{"id":2932,"date":"2022-12-09T17:38:39","date_gmt":"2022-12-09T16:38:39","guid":{"rendered":"https:\/\/lidar-ophellia.eu\/?p=2932"},"modified":"2023-01-06T21:50:35","modified_gmt":"2023-01-06T20:50:35","slug":"poster-presentation-26th-annual-symposium-of-the-ieee-benelux-photonics-chapter-2022-24-25-november-eindhoven-the-netherlands","status":"publish","type":"post","link":"https:\/\/lidar-ophellia.eu\/index.php\/2022\/12\/09\/poster-presentation-26th-annual-symposium-of-the-ieee-benelux-photonics-chapter-2022-24-25-november-eindhoven-the-netherlands\/","title":{"rendered":"Poster Presentation: 26th Annual Symposium of the IEEE BeNeLux Photonics Chapter 2022, 24-25 November, Eindhoven, The Netherlands"},"content":{"rendered":"\n<p><\/p>\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\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"683\" height=\"1024\" src=\"https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-683x1024.jpg\" alt=\"\" class=\"wp-image-2936\" srcset=\"https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-683x1024.jpg 683w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-200x300.jpg 200w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-768x1152.jpg 768w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-1024x1536.jpg 1024w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-1365x2048.jpg 1365w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_2-scaled.jpg 1707w\" sizes=\"auto, (max-width: 683px) 100vw, 683px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"683\" src=\"https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-1024x683.jpg\" alt=\"\" class=\"wp-image-2937\" srcset=\"https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-1024x683.jpg 1024w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-300x200.jpg 300w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-768x512.jpg 768w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-1536x1024.jpg 1536w, https:\/\/lidar-ophellia.eu\/wp-content\/uploads\/2023\/01\/IEEE_Benelux_2022_1-2048x1365.jpg 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Carlos E. Osnario Martinez in action during the poster session at IEEE BeNeLux Photonics Chapter Symposium 2022. <\/figcaption><\/figure>\n<\/div>\n<\/div>\n\n\n\n<p>H2020 OPHELLIA: Poster Presented at the 26th Annual Symposium of the\u00a0IEEE\u00a0Photonics Benelux Chapter 2022 titled &#8216;Design and optimization of an Er-doped Al2O3 adiabatic waveguide taper for double layer integration with Si3N4 platform\u2019 by Carlos E. Osnario-Martinez\u00a0on 25th\u00a0November 2022 in Eindhoven, The Netherlands.<\/p>\n\n\n\n<p><strong>#h2020ophellia<\/strong>&nbsp;<strong>#development<\/strong>&nbsp;<strong>#photonics<\/strong>&nbsp;<strong>#materials<\/strong>&nbsp;<strong>#lasers<\/strong>&nbsp;<strong>#amplifiers<\/strong>&nbsp;<strong>#lidar<\/strong><\/p>\n\n\n\n<p><a href=\"https:\/\/lnkd.in\/eqrmQaqT\">https:\/\/lnkd.in\/eqrmQaqT<\/a><\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p><strong>Abstract<\/strong><\/p>\n<cite>The integration of active-passive material platforms is needed to increase the number of optical components on-chip, i.e. achieve more functionalities on PICs. Adiabatic waveguide tapers are of great interest for applications that require short and low-loss transitions between different material platforms. In this work, an Er-doped Al2O3 adiabatic waveguide taper is designed for the integration with the standard asymmetric double stripe (ADS) Si3N4 TriPleX technology. The tolerance of the taper design to fabrication variations is studied in the wavelength range of 980 nm \u2013 1630 nm. The simulated total loss of the final taper design is \u2264 0.1 dB per coupler.<\/cite><\/blockquote>\n","protected":false},"excerpt":{"rendered":"<p>H2020 OPHELLIA: Poster Presented at the 26th Annual Symposium of the\u00a0IEEE\u00a0Photonics Benelux Chapter 2022 titled &#8216;Design and optimization of an Er-doped Al2O3 adiabatic waveguide taper for double layer integration with Si3N4 platform\u2019 by Carlos E. Osnario-Martinez\u00a0on 25th\u00a0November 2022 in Eindhoven, The Netherlands. #h2020ophellia&nbsp;#development&nbsp;#photonics&nbsp;#materials&nbsp;#lasers&nbsp;#amplifiers&nbsp;#lidar https:\/\/lnkd.in\/eqrmQaqT Abstract The integration of active-passive material platforms is needed to increase &hellip;<\/p>\n<p class=\"read-more\"> <a class=\"\" href=\"https:\/\/lidar-ophellia.eu\/index.php\/2022\/12\/09\/poster-presentation-26th-annual-symposium-of-the-ieee-benelux-photonics-chapter-2022-24-25-november-eindhoven-the-netherlands\/\"> <span class=\"screen-reader-text\">Poster Presentation: 26th Annual Symposium of the IEEE BeNeLux Photonics Chapter 2022, 24-25 November, Eindhoven, The Netherlands<\/span> Read More &raquo;<\/a><\/p>\n","protected":false},"author":3,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"default","ast-global-header-display":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","footnotes":""},"categories":[1],"tags":[],"class_list":["post-2932","post","type-post","status-publish","format-standard","hentry","category-non-classe"],"_links":{"self":[{"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/posts\/2932","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/comments?post=2932"}],"version-history":[{"count":3,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/posts\/2932\/revisions"}],"predecessor-version":[{"id":2940,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/posts\/2932\/revisions\/2940"}],"wp:attachment":[{"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/media?parent=2932"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/categories?post=2932"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/lidar-ophellia.eu\/index.php\/wp-json\/wp\/v2\/tags?post=2932"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}