we demonstrate a chip-scale, quantum-enabled wave flume. The wave flume exploits nanometer-thick superfluid helium films and optomechanical interactions to achieve nonlinearities surpassing those of extreme terrestrial flows. Measurements reveal wave steepening, shock fronts, and soliton fission &#8212; nonlinear behaviors long predicted in superfluid helium but never previously directly observed. Our approach enables lithography-defined wave flume geometries, optomechanical control of hydrodynamic properties, and orders of magnitude faster measurements than terrestrial flumes. Together, this opens a new frontier in hydrodynamics, combining quantum fluids and nanophotonics to explore complex wave dynamics at microscale.<\/p>\n\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h4 class=\"wp-block-heading\" id=\"1-figures\">Browse Figures<\/h4>\n\n\n<div class=\"free align wp-block-bicb-carousel\" id='bicbCarousel-1' data-attributes='{&quot;carousels&quot;:[{&quot;image&quot;:{&quot;id&quot;:1444,&quot;url&quot;:&quot;https:\\\/\\\/qo.lab.uq.edu.au\\\/wp-content\\\/uploads\\\/2025\\\/05\\\/1746671557648-c58d9730-f62b-4ba3-ae02-1538e77f8c78_1-2.png&quot;,&quot;alt&quot;:&quot;&quot;,&quot;title&quot;:&quot;1746671557648-c58d9730-f62b-4ba3-ae02-1538e77f8c78_1&quot;,&quot;caption&quot;:&quot;&quot;},&quot;action&quot;:&quot;none&quot;,&quot;link&quot;:&quot;&quot;,&quot;caption&quot;:&quot;Superfluid wave flume. (A) Landscape of terrestrial shallow wave phenomena and flumes. Conventional wave tanks and flumes cluster in a small region of size and addressable Ursell number, far from extreme terrestrial flows (12). Superfluid-based approaches open up a broader parameter space (supplementary materials, section 1.1). (B) False-color scanning electron microscope image, showing the silicon wave flume (blue) addressed by an optical fiber taper (gray). Width and thickness (220 nm) being well below its length L, the device functions effectively as a one-dimensional channel (i.e., a wave flume). (Top left inset) Photonic crystal cavity. (C) Illustration of the wave flume, including its fundamental sloshing mode. (D) Finite element simulation of the cavity optical mode at ~1598-nm wavelength. The evanescent component extending outside the cavity senses superfluid wave motion, shown here with exaggerated amplitude (white line).&quot;},{&quot;image&quot;:{&quot;id&quot;:1447,&quot;url&quot;:&quot;https:\\\/\\\/qo.lab.uq.edu.au\\\/wp-content\\\/uploads\\\/2025\\\/05\\\/1746679780504-59561806-3f3b-4d35-8f14-6e083475b147_1.png&quot;,&quot;alt&quot;:&quot;&quot;,&quot;title&quot;:&quot;1746679780504-59561806-3f3b-4d35-8f14-6e083475b147_1&quot;,&quot;caption&quot;:&quot;&quot;},&quot;action&quot;:&quot;none&quot;,&quot;link&quot;:&quot;&quot;,&quot;caption&quot;:&quot;Backward-leaning waves. (A) (i) In conventional hydrodynamics, wave crests move faster than troughs (  versus  , red arrows), which leads to forward-leaning waves. (ii) Forward-leaning waves as observed by a stationary gauge. (iii and iv) Reverse behavior is predicted for superfluid third-sound waves owing to their different effective gravity (see left). Shaded band represents the range of gvdW achievable for h varying from 2 to 30 nm. (B) Laser drive used to initialize and read out large-amplitude third-sound waves. Mean laser power is kept constant to avoid unwanted thermal drift (supplementary materials, section 2.2). (C) Photodetector voltage measured during wave initialization and readout. (D) Calibrated measurement of wave amplitude versus time for the section of the ringdown highlighted in (C).&quot;},{&quot;image&quot;:{&quot;id&quot;:1445,&quot;url&quot;:&quot;https:\\\/\\\/qo.lab.uq.edu.au\\\/wp-content\\\/uploads\\\/2025\\\/05\\\/1746679855098-e40e4bf4-17a2-4162-812a-e30d511e52e0_1.png&quot;,&quot;alt&quot;:&quot;&quot;,&quot;title&quot;:&quot;1746679855098-e40e4bf4-17a2-4162-812a-e30d511e52e0_1&quot;,&quot;caption&quot;:&quot;&quot;},&quot;action&quot;:&quot;none&quot;,&quot;link&quot;:&quot;&quot;,&quot;caption&quot;:&quot;Superfluid dispersive shock fronts. (A) Observation of dispersive shock fronts. Red arrows indicate signatures of soliton fission. The high-frequency fluctuations observed at all times in this trace are attributed to readout noise rather than wave dynamics. (B) Custom Euler model, including counterpropagation and van der Waals nonlinearities, obtained by evolving a sinusoidal wave initialized with amplitude H = 0.1h (with computation taking ~4 days on a desktop computer). More details are provided in the supplementary materials, section 5. (C) KdV solution obtained using Eq. 1.