{"id":30678,"date":"2019-07-03T00:00:59","date_gmt":"2019-07-03T00:00:59","guid":{"rendered":"https:\/\/silvaco.com\/%eb%b6%84%eb%a5%98%eb%90%98%ec%a7%80-%ec%95%8a%ec%9d%8c\/simulation-of-different-tunnel-junctions-in-ingap-gaas-ingap-cdte-dual-junction-solar-cells\/"},"modified":"2021-07-16T21:34:49","modified_gmt":"2021-07-17T04:34:49","slug":"simulation-of-different-tunnel-junctions-in-ingap-gaas-ingap-cdte-dual-junction-solar-cells","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/simulation-of-different-tunnel-junctions-in-ingap-gaas-ingap-cdte-dual-junction-solar-cells\/","title":{"rendered":"Simulation of Different Tunnel Junctions in InGaP\/GaAs, InGaP\/CdTe Dual Junction Solar Cells"},"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-30678'><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 align=\"center\">Simulation of Different Tunnel Junctions in InGaP\/GaAs, InGaP\/CdTe Dual Junction Solar Cells<\/h1>\n<p align=\"center\"><em>Tyler T. McCarthy, Yong-Hang Zhang and D. Vasileska<br \/>\nCenter for Photonics Innovation and School of Electrical, Computer and Energy Engineering<br \/>\nArizona State University, Tempe, AZ 85287, USA<\/em><\/p>\n<p><strong><em>Abstract<\/em><\/strong> \u2014 Dual junction solar cells were simulated using Silvaco TCAD tool with various tunnel junction material compositions. InGaP\/GaAs dual junction solar cells were simulated with 10 different tunnel junction combinations. The highest efficiencies were from InGaP\/AlGaAs and InGaP\/InGaP tunnel junctions at 31.82% and 31.75%. InGaP\/CdTe solar cells were also simulated with four different tunnel junction combinations. InGaP\/InGaP tunnel junction was found to be most efficient with 37.29% which is consistent with experimental data. Three of four InGaP\/CdTe dual junction solar cells were simulated to have higher efficiency values than all InGaP\/GaAs solar cells.<\/p>\n<p><em>Index Terms<\/em> \u2014 CdTe, dual junction, GaAs, InGaP, Silvaco, solar cell, tunnel junction<\/p>\n<h3>Introduction<\/h3>\n<p>The need for low-cost, high-efficiency renewable energy drives the research for photovoltaic devices, as the energy available for conversion is abundant. Under AM1.5G solar spectrum, the global standard spectrum where the sun is approximately 41\u00b0 above the horizon, the total irradiance is 100 mW\/cm2, and the spectrum used for simulations is shown in Figure 1 [1]. The AM0 solar spectrum is the spectrum used for extraterrestrial simulations and applications, and these solar cells must be able to tolerate more radiation. Silicon solar cells, 1.12 eV bandgap, are the most popular commercial photovoltaic device on the market, but have about reached their efficiency limit, and so attention has turned toward other material systems. GaAs was one of the early alternatives to Si solar cells for its direct bandgap and bandgap energy of 1.42 eV. Quickly GaAs solar cells were optimized and pushed to their efficiency limit, and multi-junction solar cells were sought after to help push these solar cell to efficiencies greater than 30%. InxGa1-xP was chosen to be the top cell of a dual junction solar cell grown on GaAs because at an In composition of 49%, the two material are lattice matched at 5.65 \u00c5, and InGaP has a wide bandgap of 1.9 eV [2].<\/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_Q3_2019_a3.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"782\" height=\"1012\" class='wp-image-18984 avia-img-lazy-loading-not-18984 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3.jpg\" alt='' title='Simulation of Different Tunnel Junctions in InGaP\/GaAs, InGaP\/CdTe Dual Junction Solar Cells'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3.jpg 782w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-232x300.jpg 232w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-768x994.jpg 768w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-545x705.jpg 545w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-29x37.jpg 29w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-43x55.jpg 43w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q3_2019_a3-37x48.jpg 37w\" sizes=\"(max-width: 782px) 100vw, 782px\" \/><\/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_Q3_2019_a3.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-30678'><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>Abstract \u2014 Dual junction solar cells were simulated using Silvaco TCAD tool with various tunnel junction material compositions. InGaP\/GaAs dual junction solar cells were simulated with 10 different tunnel junction combinations. The highest efficiencies were from InGaP\/AlGaAs and InGaP\/InGaP tunnel junctions at 31.82% and 31.75%. InGaP\/CdTe solar cells were also simulated with four different tunnel junction combinations. InGaP\/InGaP tunnel junction was found to be most efficient with 37.29% which is consistent with experimental data. Three of four InGaP\/CdTe dual junction solar cells were simulated to have higher efficiency values than all InGaP\/GaAs solar cells.<\/p>\n","protected":false},"author":3,"featured_media":18981,"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>Simulation of Different Tunnel Junctions in InGaP\/GaAs, InGaP\/CdTe Dual Junction Solar Cells - Silvaco<\/title>\n<meta name=\"description\" content=\"Dual junction solar cells were simulated using Silvaco TCAD tool with various tunnel junction material compositions. 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