{"id":20728,"date":"2022-10-26T13:45:01","date_gmt":"2022-10-26T13:45:01","guid":{"rendered":"https:\/\/peymantaeidi.net\/stem-cell\/?p=20728"},"modified":"2022-10-26T13:49:20","modified_gmt":"2022-10-26T13:49:20","slug":"researchers-compress-light-12-times-below-the-diffraction-limit-in-a-dielectric-material","status":"publish","type":"post","link":"https:\/\/peymantaeidi.net\/stem-cell\/2022\/10\/26\/researchers-compress-light-12-times-below-the-diffraction-limit-in-a-dielectric-material\/","title":{"rendered":"Researchers compress light 12 times below the diffraction limit in a dielectric material"},"content":{"rendered":"<div class=\"article-gallery lightGallery\">\n<div data-thumb=\"https:\/\/scx1.b-cdn.net\/csz\/news\/tmb\/2022\/researchers-compress-l.jpg\" data-src=\"https:\/\/scx2.b-cdn.net\/gfx\/news\/hires\/2022\/researchers-compress-l.jpg\">2) inside a \u03b4-outline is exposed uniformly with electron-beam lithography; hence, air features defining the device are uniformly tuned. e\u2013g 40\u00b0 tilted SEM images of bowtie region for \u03b4\u2009=\u2009{\u2009\u2212\u20092,\u2009\u2212\u20094,\u2009\u2212\u20096}\u2009nm. We measure the mean width of the fabricated bowties to be (8\u2009\u00b1\u20095)\u2009nm, (10\u2009\u00b1\u20095)\u2009nm, and (16\u2009\u00b1\u20095)\u2009nm for figures e, f, and g, respectively, noting the variation in width along the z-direction caused by the scallops and ~1\u00b0 negative sidewall angle represented by the uncertainty as discussed in the main text. Credit: <i>Nature Communications<\/i> (2022). DOI: 10.1038\/s41467-022-33874-w&#8221;&gt;<\/p>\n<figure class=\"article-img\">\n            <img decoding=\"async\" src=\"https:\/\/peymantaeidi.net\/stem-cell\/wp-content\/uploads\/2022\/10\/researchers-compress-l.jpg\" alt=\"Researchers compress light 12 times below the diffraction limit in a dielectric material\" \/>2) inside a \u03b4-outline is exposed uniformly with electron-beam lithography; hence, air features defining the device are uniformly tuned. e\u2013g 40\u00b0 tilted SEM images of bowtie region for \u03b4\u2009=\u2009{\u2009\u2212\u20092,\u2009\u2212\u20094,\u2009\u2212\u20096}\u2009nm. We measure the mean width of the fabricated bowties to be (8\u2009\u00b1\u20095)\u2009nm, (10\u2009\u00b1\u20095)\u2009nm, and (16\u2009\u00b1\u20095)\u2009nm for figures e, f, and g, respectively, noting the variation in width along the z-direction caused by the scallops and ~1\u00b0 negative sidewall angle represented by the uncertainty as discussed in the main text. Credit: <i>Nature Communications<\/i> (2022). DOI: 10.1038\/s41467-022-33874-w&#8221; width=&#8221;800&#8243; height=&#8221;383&#8243;&gt;<figcaption class=\"text-darken text-low-up text-truncate-js text-truncate mt-3\">\n                Fabrication of topology-optimized silicon dielectric bowtie cavity (DBC). a Rendering of the DBC design generated by tolerance-constrained topology optimization. The normalized \u2223E\u2223-field is projected on the faces defining the three symmetry planes of the design. b Zoom-in of the solid silicon bowtie exhibiting a strong field confinement due to the bowtie bridge dimension of 8\u2009nm. c 40\u00b0 tilted scanning electron microscopy (SEM) image of a fabricated cavity. d Global geometry-tuning, \u03b4. Each air (black) pixel (1\u2009nm<sup>2<\/sup>) inside a \u03b4-outline is exposed uniformly with electron-beam lithography; hence, air features defining the device are uniformly tuned. e\u2013g 40\u00b0 tilted SEM images of bowtie region for \u03b4\u2009=\u2009{\u2009\u2212\u20092,\u2009\u2212\u20094,\u2009\u2212\u20096}\u2009nm. We measure the mean width of the fabricated bowties to be (8\u2009\u00b1\u20095)\u2009nm, (10\u2009\u00b1\u20095)\u2009nm, and (16\u2009\u00b1\u20095)\u2009nm for figures e, f, and g, respectively, noting the variation in width along the z-direction caused by the scallops and ~1\u00b0 negative sidewall angle represented by the uncertainty as discussed in the main text. Credit: <i>Nature Communications<\/i> (2022). DOI: 10.1038\/s41467-022-33874-w<br \/>\n            <\/figcaption><\/figure>\n<\/p><\/div>\n<\/div>\n<p>Until recently, it was widely believed among physicists that it was impossible to compress light below the so-called diffraction limit (see below), except when using metal nanoparticles, which unfortunately also absorb light. It therefore seemed impossible to compress light strongly in dielectric materials such as silicon, which are key materials in information technologies and come with the important advantage that they do not absorb light.