{"id":19,"date":"2023-11-16T10:58:52","date_gmt":"2023-11-16T15:58:52","guid":{"rendered":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/?page_id=19"},"modified":"2026-03-10T15:29:53","modified_gmt":"2026-03-10T19:29:53","slug":"graduate-student-postdoc-week","status":"publish","type":"page","link":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/graduate-student-postdoc-week\/","title":{"rendered":"Graduate Student &#8211; Postdoc Week"},"content":{"rendered":"\n<p class=\"has-text-align-center has-large-font-size wp-block-paragraph\"><strong><a href=\"https:\/\/nd.qualtrics.com\/jfe\/form\/SV_bme8CjeORq0N47s\">APPLICATION<\/a><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n\n\n\n<p class=\"has-black-color has-text-color has-link-color wp-elements-1 wp-block-paragraph\" style=\"font-size:30px\"><strong>SPEAKERS &amp; ABSTRACTS<\/strong><\/p>\n\n\n\n<p class=\"has-medium-font-size wp-block-paragraph\"><strong>Sergei Gukov<\/strong>\u00a0(California Institute of Technology)<br><em><strong>Title:<\/strong>\u00a0<\/em>&#8220;BPS <em>q<\/em>-series invariants of 3-manifolds.&#8221;<br><em><strong>Abstract:<\/strong><\/em>\u00a0<a href=\"https:\/\/acrobat.adobe.com\/link\/review?uri=urn:aaid:scds:US:f488aa59-04c2-3fde-a7e0-cae5c43a643d\">BPS <em>q<\/em>-series invariants of 3-manifolds<\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=q74gzI4JIhc\">Lecture 1<\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=4wFk73PxXbE\">Lecture 2<\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=vgql3MkmkAM\">Lecture 3<\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=j8QdSG2rHqs\">Lecture 4<\/a><\/p>\n\n\n\n<p class=\"has-medium-font-size wp-block-paragraph\"><strong>Owen Gwilliam <\/strong>(University of Massachusetts)<br><em><strong>Title:<\/strong><\/em>\u00a0&#8220;Generalized symmetries, factorization algebras, and nonabelian Poincare duality&#8221;<br><em><strong>Abstract:<\/strong><\/em>\u00a0A central result in theoretical physics is Noether&#8217;s theorem, which relates symmetries to conserved quantities in a Lagrangian field theory. It is where Lie algebras first push their way to the front of the physics stage. Recently, physicists have introduced &#8220;generalized global symmetries&#8221; as a way of understanding other important features of field theories. This lecture series aims to explain these ideas and put them in dialogue with recent developments in topology, notably the framework of factorization algebras and the nonabelian Poincare duality of Salvatore, Lurie, Ayala-Francis, and others. Thus, the lectures will touch upon\u00a0<br>* classical field theory, including Yang-Mills theories, and their Batalin-Vilkovisky (BV)                                                formulations<br>* factorization algebras as observables of field theories and as current algebras<br>* Noether&#8217;s theorem and its factorization formulation for perturbative BV theories<br>* generalized global symmetries as prefactorization\u00a0algebras<br>* the nonabelian Poincare duality theorem (NAPD)<br>* a generalization of NAPD using new Grothendieck topologies for manifolds<br><a href=\"https:\/\/www.youtube.com\/watch?v=O0Zn4xpvYRc\">Lecture 1<\/a> <br><a href=\"https:\/\/www.youtube.com\/watch?v=41bpQXyCw3k\">Lecture 2<\/a> <br><a href=\"https:\/\/www.youtube.com\/watch?v=PWtOILJX7gw\">Lecture 3 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=pMD7io9Nj2k\">Lecture 4<\/a><\/p>\n\n\n\n<div class=\"wp-block-group is-vertical is-layout-flex wp-container-core-group-is-layout-4fc3f8e1 wp-block-group-is-layout-flex\">\n<p class=\"has-text-align-left has-medium-font-size wp-block-paragraph\"><strong>Pavel Mnev <\/strong>(University of Notre Dame)<\/p>\n\n\n\n<p class=\"has-text-align-left has-medium-font-size wp-block-paragraph\"><strong><em>Title:<\/em><\/strong>&nbsp; &#8220;Combinatorial models of TQFT&#8221;<br><strong><em>Abstract:<\/em><\/strong> I will explain the construction of the topological BF theory on triangulated manifolds, with fields being cellular cochains, arising from integrating out \u201cfast fields\u201d in continuum theory. A crucial tool in the construction is the Batalin-Vilkovisky (BV) formalism and in particular the fiber BV integral. The combinatorial model can be understood as a functorial TQFT on triangulated cobordisms, \u00e0 la Atiyah, in the called BV-BFV formalism.