{"id":30687,"date":"2019-04-01T08:00:19","date_gmt":"2019-04-01T08:00:19","guid":{"rendered":"https:\/\/silvaco-stage.betagentechnologies.com\/%eb%b6%84%eb%a5%98%eb%90%98%ec%a7%80-%ec%95%8a%ec%9d%8c\/device-simulation-new-features-in-2019-baseline-release\/"},"modified":"2021-07-16T21:35:05","modified_gmt":"2021-07-17T04:35:05","slug":"device-simulation-new-features-in-2019-baseline-release","status":"publish","type":"post","link":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/device-simulation-new-features-in-2019-baseline-release\/","title":{"rendered":"Device Simulation \u2013 New Features in 2019 Baseline Release"},"content":{"rendered":"<h1 align=\"center\">Device Simulation \u2013 New Features in 2019 Baseline Release<\/h1>\n<p><strong>3.1 Atlas<\/strong><\/p>\n<blockquote><p>3.1.1 Quantum Well Exciton Model<br \/>\n3.1.2 TMM.GF Interface Roughness<br \/>\n3.1.3 Ferroelectric Field Effect Transistor<br \/>\n3.1.4 ALMA Thermal Parameters<\/p><\/blockquote>\n<p><strong>3.2 Victory Device<\/strong><\/p>\n<p>3.2.1 Simulation of Organic Devices<br \/>\n3.2.2 RF Simulation Using Fourier Power Gain Calculation<br \/>\n3.2.3 Simulation of LEDs<br \/>\n3.2.4 MixedMode Simulation using latest SmartSpice spice models<br \/>\n3.2.5 Performance Improvement<br \/>\n3.2.6 CBRAM Simulation<\/p>\n<p><strong>3.3 Atlas and Victory Device<\/strong><\/p>\n<blockquote><p>3.3.1 Cryogenic Incomplete Ionisation Model<\/p><\/blockquote>\n<p><img loading=\"lazy\" width=\"782\" height=\"1012\" src=\"https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1.jpg\" class=\"cleaned-enfold-image\" alt=\"\" decoding=\"async\" loading=\"lazy\" srcset=\"https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1.jpg 782w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-232x300.jpg 232w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-768x994.jpg 768w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-545x705.jpg 545w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-29x37.jpg 29w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-43x55.jpg 43w, https:\/\/silvaco-stage.betagentechnologies.com\/wp-content\/uploads\/2020\/03\/simstd_Q2_2019_a3-1-37x48.jpg 37w\" sizes=\"auto, (max-width: 782px) 100vw, 782px\" \/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>The effect of Coulomb interaction in the absorption spectrum of quantum wells (QWs) is responsible for the quantum confined Stark effect (QCSE), which is the physical mechanism underlying the operation of electro-absorption modulators [1].<br \/>\nA new model has been added to Atlas to simulate QCSE in QWs and can be enabled with the following command (the qwell model must also be activated):<\/p>\n","protected":false},"author":3,"featured_media":19536,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[7486],"tags":[],"class_list":["post-30687","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-simulation-standard-ko","entry","has-media"],"_links":{"self":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/posts\/30687","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/comments?post=30687"}],"version-history":[{"count":1,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/posts\/30687\/revisions"}],"predecessor-version":[{"id":30692,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/posts\/30687\/revisions\/30692"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/media\/19536"}],"wp:attachment":[{"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/media?parent=30687"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/categories?post=30687"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/silvaco-stage.betagentechnologies.com\/ko\/wp-json\/wp\/v2\/tags?post=30687"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}