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The Avogadro Meetings started in 2005 as an occasion for young Italian theoretical physicists to share their ideas and results in an informal atmosphere. The meeting is named after the University of Piemonte Orientale that hosted its first three editions.
The meeting is traditionally scheduled just before the Christmas break to facilitate the participation of Italian postdocs and PhD students working abroad who can take the chance of their travel back home for Christmas to meet young colleagues and exchange ideas.
In order to stress the pedagogical aim of the meeting, preference is given to extended presentations on general themes rather than to conventional seminars on specific works, possibly organised and illustrated by more than one speaker and followed by a long discussion session.
Consistently with the original spirit of the event, the invited speakers are usually Italian. However participation is open to anybody and non-Italians are more than welcome to join. For this reason the seminars are presented in English.
A large class of 3d SCFTs can be engineered inserting a local SL(2,Z) duality wall into the Type IIB brane system leading to the so called S-fold SCFTs. These theories are intrinsically non Lagrangian, due to the gauging of the global symmetries of a
Infra-red dualities for supersymmetric quantum field theories and their dimensional reductions can be effectively investigated using supersymmetric localization. With this technique we can compute exactly some protected quantities, like partitions functions e superconformal indices, that don't depend on the gauge coupling and should thus match between the dual theories. Morover, it allowed us to discover interesting correspondences, such as gauge/CFT correspondeces. I will discuss a particular relation of this kind, between
My name is Ayoub Mounim. I am a Phd student in Naples and I am currently working on Holographic complexity.
The idea is that this should be a new entry in the holographic dictionary. In the bulk side we define a new gravitational observable given by the value of the on-shell action computed in a bounded subregion of Ads space known as "Wheeler-DeWitt patch". This particular region is bounded by null boundaries and this brings some subtleties in the calculations. This quantity is then conjectured to be the holographic dual of the "complexity" of the corresponding quantum field theory state that lives on the boundary of the space. What do we mean by complexity of a quantum field theory is still to be defined. We know how to define the computational complexity of a quantum state form quantum information theory, what we are doing is trying to adapt this concept to quantum field theories and better explore this conjecture.
I will explore the interplay between warped throats and some recently proposed quantum gravity conjectures, namely the Weak Gravity Conjecture (WGC) and the Distance Conjecture (DC). Motivated by the properties of systems of fractional branes at singularities, I will argue for a local version of the AdS-WGC, forbidding stable non supersymmetric Anti-de Sitter vacua, to large classes of locally AdS warped throats with supersymmetry breaking ingredients, and I will discuss some instability mechanisms in detail. Finally, I will show that warped throats of the Klebanov-Strassler (KS) kind describe fully backreacted solutions of transplanckiam axion monodromy, where the axion traverses arbitrarily large distances in field space, and comment upon the relation with the DC.
In this paper, we demonstrate that not only the heat kernel techniques are useful for the computation of the parity anomaly, but also the parity anomaly turns out to be a powerful mean in studying the heat kernel. We show that the gravitational parity anomaly on 4D manifolds with boundaries can be calculated using the general structure of the heat kernel coefficient a5 for mixed boundary conditions, keeping all the weights of various geometric invariants as unknown numbers. The symmetry properties of the η-invariant allow to fix all the relevant unknowns. As a byproduct of this calculation we get an efficient and independent crosscheck (and confirmation) of the correction of the general structure of a5 for mixed boundary conditions.
Following the paper called Discrete Symmetries in Dimer Diagrams, we apply dimer diagram techniques to uncover discrete global symmetries in the fields theories on D3-branes at singularities given by general orbifolds of general toric Calabi-Yau threefold singularities. The discrete symmetries are discrete Heisenberg groups, with two generators A,B with commutation AB=BAC, with C a central element. These generators depend on the abelian orbifold. This fully generalizes observations in particular orbifolds of the flat space, the conifold and other toric Sasaki-Einstein manifolds. The generator A is realized as a shift in the dimer diagram, associated to the orbifold quantum symmetry; the action of B is determined by equations describing a 1-form in the dimer graph in the unit cell of the parent theory with twisted boundary conditions; finally, C is an element of the (mesonic and baryonic) non-anomalous U(1) symmetries, determined by geometric identities involving the elements of the dimer graph of the parent theory. These discrete global symmetries of the quiver gauge theories are holographically dual to discrete gauge symmetries from torsion cycles in the horizon. Our findings allow to easily construct the discrete symmetries for infinite classes of orbifolds.
In recent years the idea of bosonic ultralight CDM (also called fuzzy dark matter, FDM) has been proposed, in one of its prominent versions it states that DM is made of ultralight axion-like particles that form halos as Bose-Einstein condensates. In this theory each axionic particle can develop structures on de Broglie scale thanks to gravitational effects. A prominent soliton, i.e. a state where self-gravity is balanced by the effective pressure arising from the uncertainty principle, develops at the center of every bound halo. The extremely high value of the decay constant together with the possible multiple axionic nature of FDM have been claimed to be a possible sign in favour of the string axiverse, where a plenitude of axion like particle naturally arise in 4D effective theory. I will point out that obtaining a fuzzy dark matter axion with the correct mass and decay constant is a big challenge for string theory, being also its existence in contrast with WGC .