<\/p>\n\n\n\n<p class=\"has-text-align-left wp-block-paragraph\">I will also explain 1d Chern-Simons theory on cochains of a polygon, constructed in similar spirit.<\/p>\n\n\n\n<p class=\"has-text-align-left wp-block-paragraph\">Towards the end, I will talk about a combinatorial model of 2d topological conformal field theory arising as an \u201cup-to-homotopy\u201d version of 2d Dijkgraaf-Witten model.<br><a href=\"https:\/\/www.youtube.com\/watch?v=FALrSjIdDkc\">Lecture 1 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=g8paGrz8XkQ\">Lecture 2 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=GByF3UIzWak\">Lecture 3 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=Qj-6WEiPIx0\">Lecture 4<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n<\/div>\n\n\n\n<p class=\"has-medium-font-size wp-block-paragraph\"><strong>Konstantin Wernli<\/strong>\u00a0(University of Southern Denmark),<br><em><strong>Title:<\/strong>\u00a0<\/em>\u00a0&#8220;Locality and Globalization in Perturbative Quantum Field Theory.&#8221; \u00a0<br><strong><em>Abstract:<\/em><\/strong>\u00a0The formulation of QFT via functional integrals is beautiful, but in most cases mathematically ill-defined. Perturbative QFT aims to make sense of those ill-defined integrals by formally applying the principle of stationary phase. To reconcile it with the functorial approach to field theory due to Atiyah and Segal, one needs to study the behaviour of perturbative QFT with respect to cutting and gluing of spacetime manifolds. Most examples of functorial field theories come from gauge theories, for those, one needs to resort to the BV-BFV formalism to define the perturbative QFT on manifolds with boundary.\u00a0<br>I will give an introduction to the BV-BFV formalism aimed at a mathematical audience and discuss examples. Then I will discuss the problem of globalization in perturbative QFT and sketch a program to reconcile (or construct) TQFTs with perturbative\u00a0QFT.<br><a href=\"https:\/\/www.youtube.com\/watch?v=95jzHnkHYc4\">Lecture 1 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=tLNJW64UCSE\">Lecture 2 <\/a><br><a href=\"https:\/\/www.youtube.com\/watch?v=IxdQJHK_Sak\">Lecture 3<\/a> <br><a href=\"https:\/\/www.youtube.com\/watch?v=_cB3UYb8BsU\">Lecture 4<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><\/p>\n","protected":false},"excerpt":{"rendered":"<p>APPLICATION SPEAKERS &amp; ABSTRACTS Sergei Gukov\u00a0(California Institute of Technology)Title:\u00a0&#8220;BPS q-series invariants of 3-manifolds.&#8221;Abstract:\u00a0BPS q-series invariants of 3-manifoldsLecture 1Lecture 2Lecture 3Lecture 4 Owen Gwilliam (University of Massachusetts)Title:\u00a0&#8220;Generalized symmetries, factorization algebras, and nonabelian Poincare duality&#8221;Abstract:\u00a0A central result in theoretical physics is Noether&#8217;s theorem, which relates symmetries to conserved quantities in a Lagrangian field theory. It is where [&hellip;]<\/p>\n","protected":false},"author":3983,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-19","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/pages\/19","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/users\/3983"}],"replies":[{"embeddable":true,"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/comments?post=19"}],"version-history":[{"count":16,"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/pages\/19\/revisions"}],"predecessor-version":[{"id":117,"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/pages\/19\/revisions\/117"}],"wp:attachment":[{"href":"https:\/\/sites.nd.edu\/2024cmndthematicprogram\/wp-json\/wp\/v2\/media?parent=19"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}