&quot;},{&quot;image&quot;:{&quot;id&quot;:1446,&quot;url&quot;:&quot;https:\\\/\\\/qo.lab.uq.edu.au\\\/wp-content\\\/uploads\\\/2025\\\/05\\\/1746679884666-c73e5e38-6805-4124-824d-1c5b2ccf5bd3_1.png&quot;,&quot;alt&quot;:&quot;&quot;,&quot;title&quot;:&quot;1746679884666-c73e5e38-6805-4124-824d-1c5b2ccf5bd3_1&quot;,&quot;caption&quot;:&quot;&quot;},&quot;action&quot;:&quot;none&quot;,&quot;link&quot;:&quot;&quot;,&quot;caption&quot;:&quot;Multisoliton fission. (A) Observation of solitary wave fission, superimposed over a sinusoidal modulation at the drive frequency with amplitude H = 1.5 nm (dashed red line). (B) Corrected experimental data, with sinusoidal background subtracted. (C) Custom Euler model. (D) Third-sound KdV solution obtained using Eq. 1, showing the formation of a soliton train. (E) Gravity wave KdV solution obtained using Eq. 1, with reversed nonlinear coefficient \\u03b1. a.u., arbitrary units.&quot;}],&quot;carouselOptions&quot;:{&quot;columns&quot;:{&quot;desktop&quot;:1,&quot;tablet&quot;:2,&quot;mobile&quot;:1},&quot;columnGap&quot;:30,&quot;isLoop&quot;:true,&quot;allowTouchMove&quot;:false,&quot;speed&quot;:1.5,&quot;autoplayOptions&quot;:{&quot;enabled&quot;:true,&quot;delay&quot;:1.5,&quot;disableOnInteraction&quot;:false,&quot;reverseDirection&quot;:false,&quot;pauseOnMouseEnter&quot;:false,&quot;stopOnLastSlide&quot;:false},&quot;freeMode&quot;:{&quot;enabled&quot;:false,&quot;sticky&quot;:false},&quot;effect&quot;:&quot;slide&quot;,&quot;mousewheel&quot;:{&quot;enabled&quot;:false},&quot;pagination&quot;:{&quot;inTablet&quot;:true,&quot;inMobile&quot;:true,&quot;clickable&quot;:true,&quot;dynamicBullets&quot;:false,&quot;border&quot;:[]},&quot;navigation&quot;:{&quot;inTablet&quot;:true,&quot;inMobile&quot;:true}},&quot;align&quot;:&quot;&quot;,&quot;layout&quot;:&quot;&quot;,&quot;width&quot;:{&quot;desktop&quot;:&quot;100%&quot;,&quot;tablet&quot;:&quot;100%&quot;,&quot;mobile&quot;:&quot;100%&quot;},&quot;height&quot;:{&quot;desktop&quot;:&quot;&quot;,&quot;tablet&quot;:&quot;&quot;,&quot;mobile&quot;:&quot;&quot;},&quot;elements&quot;:{&quot;linkNewTab&quot;:false,&quot;linkOn&quot;:&quot;image&quot;},&quot;alignment&quot;:&quot;center&quot;,&quot;background&quot;:{&quot;color&quot;:&quot;#0000&quot;},&quot;padding&quot;:{&quot;vertical&quot;:&quot;30px&quot;,&quot;horizontal&quot;:&quot;10px&quot;},&quot;isPage&quot;:true,&quot;pageSize&quot;:&quot;12px&quot;,&quot;pageColor&quot;:&quot;#146ef5&quot;,&quot;isPrevNext&quot;:true,&quot;prevNextSize&quot;:&quot;25px&quot;,&quot;prevNextColor&quot;:&quot;#fff&quot;,&quot;image&quot;:{&quot;width&quot;:&quot;100%&quot;},&quot;caption&quot;:{&quot;display&quot;:&quot;none&quot;,&quot;position&quot;:&quot;onImage&quot;,&quot;verticalAlign&quot;:&quot;bottom&quot;,&quot;typo&quot;:{&quot;fontSize&quot;:{&quot;desktop&quot;:16,&quot;tablet&quot;:15,&quot;mobile&quot;:15}},&quot;textAlign&quot;:&quot;left&quot;,&quot;colors&quot;:{&quot;color&quot;:&quot;#fff&quot;,&quot;bg&quot;:&quot;#0000&quot;},&quot;overlay&quot;:{&quot;type&quot;:&quot;gradient&quot;,&quot;gradient&quot;:&quot;linear-gradient(0deg, #000 0%, #0000 50%, #0000 100%)&quot;},&quot;padding&quot;:{&quot;top&quot;:&quot;5px&quot;,&quot;right&quot;:&quot;8px&quot;,&quot;bottom&quot;:&quot;5px&quot;,&quot;left&quot;:&quot;8px&quot;}}}'><\/div>\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h4 class=\"wp-block-heading\" id=\"1-figures\">Authors<\/h4>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-28f84493 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"2500\" height=\"1669\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1.jpeg\" alt=\"\" class=\"wp-image-1472\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1.jpeg 2500w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1-300x200.jpeg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1-1024x684.jpeg 1024w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1-768x513.jpeg 768w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1-1536x1025.jpeg 