<\/p>\n<section class=\"article-banner first-banner ads-336x280\">\n<\/section>\n<p>Interestingly, it was shown theoretically in 2006 that the diffraction limit also does not apply to dielectrics. Still, no one has succeeded in showing this in the <a href=\"https:\/\/phys.org\/tags\/real+world\/\" rel=\"tag\" class=\"textTag\">real world<\/a>, simply because no one has been able to build the necessary <a href=\"https:\/\/phys.org\/tags\/dielectric\/\" rel=\"tag\" class=\"textTag\">dielectric<\/a> nanostructures until now.<\/p>\n<p>A research team from DTU has successfully designed and built a structure, a so-called dielectric nanocavity, which concentrates light in a volume 12 times below the diffraction limit. The result is groundbreaking in optical research and has just been published in <i>Nature Communications<\/i>.<\/p>\n<p>&#8220;Although <a href=\"https:\/\/phys.org\/tags\/computer+calculations\/\" rel=\"tag\" class=\"textTag\">computer calculations<\/a> show that you can concentrate light at an infinitely small point, this only applies in theory. The actual results are limited by how small details can be made, for example, on a microchip,&#8221; says Marcus Albrechtsen, Ph.D.-student at DTU Electro and first author of the new article.<\/p>\n<p>&#8220;We programmed our knowledge of real photonic nanotechnology and its current limitations into a computer. Then we asked the computer to find a pattern that collects the photons in an unprecedentedly small area\u2014in an optical nanocavity\u2014which we were also able to build in the laboratory.&#8221;<\/p>\n<p>Optical nanocavities are structures specially designed to retain light so that it does not propagate as we are used to but is thrown back and forth as if you put two mirrors facing each other. The closer you place the mirrors to each other, the more intense the light between the mirrors becomes. For this experiment, the researchers have designed a so-called bowtie structure, which is particularly effective at squeezing the photons together due to its special shape.<\/p>\n<p>The nanocavity is made of silicon, the dielectric material on which most advanced modern technology is based. The material for the nanocavity was developed in cleanroom laboratories at DTU, and the patterns on which the cavity is based are optimized and designed using a unique method for topology optimization developed at DTU. Initially developed to design bridges and aircraft wings, it is now also used for nanophotonic structures.<\/p>\n<p>&#8220;It required a great joint effort to achieve this breakthrough. It has only been possible because we have managed to combine world-leading research from several research groups at DTU,&#8221; says associate professor S\u00f8ren Stobbe, who has led the research work.&#8221;<\/p>\n<p><b>Important breakthrough for energy-efficient technology<\/b><\/p>\n<p>The discovery could be decisive for developing revolutionary new technologies that may reduce the amount of energy-guzzling components in data centers, computers, telephones, and so on.<\/p>\n<p>The <a href=\"https:\/\/phys.org\/tags\/energy+consumption\/\" rel=\"tag\" class=\"textTag\">energy consumption<\/a> for computers and data centers continues to grow, and there is a need for more sustainable chip architectures that use less energy. This can be achieved by replacing the electrical circuits with optical components. The researchers&#8217; vision is to use the same division of labor between light and electrons used for the Internet, where light is used for communication and electronics for data processing. The only difference is that both functionalities must be built into the same chip, which requires that the light be compressed to the same size as the electronic components. The breakthrough at DTU shows that it is, in fact, possible.<\/p>\n<p>&#8220;There is no doubt that this is an important step to developing a more energy-efficient technology for, e.g., nanolasers for optical connections in <a href=\"https:\/\/phys.org\/tags\/data+centers\/\" rel=\"tag\" class=\"textTag\">data centers<\/a> and future computers\u2014but there is still a long way to go,&#8221; says Marcus Albrechtsen.<\/p>\n<p>The researchers will now work further and refine methods and materials to find the optimal solution.<\/p>\n<p>&#8220;Now that we have the theory and method in place, we will be able to make increasingly intense photons as the surrounding technology develops. I am convinced that this is just the first of a long series of major developments in physics and photonic nanotechnology centered around these principles,&#8221; says S\u00f8ren Stobbe.