{"id":29443,"date":"2002-11-01T22:36:45","date_gmt":"2002-11-01T22:36:45","guid":{"rendered":"https:\/\/silvaco-stage.betagentechnologies.com\/uncategorized\/simulation-of-a-double-ridge-edge-emitting-ingaasp-inp-mqw-laser\/"},"modified":"2026-09-14T09:22:55","modified_gmt":"2026-09-14T16:22:55","slug":"simulation-of-a-double-ridge-edge-emitting-ingaasp-inp-mqw-laser","status":"publish","type":"post","link":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/simulation-of-a-double-ridge-edge-emitting-ingaasp-inp-mqw-laser\/","title":{"rendered":"Simulation of a Double Ridge Edge Emitting InGaAsP\/InP MQW Laser"},"content":{"rendered":"<h1>Simulation of a Double Ridge Edge Emitting InGaAsP\/InP MQW Laser<\/h1>\n<h3>Introduction<\/h3>\n<p>In order to investigate the influence of ridge separation on the transverse optical modes of a double ridge edge multiple quantum well (MQW) emitting laser, we have designed a generic device based on the InGaAsP\/InP MQW 1.5\u00b5m wavelength emission. The aim of this study is to investigate power loading in the structure with increasing bias using the bottom layer as the reference plane.<\/p>\n<p>To do this, the first three transverse modes were considered and the power associated with each mode was monitored as a function of the device design. Silvaco\u00a0<b><i>ATLAS LASER<\/i><\/b>\u00a0was used for this investigation.<\/p>\n<p><img loading=\"lazy\" width=\"1287\" height=\"1669\" src=\"https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2.jpg\" class=\"cleaned-enfold-image\" alt=\"\" decoding=\"async\" loading=\"lazy\" srcset=\"https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2.jpg 1287w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-231x300.jpg 231w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-794x1030.jpg 794w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-768x996.jpg 768w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-1184x1536.jpg 1184w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-1157x1500.jpg 1157w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-544x705.jpg 544w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-29x37.jpg 29w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-42x55.jpg 42w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2002_a2-37x48.jpg 37w\" sizes=\"auto, (max-width: 1287px) 100vw, 1287px\" \/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>In order to investigate the influence of ridge separation on the transverse optical modes of a double ridge edge multiple quantum well (MQW) emitting laser, we have designed a generic device based on the InGaAsP\/InP MQW 1.5\u00b5m wavelength emission. The aim of this study is to investigate power loading in the structure with increasing bias using the bottom layer as the reference plane.<\/p>\n","protected":false},"author":2,"featured_media":22283,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7570],"tags":[],"class_list":["post-29443","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-simulation-standard","entry","has-media"],"_links":{"self":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/posts\/29443","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/comments?post=29443"}],"version-history":[{"count":2,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/posts\/29443\/revisions"}],"predecessor-version":[{"id":66838,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/posts\/29443\/revisions\/66838"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/media\/22283"}],"wp:attachment":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/media?parent=29443"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/categories?post=29443"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ja\/wp-json\/wp\/v2\/tags?post=29443"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}