1536w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/matt_headshot-1-2048x1367.jpeg 2048w\" sizes=\"auto, (max-width: 2500px) 100vw, 2500px\" \/><figcaption class=\"wp-element-caption\">Matt Reeves<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"444\" height=\"666\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/03\/walter_wasserman-edited.jpg\" alt=\"\" class=\"wp-image-461\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/03\/walter_wasserman-edited.jpg 444w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2021\/03\/walter_wasserman-edited-200x300.jpg 200w\" sizes=\"auto, (max-width: 444px) 100vw, 444px\" \/><figcaption class=\"wp-element-caption\">Walter Wasserman<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"800\" height=\"800\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/ray_headshot.jpg\" alt=\"\" class=\"wp-image-1473\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/ray_headshot.jpg 800w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/ray_headshot-300x300.jpg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/ray_headshot-150x150.jpg 150w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/ray_headshot-768x768.jpg 768w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><figcaption class=\"wp-element-caption\">Raymond Harrison<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><a href=\"https:\/\/qo.lab.uq.edu.au\/index.php\/team-members\/dr-igor-marinkovic\/\"><img loading=\"lazy\" decoding=\"async\" width=\"476\" height=\"512\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/igor_headshot.jpeg\" alt=\"\" class=\"wp-image-1215\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/igor_headshot.jpeg 476w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/igor_headshot-279x300.jpeg 279w\" sizes=\"auto, (max-width: 476px) 100vw, 476px\" \/><\/a><figcaption class=\"wp-element-caption\">Igor Marinkovi\u0107<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large\"><a href=\"https:\/\/qo.lab.uq.edu.au\/index.php\/team-members\/nicole-luu\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1018\" height=\"1024\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot-1018x1024.jpg\" alt=\"\" class=\"wp-image-1231\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot-1018x1024.jpg 1018w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot-298x300.jpg 298w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot-150x150.jpg 150w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot-768x773.jpg 768w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/headshot.jpg 1457w\" sizes=\"auto, (max-width: 1018px) 100vw, 1018px\" \/><\/a><figcaption class=\"wp-element-caption\">Nicole Luu<\/figcaption><\/figure>\n<\/div><\/div>\n<\/div>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-28f84493 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"800\" height=\"800\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/andreas_headshot.jpg\" alt=\"\" class=\"wp-image-1474\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/andreas_headshot.jpg 800w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/andreas_headshot-300x300.jpg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/andreas_headshot-150x150.jpg 150w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/andreas_headshot-768x768.jpg 768w\" sizes=\"auto, (max-width: 800px) 100vw, 800px\" \/><figcaption class=\"wp-element-caption\">Andreas Sawadsky<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"769\" height=\"1024\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/yasmine_headshot-769x1024.jpg\" alt=\"\" class=\"wp-image-1475\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/yasmine_headshot-769x1024.jpg 769w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/yasmine_headshot-225x300.jpg 225w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/yasmine_headshot-768x1022.jpg 768w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/yasmine_headshot.jpg 1005w\" sizes=\"auto, (max-width: 769px) 100vw, 769px\" \/><figcaption class=\"wp-element-caption\">Yasmine Sfendla<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"482\" height=\"482\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/glen_headshot.png\" alt=\"\" class=\"wp-image-1460\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/glen_headshot.png 482w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/glen_headshot-300x300.png 