{"id":2023,"date":"2014-10-29T10:05:49","date_gmt":"2014-10-29T17:05:49","guid":{"rendered":"http:\/\/theoryofeverything.org\/MyToE\/?p=2023"},"modified":"2014-10-29T10:05:49","modified_gmt":"2014-10-29T17:05:49","slug":"hyperbolic-dynkin-136-detail","status":"publish","type":"post","link":"http:\/\/theoryofeverything.org\/theToE\/2014\/10\/29\/hyperbolic-dynkin-136-detail\/","title":{"rendered":"Hyperbolic Dynkin #136 Detail"},"content":{"rendered":"<p>In followup to <a href=\"https:\/\/plus.google.com\/u\/0\/117663015413546257905\/posts\">John Baez&#8217; G+<\/a> thread on <a href=\"https:\/\/plus.google.com\/u\/0\/photos\/117663015413546257905\/albums\/6073419788829018033\/6073419794070545234\">Hyperbolic Dynkin diagrams<\/a>, specifically on the only rank 4 compact symmetrizable diagram 136, I used my <a href=\"http:\/\/theoryofeverything.org\/TOE\/JGM\/ToE_Demonstration.nb\">&#8220;VisibLie&#8221; notebook<\/a> (which includes the <a href=\"http:\/\/www.equaonline.com\/math\/SuperLie\/\">&#8220;SuperLie&#8221; package<\/a> for analyzing Lie Algebras) to get the following information:\ufeff<\/p>\n<p><a href=\"http:\/\/theoryofeverything.org\/MyToE\/?attachment_id=2050\" rel=\"attachment wp-att-2050\"><img decoding=\"async\" src=\"http:\/\/theoryofeverything.org\/MyToE\/wp-content\/uploads\/2014\/10\/H136_detail31.png\" alt=\"H136_detail3\" width=\"500\" class=\"alignnone size-full wp-image-2050\" \/><\/a><\/p>\n<p>Using the <a href=\"https:\/\/code.google.com\/p\/simplie\/\">&#8220;SimpLie&#8221; Google Code OpenSource software<\/a>, we get Hasse diagram of:<br \/>\n<a href=\"http:\/\/theoryofeverything.org\/MyToE\/?attachment_id=2036\" rel=\"attachment wp-att-2036\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/theoryofeverything.org\/MyToE\/wp-content\/uploads\/2014\/10\/Projection-of-H136.jpg\" alt=\"Projection of H136\" width=\"500\" height=\"500\" class=\"alignnone size-full wp-image-2036\" \/><\/a><br \/>\nSymmetrized Cartan matrix:<br \/>\n 1   -1    0   -1\/2<br \/>\n-1    2   -1    0<br \/>\n 0   -1    2   -1<br \/>\n-1\/2  0   -1    1<\/p>\n<p>One possible set of basis vectors for this is:<br \/>\nsrH136={{0,2,0,0},{0,-1,1,0},{0,0,-1,1},{Sqrt[-7],-1,-1,-3}};<\/p>\n<p>with 4D angles between each node of:<br \/>\n{{1->2,135.},{2->3,120.},{3->4,135.},{4->1,120.},{1->3,90.},{2->4,90.}}<\/p>\n<p>Norm&#8217;d Length between nodes is:<br \/>\n{2, Sqrt[2], Sqrt[2], 2}<\/p>\n<p>as visualized in 2D and 3D, with 42 vertices and 26 edges of Norm&#8217;d 4D length of 2 and 94 at Sqrt[2]:<br \/>\n<a href=\"http:\/\/theoryofeverything.org\/MyToE\/?attachment_id=2102\" rel=\"attachment wp-att-2102\"><img decoding=\"async\" src=\"http:\/\/theoryofeverything.org\/MyToE\/wp-content\/uploads\/2014\/10\/H136_Lowe_projection7.png\" alt=\"H136_Lowe_projection7\" width=\"500\" class=\"alignnone size-full wp-image-2102\" \/><\/a><\/p>\n<p><a href=\"http:\/\/theoryofeverything.org\/MyToE\/?attachment_id=2103\" rel=\"attachment wp-att-2103\"><img decoding=\"async\" src=\"http:\/\/theoryofeverything.org\/MyToE\/wp-content\/uploads\/2014\/10\/H136_Lowe_projection8.png\" alt=\"H136_Lowe_projection8\" width=\"500\" class=\"alignnone size-full wp-image-2103\" \/><\/a><\/p>\n<p><a href=\"http:\/\/theoryofeverything.org\/MyToE\/?attachment_id=2099\" rel=\"attachment wp-att-2099\"><img decoding=\"async\" src=\"http:\/\/theoryofeverything.org\/MyToE\/wp-content\/uploads\/2014\/10\/JGM_ToE-now-21d.png\" alt=\"JGM_ToE-now-21d\" width=\"500\" class=\"alignnone size-full wp-image-2099\" \/><\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>In