{"id":929908,"date":"2022-11-11T15:38:57","date_gmt":"2022-11-11T15:38:57","guid":{"rendered":"https:\/\/projects.ift.uam-csic.es\/holotube\/?p=929908"},"modified":"2022-11-17T11:39:14","modified_gmt":"2022-11-17T11:39:14","slug":"november-15-holographic-meissner-effect-by-makoto-natsuume","status":"publish","type":"post","link":"https:\/\/projects.ift.uam-csic.es\/holotube\/2022\/11\/11\/november-15-holographic-meissner-effect-by-makoto-natsuume\/","title":{"rendered":"November 15: &#8220;Holographic Meissner effect&#8221; by Makoto Natsuume"},"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 : November 15, 2022, 14:00 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>Makoto Natsuume<\/strong><\/strong> (KEK, Japan)<\/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>Holographic Meissner effect<\/strong><\/p>\n\n\n\n<p>Abstract: The holographic superconductor is the holographic dual of superconductivity, but there is no Meissner effect in conventional holographic superconductors. This is because the boundary Maxwell field is added as an external source and is not dynamical. We explain how to implement the Meissner effect by changing the boundary condition and show the effect analytically.<\/p>\n<\/div><\/div>\n\n\n<iframe loading=\"lazy\"  style=\"display: block; margin: 0px auto;\"  id=\"_ytid_89270\"  width=\"1170\" height=\"878\"  data-origwidth=\"1170\" data-origheight=\"878\" src=\"https:\/\/www.youtube.com\/embed\/QzQQlSkcxRQ?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\/11\/holotube_natsuume.pdf\" type=\"application\/pdf\" style=\"width:100%;height:600px\" aria-label=\"Embed of Embed of Slides..\"><\/object><a id=\"wp-block-file--media-d6802ef6-ebae-43df-bad3-2410ff6823ed\" href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2022\/11\/holotube_natsuume.pdf\">Slides<\/a><a href=\"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-content\/uploads\/2022\/11\/holotube_natsuume.pdf\" class=\"wp-block-file__button\" download aria-describedby=\"wp-block-file--media-d6802ef6-ebae-43df-bad3-2410ff6823ed\">Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Date : November 15, 2022, 14:00 CET Makoto Natsuume (KEK, Japan) Link:&nbsp;https:\/\/zoom.us\/j\/98260147834?pwd=VW5BQStqUGUrUFFzWG1jL2tuWXJoZz09 Holographic Meissner effect Abstract: The holographic superconductor is the holographic dual of superconductivity, but there is no Meissner effect in conventional holographic superconductors. This is because the boundary Maxwell field is added as an external source and is not dynamical. We explain how [&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-929908","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\/929908","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=929908"}],"version-history":[{"count":3,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/929908\/revisions"}],"predecessor-version":[{"id":929917,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/posts\/929908\/revisions\/929917"}],"wp:attachment":[{"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/media?parent=929908"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/categories?post=929908"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/projects.ift.uam-csic.es\/holotube\/wp-json\/wp\/v2\/tags?post=929908"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}