









Speaker: Avner KarasikTitle: Candidates for NonSupersymmetric DualitiesVenue: virtualQuantum Matter in Mathematics and Physics Speaker: Avner Karasik (University of Cambridge, UK) Title: Candidates for NonSupersymmetric Dualities Abstract: In the talk I will discuss the possibility and the obstructions of finding nonsupersymmetric dualities for 4d gauge theories. I will review consistency conditions based on Weingarten inequalities, anomalies and large N, and clarify some subtle points and misconceptions about them. Later I will go over some old and new examples of candidates for nonsupersymmetric dualities. The will be based on 2208.07842 

Speaker: Yichul ChoTitle: Noninvertible Symmetries in NatureVenue: VirtualQuantum Matter in Mathematics and Physics Speaker: Yichul Cho (SUNY Stony Brook) Title: Noninvertible Symmetries in Nature Abstract: In this talk, I will discuss noninvertible symmetries in familiar 3+1d quantum field theories describing our Nature. In massless QED, the classical U(1) axial symmetry is not completely broken by the ABJ anomaly. Instead, it turns into a discrete, noninvertible symmetry. The noninvertible symmetry operator is obtained by dressing the naïve U(1) axial symmetry operator with a fractional quantum Hall state. We also find a similar noninvertible symmetry in the massless limit of QCD, which provides an alternative explanation for the neutral pion decay. In the latter part of the talk, I will discuss noninvertible timereversal symmetries in 3+1d gauge… 

Speaker: Zhengyan Darius ShiTitle: Gifts from anomalies: new results on quantum critical transport in non Fermi liquidsVenue: CMSA Room G10Quantum Matter in Mathematics and Physics Seminar Speaker: Zhengyan Darius Shi (MIT) Title: Gifts from anomalies: new results on quantum critical transport in nonFermi liquids Abstract: NonFermi liquid phenomena arise naturally near Landau ordering transitions in metallic systems. Here, we leverage quantum anomalies as a powerful nonperturbative tool to calculate optical transport in these models in the infrared limit. While the simplest such models with a single boson flavor (N=1) have zero incoherent conductivity, a recently proposed large N deformation involving flavorrandom Yukawa couplings between N flavors of bosons and fermions admits a nontrivial incoherent conductivity (z is the boson dynamical exponent) when the order parameter is odd under inversion. The presence of incoherent conductivity in the random flavor model… 

Speaker: John McGreevy (UCSD)Title: The Generalized Landau Paradigm (a review of generalized symmetries in condensed matter)Venue: VirtualAbstract: Recent advances in our understanding of symmetry in quantum manybody systems offer the possibility of a generalized Landau paradigm that encompasses all equilibrium phases of matter. This talk will be an elementary review of some of these developments, based on: https://arxiv.org/abs/2204.03045 

Speaker: Cari Cesarotti (Harvard)Title: Oblique Lessons from the W Mass Measurement at CDF IIVenue: VirtualAbstract: The CDF collaboration recently reported a new precise measurement of the W boson mass MW with a central value significantly larger than the SM prediction. We explore the effects of including this new measurement on a fit of the Standard Model (SM) to electroweak precision data. We characterize the tension of this new measurement with the SM and explore potential beyond the SM phenomena within the electroweak sector in terms of the oblique parameters S, T and U. We show that the large MW value can be accommodated in the fit by a large, nonzero value of U, which is difficult to construct in explicit models. Assuming U = 0, the electroweak fit strongly prefers large, positive values… 

Speaker: Brian Swingle (Brandeis)Title: Cosmology from the vacuumVenue: VirtualAbstract: We are familiar with the idea that quantum gravity in AdS can holographically emerge from complex patterns of entanglement, but can the physics of big bang cosmology emerge from a quantum manybody system? In this talk I will argue that standard tools of holography can be used to describe fully nonperturbative microscopic models of cosmology in which a period of accelerated expansion may result from the positive potential energy of timedependent scalar fields evolving towards a region with negative potential. In these models, the fundamental cosmological constant is negative, and the universe eventually recollapses in a timereversal symmetric way. The microscopic description naturally selects a special state for the cosmology. In this framework, physics in the cosmological spacetime is dual to the vacuum physics in a static planar asymptotically AdS Lorentzian… 