followup to John Baez&#8217; G+ thread on Hyperbolic Dynkin diagrams, specifically on the only rank 4 compact symmetrizable diagram 136, I used my &#8220;VisibLie&#8221; notebook (which includes the &#8220;SuperLie&#8221; package for analyzing Lie Algebras) to get the following information:\ufeff Using the &#8220;SimpLie&#8221; Google Code OpenSource software, we get Hasse diagram of: Symmetrized Cartan matrix: &hellip; <a href=\"http:\/\/theoryofeverything.org\/theToE\/2014\/10\/29\/hyperbolic-dynkin-136-detail\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Hyperbolic Dynkin #136 Detail<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[3],"tags":[18,26],"class_list":["post-2023","post","type-post","status-publish","format-standard","hentry","category-physics","tag-dynkin","tag-hasse"],"aioseo_notices":[],"aioseo_head":"\n\t\t<!-- All in One SEO 4.9.9 - 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Visualizing a Theory of Everything!\" \/>\n\t\t<meta property=\"og:description\" content=\"In followup to John Baez&#039; G+ thread on Hyperbolic Dynkin diagrams, specifically on the only rank 4 compact symmetrizable diagram 136, I used my &quot;VisibLie&quot; notebook (which includes the &quot;SuperLie&quot; package for analyzing Lie Algebras) to get the following information:\ufeff Using the &quot;SimpLie&quot; Google Code OpenSource software, we get Hasse diagram of: Symmetrized Cartan matrix:\" \/>\n\t\t<meta property=\"og:url\" content=\"http:\/\/theoryofeverything.org\/theToE\/2014\/10\/29\/hyperbolic-dynkin-136-detail\/\" \/>\n\t\t<meta property=\"article:published_time\" content=\"2014-10-29T17:05:49+00:00\" \/>\n\t\t<meta property=\"article:modified_time\" content=\"2014-10-29T17:05:49+00:00\" \/>\n\t\t<meta name=\"twitter:card\" content=\"summary\" \/>\n\t\t<meta name=\"twitter:title\" content=\"Hyperbolic Dynkin #136 Detail - Visualizing a Theory of Everything!\" \/>\n\t\t<meta name=\"twitter:description\" content=\"In followup to John Baez&#039; G+ thread on Hyperbolic Dynkin diagrams, specifically on the only rank 4 compact symmetrizable diagram 136, I used my &quot;VisibLie&quot; notebook (which includes the &quot;SuperLie&quot; package for analyzing Lie Algebras) to get the following information:\ufeff Using the &quot;SimpLie&quot; Google Code OpenSource software, we get Hasse diagram of: Symmetrized Cartan matrix:\" \/>\n\t\t<script type=\"application\/ld+json\" class=\"aioseo-schema\">\n\t\t\t{\"@context\":\"https:\\\/\\\/schema.org\",\"@graph\":[{\"@type\":\"BlogPosting\",\"@id\":\"http:\\\/\\\/theoryofeverything.org\\\/theToE\\\/2014\\\/10\\\/29\\\/hyperbolic-dynkin-136-detail\\\/#blogposting\",\"name\":\"Hyperbolic Dynkin #136 Detail - 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Dedicated to the pursuit of beauty and Truth in Nature!","og:type":"article","og:title":"Hyperbolic Dynkin #136 Detail - Visualizing a Theory of Everything!","og:description":"In followup to John Baez' G+ thread on Hyperbolic Dynkin diagrams, specifically on the only rank 4 compact symmetrizable diagram 136, I used my &quot;VisibLie&quot; notebook (which includes the &quot;SuperLie&quot; package for analyzing Lie Algebras) to get the following information:\ufeff Using the &quot;SimpLie&quot; Google Code OpenSource software, we get Hasse diagram of: Symmetrized Cartan matrix:","og:url":"http:\/\/theoryofeverything.org\/theToE\/2014\/10\/29\/hyperbolic-dynkin-136-detail\/","article:published_time":"2014-10-29T17:05:49+00:00","article:modified_time":"2014-10-29T17:05:49+00:00","twitter:card":"summary","twitter:title":"Hyperbolic