<\/p>\n<p><b>The diffraction limit<\/b><\/p>\n<p>The theory of the diffraction limit describes that light cannot be focused to a volume smaller than half the wavelength in an optical system\u2014for example, this applies to the resolution in microscopes.<\/p>\n<p>However, nanostructures can consist of elements much smaller than the wavelength, which means that the <a href=\"https:\/\/phys.org\/tags\/diffraction+limit\/\" rel=\"tag\" class=\"textTag\">diffraction limit<\/a> is no longer a fundamental limit. Bowtie structures, in particular, can compress the light into very small volumes limited by the sizes of the bowtie and, thus, the quality of the nanofabrication.<\/p>\n<p>When the light is compressed, it becomes more intense, enhancing interactions between light and materials such as atoms, molecules and 2D materials.<\/p>\n<p><b>Dielectric materials<\/b><\/p>\n<p>Dielectric materials are electrically insulating. Glass, rubber, and plastic are examples of <a href=\"https:\/\/phys.org\/tags\/dielectric+materials\/\" rel=\"tag\" class=\"textTag\">dielectric materials<\/a>, and they contrast with metals, which are electrically conductive.<\/p>\n<p>An example of a dielectric material is silicon, which is often used in electronics but also photonics.<\/p>\n<hr \/>\n<div class=\"article-main__explore my-4 d-print-none\">\n<div class=\"d-flex align-items-center\">\n<p class=\"text-bold mb-0 ml-2\">Explore further<\/p>\n<\/p><\/div>\n<p>                                            <a class=\"text-medium text-info mt-2 d-inline-block\" href=\"https:\/\/phys.org\/news\/2021-03-high-q-resonant-modes-dielectric-nanocavity.html\">Finding high-Q resonant modes in a dielectric nanocavity<\/a>\n\t\t\t\t\t\t\t\t\t\t<\/div>\n<hr class=\"mb-4\" \/>\n<div class=\"article-main__more p-4\">\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<strong>More information:<\/strong><br \/>\n\t\t\t\t\t\t\t\t\t\t\t\tMarcus Albrechtsen et al, Nanometer-scale photon confinement in topology-optimized dielectric cavities, <i>Nature Communications<\/i> (2022).  <a data-doi=\"1\" href=\"https:\/\/dx.doi.org\/10.1038\/s41467-022-33874-w\" target=\"_blank\" rel=\"noopener\">DOI: 10.1038\/s41467-022-33874-w<\/a><\/p><\/div>\n<div class=\"d-inline-block text-medium my-4\">\n\t\t\t\t\t\t\t\t\t\t\t\tProvided by<br \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<a href=\"https:\/\/phys.org\/partners\/technical-university-of-denmark\/\">Technical University of Denmark<\/a><br \/>\n\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t\t<a class=\"icon_open\" href=\"http:\/\/www.dtu.dk\/English.aspx\" target=\"_blank\" rel=\"nofollow noopener\"><\/p>\n<p>\t\t\t\t\t\t\t\t\t\t\t\t\t<\/a><\/p><\/div>\n<div class=\"d-none d-print-block\">\n<p>\n                                                 <strong>Citation<\/strong>:<br \/>\n                                                 Researchers compress light 12 times below the diffraction limit in a dielectric material (2022, October 26)<br \/>\n                                                 retrieved 26 October 2022<br \/>\n                                                 from https:\/\/phys.org\/news\/2022-10-compress-diffraction-limit-dielectric-material.html\n                                            <\/p>\n<p>\n                                            This document is subject to copyright. Apart from any fair dealing for the purpose of private study or research, no<br \/>\n                                            part may be reproduced without the written permission. The content is provided for information purposes only.\n                                            <\/p>\n<\/p><\/div>\n","protected":false},"excerpt":{"rendered":"<p>2) inside a \u03b4-outline is exposed uniformly with electron-beam lithography; hence, air features defining the<\/p>\n","protected":false},"author":1,"featured_media":20730,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"_links":{"self":[{"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/posts\/20728"}],"collection":[{"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/comments?post=20728"}],"version-history":[{"count":2,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/posts\/20728\/revisions"}],"predecessor-version":[{"id":20731,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/posts\/20728\/revisions\/20731"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/media\/20730"}],"wp:attachment":[{"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/media?parent=20728"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/categories?post=20728"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/peymantaeidi.net\/stem-cell\/wp-json\/wp\/v2\/tags?post=20728"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}