Abstract: This is a general introductory talk to the theory of sums and (stable) intersections of Cantor sets: the notion of thickness, Newhouse gap lemma, and a subset of Hall's ray in Lagrange/Markov spectra as an application to the number theory.
The talk will be devoted to the construction of a C^1-version of the Denjoy example that is still exactly affine on the intervals of the complement to the minimal set. This is our recent work with Andrés Navas.
In classical (i.e., IID) random matrix dynamics, a question that arises frequently is whether the Lyapunov spectrum is "simple." There are several criteria that imply the existence of a maximal number of distinct Lyapunov exponents for random matrix products and these have been used in various applications. Recently, there have been papers extending this classical theory to specific classes of non-stationary matrix products. In this talk, we will discuss two recent papers ([arXiv:2312.03181] and [arXiv.2507.04058]) which establish gaps between non-stationary analogs of Lyapunov exponents. Strategies and key ideas will be presented, with a brief discussion about applications to Anderson localization.
Abstract: Measure-theoretical and topological entropy play a central role in structural questions for dynamical systems and serve as crucial tools in detecting chaoticity of a system. However, entropy is positive if and only if the system has exponential growth of distinguishable orbit types and it does not provide any information for systems with slower orbit growth. To measure the complexity of systems with subexponential orbit growth several different invariants have been studied. For instance, Anatole Katok and Jean-Paul Thouvenot introduced the concept of slow entropy. In this talk we discuss flexibility results on the values of measure-theoretical slow entropy for rigid transformations and finite-rank systems.
Abstract: The Anderson model has been a key tool in the study of disordered alloys and their transport properties. In the one-dimensional discrete model, it is known that any amount of randomness leads to "localization," or a lack of electron transport. Comprehensive results in higher dimensions have been elusive in part due to the loss of one-dimensional tools. As a transitional step to higher dimensions, we consider the quasi-one-dimensional Anderson model on the strip. In this talk, we will discuss existing work to prove spectral localization (with exponentially decaying eigenfunctions) for this class of Anderson model. We will also explore how to extend localization results for IID potentials to potentials that are independent but non-stationary.
Motivated by the spectral analysis of Sturmian Hamiltonians, we investigate their underlying dynamical systems. This class of subshifts admits a natural extension to a larger family parameterized by the unit interval. In this talk, we study continuity properties of this parametrization with respect to the Hausdorff distance. Starting from the well known fact that these discontinuities arise at rational parameters only, we will pass to a non-Euclidean metric in order to characterize limits at rational parameters. If time permits we briefly discuss immediate implications for Sturmian Hamiltonians.
This talk is based on a joint work with Siegfried Beckus and Jean Bellissard.
Abstract: When a spatially homogeneous state destabilizes, localized perturbations can grow into large amplitude spatial patterns, which spread into the bulk, invading the unstable state. The nature and properties of the patterns which appear, such as wavelength, orientation, and amplitude, are frequently determined by the behavior in the leading edge of the spreading process. We consider such pattern-forming fronts in the FitzHugh–Nagumo PDE in the so-called oscillatory regime. The pattern is selected from a family of periodic traveling wave train solutions by an invasion front. Using geometric singular perturbation techniques, we construct “pushed” and “pulled” pattern-forming fronts as heteroclinic orbits between the unstable steady state and a periodic orbit representing the wave train in the wake. In the case of pushed fronts, the wave train necessarily passes near a pair of nonhyperbolic fold points on the associated critical manifold. We also discuss implications for the stability of the pattern-forming fronts and the challenges introduced by the fold points in the corresponding spectral stability problem.