Dynkin #136 Detail - Visualizing a Theory of Everything!","twitter:description":"In followup to John Baez' G+ thread on Hyperbolic Dynkin diagrams, specifically on the only rank 4 compact symmetrizable diagram 136, I used my &quot;VisibLie&quot; notebook (which includes the &quot;SuperLie&quot; package for analyzing Lie Algebras) to get the following information:\ufeff Using the &quot;SimpLie&quot; Google Code OpenSource software, we get Hasse diagram of: Symmetrized Cartan matrix:"},"aioseo_meta_data":{"post_id":"2023","title":null,"description":null,"keywords":null,"keyphrases":null,"primary_term":null,"canonical_url":null,"og_title":null,"og_description":null,"og_object_type":"default","og_image_type":"default","og_image_url":null,"og_image_width":null,"og_image_height":null,"og_image_custom_url":null,"og_image_custom_fields":null,"og_video":null,"og_custom_url":null,"og_article_section":null,"og_article_tags":null,"twitter_use_og":false,"twitter_card":"default","twitter_image_type":"default","twitter_image_url":null,"twitter_image_custom_url":null,"twitter_image_custom_fields":null,"twitter_title":null,"twitter_description":null,"schema":{"blockGraphs":[],"customGraphs":[],"default":{"data":{"Article":[],"Course":[],"Dataset":[],"FAQPage":[],"Movie":[],"Person":[],"Product":[],"ProductReview":[],"Car":[],"Recipe":[],"Service":[],"SoftwareApplication":[],"WebPage":[]},"graphName":"","isEnabled":true},"graphs":[],"defaultGraph":"","defaultPostTypeGraph":""},"schema_type":"default","schema_type_options":null,"pillar_content":false,"robots_default":true,"robots_noindex":false,"robots_noarchive":false,"robots_nosnippet":false,"robots_nofollow":false,"robots_noimageindex":false,"robots_noodp":false,"robots_notranslate":false,"robots_max_snippet":null,"robots_max_videopreview":null,"robots_max_imagepreview":"large","priority":null,"frequency":null,"local_seo":null,"limit_modified_date":false,"created":"2022-04-06 04:10:05","updated":"2025-06-10 15:39:57"},"aioseo_breadcrumb":"<div class=\"aioseo-breadcrumbs\"><span class=\"aioseo-breadcrumb\">\n\t\t\t<a href=\"http:\/\/theoryofeverything.org\/theToE\" title=\"Home\">Home<\/a>\n\t\t<\/span><span class=\"aioseo-breadcrumb-separator\">\u00bb<\/span><span class=\"aioseo-breadcrumb\">\n\t\t\t<a href=\"http:\/\/theoryofeverything.org\/theToE\/topics\/physics\/\" title=\"Physics\">Physics<\/a>\n\t\t<\/span><span class=\"aioseo-breadcrumb-separator\">\u00bb<\/span><span class=\"aioseo-breadcrumb\">\n\t\t\tHyperbolic Dynkin #136 Detail\n\t\t<\/span><\/div>","aioseo_breadcrumb_json":[{"label":"Home","link":"http:\/\/theoryofeverything.org\/theToE"},{"label":"Physics","link":"http:\/\/theoryofeverything.org\/theToE\/topics\/physics\/"},{"label":"Hyperbolic Dynkin #136 Detail","link":"http:\/\/theoryofeverything.org\/theToE\/2014\/10\/29\/hyperbolic-dynkin-136-detail\/"}],"_links":{"self":[{"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/posts\/2023","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/comments?post=2023"}],"version-history":[{"count":1,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/posts\/2023\/revisions"}],"predecessor-version":[{"id":5180,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/posts\/2023\/revisions\/5180"}],"wp:attachment":[{"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/media?parent=2023"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/categories?post=2023"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/theoryofeverything.org\/theToE\/wp-json\/wp\/v2\/tags?post=2023"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}