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BT 222.992 716.845 Td /F2 24.0 Tf [(Workshop Schedule)] TJ ET
BT 283.271 677.782 Td /F2 18.0 Tf [(Events for:)] TJ ET
BT 129.029 656.355 Td /F2 18.0 Tf [(Monday, September 19th - Friday, September 23rd)] TJ ET
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BT 250.377 620.083 Td /F2 14.0 Tf [(Monday, September 19th)] TJ ET
BT 36.266 602.206 Td /F1 12.0 Tf [(9:30am)] TJ ET
BT 84.669 601.601 Td /F2 12.0 Tf [(Kantaro Ohmori - SCGP 102)] TJ ET
BT 84.669 572.230 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 572.230 Td /F1 12.0 Tf [(Kantoro Ohmori )] TJ ET
BT 84.669 543.430 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 543.430 Td /F1 12.0 Tf [(Developments in Non-invertible symmetry: Recent and Near Future )] TJ ET
BT 84.669 514.745 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 514.745 Td /F1 12.0 Tf [(In this talk, I will review the recent developments in the topic of non-invertible )] TJ ET
BT 84.669 500.489 Td /F1 12.0 Tf [(symmetry, which is under intense and rapid research recently. I will review the case of the1+1d )] TJ ET
BT 84.669 486.233 Td /F1 12.0 Tf [(critical Ising CFT, and see how that examples can be generalized in the higher dimensions in )] TJ ET
BT 84.669 471.862 Td /F1 12.0 Tf [(various ways. Then I will describe possible directions regarding the topic. )] TJ ET
BT 36.266 428.782 Td /F1 12.0 Tf [(10:30am)] TJ ET
BT 84.669 428.177 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 408.526 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 84.669 407.921 Td /F2 12.0 Tf [(Sahand Seifnashri - SCGP 102)] TJ ET
BT 84.669 378.550 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 378.550 Td /F1 12.0 Tf [(Sahand Seifnashri )] TJ ET
BT 84.669 349.750 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 349.750 Td /F1 12.0 Tf [(Representation theory for non-invertible symmetries and asymptotic density of states )] TJ ET
BT 84.669 321.065 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 321.065 Td /F1 12.0 Tf [(We find the appropriate notion of representation for non-invertible symmetries needed to )] TJ ET
BT 84.669 306.809 Td /F1 12.0 Tf [(derive selection rules on correlation functions. We use this understanding to derive a Cardy-like )] TJ ET
BT 84.669 292.553 Td /F1 12.0 Tf [(formula for 2d CFTs with a finite non-invertible symmetry. More specifically, we derive a )] TJ ET
BT 84.669 278.297 Td /F1 12.0 Tf [(universal formula for the asymptotic density of states transforming in an irreducible representation )] TJ ET
BT 84.669 263.926 Td /F1 12.0 Tf [(of a non-invertible symmetry. )] TJ ET
BT 36.266 220.846 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 84.669 220.241 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 200.590 Td /F1 12.0 Tf [(2:30pm)] TJ ET
BT 84.669 199.985 Td /F2 12.0 Tf [(Yunqin Zheng - SCGP 103)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Yunqin Zheng )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(Symmetry TFT for non-invertible duality defects )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(Symmetry TFT \(SymTFT\) is a useful tool to decouple the universal data including )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(global symmetries and their ’t Hooft anomalies from the dynamics of quantum field theories. In )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(this talk, we will discuss the SymTFT for the recently widely studied non-invertible duality )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(symmetries in both \(1+1\)d and \(3+1\)d. In particular, we will explain how the non-invertible fusion )] TJ ET