Speaker: Shlomo S. Razamat (Technion)Title: Aspects of d supersymmetric dynamics and geometryVenue: VirtualAbstract: We will overview the program of geometrically engineering four dimensional supersymmetric QFTs as compactifications of six dimensional SCFTs. In particular we will discuss how strong coupling phenomena in four dimensions, such as duality and emergence of symmetry, can be better understood in such geometric constructions. 

Speaker: Ruben Verresen (Harvard)Title: Higgs = SPTVenue: VirtualAbstract: The Higgs phase of a gauge theory is important to both fundamental physics (e.g., electroweak theory) as well as condensed matter systems (superconductors and other emergent phenomena). However, such a charge condensate seems subtle and is sometimes described as the spontaneous breaking of gauge symmetry (or a global subgroup). In this talk, I will argue that the Higgs phase is best understood as a symmetryprotected topological (SPT) phase. The concept of SPT phases arose out of the condensed matter community, to describe systems with shortrange entanglement and edge modes which cannot be removed in the presence of certain symmetries. The perspective that the Higgs phase is an SPT phase recovers known properties of the Higgs phase and provides… 

Speaker: Latham Boyle (Perimeter)Title: Cancellation of the vacuum energy and Weyl anomaly in the standard model, and a twosheeted, CPTsymmetric universeVenue: VirtualAbstract: I will explain a mechanism to cancel the vacuum energy and both terms in the Weyl anomaly in the standard model of particle physics, using conformallycoupled dimensionzero scalar fields. Remarkably, given the standard model gauge group SU(3)xSU(2)xU(1), the cancellation requires precisely 48 Weyl spinors — i.e. three generations of standard model fermions, including righthanded neutrinos. Moreover, the scalars possess a scaleinvariant power spectrum, suggesting a new explanation for the observed primordial density perturbations in cosmology (without the need for inflation). As context, I will also introduce a related cosmological picture in which this cancellation mechanism plays an essential role. Our universe seems to be dominated by radiation at early times, and positive vacuum energy at late times. Taking… 

Speaker: Yoshio Kikukawa (U Tokyo)Title: Why is the mission impossible? Decoupling the mirror GinspargWilson fermions in the lattice models for twodimensional abelian chiral gauge theoriesVenue: VirtualAbstract: It has been known that the fourdimensional abelian chiral gauge theories of an anomalyfree set of Wely fermions can be formulated on the lattice preserving the exact gauge invariance and the required locality property in the framework of the Ginsparg Wilson relation. This holds true in two dimensions. However, in the related formulation including the mirror GinspargWilson fermions, it has been argued that the mirror fermions do not decouple: in the 3450 model with Dirac and MajoranaYukawa couplings to XYspin field, the two point vertex function of the (external) gauge field in the mirror sector shows a singular nonlocal behavior in the socalled ParaMagnetic Strongcoupling(PMS) phase. We reexamine why the attempt seems a “Mission: Impossible” in the 3450… 

Speaker: Jung Hoon Han (Sungkyunkwan University, Suwon, South Korea)Title: Lattice Gauge Theory View of Toric Codes, Xcube, and MoreVenue: VirtualAbstract: Exactly solvable spin models such as toric codes and Xcube model have heightened our understanding of spin liquids and topological matter in two and three dimensions. Their exact solvability, it turns out, is rooted in the existence of commuting generators in their parent lattice gauge theory (LGT). We can understand the toric codes as Higgsed descendants of the rank1 U(1) LGT in two and three dimensions, and the Xcube model as that of rank2 U(1) LGT in three dimensions. Furthermore, the transformation properties of the gauge fields in the respective LGT is responsible for, and nearly determines the structure of the effective field theory (EFT) of the accompanying matter fields. We show how to construct the EFT of… 