{"id":64153,"date":"2026-01-20T14:14:13","date_gmt":"2026-01-20T22:14:13","guid":{"rendered":"https:\/\/silvaco.com\/uncategorized\/simulation-standard-enabling-the-next-generation-of-high-voltage-power-ga2o3-trench-schottky-diodes-from-simulation-to-system\/"},"modified":"2026-01-22T10:11:07","modified_gmt":"2026-01-22T18:11:07","slug":"simulation-standard-enabling-the-next-generation-of-high-voltage-power-ga2o3-trench-schottky-diodes-from-simulation-to-system","status":"publish","type":"post","link":"https:\/\/silvaco.com\/ja\/simulation-standard\/enabling-the-next-generation-of-high-voltage-power-ga2o3-trench-schottky-diodes-from-simulation-to-system\/","title":{"rendered":"Enabling the Next Generation of High-Voltage Power: Gallium Oxide Trench Schottky Diodes from Simulation to System"},"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-64153'><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 class=\"p1\"><b> Enabling the Next Generation of High-Voltage Power: Ga<\/b><b><sub>2<\/sub><\/b><b>O<\/b><b><sub>3<\/sub><\/b><b> Trench Schottky Diodes from Simulation to System<\/b><\/h1>\n<p class=\"p1\"><span class=\"s1\"><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-64126 alignright\" src=\"https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2.png\" alt=\"\" width=\"190\" height=\"149\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2.png 664w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2-300x236.png 300w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2-43x34.png 43w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2-63x50.png 63w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/image2-48x38.png 48w\" sizes=\"(max-width: 190px) 100vw, 190px\" \/>\u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> is set to revolutionize high-voltage power conve<\/span>rsion, with ultra-low losses and a high critical electric field that make it ideal for next-generation power devices [1], enabling three-phase HVDC AC\/DC and DC\/AC conversion in the 1\u20136 kV, 0.5\u20130.8 kA range for AI data centre power delivery, renewable energy systems [2], high-voltage circuit breakers, and ESD protection [3].<\/p>\n<p class=\"p1\">Achieving p-type \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> is challenging due to inherent <span class=\"s1\">material properties inhibiting practical hole conductivity [4], thus limiting the formation of p-n junctions which are widely utilized in power and logic devices for curr<\/span>ent rectification.<span class=\"Apple-converted-space\">\u00a0 <\/span>In the absence of p\u2013n homojunctions, \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> diodes initially must rely on Schottky junction architectures [5]. In recent years, lateral \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> SBDs with field-plate structures have demonstrated impressive b<span class=\"s1\">reakdown voltages (BV) (&gt;10 kV) [8]. However, vertica<\/span>l <span class=\"s2\">device architectures are preferred for their inherent abil<\/span>ity to<span class=\"s2\"> scale to higher currents and voltages by adjustin<\/span>g the epitaxial layer thickness while conserving die area [9]. Furthermore, reduced surface field (RESURF) techniques are applied to \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub>-based Schottky barrier diodes (SBDs) in order to mitigate high electric fields at the Schottky contact, and thus suppress reverse leakage (JR) that can occur due to thermionic field emission [6], <span class=\"s3\">i<\/span><span class=\"s4\">mage-force barrier lowering [6], and trap-assisted tunnelling from plasma etching [7]. This has resulted in the \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> vertical trench Schottky barrier diode (TSBD) being preferred device architecture, in which fins used for Schottky contact formation are separated by trenches that enable the RESURF effect to be implemented through use of an Al<sub>2<\/sub>O<sub>3<\/sub>-enabled vertical metal-oxide-semiconductor (MOS) junction on the fin sidewall. The failure of TSBD is governed by dielectric breakdown rather than the metal\u2013semiconductor junction. While Al<sub>2<\/sub>O<sub>3<\/sub> can sustain fields u<\/span>p to ~8.7 MV\/cm [10], electric field crowding at the trench corner leads to the critical electric field being <span class=\"s2\">exceeded in the dielectric layer in that region. Thus, under<\/span> reverse bias, high fields in the dielectric can cause catastrophic failure, and thicker dielectrics &#8211; although more robust, may reduce RESURF effectiveness in the fins [9]. It is essential to develop simulation models at an early stage to study the effect of device geometries on the device handling capabilities and develop compact models for SPICE-based circuit simulations.<\/p>\n<p class=\"p1\"><span class=\"s3\">This simulation report showcases a \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> TSBD, pro<\/span>gressing from experimentally derived TCAD modelling to compact model extraction and SPICE-level circuit <span class=\"s3\">analysis. The \u03b2-Ga<sub>2<\/sub>O<sub>3<\/sub> TSBDs are fabricated and electri<\/span>cally tested at University of Bristol cleanroom and characterization lab facilities, process simulation is defined using Victory Process, Victory Mesh, Victory Device and the SPICE modelling were performed using Utmost4, Gateway and SmartSpice tools.<\/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=SS_Q1_JAN2026.pdf\" class='avia_image' target=\"_blank\" rel=\"noopener noreferrer\"><img decoding=\"async\" width=\"575\" height=\"754\" class='wp-image-64132 avia-img-lazy-loading-not-64132 avia_image' src=\"https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026.png\" alt='' title='SS_Q1_JAN2026'  itemprop=\"thumbnailUrl\" srcset=\"https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026.png 575w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026-229x300.png 229w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026-538x705.png 538w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026-28x37.png 28w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026-42x55.png 42w, https:\/\/silvaco.com\/wp-content\/uploads\/2026\/01\/SS_Q1_JAN2026-37x48.png 37w\" sizes=\"(max-width: 575px) 100vw, 575px\" \/><\/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=SS_Q1_JAN2026.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>\u03b2-Ga2O3 is set to revolutionize high-voltage power conversion, with ultra-low losses and a high critical electric field that make it ideal for next-generation power devices, enabling three-phase HVDC AC\/DC and DC\/AC conversion in the 1\u20136 kV, 0.5\u20130.8 kA range for AI data centre power delivery, renewable energy systems, high-voltage circuit breakers, and ESD protection.<\/p>\n","protected":false},"author":8,"featured_media":64132,"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>Enabling the Next Generation of High-Voltage Power<\/title>\n<meta name=\"description\" content=\"\u03b2-Ga2O3 is set to revolutionise high-voltage power conversion, with 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