February 23 - 27, 2026 HSM Special Topic School
Europe/Berlin timezone

Scientific Program

Minicourses

Andrea Braides
University of Tor Vergata
Gamma-convergence and non-local Functionals
One of De Giorgi's first observations on Gamma-convergence is that local integral functionals are a stable class under some very general polynomial growth conditions on the integrands. This is not the case for classes of nonlocal functionals, even for simple energies given by double integrals. We will analyze some problems, often set in fractional Sobolev spaces, in which the usual theories of homogenization, dimensional reduction, phase transitions, approximation of free discontinuity problems, discretization, etc., exhibit unexpected behaviors and pose new challenges.

Irene Fonseca
Carnegie Mellon University
Phase Transitions of Heterogeneous Materials and Stochastic Homogenization in the $ \mathcal{A} $-Free Setting
{In this series of lectures, using the notion of $ \Gamma $-convergence as introduced by De Giorgi in 1975 we derive a variational model for phase transitions between two uids as an asymptotic limit of a family of Cahn-Hilliard energies (also known as the Modica-Mortola functional, in the mathematical community). We will then consider a variational model for the interaction between homogenization and phase separation when small scale heterogeneities are present in the uids. Three regimes will be considered: when the phase separation occurs at the same scale as the homogenization, when the latter is faster than the former (the supercritical case), and when homogenization is faster than the phase transition (the subcritial case).

As time will permit, we will address a compactness result for $ \Gamma $-convergence of integral functionals de ned on $ \mathcal{A} $-free elds, leading to a theory of homogenization without periodicity assumptions that extends the "classical" context of energies depending on gradients, and ultimately this is used to study stochastic homogenization in the $ \mathcal{A} $-free setting.

Carolin Kreisbeck
KU Eichstätt-Ingolstadt
Nonlocal Gradients in Variational Problems - and How to Deal with Them
Motivated by new nonlocal models in hyperelasticity, this mini-course will explore a class of variational problems with integral functionals that depend on fractional and nonlocal gradients. After introducing these non-classical derivative operators, along with their basic properties and their associated Sobolev-type function spaces, we will discuss various aspects of the existence theory for such nonlocal problems and analyze their asymptotic behavior. In particular, we will address the tasks of identifying the appropriate notion of convexity for these problems, deriving new relaxation and homogenization results, and establishing localization limits, which provide a rigorous bridge between nonlocal and classical variational theories. An important ingredient in our analysis is the use of suitable translation operators, which enable us to pass between nonlocal and classical gradients and thus serve as effective technical tools for transferring results from one framework to the other.
Further topics to touch on include the characterization of functions with zero nonlocal gradients and nonlocal Neumann problems, heterogeneous nonlocal gradients with varying horizons and local boundary conditions, as well as rigorous linearization of models in nonlocal hyperelasticity.

These lectures are based mainly on a series of recent works with Hidde Schönberger (UCLouvain) and Javier Cueto (Universidad Autónoma de Madrid), and on ongoing joint work with Carlos Mora-Corral (Universidad Autónoma de Madrid), Felix Seifert (KU Eichstätt-Ingolstadt).

Xavier Lamy
University of Toulouse
Around the Aviles-Giga Conjecture
The Aviles-Giga energy is a phase transition model for gradient fields in two dimensions. It involves approximations of weak solutions to the eikonal equation $|\nabla u|=1$. These approximations are assigned an energy cost depending on a transition scale $\epsilon\to 0$. At main order, the energy is conjectured to concentrate on the one-dimensional jump set of $\nabla u$. A major difficulty is to understand the structure of the non-standard class of weak solutions (to the eikonal
equation) selected by these approximations. In this minicourse, I will describe some of the ideas and methods generated by this open problem over the last three decades.

Talks

André Guerra
University of Cambridge
Differential Inclusions, the Monge-Ampère equation, and Morse Theory
I will begin by giving a brief overview of rigidity and flexibility results in the theory of differential inclusions, a prime example being isometric embeddings. In two dimensions, the rigidity/flexibility of isometric embeddings is closely related to rigidity/flexibility of non-convex solutions to the Monge-Ampère equation. I will then discuss a recent result, obtained with R. Tione, which gives a complete rigidity/flexibility result for solutions of the Monge-Ampère equation in general dimension, as conjectured by Šverák in 1992. The proof relies on Morse theory for non-smooth functions.

Leonard Kreutz
Technical University of Munich
Geomtric Rigidity in Variable Domains and Applications in Dimension Reduction
In this talk we present a quantitative geometric rigidity estimate in dimensions $\textit{d} $=$ 2,3$ generalising a celebrated result by Friesecke, James and Müller to the setting of variable domains. Loosely speaking, we show that for each function $\textit{y} \in \textit{H} ^{1} (\mathbf{U};\mathbb{R} ^{3})$ and for each connected component of an open bounded set $\mathbf{U} \subset \mathbb{R}^{\textit{d}} $, the $\textit{L}^{2}$-distance of $ \nabla\textit{y}$ from a single rotation can be controlled up to a constant by its $\textit{L}^{2}$-distance from the group $\textit{SO(d)}$, with the constant not depending on the precise shape of $\mathbf{U}$, but only on an integral curvature functional related to $\partial\mathbf{U}$. We fruther show that for linear strains the estimate can be refined, leading to a uniform control independent of the $\mathbf{U}$. The estimate can be used to establish compactness in the space of generalized special funcions of bounded deformation (GSBD) for sequences of displacements related to deformations with uniformly bounded elastic energy. We show how this estimate can be applied in the context of dimension reduction by calculating the $\Gamma$-limits for thin elastic solids containing voids in different energy scaling regimes in terms of their thickness. This is seminar based on joint work on with Manuel Friedrich (Johannes Kepler Universität Linz) and Konstantinos Zemas (Universität Bonn).

Anna Skorobogatova
ETH Zürich
Non-uniqueness of Locally Minimizing Clusters via Sinuglar Cones
We study a variant of the multiple bubble problem in $\mathbb{R}^n$ with more than one infinite-volume chamber. Unlike the classical multiple bubble problem, this variant of the problem is global in nature, and crucially relies on understanding the geometry of the cluster at infinity. We provide an explicitly computable criterion that guarantees the existence of local minimizers with one finite-volume chamber and two infinite-volume chambers whose interface has a blowdown that is a singular minimizing cone. We verify that this criterion holds for a large number of dimensions $n\geq 8$, which in particular guarantees non-uniqueness of such local minimizers in such dimensions, in contrast to the case $n\leq 7$ which was settled by Bronsard and Novack. This is joint work with Lia Bronsard, Robin Neumayer and Mike Novack.

  • Hausdorff School: "Modern Methods in the Calculus of Variations"