{"id":29543,"date":"2000-11-01T23:19:55","date_gmt":"2000-11-01T23:19:55","guid":{"rendered":"https:\/\/silvaco.com\/uncategorized\/simulating-impurity-freeze-out-during-low-temperature-operation\/"},"modified":"2021-07-08T18:41:51","modified_gmt":"2021-07-09T01:41:51","slug":"simulating-impurity-freeze-out-during-low-temperature-operation","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ja\/simulation-standard\/simulating-impurity-freeze-out-during-low-temperature-operation\/","title":{"rendered":"Simulating Impurity Freeze-Out During Low Temperature Operation"},"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-29543'><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>Simulating Impurity Freeze-Out During Low Temperature Operation<\/h1>\n<h3>Introduction<\/h3>\n<p>The low temperature operation of many device structures has been shown as an effective method for improving device performance without reducing device size. Performance improvements for MOS-based technologies include increased operating speed, enhanced latch-up immunity, and better subthreshold characteristics [1]. By modeling low temperature phenomena, numerical simulation of device operation at low temperatures provides an effective means for analyzing such performance improvements before investing manufacturing time or money. It is the purpose of this paper to discuss the modeling of the dopant freeze-out phenomenon in\u00a0<i><b>ATLAS<\/b><\/i>\u00a0and provide an application example of its use.<\/p>\n<p>At low temperatures, the thermal energy within a semiconductor is not high enough to fully activate all of the donor and acceptor impurity atoms. As a result, the carrier concentrations will not equal the concentration of dopant atoms. Figure 1 shows simulated data of the equilibrium electron concentration as a function of temperature for n-type silicon doped at 10cm. Below 100 K there is not enough thermal energy within the silicon to fully ionize the impurity atoms. This region of operation is known as the freeze-out regime. At temperatures between 100 K and 550 K, sufficient thermal energy resides within the silicon to fully ionize the impurity atoms. This region of operation is known as the extrinsic regime. As the temperature increases beyond 550 K, the intrinsic carrier concentration approaches and then exceeds the impurity concentration and the silicon returns to intrinsic-type behavior [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-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_nov_2000_a1.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"1290\" height=\"1669\" class='wp-image-22295 avia-img-lazy-loading-not-22295 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1.jpg\" alt='' title='simstd_nov_2000_a1'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1.jpg 1290w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-232x300.jpg 232w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-796x1030.jpg 796w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-768x994.jpg 768w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-1187x1536.jpg 1187w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-1159x1500.jpg 1159w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-545x705.jpg 545w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-29x37.jpg 29w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-43x55.jpg 43w, https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2000_a1-37x48.jpg 37w\" sizes=\"(max-width: 1290px) 100vw, 1290px\" \/><\/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_2000_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>The low temperature operation of many device structures has been shown as an effective method for improving device performance without reducing device size.  By modeling low temperature phenomena, numerical simulation of device operation at low temperatures provides an effective means for analyzing such performance improvements before investing manufacturing time or money. It is the purpose of this paper to discuss the modeling of the dopant freeze-out phenomenon in ATLAS and provide an application example of its use.<\/p>\n","protected":false},"author":2,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7570],"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>Simulating Impurity Freeze-Out During Low Temperature Operation - \u30b7\u30eb\u30d0\u30b3\u30fb\u30b8\u30e3\u30d1\u30f3 : Silvaco Japan<\/title>\n<meta name=\"description\" content=\"Simulating Impurity Freeze-Out During Low Temperature Operation\" \/>\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\/ja\/simulation-standard\/simulating-impurity-freeze-out-during-low-temperature-operation\/\" \/>\n<meta property=\"og:locale\" content=\"ja_JP\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Simulating Impurity Freeze-Out During Low Temperature Operation\" \/>\n<meta property=\"og:description\" content=\"Simulating Impurity Freeze-Out During Low Temperature Operation\" \/>\n<meta property=\"og:url\" content=\"https:\/\/silvaco.com\/ja\/simulation-standard\/simulating-impurity-freeze-out-during-low-temperature-operation\/\" \/>\n<meta property=\"og:site_name\" content=\"\u30b7\u30eb\u30d0\u30b3\u30fb\u30b8\u30e3\u30d1\u30f3 : Silvaco Japan\" \/>\n<meta property=\"article:publisher\" content=\"https:\/\/www.facebook.com\/SilvacoSoftware\/\" \/>\n<meta property=\"article:published_time\" content=\"2000-11-01T23:19:55+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2021-07-09T01:41:51+00:00\" \/>\n<meta name=\"author\" content=\"Graham Bell\" \/>\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=\"\u57f7\u7b46\u8005\" \/>\n\t<meta name=\"twitter:data1\" content=\"Graham Bell\" \/>\n\t<meta name=\"twitter:label2\" content=\"\u63a8\u5b9a\u8aad\u307f\u53d6\u308a\u6642\u9593\" \/>\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\/ja\/simulation-standard\/simulating-impurity-freeze-out-during-low-temperature-operation\/\",\"url\":\"https:\/\/silvaco.com\/ja\/simulation-standard\/simulating-impurity-freeze-out-during-low-temperature-operation\/\",\"name\":\"Simulating Impurity Freeze-Out During Low Temperature Operation - 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