{"id":31107,"date":"2004-11-01T00:05:08","date_gmt":"2004-11-01T00:05:08","guid":{"rendered":"https:\/\/silvaco.com\/%eb%b6%84%eb%a5%98%eb%90%98%ec%a7%80-%ec%95%8a%ec%9d%8c\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/"},"modified":"2021-07-16T21:50:20","modified_gmt":"2021-07-17T04:50:20","slug":"transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/","title":{"rendered":"Transient Simulations of Edge Emitting Fabry-Perot InP\/InGaAsP Laser Diode Using Silvaco TCAD Tools"},"content":{"rendered":"<div id='template_overview'  class='avia-section main_color avia-section-small avia-no-border-styling  avia-bg-style-scroll  avia-builder-el-0  el_before_av_section  avia-builder-el-first   container_wrap fullsize' style='background-color: #ffffff;  margin-top:0px; margin-bottom:0px; '  ><div class='container' ><main  role=\"main\" itemprop=\"mainContentOfPage\"  class='template-page content  av-content-full alpha units'><div class='post-entry post-entry-type-page post-entry-31107'><div class='entry-content-wrapper clearfix'>\n<div class='flex_column_table av-equal-height-column-flextable -flextable' style='margin-top:20px; margin-bottom:0px; '><div class=\"flex_column av_three_fourth  flex_column_table_cell av-equal-height-column av-align-top first  avia-builder-el-1  el_before_av_one_fourth  avia-builder-el-first  \" style='padding:0px 0px 0px 0px ; border-radius:0px; '><section class=\"av_textblock_section \"  itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/BlogPosting\" itemprop=\"blogPost\" ><div class='avia_textblock  '   itemprop=\"text\" ><h1>Transient Simulations of Edge Emitting Fabry-Perot InP\/InGaAsP Laser Diode Using Silvaco TCAD Tools<\/h1>\n<p class=\"regular\" align=\"center\"><em>M. Nadeem Akram, Richard Schatz<br \/>\nRoyal Institute of Technology, Laboratory of Photonics and MicrowaveEngineering<br \/>\nELECTRUM 229, SE-164 40 Kista-Stockholm, SWEDEN<br \/>\nA.Nejim Silvaco Data Systems Europe Ltd, Compass Point, St. Ives, Cambridgeshire, PE27 5JL, UK<\/em><\/p>\n<p>In this communication we present a brief description of our initial results of transient simulation of InP\/InGaAsP Fabry-Perot edge emitting laser diode structure Using Silvaco\u00a0<em><strong>ATLAS\/Blaze<\/strong><\/em>\u00a0and\u00a0<strong>Laser<\/strong>\u00a0modules. The data presented here have not been optimized and it represents work in progress. This initial simulation presented here represents a heterostructure of bulk materials without any quantum confinement calculations or strain effects. This naturally will impact on the calculated lasing frequency.<\/p>\n<p>The simulated device is an n-i-p InP diode with InP active region containing a 200nm thick InGaAsP layer. Semi-insulating current blocking regions were also used in the simulated structure. Due to the presence of Fe in these regions, traps were introduced at 0.62eV in the band gap for these layers. Figure 1 shows the general structure of the diode together with the band gap diagram at a bias point of 1.2 volt at the anode.<\/p>\n<p>Simple doping profiles were used as shown in Figure 2 to achieve the current blocking effect. This can be seen clearly in Figure 3 where the total current contours can be seen. Each of the colored contours represents an equal portion of the total current running through the device at the chosen bias of 1.2 volts. Also shown at this bias is the light intensity from the active region of the laser diode. Figure 5 shows the energy spectrum of the emitted photons at the same bias of 1.2V.<\/p>\n<\/div><\/section><\/div><div class='av-flex-placeholder'><\/div><div class=\"flex_column av_one_fourth  flex_column_table_cell av-equal-height-column av-align-top av-zero-column-padding   avia-builder-el-3  el_after_av_three_fourth  avia-builder-el-last  \" style='border-radius:0px; ' id=\"whitepaper\" ><p><div  class='avia-builder-widget-area clearfix  avia-builder-el-4  el_before_av_image  avia-builder-el-first '><div id=\"nav_menu-29\" class=\"widget clearfix widget_nav_menu\"><div class=\"menu-simulation-standard-side-menu-korean-container\"><ul id=\"menu-simulation-standard-side-menu-korean\" class=\"menu\"><li id=\"menu-item-25039\" class=\"menu-item menu-item-type-post_type menu-item-object-page menu-item-25039\"><a href=\"https:\/\/silvaco.com\/ko\/technical-library\/simulation-standard\/\">Simulation Standard<\/a><\/li>\n<\/ul><\/div><\/div><\/div><br \/>\n<div  class='avia-image-container  av-styling-    avia-builder-el-5  el_after_av_sidebar  el_before_av_button  avia-align-center '  itemprop=\"image\" itemscope=\"itemscope\" itemtype=\"https:\/\/schema.org\/ImageObject\"  ><div class='avia-image-container-inner'><div class='avia-image-overlay-wrap'><a href=\"\/dynamicweb\/jsp\/downloads\/DownloadDocStepsAction.do?req=download&amp;nm=simstd_nov_2004_a1.