BT 84.669 617.705 Td /F1 12.0 Tf [(rules can be reproduced from the SymTFT, and will also comment on how one can use SymTFT to )] TJ ET
BT 84.669 603.449 Td /F1 12.0 Tf [(distinguish the intrinsically non-invertible symmetry from non-intrinsically non-invertible )] TJ ET
BT 84.669 589.078 Td /F1 12.0 Tf [(symmetry. )] TJ ET
BT 36.266 545.998 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 84.669 545.393 Td /F2 12.0 Tf [(Tea - SCGP Cafe)] TJ ET
BT 36.266 525.742 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 84.669 525.137 Td /F2 12.0 Tf [(Shu-Heng Shao - SCGP 103)] TJ ET
BT 84.669 495.766 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 495.766 Td /F1 12.0 Tf [(Shu-Heng Shao )] TJ ET
BT 84.669 466.966 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 466.966 Td /F1 12.0 Tf [(Non-invertible time-reversal symmetry )] TJ ET
BT 84.669 438.281 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 438.281 Td /F1 12.0 Tf [(In gauge theory, it is commonly stated that time-reversal symmetry only exists at )] TJ ET
BT 84.669 424.025 Td /F1 12.0 Tf [($\\theta=0$ or $\\pi$ for a $2\\pi$-periodic $\\theta$-angle. In this paper, we point out that in both the )] TJ ET
BT 84.669 409.769 Td /F1 12.0 Tf [(free Maxwell theory and massive QED, there is a non-invertible time-reversal symmetry at every )] TJ ET
BT 84.669 395.513 Td /F1 12.0 Tf [(rational $\\theta$-angle, i.e., $\\theta= \\pi p/N$. The non-invertible time-reversal symmetry is )] TJ ET
BT 84.669 381.257 Td /F1 12.0 Tf [(implemented by a conserved, anti-linear operator without an inverse. It is a composition of the )] TJ ET
BT 84.669 367.001 Td /F1 12.0 Tf [(naive time-reversal transformation and a fractional quantum Hall state. We also find similar non-)] TJ ET
BT 84.669 352.745 Td /F1 12.0 Tf [(invertible time-reversal symmetries in non-Abelian gauge theories, including the $\\mathcal{N}=4$ )] TJ ET
BT 84.669 338.374 Td /F1 12.0 Tf [($SU\(2\)$ super Yang-Mills theory along the locus $|\\tau|=1$ on the conformal manifold. )] TJ ET
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BT 249.985 292.039 Td /F2 14.0 Tf [(Tuesday, September 20th)] TJ ET
BT 36.266 274.162 Td /F1 12.0 Tf [(9:30am)] TJ ET
BT 84.669 273.557 Td /F2 12.0 Tf [(Justin Kaidi - Zoom)] TJ ET
BT 84.669 244.186 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 244.186 Td /F1 12.0 Tf [(Justin Kaidi )] TJ ET
BT 84.669 215.386 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 215.386 Td /F1 12.0 Tf [(Non-Invertible Symmetries and Arithmetic )] TJ ET
BT 84.669 186.701 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 186.701 Td /F1 12.0 Tf [(I will begin by explaining how the spectrum of non-invertible symmetries in N=4 SU\(p\) )] TJ ET
BT 84.669 172.445 Td /F1 12.0 Tf [(SYM theory for prime p boils down to some simple statements in modular arithmetic. I will then )] TJ ET
BT 84.669 158.189 Td /F1 12.0 Tf [(generalize to an infinite family of 4d N=2 theories obtained by compactifying the 6d \(2,0\) theory of )] TJ ET
BT 84.669 143.933 Td /F1 12.0 Tf [(type A_{p-1} on a genus g Riemann surface with no punctures. As a concrete example, I will )] TJ ET
BT 84.669 129.677 Td /F1 12.0 Tf [(provide a classification of all invertible and non-invertible symmetries descending from the )] TJ ET
BT 84.669 115.306 Td /F1 12.0 Tf [(modular group Sp\(4,Z\) at genus 2. )] TJ ET
BT 36.266 72.226 Td /F1 12.0 Tf [(10:30am)] TJ ET
