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Sridip Pal (Institute for Advanced Study, Princeton)04/07/2022, 09:30
The usual state-operator correspondence in Non Relativistic CFT maps the positively charged operators to the states in a harmonic trap. We point out that there exists a notion of state-operator correspondence which levarages the SL(2,R) subgroup of Schrodinger group and can be used to extend the state-operator map to the sector with zero charge. We can rederive the unitarity bounds using this...
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Nicola Andrea Dondi (University of Bern)04/07/2022, 11:00
The conformal data of CFTs involving heavy charged operators can be organised as a series in inverse powers of the global charges involved. When extrapolating these expansions to light low-charge sectors, it is relevant to ask whether these series are divergent and Borel-summable. In this talk, I will show that, generically, one would expect large-charge expansions to be divergent faster than...
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Ioannis Kalogerakis (University of Bern)04/07/2022, 11:30
In this talk I systematically study spinning correlators of a
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generic non-parity violating CFT, with an O(2) internal symmetry at
sectors of large charge. At the beginning I will show the equivalence
between canonical and path integral quantization to the leading order
result, and subsequently I will use the former to compute three- and
four-point functions with conserved current... -
Oleg Antipin (Institut Rudjer Boskovic)04/07/2022, 14:00
I will review the applications of the fixed-charge semiclassical method to various models
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concentrating mostly on the perturbative aspects of the calculation.
I will elucidate the identification of the lowest-lying operator, analytic structure of the large charge expansion and application to various proposed dualities at the critical point. I will conclude with several open problems. -
Matías Torres Sandoval (Università Napoli Federico ii)04/07/2022, 15:30
In this talk, I will focus on two different methods that allow us to go beyond standard perturbation theory: the large charge expansion and resurgence. In particular, I will talk about the scaling dimension associated to charged operators in the O(N) model near d=4 and d=3 and monopoles operators in QED3. I will present their analytic structure for large and small values of the charge and...
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Shota Komatsu (CERN)05/07/2022, 09:30
N=4 super Yang-Mills (SYM) in four dimensions is integrable in the planar limit, allowing exact computations of a variety of observables. In this talk, I will provide evidence that the large charge sector of N=4 SYM with the SU(2) gauge group provides another interesting solvable corner, which is far from the planar limit but nevertheless exhibits similar structures. Specifically, we consider...
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Jahmall Bersini (Rudjer Boskovic Institute)05/07/2022, 11:00
I will discuss the large-charge expansion in cases where more than one charge is taken to be large.
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As an illustration, I will consider the first known example of a Standard Model-like theory featuring asymptotic safety in four dimensions. In particular, I will present the contribution to the scaling dimension of charged operators stemming from quartic, Yukawa, and gauge interactions, and... -
Vito Pellizzani (University of Bern)05/07/2022, 11:30
I will discuss the large-charge expansion of the conformal dimension Δ(Q) of the lowest operator of charge Q in nonrelativistic CFTs using the state-operator correspondence. The latter requires coupling the theory to an external harmonic trap that confines the particles to a spherical cloud, at the edge of which the effective theory breaks down and leads to divergences. I will show how to...
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Pantelis Panopoulos (Rudjer Boskovic Institute, Croatia)05/07/2022, 14:30
Using large charge methods we evaluate the contributions from gauge invariant interactions to the scalar field anomalous dimensions in various models between 2 and 4 dimensions. Examples contain scalar QED, Nambu-Jona-Lasinio and Gross-Neveu-Yukawa models. In some of these, superconformal field theories emerge at the fixed points, exhibiting a rich structure and relation between actions...
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Eran Palti (Ben-Gurion University)06/07/2022, 09:30
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Francesco Sannino (Federico II, CP3-Origins, Danish-IAS, CERN, Scuola Superiore Meridionale)06/07/2022, 11:00
We explore the quantum nature of black holes by introducing an effective frame- work that takes into account deviations from the classical results. The approach is based on introducing quantum corrections to the classical Schwarzschild geometry in a way that is consistent with the physical scales of the black hole and its classical symmetries. This is achieved by organizing the quantum...
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Raffaele Savelli (University of Rome "Tor Vergata")07/07/2022, 09:30
There are special classes of N=2 superconformal field theories in four dimensions, such as those of the “Argyres-Douglas” type, that feature an intrinsically strong dynamics. Due to the lack of a Lagrangian description, determining their properties quantitatively is a challenge. In this talk, I will present a general formula, which, inspired by the techniques of localization in gauge theory,...
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Masataka Watanabe (Weizmann Institute of Science)07/07/2022, 11:00
I will argue for the instability of the O(N) Wilson-Fisher fixed point above four dimensions, using the epsilon expansion.
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By computing the lowest operator dimension in the rank-Q symmetric rep in the double-scaling limit where epsilonQ fixed, I will show that its imaginary part never vanishes for any epsilonQ.
The mechanism for the imaginary part is different for small and large... -
Diego Rodriguez-Gomez (U. of Oviedo)07/07/2022, 14:00
Defect operators in field theory are very interesting for a number of reasons. Drawing inspiration from techniques which have been very recently applied to uncover interesting properties of sectors of operators with large charge under a global symmetry, we will study simple defects in the Wilson-Fisher fixed point near d=4,6 dimensions. Combining with localization, we will also introduce a...
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Elizabeth Helfenberger (Princeton University)07/07/2022, 15:30
We study operators with large charge $j$ in the $d$-dimensional $O(N)$ model with long range interactions that decrease with the distance as $1/r^{d+s}$, where $s$ is a continuous parameter. We consider the double scaling limit of large $N$, large $j$ with $j/N=\hat{j}$ fixed, and identify the semiclassical saddle point that captures the two-point function of the large charge operators in this...
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Riccardo Rattazzi (EPFL)08/07/2022, 09:30
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Gil Badel (EPFL)08/07/2022, 11:00
The Large Charge sector of Conformal Field Theory can generically be described through a semiclassical expansion around a superfluid background. Focussing on $U(1)$ invariant Wilson-Fisher fixed points, I will discuss the spectrum of spinning large charge operators. For sufficiently low spin these correspond to the phonon excitations of the superfluid state. I will describe the organization of...
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Eren Firat (EPFL)08/07/2022, 11:30
I will talk about charge and energy flux correlators in a Lorentzian CFT in the presence of a large U(1) charge n produced by an external excitation. This type of object is particularly interesting as it is very close to observables used in collider physics. Even considering a weakly coupled theory, the standard perturbative expansion breaks down at large λn, with λ the theory’s coupling. In...
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