{"id":29157,"date":"2006-08-01T00:05:38","date_gmt":"2006-08-01T00:05:38","guid":{"rendered":"https:\/\/silvaco.com\/uncategorized\/how-to-obtain-a-stable-grid-and-smooth-doping-profile-in-non-planar-a-si-tft-using-athena-elite\/"},"modified":"2021-07-08T18:24:58","modified_gmt":"2021-07-09T01:24:58","slug":"how-to-obtain-a-stable-grid-and-smooth-doping-profile-in-non-planar-a-si-tft-using-athena-elite","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ja\/simulation-standard\/how-to-obtain-a-stable-grid-and-smooth-doping-profile-in-non-planar-a-si-tft-using-athena-elite\/","title":{"rendered":"How to obtain a stable grid and smooth doping profile in non-planar a-Si TFT using Athena\/Elite?"},"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-29157'><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>Hints, Tips and Solutions &#8211; August 2006<\/h1>\n<p><strong>Q.<\/strong>\u00a0How to obtain a stable grid and smooth doping profile in non-planar a-Si TFT using\u00a0<em>ATHENA\/Elite<\/em>?<\/p>\n<p><strong>A.<\/strong>\u00a0Silvaco process and device simulation tools have been successfully used for many TFT applications. It has been shown that if accurate density of state distributions are specified the transfer characteristics of TFT devices show good agreement with experiments. The typical configuration of TFT includes a non-planar n+ doping source\/drain region around the metal gate. Such a non-planar structure could be simulated only by the process simulator\u00a0<strong><em>ATHENA<\/em><\/strong>\u00a0because\u00a0<strong><em>ATLAS<\/em><\/strong>\u00a0cannot generate the regions with rounded shapes.<\/p>\n<p>The accuracy of\u00a0<strong><em>ATLAS<\/em><\/strong>\u00a0device simulation strongly depends on grid quality and uniformity of doping along the surface of a-Si region. The internal\u00a0<em><strong>SSuprem4<\/strong><\/em>\u00a0deposition algorithm does not produce a smooth grid and consequently uniform doping. To overcome this difficulty the advanced topography simulation module of\u00a0<strong><em>ATHENA<\/em><\/strong>\u00a0must be used for a-Si deposition step.\u00a0<strong><em>Elite<\/em><\/strong>\u00a0produces much better grid and avoids non-uniform doping as seen in the left plot of Figure 1.<\/p>\n<p>Figure 2 shows that experimentally proved IV-curves can only be obtained when\u00a0<strong><em>Elite<\/em><\/strong>\u00a0module is used for simulation of the critical a-Si deposition step. If\u00a0<strong><em>Elite<\/em><\/strong>\u00a0is not used the reverse biased trend of the IV-curve disappears which means that these characteristics are very sensitive to the grid and doping quality. Therefore, we strongly recommend to use\u00a0<strong><em>Elite<\/em><\/strong>\u00a0deposition for simulation of non-planar TFT devices.<\/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-japanese-container\"><ul id=\"menu-simulation-standard-side-menu-japanese\" class=\"menu\"><li id=\"menu-item-26253\" class=\"menu-item menu-item-type-post_type menu-item-object-page menu-item-26253\"><a href=\"https:\/\/silvaco.com\/ja\/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_aug_2006_hints.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"644\" height=\"800\" class='wp-image-21644 avia-img-lazy-loading-not-21644 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_aug_2006_hints-e1611193214797.jpg\" alt='' title='simstd_aug_2006_hints'  itemprop=\"thumbnailUrl\"  \/><\/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_aug_2006_hints.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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