{"id":73,"date":"2021-12-09T10:20:18","date_gmt":"2021-12-09T08:20:18","guid":{"rendered":"https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/?page_id=73"},"modified":"2022-07-11T08:50:45","modified_gmt":"2022-07-11T05:50:45","slug":"program","status":"publish","type":"page","link":"https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/program\/","title":{"rendered":"Program"},"content":{"rendered":"\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"325\" src=\"https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/wp-content\/uploads\/sites\/65\/2022\/04\/image-4-1024x325.png\" alt=\"\" class=\"wp-image-277\" srcset=\"https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/wp-content\/uploads\/sites\/65\/2022\/04\/image-4-1024x325.png 1024w, https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/wp-content\/uploads\/sites\/65\/2022\/04\/image-4-300x95.png 300w, https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/wp-content\/uploads\/sites\/65\/2022\/04\/image-4-768x244.png 768w, https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/wp-content\/uploads\/sites\/65\/2022\/04\/image-4.png 1318w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<p><strong>Fabio Apruzzi<\/strong>              &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/6msie7gr0iptky9\/HFS-Defect-Boundaries-Technion22.pdf?dl=0\">&#8220;&nbsp;Higher Form Symmetries TFTs&#8221;<\/a><\/p>\n\n\n\n<p><em>Abstract: Symmetry topological field theories (TFTs) encode the symmetry and anomalies data of a d-dimensional QFT in a (d+1)-dimensional topological action. I will present two methods to obtain the higher form symmetries TFTs for 5 and 6-dimensional superconformal field theories (SCFTs). The first one is a IR method relying on the Coulomb and tensor branch low-energy descriptions respectively. The second one, which can be considered as UV approach, consists of deriving the symmetry TFTs by looking at \u2018near-horizon&#8217; like limits of the brane configurations that engineer the studied SCFTs. In explicit example,&nbsp;I will then describe what are the properties of the SCFTs that can be extracted from these symmetry TFTs.<\/em><\/p>\n\n\n\n<p><strong>Ibrahima Bah<\/strong>                      &#8212; &#8220;&nbsp;Geometry of Decoupling Fields&#8221;<\/p>\n\n\n\n<p><strong>Marieke van Beest<\/strong>            &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/ad73fyozfya7mmn\/Technion1.pdf?dl=0\">&#8220;Holography, 1-Form Symmetries, and IR Physics of QFTs&#8221;<\/a><\/p>\n\n\n\n<p><em>Abstract:  I will discuss higher-form symmetries and &#8216;t Hooft anomalies in the context of holography, and derive implications for the IR physics of the dual QFT.&nbsp;An interesting case is holography in a non-conformal setting, where the existence of a 1-form symmetry can have implications for confinement. I will focus on 4d N=1 SU(N) SYM, realized holographically by the Klebanov-Strassler solution, and identify the&nbsp;1-form symmetry&nbsp;and a mixed 0-\/1-form symmetry anomaly, which is closely related to chiral symmetry breaking. Moreover, from the dual gravity description I will identify the IR 4d topological field theory, which matches the mixed anomaly.&nbsp;Finally, building on these methods,&nbsp;I will discuss some work in progress on&nbsp;3d SCFTs from M-theory, with a particular focus on effects of torsion, which give rise to new background gauge fields for discrete symmetries.<\/em><\/p>\n\n\n\n<p><strong>Federico Bonetti<\/strong>            &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/9w2lffc2fzvl2la\/bonetti_technion.pdf?dl=0\">&#8220;Symmetry TFTs and geometric engineering&#8221;<\/a><\/p>\n\n\n\n<p><em>Abstract: The global symmetries of a d-dimensional quantum field theory (QFT), and their \u2019t Hooft anomalies, are conveniently captured by a topological field theory (TFT) in (d+1) dimensions, which we may refer to as the&nbsp;Symmetry TFT of the given d-dimensional QFT. This point of view has a vast range of applicability: it encompasses both ordinary symmetries, as well as generalized symmetries, and also accounts for global&nbsp;structures. The notion of Symmetry TFT is particularly interesting in the context of QFTs realized in string theory. A natural question in this framework is: can we&nbsp;systematically extract the Symmetry TFT from the data that define the string setup? In this talk, I\u2019ll illustrate concrete realizations of this program via examples in&nbsp;geometric engineering.