{"id":930008,"date":"2023-02-27T07:05:32","date_gmt":"2023-02-27T07:05:32","guid":{"rendered":"https:\/\/projects.ift.uam-csic.es\/holotube\/?p=930008"},"modified":"2023-02-28T15:03:56","modified_gmt":"2023-02-28T15:03:56","slug":"february-28-zero-sound-and-higher-form-symmetries-in-compressible-holographic-phases-by-eric-mefford","status":"publish","type":"post","link":"https:\/\/projects.ift.uam-csic.es\/holotube\/2023\/02\/27\/february-28-zero-sound-and-higher-form-symmetries-in-compressible-holographic-phases-by-eric-mefford\/","title":{"rendered":"February 28: &#8220;Zero sound and higher-form symmetries in compressible holographic phases&#8221; by Eric Mefford"},"content":{"rendered":"\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-flow wp-block-group-is-layout-flow\">\n<p class=\"has-black-color has-text-color\"><strong>Date : February 28, 2023, 16:00 CET<\/strong> <\/p>\n\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-flow wp-block-group-is-layout-flow\">\n<p><strong><strong>Eric Mefford<\/strong><\/strong> (University of Victoria)<\/p>\n<\/div><\/div>\n\n\n\n<p><strong>Link:<\/strong>&nbsp;<a href=\"https:\/\/zoom.us\/j\/98260147834?pwd=VW5BQStqUGUrUFFzWG1jL2tuWXJoZz09\">https:\/\/zoom.us\/j\/98260147834?pwd=VW5BQStqUGUrUFFzWG1jL2tuWXJoZz09<\/a><\/p>\n\n\n\n<p><strong>Zero sound and higher-form symmetries in compressible holographic phases<\/strong><\/p>\n\n\n\n<p><strong>Abstract: <\/strong> Certain holographic states of matter with a global U(1) symmetry support a sound mode at zero temperature, caused neither by spontaneous symmetry breaking of the global U(1) nor by the emergence of a Fermi surface in the infrared. In this talk, I will&nbsp;present recent work that illustrates that such a mode is also found in zero density holographic quantum critical states. I will argue that the appearance of a zero temperature sound mode is the consequence of a mixed \u2018t Hooft anomaly between the global U(1) symmetry and an emergent higher-form symmetry. At non-zero temperatures, the presence of a black hole horizon weakly breaks the emergent symmetry and gaps the collective mode, giving rise to a sharp Drude-like peak in the electric conductivity. Time permitting, I will present evidence that the same physics emerges in certain finite density holographic quantum critical states at low temperatures.<\/p>\n<\/div><\/div>\n\n\n\n<div data-wp-interactive=\"core\/file\" class=\"wp-block-file\"><object data-wp-bind--hidden=\"!state.hasPdfPreview\" hidden class=\"wp-block-file__embed\" data=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2023\/02\/ZeroSound.pdf\" type=\"application\/pdf\" style=\"width:100%;height:600px\" aria-label=\"Embed of Embed of ZeroSound..\"><\/object><a id=\"wp-block-file--media-40e8c9b4-a2df-4049-8919-2901865b54a8\" href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2023\/02\/ZeroSound.pdf\">ZeroSound<\/a><a href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2023\/02\/ZeroSound.pdf\" class=\"wp-block-file__button\" download aria-describedby=\"wp-block-file--media-40e8c9b4-a2df-4049-8919-2901865b54a8\">Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Date : February 28, 2023, 16:00 CET Eric Mefford (University of Victoria) Link:&nbsp;https:\/\/zoom.us\/j\/98260147834?pwd=VW5BQStqUGUrUFFzWG1jL2tuWXJoZz09 Zero sound and higher-form symmetries in compressible holographic phases Abstract: Certain holographic states of matter with a global U(1) symmetry support a sound mode at zero temperature, caused neither by spontaneous symmetry breaking of the global U(1) nor by the emergence of [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_bbp_topic_count":0,"_bbp_reply_count":0,"_bbp_total_topic_count":0,"_bbp_total_reply_count":0,"_bbp_voice_count":0,"_bbp_anonymous_reply_count":0,"_bbp_topic_count_hidden":0,"_bbp_reply_count_hidden":0,"_bbp_forum_subforum_count":0,"footnotes":""},"categories":[1],"tags":[],"class_list":["post-930008","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/930008","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/comments?post=930008"}],"version-history":[{"count":2,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/930008\/revisions"}],"predecessor-version":[{"id":930014,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/930008\/revisions\/930014"}],"wp:attachment":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/media?parent=930008"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/categories?post=930008"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/tags?post=930008"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}