{"id":30755,"date":"2017-04-01T18:10:39","date_gmt":"2017-04-01T18:10:39","guid":{"rendered":"https:\/\/silvaco.com\/%eb%b6%84%eb%a5%98%eb%90%98%ec%a7%80-%ec%95%8a%ec%9d%8c\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/"},"modified":"2021-07-16T21:38:15","modified_gmt":"2021-07-17T04:38:15","slug":"effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/","title":{"rendered":"Effect of Fin Thickness on Subthreshold Characteristics of 10 nm FinFETs Using 3D TCAD"},"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  avia-builder-el-no-sibling   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-30755'><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><span style=\"font-size: 34px; letter-spacing: 0px;\">Effect of Fin Thickness on Subthreshold Characteristics of 10 nm FinFETs Using 3D TCAD<\/span><\/h1>\n<p align=\"center\"><em>This work was submitted to Silvaco Inc. by Rochester Institute of Technology, Department of Electrical &amp; Microelectronic Engineering.<br \/>\nSilvaco would like to thank the authors Abhijeet Walke and Santosh K. Kurinec<\/em><\/p>\n<p><strong>Introduction<\/strong><\/p>\n<p>The planar bulk Si metal-oxide semiconductor field-effect transistor (MOSFET) has reached its scaling limit due to various short channel effects (SCE). With 20 nm advanced planar technology, the source and drain encroached into channel resulting in off state leakage current. Tri gate FinFET devices have already replaced conventional planar MOSFETs for 14nm and beyond due to their superior control over the channel resulting in lower values of subthreshold swing (SS) and reduced drain induced barrier lowering (DIBL). Nevertheless, gate induced drain leakage is found to be the limiting factor in achieving ultralow (&lt;100pA\/um) values of IOFF. In this work, we have studied the effect of fin thickness on subthreshold characteristics of bulk nFinFET using three dimensional simulation.<\/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; '><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_Q2_2017_a1.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"232\" height=\"300\" class='wp-image-19098 avia-img-lazy-loading-not-19098 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-232x300.jpg\" alt='' title='simstd_Q2_2017_a1'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-232x300.jpg 232w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-768x994.jpg 768w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-545x705.jpg 545w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-29x37.jpg 29w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-43x55.jpg 43w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1-37x48.jpg 37w, https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1.jpg 782w\" sizes=\"(max-width: 232px) 100vw, 232px\" \/><\/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_Q2_2017_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 -->\n","protected":false},"excerpt":{"rendered":"<p>The planar bulk Si metal-oxide semiconductor field-effect transistor (MOSFET) has reached its scaling limit due to various short channel effects (SCE). With 20 nm advanced planar technology, the source and drain encroached into channel resulting in off state leakage current. Tri gate FinFET devices have already replaced conventional planar MOSFETs for 14nm and beyond due to their superior control over the channel resulting in lower values of subthreshold swing (SS) and reduced drain induced barrier lowering (DIBL). Nevertheless, gate induced drain leakage is found to be the limiting factor in achieving ultralow (<100pA\/um) values of IOFF. In this work, we have studied the effect of fin thickness on subthreshold characteristics of bulk nFinFET using three dimensional simulation.\n\n\n<\/p>\n","protected":false},"author":5,"featured_media":19098,"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>Effect of Fin Thickness on Subthreshold Characteristics of 10 nm FinFETs Using 3D TCAD - Silvaco<\/title>\n<meta name=\"description\" content=\"The planar bulk Si metal-oxide semiconductor field-effect transistor (MOSFET) has reached its scaling limit due to various short channel effects (SCE).\" \/>\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\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/\" \/>\n<meta property=\"og:locale\" content=\"ko_KR\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Effect of Fin Thickness on Subthreshold Characteristics of 10 nm FinFETs Using 3D TCAD\" \/>\n<meta property=\"og:description\" content=\"The planar bulk Si metal-oxide semiconductor field-effect transistor (MOSFET) has reached its scaling limit due to various short channel effects (SCE).\" \/>\n<meta property=\"og:url\" content=\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/\" \/>\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=\"2017-04-01T18:10:39+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2021-07-17T04:38:15+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/silvaco.com\/wp-content\/uploads\/2020\/02\/simstd_Q2_2017_a1.jpg\" \/>\n\t<meta property=\"og:image:width\" content=\"782\" \/>\n\t<meta property=\"og:image:height\" content=\"1012\" \/>\n\t<meta property=\"og:image:type\" content=\"image\/jpeg\" \/>\n<meta name=\"author\" content=\"Ingrid Schwarz\" \/>\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=\"Ingrid Schwarz\" \/>\n\t<meta name=\"twitter:label2\" content=\"\uc608\uc0c1 \ub418\ub294 \ud310\ub3c5 \uc2dc\uac04\" \/>\n\t<meta name=\"twitter:data2\" content=\"4\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\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/\",\"url\":\"https:\/\/silvaco.com\/ko\/simulation-standard-ko\/effect-of-fin-thickness-on-subthreshold-characteristics-of-10-nm-finfets-using-3d-tcad\/\",\"name\":\"Effect of Fin Thickness on Subthreshold Characteristics of 10 nm FinFETs Using 3D TCAD - 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