BT 84.669 71.621 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 51.970 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 84.669 51.365 Td /F2 12.0 Tf [(Lakshya Bhardwaj - SCGP 102)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Lakshya Bardwaj )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(Universal Non-Invertible Symmetries )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(It is well-known that gauging a finite 0-form symmetry group G in a quantum field )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(theory leads to a dual symmetry generated by topological Wilson line defects. I will argue that one )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(also obtains other dual symmetries described by higher-dimensional topological defects, which are )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(generically non-invertible. The dual topological surface defects can all be shown to be )] TJ ET
BT 84.669 617.705 Td /F1 12.0 Tf [(condensation defects obtained by higher-gauging the dual topological Wilson line defects. The dual )] TJ ET
BT 84.669 603.449 Td /F1 12.0 Tf [(topological surfaces and lines form a 2-category 2Rep\(G\) which is the 2-category of 2-)] TJ ET
BT 84.669 589.193 Td /F1 12.0 Tf [(representations of G. I will also discuss the dual symmetries obtained by gauging a finite 2-group )] TJ ET
BT 84.669 574.937 Td /F1 12.0 Tf [(symmetry. In this case, not all dual topological surface defects are condensation defects and the 2-)] TJ ET
BT 84.669 560.681 Td /F1 12.0 Tf [(category formed by dual topological surfaces and lines can be recognized as the 2-category of 2-)] TJ ET
BT 84.669 546.425 Td /F1 12.0 Tf [(representations of the 2-group. These 2-categories describe symmetries of gauge theories with )] TJ ET
BT 84.669 532.054 Td /F1 12.0 Tf [(continuous disconnected gauge groups in various spacetime dimensions. )] TJ ET
BT 36.266 488.974 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 84.669 488.369 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 468.718 Td /F1 12.0 Tf [(1:15pm)] TJ ET
BT 84.669 468.113 Td /F2 12.0 Tf [(Ibrahima Bah \(SCGP Weekly Talk\) - SCGP 102)] TJ ET
BT 84.669 438.742 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 438.742 Td /F1 12.0 Tf [(Ibrahima Bah )] TJ ET
BT 84.669 409.942 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 409.942 Td /F1 12.0 Tf [(Symmetry structure from the bulk and holography )] TJ ET
BT 84.669 381.257 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 381.257 Td /F1 12.0 Tf [(Recently there has been a revival in the study of symmetries of physical systems due to )] TJ ET
BT 84.669 367.001 Td /F1 12.0 Tf [(the novel perspective that symmetries characterize topological aspects of quantum mechanical )] TJ ET
BT 84.669 352.745 Td /F1 12.0 Tf [(systems. Significant efforts by many researchers from condensed matter physics, to high energy )] TJ ET
BT 84.669 338.489 Td /F1 12.0 Tf [(physics and mathematics have been devoted to fully exploring the consequences of this perspective )] TJ ET
BT 84.669 324.233 Td /F1 12.0 Tf [(in physics. An important aspect to this is the understanding that symmetries, and their associated )] TJ ET
BT 84.669 309.977 Td /F1 12.0 Tf [(structures in a given quantum system, can be characterized in one dimension higher by a )] TJ ET
BT 84.669 295.721 Td /F1 12.0 Tf [(topological field theory via inflow mechanics. Such descriptions can naturally emerge whenever we )] TJ ET
BT 84.669 281.465 Td /F1 12.0 Tf [(can construct quantum field theories from decoupling limits of string theory or supergravity. In this )] TJ ET
BT 84.669 267.209 Td /F1 12.0 Tf [(talks I will review recent progress in these endeavors and discuss the critical questions that we hope )] TJ ET
BT 84.669 252.838 Td /F1 12.0 Tf [(to address. )] TJ ET
BT 36.266 209.758 Td /F1 12.0 Tf [(2:30pm)] TJ ET