Machine learning has revolutionized most fields it has penetrated, and the range of its applications is growing rapidly. The last years has seen efforts towards bringing the tools of machine learning to lattice QFT and to string theory. After giving a general idea of what is machine learning, I will present two recent results on lattice QFT: 1) computing the Casimir energy for a 3d QFT with arbitrary Dirichlet boundary conditions, 2) predicting the critical temperature of the confinement phase transition in 2+1 QED at different lattice sizes.
In recent progress in second quantization of the RNS string a crucial role is played by line integral Picture Changing Operators (PCO) which avoid the singularities associated with local PCOs.
We show how this approach can be generalized to a "democratic" theory involving vertices with arbitrary picture number. The usual cohomology problem in the Large Hilber Space can then be reformulated in terms of a dual problem with a two parameters gauge symmetry. The interactions then emerge in a way analogous to Berkovits' picture zero NS theory and do not exhibit an explicit
Asymptotic symmetries at null infinity do not seem to play a fundamental role in higher dimensions: in constrast with the four-dimensional case, in
We investigate this issue studying memory effects associated to Abelian and non-Abelian radiation getting to null infinity, in arbitrary even spacetime dimensions. Together with classical memories, linear and non-linear, given by permanent kicks in the velocity of probe particles, we also discuss the higher-dimensional counterparts of quantum memory effects, manifesting themselves in modifications of the relative phases describing a configuration of several probes.
Adopting the Lorenz gauge, we illustrate how one can interpret such memory effects as the action of suitable residual symmetries acting near null infinity and propose a strategy for defining infinite-dimensional asymptotic symmetries of Maxwell’s theory in any dimension, eiher even and odd.
After the atomic classification of 6d (1,0) SCFTs, one important question is how to compute the elliptic genera and refined BPS invariants of all such theories. In a series of papers, we develop the elliptic blowup equations to answer this question universally. Such equations can be regarded as an elliptic version of Gottsche-Nakajima-Yoshioka's K-theoretic blowup equations. I will focus on the rank one (1,0) SCFTs with matters and show how blowup equations determine the elliptic genera and refined BPS invariants.
We show a new method to compute the correlator of an arbitrary number of (excited) spin fields based on a time dependent defect CFT procedure, with the possibility to extend it to (excited) twist fields, both in the Abelian and non Abelian cases.
We consider two-dimensional fermions in the presence of point-like defects in the time-like direction corresponding to spin fields which provide non trivial boundary conditions. We solve them and the equations of motion to define a basis of modes in the Euclidean formulation. We compute the algebra of creation and annihilation operators necessary to build the Fock space in the presence of defects. With the definition of the in-vacuum, we then compute the contractions of the fields and the stress-energy tensor which shows that we are indeed considering a CFT, notwithstanding the time dependent defects. We then proceed to build the Hermitian conjugate vacuum in order to compute the correlators of the spin fields.
Higher algebraic structures are ubiquitous in fundamental physics. For instance,
The famous paper [1] by Kawai, Lewellen and Tye (KLT) showed that
We analytically compute subsystem action complexity for a segment in the BTZ black hole background up to the finite term, and we find that it is equal to the sum of a linearly divergent term proportional to the size of the subregion and of a term proportional to the entanglement entropy. This elegant structure does not survive to more complicated geometries: in the case of a two segments subregion in AdS_3, complexity has additional finite contributions. We give analytic results for the mutual action complexity of a two segments subregion.
Numerical Worldline (WL) Monte Carlo (MC) techniques for particle path integrals in flat spacetimes have been deeply developed in order to extract physical information from QFT systems. It is however possible to extend such procedures to the case of (Euclidean) curved spaces, where the proper-time discretization of a bosonic worldline point-particle is treated similarly to a time-slicing regularization for the associated quantum path integral. In particular, it induces a well-known counterterm in the theory which, together with curvature effects arising directly from the curved metric tensor, plays the role of an additional potential. To test the setup, the numerical evaluation of the heat kernel of a free scalar point-particle on a 4-hyperboloid is presented; such system was already studied analytically, and the expressions of the associated effective potential and of the metric tensor were provided in closed form. The curved space problem was turned into a flat space one, allowing for a direct comparison between WLMC techniques in curved (the test) and in flat (the check) space.
We investigate the production of hidden sector Dark Matter (DM) in type IIB LVS scenarios. We study the possibility of Moduli fields playing the role of a portal during the production. By matching the observed DM abundance we make predictions for the masses of different DM types.
Starting with a general string field theory action which possesses an
We look at the geometric structure of the Higgs branch of supersymmetric gauge theories with 8 supercharges in various dimensions. In particular, the partial ordering between different subspaces of the Higgs branch which can be neatly encoded in a diagram called a Hasse diagram. Recent introduction of magnetic quivers allows a very efficient construction of such diagrams, giving consistent (and more) information compared to the traditional method of partial Higgsing.