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/05\/glen_headshot-150x150.png 150w\" sizes=\"auto, (max-width: 482px) 100vw, 482px\" \/><figcaption class=\"wp-element-caption\">Glen Harris<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-large\"><a href=\"https:\/\/qo.lab.uq.edu.au\/index.php\/team-members\/warwick-bowen\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"1024\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot-1024x1024.jpg\" alt=\"\" class=\"wp-image-1157\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot-1024x1024.jpg 1024w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot-300x300.jpg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot-150x150.jpg 150w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot-768x768.jpg 768w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/warwick_headshot.jpg 1080w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/a><figcaption class=\"wp-element-caption\">Warwick Bowen<\/figcaption><\/figure>\n<\/div><\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><a href=\"https:\/\/qo.lab.uq.edu.au\/index.php\/team-members\/dr-christopher-baker\/\"><img loading=\"lazy\" decoding=\"async\" width=\"473\" height=\"472\" src=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/chris_headshot.jpg\" alt=\"\" class=\"wp-image-1204\" style=\"aspect-ratio:1;object-fit:cover\" srcset=\"https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/chris_headshot.jpg 473w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/chris_headshot-300x300.jpg 300w, https:\/\/qo.lab.uq.edu.au\/wp-content\/uploads\/2025\/04\/chris_headshot-150x150.jpg 150w\" sizes=\"auto, (max-width: 473px) 100vw, 473px\" \/><\/a><figcaption class=\"wp-element-caption\">Christopher Baker<\/figcaption><\/figure>\n<\/div><\/div>\n<\/div>\n\n\n\n<div style=\"height:50px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n<div style=\"gap: 20px;\" class=\"align-button-center ub-buttons orientation-button-row ub-flex-wrap wp-block-ub-button\" id=\"ub-button-0ac56672-1cec-4e19-8169-4276189ac9d7\"><div class=\"ub-button-container ub-button-full-container\">\n\t\t\t<a href=\"https:\/\/www.science.org\/doi\/10.1126\/science.ady3042\" target=\"_blank\" rel=\"noopener noreferrer\" class=\"ub-button-block-main  ub-button-full-width \" role=\"button\" style=\"--ub-button-background-color: #9362c4; --ub-button-color: #ffffff; --ub-button-border: none; --ub-button-hover-background-color: #000000; --ub-button-hover-color: #ffffff; --ub-button-hover-border: none; 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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_bfd54733-329e-41db-b48c-1258ff8d655f\"><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","protected":false},"excerpt":{"rendered":"<p>17 Apr 2025 Abstract Shallow water waves are a striking example of nonlinear hydrodynamics, giving rise to phenomena such as tsunamis and undular waves. These dynamics are typically studied in hundreds-of-meter-long wave flumes. Here, we demonstrate a chip-scale, quantum-enabled wave flume. The wave flume exploits nanometer-thick superfluid helium films and optomechanical interactions to achieve nonlinearities [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":1387,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"cybocfi_hide_featured_image":"yes","footnotes":""},"categories":[1],"tags":[],"class_list":["post-1383","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\/hydrodynamics_post-1.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\/hydrodynamics_post-1.png","_links":{"self":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1383","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=1383"}],"version-history":[{"count":15,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1383\/revisions"}],"predecessor-version":[{"id":1820,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/posts\/1383\/revisions\/1820"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=\/wp\/v2\/media\/1387"}],"wp:attachment":[{"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1383"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1383"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/qo.lab.uq.edu.au\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1383"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}