BT 84.669 209.153 Td /F2 12.0 Tf [(Mathew Bullimore - SCGP 103)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Mathew Bullimore )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(Higher representations and BPS line operators )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(The talk concerns generalised group-like symmetries in supersymmetric theories in three )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(dimensions. I will explain how the category of BPS line defects supports a 2-representation of the )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(symmetry category. I will also discuss a geometric formulation in terms of the moduli stack of )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(vacua, which is an enhancement of the moduli space of vacua that captures topological sectors in )] TJ ET
BT 84.669 617.705 Td /F1 12.0 Tf [(the infrared. This could be seen as a small step towards the broader goal of understanding how )] TJ ET
BT 84.669 603.334 Td /F1 12.0 Tf [(categorical symmetries act on the extended operator spectrum of a general quantum field theory. )] TJ ET
BT 36.266 560.254 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 84.669 559.649 Td /F2 12.0 Tf [(Tea - SCGP Cafe)] TJ ET
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BT 241.823 536.743 Td /F2 14.0 Tf [(Wednesday, September 21st)] TJ ET
BT 36.266 518.866 Td /F1 12.0 Tf [(9:30am)] TJ ET
BT 84.669 518.261 Td /F2 12.0 Tf [(Apoorv Tiwari - Zoom)] TJ ET
BT 84.669 488.890 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 488.890 Td /F1 12.0 Tf [(Apoorv Tiwari )] TJ ET
BT 84.669 460.090 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 460.090 Td /F1 12.0 Tf [(Topological Holography: phase diagrams of generalized spin models from symmetry TFTs )] TJ ET
BT 84.669 431.405 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 431.405 Td /F1 12.0 Tf [(Owing to recent developments, it is increasingly clear that the finite symmetry of a d-)] TJ ET
BT 84.669 417.149 Td /F1 12.0 Tf [(dimensional quantum model can be encapsulated in a d+1-dimensional "symmetry topological field )] TJ ET
BT 84.669 402.893 Td /F1 12.0 Tf [(theory" \(symmetry TFT\). In this talk, I will describe how symmetry TFTs may be used to organize )] TJ ET
BT 84.669 388.522 Td /F1 12.0 Tf [(phase diagrams of generalized lattice spin systems. )] TJ ET
BT 36.266 345.442 Td /F1 12.0 Tf [(10:30am)] TJ ET
BT 84.669 344.837 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 325.186 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 84.669 324.581 Td /F2 12.0 Tf [(Christian Copetti - SCGP 102)] TJ ET
BT 84.669 295.210 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 295.210 Td /F1 12.0 Tf [(Christian Copetti )] TJ ET
BT 84.669 266.410 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 266.410 Td /F1 12.0 Tf [(Self duality defects from holography. )] TJ ET
BT 84.669 237.725 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 237.725 Td /F1 12.0 Tf [(We explain how non invertible duality \(and more generally n-ality\) defects may emerge )] TJ ET
BT 84.669 223.469 Td /F1 12.0 Tf [(for theories with a dual holographic description. The key observation is that, at the self duality )] TJ ET
BT 84.669 209.213 Td /F1 12.0 Tf [(point, a discrete gauge field emerges in the bulk. We discuss its action through the example of N=4 )] TJ ET
BT 84.669 194.957 Td /F1 12.0 Tf [(SYM and develop a formalism to describe the fusion of the ensuing non-invertible defects. Time )] TJ ET
BT 84.669 180.586 Td /F1 12.0 Tf [(permitting we mention generalizations to theories of class S. )] TJ ET
BT 36.266 137.506 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 84.669 136.901 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 117.250 Td /F1 12.0 Tf [(2:30pm)] TJ ET
