{"id":36460,"date":"2007-02-01T00:01:28","date_gmt":"2007-02-01T00:01:28","guid":{"rendered":"https:\/\/silvaco.com\/%e6%9c%aa%e5%88%86%e7%b1%bb\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/"},"modified":"2021-10-13T10:31:00","modified_gmt":"2021-10-13T17:31:00","slug":"a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures","status":"publish","type":"post","link":"https:\/\/silvaco.com\/zh-hans\/simulation-standard-zh-hans\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/","title":{"rendered":"A Semi-Analytical Model for the Subthreshold Behavior of FinFLASH Structures"},"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-36460'><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>A Semi-Analytical Model for the Subthreshold Behavior of FinFLASH Structures<\/h1>\n<p style=\"text-align: center;\"><em>L. Perniola, J. Razafindramora, P. Scheiblin, F. Daug\u00b4e, C. Jahan, B. De Salvo, G. Reimbold, F. Boulanger<br \/>\nCEA-LETI<br \/>\n17, Rue des Martyrs, F &#8211; 38054, Grenoble, France, luca.perniola@cea.fr<br \/>\nG. Ghibaudo<br \/>\nINP Grenoble MINATEC<br \/>\n3, Parvis Louis N\u00b4eel, BP 257, 38016 Grenoble Cedex 1<\/em><\/p>\n<h3>Abstract<\/h3>\n<p>In this paper we present an original semi-analytical model for the subthreshold electrical behavior of complex 3D structures as the SOI FinFLASH devices. This physically-based model, which does not need any fitting parameter, solves the Poisson equation for a fin covered by trapped charges in the active dielectrics. The analytical results are compared with fully 3D numerical simulations and a good agreement is obtained down to fins with very small feature sizes (order of tens of nm). This model can be efficiently used to gain information on important cell electrical behaviors as the threshold voltage shift Vth and the subthreshold slope factor S.<\/p>\n<h3 class=\"feature\">Introduction<\/h3>\n<p>The FinFLASH device in trigate (W \u2248 H, see Fig. 1) or double-gate (H _ W) configuration is currently investigated as one of the most promising solutions to replace conventional planar FLASH structures beyond the 32 nm technology node[1]-[2]. The main advantages of the FinFLASH device are its compact layout, moreover fully compatible with future generations of multi-gate CMOS, and its excellent electrical performance due to the enhanced coupling between the gate and the active channel. In this frame, it is today of utmost importance to provide a simple approach which allows us to describe the most important electrical parameters of the memory operation without applying time consuming 3D numerical simulations.<\/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-chinese-simplified-container\"><ul id=\"menu-simulation-standard-side-menu-chinese-simplified\" class=\"menu\"><li id=\"menu-item-35571\" class=\"menu-item menu-item-type-post_type menu-item-object-page menu-item-35571\"><a href=\"https:\/\/silvaco.com\/zh-hans\/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_feb_2007_a1.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"1252\" height=\"1669\" class='wp-image-21814 avia-img-lazy-loading-not-21814 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1.jpg\" alt='' title='simstd_feb_2007_a1'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1.jpg 1252w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-225x300.jpg 225w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-773x1030.jpg 773w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-768x1024.jpg 768w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-1152x1536.jpg 1152w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-1125x1500.jpg 1125w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-529x705.jpg 529w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-28x37.jpg 28w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_a1-41x55.jpg 41w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_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_feb_2007_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. 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Autoclose: 1 -->\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Abstract<\/p>\n<p>In this paper we present an original semi-analytical model for the subthreshold electrical behavior of complex 3D structures as the SOI FinFLASH devices. This physically-based model, which does not need any fitting parameter, solves the Poisson equation for a fin covered by trapped charges in the active dielectrics. The analytical results are compared with fully 3D numerical simulations and a good agreement is obtained down to fins with very small feature sizes (order of tens of nm). This model can be efficiently used to gain information on important cell electrical behaviors as the threshold voltage shift Vth and the subthreshold slope factor S.<\/p>\n","protected":false},"author":3,"featured_media":21814,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7723],"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>A Semi-Analytical Model for the Subthreshold Behavior of FinFLASH Structures - Silvaco<\/title>\n<meta name=\"description\" content=\"In this paper we present an original semi-analytical model for the subthreshold electrical behavior of complex 3D structures\" \/>\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\/simulation-standard\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/\" \/>\n<meta property=\"og:locale\" content=\"zh_CN\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"A Semi-Analytical Model for the Subthreshold Behavior of FinFLASH Structures\" \/>\n<meta property=\"og:description\" content=\"In this paper we present an original semi-analytical model for the subthreshold electrical behavior of complex 3D structures\" \/>\n<meta property=\"og:url\" content=\"https:\/\/silvaco.com\/simulation-standard\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/\" \/>\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=\"2007-02-01T00:01:28+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2021-10-13T17:31:00+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_feb_2007_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=\"\u4f5c\u8005\" \/>\n\t<meta name=\"twitter:data1\" content=\"Erick Castellon\" \/>\n\t<meta name=\"twitter:label2\" content=\"\u9884\u8ba1\u9605\u8bfb\u65f6\u95f4\" \/>\n\t<meta name=\"twitter:data2\" content=\"5 \u5206\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"https:\/\/silvaco.com\/simulation-standard\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/\",\"url\":\"https:\/\/silvaco.com\/simulation-standard\/a-semi-analytical-model-for-the-subthreshold-behavior-of-finflash-structures\/\",\"name\":\"A Semi-Analytical Model for the Subthreshold Behavior of FinFLASH Structures - 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