{"id":36443,"date":"2007-11-01T00:01:49","date_gmt":"2007-11-01T00:01:49","guid":{"rendered":"https:\/\/silvaco.com\/%e6%9c%aa%e5%88%86%e7%b1%bb\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/"},"modified":"2021-10-13T10:30:08","modified_gmt":"2021-10-13T17:30:08","slug":"a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation","status":"publish","type":"post","link":"https:\/\/silvaco.com\/zh-hans\/simulation-standard-zh-hans\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/","title":{"rendered":"A Novel Approach to Three-Dimensional Semiconductor Process Simulation: Application to Thermal Oxidation"},"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-36443'><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\">A Novel Approach to Three-Dimensional Semiconductor Process Simulation: Application to Thermal Oxidation<\/h1>\n<p align=\"center\"><em>VASILY SUVOROV, ANDREAS H\u00d6SSINGER,<br \/>\nZORAN DJURIC and NEBOYSHA LJEPOJEVIC<br \/>\nSilvaco Technology Center, Compass Point, St Ives, Cambridgeshire, PE27 5JL, UK.<br \/>\nJournal of Computational Electronics Volume 5, Number 4, 2006c<br \/>\n2006 Springer Science Business Media, Inc. Manufactured in The Netherlands<\/em><\/p>\n<h3 align=\"left\"><strong>Abstract<\/strong><\/h3>\n<p align=\"left\">The paper presents a new approach to three-dimensional semiconductor process simulation that overcomes the problem of moving boundaries and mesh generation. Contrary to using unstructured meshes, the approach makes use of the level set method on fixed Cartesian meshes. A concept of multi-layer structure is introduced to capture an arbitrary complex structure. To handle a big geometrical scale ratio in a structure, the concept of adaptive mesh refinement is used. A special in-house finite-difference scheme is designed to approximate the relevant equations near material interfaces. In the bulk of regular nodes the standard finite difference schemes are used. Application of the approach to the modeling of oxidation of some typical types of structures used in semiconductor technology is demonstrated.<\/p>\n<p align=\"left\"><strong>Keywords<\/strong><\/p>\n<p align=\"left\">Semiconductor technology, modeling, thermal oxidation of silicon.<\/p>\n<p align=\"left\"><strong>1. Introduction<\/strong><\/p>\n<p align=\"left\">The 2005 edition of International Technology Roadmap for Semiconductors estimates that the technology-development costs can be reduced by 40% by 2013 due to use of Technology CAD. To achieve this goal, one needs to overcome a problem of mesh generation that has become a major issue in simulation of 3D process, mainly because of moving material interfaces. The standard approach that uses unstructured meshes involves very complex and often unstable mesh generation algorithms. Alternatively, we apply the level set approach [1]. All interfaces are given implicitly as signed distance (level set) functions, defined on fixed Cartesian meshes. Any changes of interfaces, caused by a given process, can be calculated by updating their level set functions. Every signed distance function satisfies the level set equation, which can be solved by standard methods.<\/p>\n<p align=\"left\">The Cartesian meshes for the level set functions also serve as a framework for solving all other differential equations, which describe our simulated processes. The advantages of such an approach are numerous: numerical schemes for various equations are well known, stable and accurate; the coding is much simpler; the memory requirements per computational cell are smaller than for the finite elements methods. However, there are two problems associated with this methodology: approximating of general-type boundary conditions near interfaces and handling of a big scale ratio of sizes in complex structures. In recent decades, considerable progress has been achieved in resolving both issues (e.g. [2], [3], [4] ). In our development we use our original in-house numerical method, the method described in [3] and the concept of Adaptive Mesh Refinement (AMR) [4]. The above principles are cornerstones of a software package Victory-Process, Silvaco\u2019s three-dimensional process simulation framework. In this work we demonstrate Victory\u2019s capability to simulate numerically the most demanding process, namely thermal oxidation.<\/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_nov_2007_a1.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"750\" height=\"1000\" class='wp-image-22345 avia-img-lazy-loading-not-22345 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2007_a1-e1611191624800.jpg\" alt='' title='simstd_nov_2007_a1'  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_nov_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. 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-36443'><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<\/p>\n<p>The paper presents a new approach to three-dimensional semiconductor process simulation that overcomes the problem of moving boundaries and mesh generation. Contrary to using unstructured meshes, the approach makes use of the level set method on fixed Cartesian meshes. A concept of multi-layer structure is introduced to capture an arbitrary complex structure. To handle a big geometrical scale ratio in a structure, the concept of adaptive mesh refinement is used. A special in-house finite-difference scheme is designed to approximate the relevant equations near material interfaces. In the bulk of regular nodes the standard finite difference schemes are used. Application of the approach to the modeling of oxidation of some typical types of structures used in semiconductor technology is demonstrated.<\/p>\n","protected":false},"author":3,"featured_media":22345,"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 Novel Approach to Three-Dimensional Semiconductor Process Simulation: Application to Thermal Oxidation - Silvaco<\/title>\n<meta name=\"description\" content=\"The paper presents a new approach to three-dimensional semiconductor process simulation that overcomes the problem of moving boundaries and mesh\" \/>\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\/zh-hans\/simulation-standard-zh-hans\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/\" \/>\n<meta property=\"og:locale\" content=\"zh_CN\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"A Novel Approach to Three-Dimensional Semiconductor Process Simulation: Application to Thermal Oxidation\" \/>\n<meta property=\"og:description\" content=\"The paper presents a new approach to three-dimensional semiconductor process simulation that overcomes the problem of moving boundaries and mesh\" \/>\n<meta property=\"og:url\" content=\"https:\/\/silvaco.com\/zh-hans\/simulation-standard-zh-hans\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/\" \/>\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=\"2007-11-01T00:01:49+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2021-10-13T17:30:08+00:00\" \/>\n<meta property=\"og:image\" content=\"https:\/\/silvaco.com\/wp-content\/uploads\/simulationstandard\/simstd_nov_2007_a1-e1611191624800.jpg\" \/>\n\t<meta property=\"og:image:width\" content=\"750\" \/>\n\t<meta property=\"og:image:height\" content=\"1000\" \/>\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=\"6 \u5206\" \/>\n<script type=\"application\/ld+json\" class=\"yoast-schema-graph\">{\"@context\":\"https:\/\/schema.org\",\"@graph\":[{\"@type\":\"WebPage\",\"@id\":\"https:\/\/silvaco.com\/zh-hans\/simulation-standard-zh-hans\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/\",\"url\":\"https:\/\/silvaco.com\/zh-hans\/simulation-standard-zh-hans\/a-novel-approach-to-three-dimensional-semiconductor-process-simulation-application-to-thermal-oxidation\/\",\"name\":\"A Novel Approach to Three-Dimensional Semiconductor Process Simulation: Application to Thermal Oxidation - 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