<\/em><\/p>\n\n\n\n<p><strong>Matthew Buican<\/strong>             &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/dkleevw3c1sk58n\/Buican.pdf?dl=0\">&#8220;Galois Actions and Symmetries in TQFT&#8221;<\/a><\/p>\n\n\n\n<p><strong>Christopher Herzog<\/strong>     &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/yjs723qfa22btqv\/Technion2022forexport.pdf?dl=0\">&#8220;Conformal Surface Defects in Maxwell Theory are Trivial&#8221;<\/a><\/p>\n\n\n\n<p><strong>Christian Jepsen <\/strong>          &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/s6risg1u784oulo\/JepsenSlides.pdf?dl=0\">&#8220;Generalized Free Maxwell Theory&#8221;<\/a><\/p>\n\n\n\n<p><strong>Hee-Cheol Kim<\/strong>               &#8212; <a href=\"https:\/\/www.dropbox.com\/s\/ywts3ly7i0qh023\/Folding.pdf?dl=0\"> &#8220;Folding 5d SCFTs&#8221;<\/a><\/p>\n\n\n\n<p><strong>Neil Lambert<\/strong>                  &#8212;  <a href=\"https:\/\/www.dropbox.com\/s\/nglyvdmlwvwfqdb\/Haifa.pdf?dl=0\">&#8220;Building a Better DLCQ&#8221;<\/a><\/p>\n\n\n\n<p><em>Absract: We discuss interacting five-dimensional gauge theories with an &nbsp;OSp(6|4) symmetry group &#8211; same as ABJM &#8211; but with the role of spacetime and R-symmetries interchanged. &nbsp;These are obtained by a conformal compactification of six-dimensional SCFT\u2019s and admit towers of Omega-deformed instantons that reproduce the KK spectrum. The SU(1,3) spacetime symmetry places interesting constraints on the correlation functions which can be used to reconstruct the six-dimensional correlators. In the limit that the Omega-deformation is turned off one recovers the standard DLCQ construction and associated Schrodinger Symmetry.<\/em><\/p>\n\n\n\n<p><strong>Elli Pomoni<\/strong>                      &#8212;  <a href=\"https:\/\/www.dropbox.com\/s\/1eckwg36c1zt5y2\/Technion-May-2022.pdf?dl=0\">&#8220;4d N=2 Dynamics: Dynamical spin chains and quantum groups&#8221;<\/a><\/p>\n\n\n\n<p><strong>Avia Raviv Moshe<\/strong>         &#8212;  <a href=\"https:\/\/www.dropbox.com\/s\/yfj6bp30arrn2w0\/TechnionMay22%202.pdf?dl=0\">&#8220;Line Defects in CFTs: RG flows and Applications&#8221;<\/a><\/p>\n\n\n\n<p><strong>Christoph Uhlemann<\/strong>    &#8212;  <a href=\"https:\/\/www.dropbox.com\/s\/slc0mwngvo7qhay\/BCFT-BH.pdf?dl=0\">&#8220;From 4d BCFTs to Page curves in Type IIB&#8221;<\/a><\/p>\n\n\n\n<p><strong>Irene Valenzuela<\/strong>             &#8212;  <a href=\"https:\/\/www.dropbox.com\/s\/jf4p7vfhytaraog\/talk_irene_technion21.pdf?dl=0\">&#8220;The absence of global symmetries&#8221;<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Fabio Apruzzi &#8212; &#8220;&nbsp;Higher Form Symmetries TFTs&#8221; Abstract: Symmetry topological field theories (TFTs) encode the symmetry and anomalies data of a d-dimensional QFT in a (d+1)-dimensional topological action. I will present two methods to obtain the higher form symmetries TFTs for 5 and 6-dimensional superconformal field theories (SCFTs). The first one is a IR method [&hellip;]<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"class_list":{"0":"post-73","1":"page","2":"type-page","3":"status-publish","5":"entry"},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.4 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Program - Higher form symmetries, defects, and boundaries in QFT<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/phsites.technion.ac.il\/higher-form-symmetries-defects-and-boundaries-in-qft\/program\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Program - Higher form symmetries, defects, and boundaries in QFT\" \/>\n<meta property=\"og:description\" content=\"Fabio Apruzzi &#8212; &#8220;&nbsp;Higher Form Symmetries TFTs&#8221; Abstract: Symmetry topological field theories (TFTs) encode the symmetry and anomalies data of a d-dimensional QFT in a (d+1)-dimensional topological action. 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