Théorie

Core-collapse supernovae host the densest neutrino environments in the Universe. In these extreme conditions, neutrinos exchange flavor with each other more rapidly than they stream out of the star, forming a collective many-body system whose dynamics are dominated by weak interactions. In this talk, I will present a unified theoretical framework showing that this system behaves as a neutrino plasma, supporting collective flavor-wave excitations—flavomons—that are the exact analogs of collective electromagnetic fields in ordinary plasmas. The stimulated emission of flavomons produces an instability, with consequent restructuring of the neutrino flavor distribution which impacts the supernova explosion and multi-messenger signature. I will show that the conditions for triggering these instabilities naturally descend from detailed balanc of neutrino-flavomon interactions. By this approach, I will show that the accretion-powered neutrino outflow of supernovae generically develops neutrino-mass-induced instabilities immediately after the neutronization burst.
High-energy physics often motivates multi-field inflationary scenarios where stochastic effects play a crucial role. Peculiar to multi-field models, the noise-induced centrifugal force results in a longer duration of inflation depending on the number of fields, even when the stochastic noises themselves are small. We show that, in such small-noise regimes, the number of fields generically discriminates whether inflation successfully terminates or lasts forever. Our results indicate that inflation with an extremely large number of fields may fail to realise our observable Universe.
I will present cuHARM, a general relativistic radiation magnetohydrodynamic solver optimized to exploit exascale computing facilities. After describing the core numerical strategies enabling efficient calculation for multi-node and multi-GPU architectures, I will discuss how radiative cooling changes the dynamics of magnetically arrested accretion disks. In the second part of the talk, I will detail how radiation and its feedback on the dynamics are modeled. In cuHARM, the specific intensity is discretized in space and momentum, and is evolved through the solution of the radiative transfer equation via the discrete ordinate method. This approach eliminates the need for a closure relation and enables to resolve the anisotropy of the specific intensity. Finally, I will present the first results obtained for a radiative accretion disk operating at 0.1 times the Eddington luminosity.
Almost four decades have passed since the generalization of vacuum Kerr solutions to higher dimensions in the form of Myers-Perry black holes, yet an exact solution generalizing their charged extension (Kerr-Newman) to higher dimensions remains unknown in Einstein-Maxwell theory. Likewise, an exact solution for charged multi-NUT spacetimes in higher dimensions is still missing. In the first part of my talk, considering the Kerr-Schild class in Einstein-Maxwell theory, I will discuss a "No-Go" result related to the charging of Myers-Perry black holes that we obtained in arXiv:2309.02900. In the second part, I will present a slightly stronger generalization of this "No-Go" result in the context of generalized Kerr-Schild spacetimes, which also addresses the charging of multi-NUT solutions. Time permitting, I will further discuss some of the different classes of solutions identified in our analyses.

The Standard Model Higgs can be the inflaton, providing an attractively economical scenario. The core idea is simple, but there are complications both on the side of quantum corrections and gravity. I will discuss possibilities and problems due to such complications. In particular I will cover how the predictions of Higgs inflation depend on what is the correct formulation of general relativity: metric, Palatini or something else.

Understanding the complex transport of particles in turbulent plasmas is of great relevance in various fields. In astrophysics, the diffusive transport of high-energy particles is often described in an ensemble-averaged way, employing a transport equation that describes the time evolution of the particles distribution function in space and momentum. The standard transport equation can also be re-written into a set of stochastic differential equation.

Warm Inflation is a variant inflationary scenario where the inflaton field continuously dissipates its energy to a subdominant radiation bath during inflation. Among the many advantages that WI has over its more standard counterpart, which we will refer to as Cold Inflation, is that WI smoothly transits to a radiation dominated Universe post inflation without invoking the need of a reheating phase, dynamics of which is still quite unknown. The dissipation effects effective during Warm Inflation makes the dynamics of the inflation quite intricate. Even the simple graceful exit in Cold Inflation turns out to be not so simple in Warm Inflation. In this talk, we will do the background analysis of Warm Inflation and shed light on how Warm Inflation ends or gracefully exits. These graceful exit criteria also constrain the form of the potential and the dissipative coefficients that one may choose for their Warm Inflationary model. Moreover, it indicates whether Warm Inflation can at all exit to a radiation dominated epoch or not.
Cosmological correlators encode the signatures of the universe's evolution, and by measuring correlations in the late universe we infer the dynamics and contents of the universe. I will review some recent developments in the study of the structure of quantum field theory in curved spacetimes, and the computation of cosmological correlators.