{"id":929860,"date":"2022-10-09T22:00:22","date_gmt":"2022-10-09T22:00:22","guid":{"rendered":"https:\/\/projects.ift.uam-csic.es\/holotube\/?p=929860"},"modified":"2022-11-11T15:30:23","modified_gmt":"2022-11-11T15:30:23","slug":"critical-and-near-critical-relaxation-of-holographic-superfluids","status":"publish","type":"post","link":"https:\/\/projects.ift.uam-csic.es\/holotube\/2022\/10\/09\/critical-and-near-critical-relaxation-of-holographic-superfluids\/","title":{"rendered":"Critical and near-critical relaxation of holographic superfluids"},"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><strong>Date : October 11, 2022, 16:30 CEST<\/strong> (unusual time!)<\/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>Sebastian Grieninger<\/strong><\/strong> (Stony Brook University)<\/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>Critical and near-critical relaxation of holographic superfluids<\/strong><\/p>\n\n\n\n<p>Abstract: We investigate the relaxation of holographic superfluids after quenches with end state is either exactly on the critical point, or very close to it. In the former case the system exhibits a power law falloff as well as an emergent discrete scale invariance. Moreover, we postulate a phenomenological Gross\u2013Pitaevskii-like equation that is able to make quantitative predictions for the behavior after near-critical quenches. Intriguingly, within holography all parameters of our phenomenological equation may be fixed with information from the static equilibrium solutions and linear response theory.<\/p>\n<\/div><\/div>\n\n\n<iframe loading=\"lazy\"  style=\"display: block; margin: 0px auto;\"  id=\"_ytid_66715\"  width=\"1170\" height=\"658\"  data-origwidth=\"1170\" data-origheight=\"658\" src=\"https:\/\/www.youtube.com\/embed\/S4AyoIAKgts?enablejsapi=1&#038;autoplay=0&#038;cc_load_policy=0&#038;cc_lang_pref=&#038;iv_load_policy=1&#038;loop=0&#038;rel=1&#038;fs=1&#038;playsinline=0&#038;autohide=2&#038;theme=dark&#038;color=red&#038;controls=1&#038;\" class=\"__youtube_prefs__  no-lazyload\" title=\"YouTube player\"  allow=\"fullscreen; accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture\" allowfullscreen data-no-lazy=\"1\" data-skipgform_ajax_framebjll=\"\"><\/iframe>\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\/2022\/10\/Holotube_Grieninger.pdf\" type=\"application\/pdf\" style=\"width:100%;height:600px\" aria-label=\"Embed of Embed of Slides..\"><\/object><a id=\"wp-block-file--media-eb30dbfa-2859-47f9-bea3-51701d981f28\" href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2022\/10\/Holotube_Grieninger.pdf\">Slides<\/a><a href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2022\/10\/Holotube_Grieninger.pdf\" class=\"wp-block-file__button\" download aria-describedby=\"wp-block-file--media-eb30dbfa-2859-47f9-bea3-51701d981f28\">Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Date : October 11, 2022, 16:30 CEST (unusual time!) Sebastian Grieninger (Stony Brook University) Link:&nbsp;https:\/\/zoom.us\/j\/98260147834?pwd=VW5BQStqUGUrUFFzWG1jL2tuWXJoZz09 Critical and near-critical relaxation of holographic superfluids Abstract: We investigate the relaxation of holographic superfluids after quenches with end state is either exactly on the critical point, or very close to it. In the former case the system exhibits a [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","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-929860","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\/929860","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=929860"}],"version-history":[{"count":3,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/929860\/revisions"}],"predecessor-version":[{"id":929903,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/929860\/revisions\/929903"}],"wp:attachment":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/media?parent=929860"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/categories?post=929860"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/tags?post=929860"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}