BT 84.669 116.645 Td /F2 12.0 Tf [(Juven Wang - SCGP 103)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Juven Wang )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(Ultra Quantum Matter to Beyond the Standard Model Forecast )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(Ideas developed from the quantum matter and quantum field theory frontier may guide )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(us to explore new physics beyond the 4d Standard Model. I propose a few such ideas. First, new )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(physics for neutrinos: right-handed neutrinos carry a Z_{16} class mixed gauge-gravitational )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(global anomaly index, which could be replaced by 4d or 5d topological quantum field theory, or 4d )] TJ ET
BT 84.669 617.705 Td /F1 12.0 Tf [(interacting conformal field theory \(CFT\). These theories provide possible new neutrino mass )] TJ ET
BT 84.669 603.449 Td /F1 12.0 Tf [(mechanisms [arXiv:2012.15860]. Second, deconfined quantum criticality between Grand Unified )] TJ ET
BT 84.669 589.193 Td /F1 12.0 Tf [(Theories: dictated by a Z_2 class global anomaly, a gapless quantum critical CFT region can )] TJ ET
BT 84.669 574.937 Td /F1 12.0 Tf [(happen between Georgi-Glashow and Pati-Salam models as deformation of the Standard Model, )] TJ ET
BT 84.669 560.681 Td /F1 12.0 Tf [(where Beyond the Standard Model physics and Dark Gauge sector occur as neighbor phases )] TJ ET
BT 84.669 546.425 Td /F1 12.0 Tf [([arXiv:2106.16248, arXiv:2112.14765, arXiv:2204.08393]. I will also comment on the generalized )] TJ ET
BT 84.669 532.169 Td /F1 12.0 Tf [(higher symmetries and potential noninvertible symmetries pertinent to Grand Unified Theories. )] TJ ET
BT 84.669 517.913 Td /F1 12.0 Tf [(Third, the Strong CP problem may be solved by a new solution involving Symmetric Mass )] TJ ET
BT 84.669 503.657 Td /F1 12.0 Tf [(Generation [arXiv:2204.14271, arXiv:2207.14813, to appear]. The collaborators of these works )] TJ ET
BT 84.669 489.286 Td /F1 12.0 Tf [(include Yuta Hamada, Zheyan Wan, and Yizhuang You. )] TJ ET
BT 36.266 446.206 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 84.669 445.601 Td /F2 12.0 Tf [(Tea - SCGP Cafe)] TJ ET
BT 36.266 425.950 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 84.669 425.345 Td /F2 12.0 Tf [(Gong Show - SCGP 103)] TJ ET
BT 36.266 405.694 Td /F1 12.0 Tf [(6:00pm)] TJ ET
BT 84.669 405.089 Td /F2 12.0 Tf [(Banquet)] TJ ET
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BT 244.532 382.183 Td /F2 14.0 Tf [(Thursday, September 22nd)] TJ ET
BT 36.266 364.306 Td /F1 12.0 Tf [(9:30am)] TJ ET
BT 84.669 363.701 Td /F2 12.0 Tf [(Ho Tat Lam - SCGP 102)] TJ ET
BT 84.669 334.330 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 334.330 Td /F1 12.0 Tf [(Ho Tat Lam )] TJ ET
BT 84.669 305.530 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 305.530 Td /F1 12.0 Tf [(Exotic Theories with Dipole Symmetries )] TJ ET
BT 84.669 276.845 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 276.845 Td /F1 12.0 Tf [(I will discuss exotic theories with dipole global symmetries and dipole gauge )] TJ ET
BT 84.669 262.589 Td /F1 12.0 Tf [(symmetries. Examples of these theories include the compact Lifshitz theory and a tensor gauge )] TJ ET
BT 84.669 248.333 Td /F1 12.0 Tf [(theory that has fractons. To resolve various subtleties in the precise meaning of these global or )] TJ ET
BT 84.669 234.077 Td /F1 12.0 Tf [(gauge symmetries, we place these theories on a lattice and then take the continuum limit. )] TJ ET
