Welcome address Room: Amphithéâtre Hermite

Jackiw-Teitelboim Quantum Gravity from First Principles

• Frank Ferrari (Université Libre de Bruxelles and International Solvay Institutes)

Room: Amphithéâtre Hermite

Emergent Gravity, hidden sectors and TT Deformations

• Elias Kiritsis (APC and University of Crete)

Room: Amphithéâtre Hermite We investigate emergent gravity extending the paradigm of the AdS/CFT correspondence. The emergent graviton is associated to the (dynamical) expectation value of the energy-momentum tensor. We derive the general effective description of such dynamics, and apply it to the case where a hidden theory generates gravity that is coupled to the Standard Model. In the linearized description, generically, such gravity is (effectively) massive with the presence of an extra scalar degree of freedom. The propagators of both the spin-two and spin-zero modes are positive and well defined. The associated emergent gravitational theory is a bi-gravity theory, as is (secretly) the case in holography. The background metric on which the QFTs are defined, plays the role of dark energy and the emergent theory has always as a solution the original background (flat) metric. In the case where the hidden theory is holographic, the overall description yields a higher-dimensional bulk theory coupled to a brane. The effective graviton on the brane has four-dimensional characteristics both in the UV and IR and is always massive. The setup realizes the self-tuning mechanism of the cosmological constant.

Thermodynamics and conformal operators of the Sachdev-Ye-Kitaev model [IN REMOTE]

• Grigory Tarnopolsky

Room: Amphithéâtre Hermite Quantum mechanical models with random interactions have an infinite number of bilinear operators, the scaling dimensions of which can be computed explicitly in the large N limit. The lowest dimension operators play an important role in thermodynamical properties of these models and define the behavior of various correlation functions in the infrared limit. In this talk I’ll discuss effects of these operators on the SYK model free-energy and its numerical observation.

Group Invariant States as Quantum Many-Body Scars [IN REMOTE]

• Igor Klebanov

Room: Amphithéâtre Hermite

Holography of Information in AdS/CFT

• Robert de Mello Koch

Room: Amphithéâtre Hermite The principle of the holography of information states that in a theory of quantum gravity a copy of all the information available on a Cauchy slice is also available near the boundary of the Cauchy slice. This redundancy in the theory is already present at low energy. In the context of the AdS/CFT correspondence, this principle can be translated into a statement about the dual conformal field theory. We carry out this translation and demonstrate that the principle of the holography of information holds in the setting of the duality between the free O(N) vector model and higher spin gravity.

Higher-spin gravity in two dimensions

• Xavier Bekaert (Université de Tours)

Room: Amphithéâtre Hermite A non-abelian higher-spin theory in two dimensions is proposed, describing an infinite multiplet of massive scalar fields, with fine-tuned masses, interacting with infinitely many topological gauge fields together with their dilaton-like partners. The corresponding action functional is of BF-type and generalizes the known higher-spin extension of Jackiw-Teitelboim gravity. Finally, we discuss the holographic CFT1 duals of the kinematical structures identified in the AdS2 bulk.

From JT to 3d pure gravity

• Thomas Mertens (Ghent University)

Room: Amphithéâtre Hermite Taking inspiration from our understanding of 2d JT gravity, we develop aspects of 3d pure gravity. In particular, we propose an effective model of 3d pure gravity and discuss its factorization across entangling surfaces. Finally, we highlight some differences between gravity in its metric formulation and its first order gauge theoretic formulation, focussing on the underlying algebraic structure. Largely based on arXiv:2210.14196 and the earlier JT story in arXiv:1812.00918.

Differential Equations for the Distribution of Ground States in JT gravity [IN REMOTE]

• Clifford Johnson

Room: Amphithéâtre Hermite

Old and new on the O(N)^3 tensor field theory

• Razvan Gurau

Room: Amphithéâtre Hermite The O(N)^3 model is one of the most studied tensor field theories with numerous interesting regimes and non trivial features. Its interest resides in the promise that one can use it as a playground for studying strongly interacting field theories. In this talk I will present a personal selection of (old, new and brand new) results on this model.

Double scaling limits of various tensor models (the O(N)^3-invariant tensor model and a couple more)

• Adrian Tanasa (Univ. Bordeaux)

Room: Amphithéâtre Hermite One of the most celebrated tools in the study of matrix models is the double scaling limit mechanism (known to be related to the continuuos limit of these models). In this talk I will first exhibit the implementation of the double scaling limit mechanism for various quartic tensor models, such as the multi-orientable tensor model and the O(N)³-invariant tensor model. In the last part of the talk I will present how this approach generalizes for a sextic tensor model, the so-called prismatic tensor model.