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"1252\" height=\"1669\" class='wp-image-22317 avia-img-lazy-loading-not-22317 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1.jpg\" alt='' title='simstd_nov_2004_a1'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1.jpg 1252w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-225x300.jpg 225w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-773x1030.jpg 773w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-768x1024.jpg 768w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-1152x1536.jpg 1152w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-1125x1500.jpg 1125w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-529x705.jpg 529w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-28x37.jpg 28w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-41x55.jpg 41w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1-36x48.jpg 36w\" sizes=\"(max-width: 1252px) 100vw, 1252px\" \/><\/a><\/div><\/div><\/div><br \/>\n<div  class='avia-button-wrap avia-button-center  avia-builder-el-6  el_after_av_image  avia-builder-el-last ' ><a href='\/dynamicweb\/jsp\/downloads\/DownloadDocStepsAction.do?req=download&amp;nm=simstd_nov_2004_a1.pdf' class='avia-button  avia-color-grey   avia-icon_select-yes-right-icon avia-size-small avia-position-center ' target=\"_blank\" rel=\"noopener noreferrer\"><span class='avia_iconbox_title' >Download Simulation Standard<\/span><span class='avia_button_icon avia_button_icon_right' aria-hidden='true' data-av_icon='\ue875' data-av_iconfont='entypo-fontello'><\/span><\/a><\/div><\/p><\/div><\/div><!--close column table wrapper. Autoclose: 1 --><\/div><\/div><\/main><!-- close content main element --><\/div><\/div><div id='av_section_2'  class='avia-section main_color avia-section-small avia-no-border-styling  avia-bg-style-scroll  avia-builder-el-7  el_after_av_section  avia-builder-el-last   container_wrap fullsize' style='background-color: #ffffff;  margin-top:0px; margin-bottom:0px; '  ><div class='container' ><div class='template-page content  av-content-full alpha units'><div class='post-entry post-entry-type-page post-entry-31107'><div class='entry-content-wrapper clearfix'>\n<div class='flex_column_table av-equal-height-column-flextable -flextable' style='margin-top:20px; margin-bottom:0px; '><div class=\"flex_column av_one_full  flex_column_table_cell av-equal-height-column av-align-top first  avia-builder-el-8  avia-builder-el-no-sibling  \" style='padding:0px 0px 0px 0px ; border-radius:0px; '><\/div><\/div><!--close column table wrapper. Autoclose: 1 -->\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>In this communication we present a brief description of our initial results of transient simulation of InP\/InGaAsP Fabry-Perot edge emitting laser diode structure Using Silvaco\u00a0ATLAS\/Blaze\u00a0and\u00a0Laser\u00a0modules. The data presented here have not been optimized and it represents work in progress. This initial simulation presented here represents a heterostructure of bulk materials without any quantum confinement calculations or strain effects. This naturally will impact on the calculated lasing frequency.<\/p>\n","protected":false},"author":3,"featured_media":22317,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7486],"tags":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO Premium plugin v24.0 (Yoast SEO v24.0) - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Transient Simulations of Edge Emitting Fabry-Perot InP\/InGaAsP Laser Diode Using Silvaco TCAD Tools - Silvaco<\/title>\n<meta name=\"description\" content=\"In this communication we present a brief description of our initial results of transient simulation of InP\/InGaAsP Fabry-Perot edge emitting laser\" \/>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/\" \/>\n<meta property=\"og:locale\" content=\"ko_KR\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Transient Simulations of Edge Emitting Fabry-Perot InP\/InGaAsP Laser Diode Using Silvaco TCAD Tools\" \/>\n<meta property=\"og:description\" content=\"In this communication we present a brief description of our initial results of transient simulation of InP\/InGaAsP Fabry-Perot edge emitting laser\" \/>\n<meta property=\"og:url\" content=\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/\" \/>\n<meta property=\"og:site_name\" content=\"Silvaco\" \/>\n<meta property=\"article:publisher\" content=\"https:\/\/www.facebook.com\/SilvacoSoftware\/\" \/>\n<meta property=\"article:published_time\" content=\"2004-11-01T00:05:08+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2021-07-17T04:50:20+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2004_a1.jpg\" \/>\n\t<meta property=\"og:image:width\" content=\"1252\" \/>\n\t<meta property=\"og:image:height\" content=\"1669\" \/>\n\t<meta property=\"og:image:type\" content=\"image\/jpeg\" \/>\n<meta name=\"author\" content=\"Erick Castellon\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:creator\" content=\"@SilvacoSoftware\" \/>\n<meta name=\"twitter:site\" content=\"@SilvacoSoftware\" \/>\n<meta name=\"twitter:label1\" content=\"\uae00\uc4f4\uc774\" \/>\n\t<meta name=\"twitter:data1\" content=\"Erick Castellon\" \/>\n\t<meta name=\"twitter:label2\" content=\"\uc608\uc0c1 \ub418\ub294 \ud310\ub3c5 \uc2dc\uac04\" \/>\n\t<meta name=\"twitter:data2\" content=\"5\ubd84\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/\",\"url\":\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/transient-simulations-of-edge-emitting-fabry-perot-inp-ingaasp-laser-diode-using-silvaco-tcad-tools\/\",\"name\":\"Transient Simulations of Edge Emitting Fabry-Perot InP\/InGaAsP Laser Diode Using Silvaco TCAD Tools - 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