SymTFT for (3+1)d gapless SPTs and obstructions to confinement
Antinucci, A Copetti, C Schäfer-Nameki, S SciPost Physics volume 18 issue 3 114 (31 Mar 2025)
Predicting Treatment Outcomes from Adaptive Therapy — A New Mathematical Biomarker
Gallagher, K Strobl, M Maini, P Anderson, A
Quantitative convergence in relative entropy for a moderately interacting particle system on Rd
Chen, L Holzinger, A Huo, X Electronic Journal of Probability volume 30 issue none (01 Jan 2025)
Real-time inference of the end of an outbreak: Temporally aggregated disease incidence data and under-reporting
Ogi-Gittins, I Polonsky, J Keita, M Ahuka-Mundeke, S Hart, W Plank, M Lambert, B Hill, E Thompson, R Infectious Disease Modelling (01 Apr 2025)
Thu, 15 May 2025
12:00
C6

Recent progress on the inverse scattering theory for ideal Alfvén waves

Mengni Li
(Southeast University, Nanjing)
Abstract

The Alfvén waves are fundamental wave phenomena in magnetized plasmas. Mathematically, the dynamics of Alfvén waves are governed by a system of nonlinear partial differential equations called the magnetohydrodynamics (MHD) equations. Let us introduce some recent results about inverse scattering of Alfvén waves in ideal MHD, which are intended to establish the relationship between Alfvén waves emanating from the plasma and their scattering fields at infinities.The proof is mainly based on the weighted energy estimates. Moreover, the null structure inherent in MHD equations is thoroughly examined, especially when we estimate the pressure term.

Thu, 22 May 2025
12:00
C6

Homogenisation for compressible fluids

Pierre Gonin-Joubert
(Université Claude Bernard Lyon 1)
Abstract

Several physical models are available to understand the dynamics of fluid mixtures, including the so-called Baer-Nunziato models. The partial differential equations associated with these models look like those of Navier-Stokes, with the addition of new relaxation terms. One strategy to obtain these models is homogenisation: starting from a mesoscopic mixture, where two pure fluids satisfying the compressible Navier-Stokes equations share the space between them, a change of scale is performed to obtain a macroscopic mixture, where the two fluids can coexist at any point in space.

This problem concerns the study of the Navier-Stokes equations with strongly oscillating initial data. We'll start by explaining some results in this framework, in one dimension of space and on the torus, for barotropic fluids. We will then detail the various steps involved in demonstrating homogenisation. Finally, we'll explain how to adapt this reasoning to homogenisation for perfect gases, with and without heat conduction.

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