Knot, matrix and tensor models...melon or meron?

• Shinobu Hikami (OIST)

Room: Amphithéâtre Hermite The Gaussian mean of $N\times N$ Hermitian matrix provides a knot configuration in the replica limit N to 0 (arXiv:2301.06003). The classical knot is related to Chern-Simons gauge theory, which shows two edges of Seifert surface are bounded, similar to two merons bounded into instanton. Higher dimensional knot (2-knot) consists of double Chern-Simons gauge field, which leads to Regge 6-j symbols tensor model for 3d gravity. We discuss the relation between the intersection numbers of p-spin curves and the quantum knots. The 4 dimensional Chern-Simons N=2 Yang Mills has an instanton, described by Nekrasov integral, which is akin to the replica formula for the intersection theory.

Effective low-temperature holographic theories

• Blaise Goutéraux (Ecole Polytechnique)

Room: Amphithéâtre Hermite Gauge/gravity duality allows us to construct exact renormalization group flows (sometimes only numerically) by turning on relevant deformations of ultraviolet conformal field theories with a gravitational dual. However, identifying the corresponding effective degrees of freedom at low temperatures and writing down an effective theory for them remains a non-trivial task. I will describe recent progress in this direction on RG flows with emergent Lorentz invariance, and finish with some comments on how this could shed light on the case of spacetimes with an emergent AdS2 factor, which are dual to higher-dimensional extensions of the SYK model.

An application of melonic CFTs: The F-theorem

• Sabine Harribey (CPHT Ecole Polytechnique - Heidelberg University)

Room: Amphithéâtre Hermite According to the F-theorem, the free energy on the sphere for a three-dimensional CFT decreases along the renormalization group flow. I will present here a generalization of this theorem to the long-range bosonic O(N)^3 tensor model. This model is a melonic CFT which displays four lines of fixed points at large N, parametrized by a purely imaginary coupling. It was non-trivial to show that the F-theorem is satisfied by this model as it was proven for unitary CFTs while the long-range O(N)^3 model presents only hints of unitarity at large N. In the first part of the talk, I will explain how to put a CFT on the sphere and will present a simple example via a flow between two gaussian CFTs. In the second part of the talk, I will quickly review the key features of the long-range O(N)^3 model and then show that it indeed satisfies the F-theorem. As an added bonus, we show how an infinite series of ladder diagrams can be resumed using conformal partial wave expansion.

SYK and turbulence [IN REMOTE]

• Vladimir Rosenhaus

Room: Amphithéâtre Hermite

Partition algebras and large N permutation symmetry in matrix quantum mechanics

• Sanjaye Ramgoolam

Room: Amphithéâtre Hermite Algebraic techniques based on Schur-Weyl duality have played an important role in the combinatorics of observables and correlators in single and multi-matrix models, of relevance to the AdS/CFT holographic dictionary. These techniques have recently been applied to study the implications of manifest permutation symmetry, for the state space and dynamics of quantum mechanical systems of matrices of general size N. The results include a solvable 11-parameter generalisation of the standard matrix harmonic oscillator. The permutation invariant sector of the Hilbert space, for general Hamiltonians, can be described using partition algebra diagrams forming the bases of a tower of partition algebras Pk(N). The integer k is interpreted as the degree of matrix oscillator polynomials in the quantum mechanics. Algebraic Hamiltonians with large ground state degeneracies can be engineered using the partition algebras. Models of quantum many-body scars are also constructed in this framework. The talk will be based on the paper https://arxiv.org/abs/2207.02166

Random Tensors, Loop Vertex Expansion and Their Cumulants

• Vincent Rivasseau (Université Paris-Saclay)

Room: Amphithéâtre Hermite In the first part of my talk I shall present some generalities about random tensor models in relation with quantum gravity. In the second part I introduce the loop vertex expansion which is a technique of constructive field theory. In the third part I construct cumulants of a $U(N)$ vector model perturbed by a quartic term. This model has a non-trivial covariance to allow for renormalisation, but is one the simplest models one could think of, because its renormalization is limited to tadpoles. Nevertheless it requires a different technique, the multi-scale loop vertex expansion, and for cumulants it has never been done. I prove their Borel summability in a cardioid of the associated coupling constant.