BT 84.669 219.821 Td /F1 12.0 Tf [(Interestingly the continuum limit is not unique. Different limits lead to different continuum )] TJ ET
BT 84.669 205.565 Td /F1 12.0 Tf [(theories, whose operators, defects, global symmetries, etc., are different. Since these theories are )] TJ ET
BT 84.669 191.309 Td /F1 12.0 Tf [(non-relativistic, we need to distinguish global symmetries that act on defects and on operators. We )] TJ ET
BT 84.669 177.053 Td /F1 12.0 Tf [(refer to the global symmetries that act on defects as timelike global symmetries. Using these )] TJ ET
BT 84.669 162.797 Td /F1 12.0 Tf [(timelike global symmetries, we can phrase the mobility restrictions of defects \(including those of )] TJ ET
BT 84.669 148.426 Td /F1 12.0 Tf [(fractons\) as consequences of global symmetries. )] TJ ET
BT 36.266 105.346 Td /F1 12.0 Tf [(10:30am)] TJ ET
BT 84.669 104.741 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 85.090 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 84.669 84.485 Td /F2 12.0 Tf [(Fabio Apruzzi - SCGP 102)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Fabio Apruzzi )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(Non-Invertible Symmetries from Holography and Branes )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(We propose a systematic approach to deriving symmetry generators of Quantum Field )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(Theories in holography. Central to this are the Gauss law constraints in the Hamiltonian )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(quantization of Symmetry Topological Field Theories \(SymTFTs\), which are obtained from )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(supergravity. In turn we realize the symmetry generators from world-volume theories of D-branes )] TJ ET
BT 84.669 617.705 Td /F1 12.0 Tf [(in holography. Our main focus is on non-invertible symmetries, which have emerged in the past )] TJ ET
BT 84.669 603.449 Td /F1 12.0 Tf [(year as a new type of symmetry in d? 4 QFTs. We exemplify our proposal in the holographic )] TJ ET
BT 84.669 589.193 Td /F1 12.0 Tf [(confinement setup, dual to 4d N=1 Super-Yang Mills. In the brane-picture, the fusion of non-)] TJ ET
BT 84.669 574.937 Td /F1 12.0 Tf [(invertible symmetries naturally arises from the Myers effect on D-branes. In turn, their action on )] TJ ET
BT 84.669 560.566 Td /F1 12.0 Tf [(line defects is modeled by the Hanany-Witten effect. )] TJ ET
BT 36.266 517.486 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 84.669 516.881 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 497.230 Td /F1 12.0 Tf [(2:30pm)] TJ ET
BT 84.669 496.625 Td /F2 12.0 Tf [(Inaki Garcia-Extebarria - SCGP 103)] TJ ET
BT 84.669 467.254 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 467.254 Td /F1 12.0 Tf [(Inaki Garcia-Extebarria )] TJ ET
BT 84.669 438.454 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 438.454 Td /F1 12.0 Tf [(Symmetries and branes for S-folds )] TJ ET
BT 84.669 409.769 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 409.769 Td /F1 12.0 Tf [(D3 brane stacks probing O3 planes and its non-perturbative generalisations known as S-)] TJ ET
BT 84.669 395.513 Td /F1 12.0 Tf [(folds have a near horizon limit of the form AdS5 × \(S_5 /Z_k\), which describes the holographic )] TJ ET
BT 84.669 381.257 Td /F1 12.0 Tf [(dual of the SCFTs living on the D3 stack. I will describe various aspects of this class of systems, )] TJ ET
BT 84.669 367.001 Td /F1 12.0 Tf [(including how to extract the higher form symmetries \(for arbitrary k\) and non-invertible )] TJ ET
BT 84.669 352.630 Td /F1 12.0 Tf [(symmetries \(for k=2\). )] TJ ET
