{"id":9679,"date":"2014-07-28T18:03:29","date_gmt":"2014-07-28T16:03:29","guid":{"rendered":"https:\/\/www.jassemajaka.com\/?p=9679"},"modified":"2019-02-27T18:15:42","modified_gmt":"2019-02-27T16:15:42","slug":"vertical-diodes-response-to-optical-and-electrical-thz-excitations","status":"publish","type":"post","link":"https:\/\/www.jassemajaka.com\/?p=9679","title":{"rendered":"Vertical diodes response to optical and electrical THz excitations"},"content":{"rendered":"<h4 dir=\"ltr\">S.Karishy; J. Ajaka et al., 2014, Vertical diodes response to optical and electrical THz excitations, Computational Electronics (IWCE), 2014 International Workshop on DOI: 10.1109\/IWCE.2014.6865858<\/h4>\n<div class=\"abstract-desktop-div hide-mobile\" dir=\"ltr\">\n<div class=\"abstract-text row\">\n<div class=\"col-12\">\n<div class=\"u-mb-1\"><strong> Abstract:<\/strong><\/p>\n<div>We use a hydrodynamic model self-consistently coupled to a 1D Poisson solver to simulate the excitation by optical beating as well as by electrical perturbation of plasma waves in n<sup>+<\/sup>nn<sup>+<\/sup> InGaAs diodes at room temperature. We calculate the electric field response and the velocity response of the carriers in the middle of the diode regions. Our results show clearly the presence of three-dimensional plasma resonances in the terahertz frequency domain for the two region types (n and n<sup>+<\/sup>). The investigation is completed by calculating the local differential mobility.<\/div>\n<div data-tealium_data=\"{&quot;docType&quot;: &quot;Conference&quot;}\"><\/div>\n<div class=\"u-pb-1 stats-document-abstract-publishedIn\" data-tealium_data=\"{&quot;docType&quot;: &quot;Conference&quot;}\"><strong>Published in: <\/strong> <a href=\"https:\/\/ieeexplore.ieee.org\/xpl\/mostRecentIssue.jsp?punumber=6857935\">2014 International Workshop on Computational Electronics (IWCE)<\/a><\/div>\n<\/div>\n<\/div>\n<\/div>\n<div class=\"row u-pt-1\">\n<div class=\"col-6\">\n<div class=\"u-pb-1 doc-abstract-confdate\"><strong>Date of Conference: <\/strong> 3-6 June 2014<\/div>\n<div class=\"u-pb-1 doc-abstract-dateadded\"><strong>Date Added to IEEE <i>Xplore<\/i>: <\/strong> 28 July 2014<\/div>\n<div class=\"u-pb-1\">\n<div>\n<div><strong>Electronic ISBN:<\/strong> 978-1-4799-5433-9<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div class=\"col-6\">\n<div class=\"u-pb-1\"><strong>INSPEC Accession Number: <\/strong> 14485087<\/div>\n<div class=\"u-pb-1 stats-document-abstract-doi\"><strong>DOI: <\/strong> <a href=\"https:\/\/doi.org\/10.1109\/IWCE.2014.6865858\" target=\"_blank\" rel=\"noopener noreferrer\">10.1109\/IWCE.2014.6865858<\/a><\/div>\n<div class=\"u-pb-1 doc-abstract-publisher\"><strong>Publisher: <\/strong> IEEE<\/div>\n<div class=\"u-pb-1 doc-abstract-conferenceLoc\"><strong>Conference Location: <\/strong> Paris, France<\/div>\n<div><\/div>\n<\/div>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>We use a hydrodynamic model self-consistently coupled to a 1D Poisson solver to simulate the excitation by optical beating as well as by electrical perturbation of plasma waves in n+nn+ InGaAs diodes at room temperature. We calculate the electric field response and the velocity response of the carriers in the middle of the diode regions. Our results show clearly the presence of three-dimensional plasma resonances in the terahertz frequency domain for the two region types (n and n+). The investigation is completed by calculating the local differential mobility.<\/p>\n","protected":false},"author":12,"featured_media":9681,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[50],"tags":[971,979,679,972,970,977,676],"class_list":["post-9679","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-50","tag-diode","tag-ieee","tag-jassem-ajaka","tag-nnn","tag-plasma-oscillation","tag-plasma-oscillations","tag-scientific-article"],"jetpack_featured_media_url":"https:\/\/www.jassemajaka.com\/wp-content\/uploads\/2019\/02\/The-I-U-characteristic-curve-for-n-nn-InGaAs-diode-of-500-500-500-nm-length.png","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/paTyQg-2w7","_links":{"self":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9679","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=9679"}],"version-history":[{"count":1,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9679\/revisions"}],"predecessor-version":[{"id":9682,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/posts\/9679\/revisions\/9682"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=\/wp\/v2\/media\/9681"}],"wp:attachment":[{"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=9679"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=9679"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.jassemajaka.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=9679"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}