BT 36.266 309.550 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 84.669 308.945 Td /F2 12.0 Tf [(Tea - SCGP Cafe)] TJ ET
BT 36.266 289.294 Td /F1 12.0 Tf [(4:00pm)] TJ ET
BT 84.669 288.689 Td /F2 12.0 Tf [(Daniel Brennan - SCGP 103)] TJ ET
BT 84.669 259.318 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 259.318 Td /F1 12.0 Tf [(Daniel Brennan )] TJ ET
BT 84.669 230.518 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 230.518 Td /F1 12.0 Tf [(Line Operator Quantum Numbers and Anomalies )] TJ ET
BT 84.669 201.833 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 201.833 Td /F1 12.0 Tf [(In this talk we will describe a new mechanism for studying anomalies of discrete )] TJ ET
BT 84.669 187.577 Td /F1 12.0 Tf [(symmetries in 4D gauge theories. This mechanism involves flowing to a pure abelian gauge theory )] TJ ET
BT 84.669 173.321 Td /F1 12.0 Tf [(where the anomaly can be computed in terms of the quantum numbers of electric and magnetic line )] TJ ET
BT 84.669 159.065 Td /F1 12.0 Tf [(operators. We demonstrate our program by computing the anomaly in SU\(2\) QCD with )] TJ ET
BT 84.669 144.694 Td /F1 12.0 Tf [(fundamental and adjoint fermions. )] TJ ET
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BT 254.269 98.359 Td /F2 14.0 Tf [(Friday, September 23rd)] TJ ET
BT 36.266 80.482 Td /F1 12.0 Tf [(10:30am)] TJ ET
BT 84.669 79.877 Td /F2 12.0 Tf [(Coffee Break - SCGP Cafe)] TJ ET
BT 36.266 60.226 Td /F1 12.0 Tf [(11:00am)] TJ ET
BT 84.669 59.621 Td /F2 12.0 Tf [(Jonathan Heckman - SCGP 102)] TJ ET
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BT 84.669 732.214 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 732.214 Td /F1 12.0 Tf [(Jonathan Heckman )] TJ ET
BT 84.669 703.414 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 703.414 Td /F1 12.0 Tf [(The Branes Behind Generalized Symmetry Operators )] TJ ET
BT 84.669 674.729 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 674.729 Td /F1 12.0 Tf [(We present a brane construction of generalized symmetry operators in supersymmetric )] TJ ET
BT 84.669 660.473 Td /F1 12.0 Tf [(QFTs engineered via string compactification. These branes link with defects, and the brane )] TJ ET
BT 84.669 646.217 Td /F1 12.0 Tf [(perspective allows us to read of various structures such as their fusion algebra. The stringy )] TJ ET
BT 84.669 631.961 Td /F1 12.0 Tf [(perspective also suggests various categorical generalizations of these objects, which we also )] TJ ET
BT 84.669 617.590 Td /F1 12.0 Tf [(discuss. Based on joint work with M. Hubner, E. Torres and H.Y. Zhang. )] TJ ET
BT 36.266 574.510 Td /F1 12.0 Tf [(12:00pm)] TJ ET
BT 84.669 573.905 Td /F2 12.0 Tf [(Lunch - SCGP Cafe)] TJ ET
BT 36.266 554.254 Td /F1 12.0 Tf [(1:15pm)] TJ ET
BT 84.669 553.649 Td /F2 12.0 Tf [(Zohar Komargodski - SCGP 102)] TJ ET
BT 84.669 524.278 Td /F2 12.0 Tf [(Speaker: )] TJ ET
BT 133.665 524.278 Td /F1 12.0 Tf [(Zohar Komargodski )] TJ ET
BT 84.669 495.478 Td /F2 12.0 Tf [(Title: )] TJ ET
BT 115.665 495.478 Td /F1 12.0 Tf [(Line Operators, RG Flows, and One-Form Symmetry )] TJ ET
BT 84.669 466.793 Td /F2 12.0 Tf [(Abstract: )] TJ ET
BT 136.317 466.793 Td /F1 12.0 Tf [(I will review general constraints on RG flows on line defects. The first constraint is from )] TJ ET
BT 84.669 452.537 Td /F1 12.0 Tf [(an inequality on a defect entropy and the second constraint is from one-form symmetry. We will )] TJ ET
BT 84.669 438.166 Td /F1 12.0 Tf [(apply these ideas to magnets and line defects in gauge theories. )] TJ ET
BT 36.266 395.086 Td /F1 12.0 Tf [(3:30pm)] TJ ET
BT 84.669 394.481 Td /F2 12.0 Tf [(Tea - SCGP Cafe)] TJ ET
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